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		<updated>2012-05-18T11:00:20Z</updated>
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	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Dynamical_density-functional_theory</id>
		<title>Dynamical density-functional theory</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Dynamical_density-functional_theory"/>
				<updated>2012-02-27T20:40:20Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Created page with &amp;quot;'''Dynamical Density functional theory''' is a set of theories in statistical mechanics that extends  Density functional theory ...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Dynamical Density functional theory''' is a set of theories in [[statistical mechanics]] that&lt;br /&gt;
extends [[equilibrium density functional theory | Density functional theory]] to&lt;br /&gt;
situations away from equilibrium. In the simplest case, only small deviations from equilibrium are&lt;br /&gt;
considered, so that linear response theory can be applied.&lt;br /&gt;
&lt;br /&gt;
A simple approach in this line is to consider this evolution of the density field:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{\partial\rho}{\partial t}=  - \mu \frac{\delta A}{\delta\rho}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In equilibrium, the left hand side vanishes and we are left with the usual density functional&lt;br /&gt;
expression. Away from it, an increase in the free energy ''A'' causes&lt;br /&gt;
a decrease in the density, mediated by the mobility coefficient &amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
This sort of evolution will not satisfy conservation of the number of particles&lt;br /&gt;
(that is, the space integral of the density field), and is therefore termed ''non-conserved dynamics''. This can be valid in cases in which this field is in fact not conserved, such as the magnetization field in a model for magnets (such as the [[Ising model]]).&lt;br /&gt;
&lt;br /&gt;
In other cases, for example with actual particles,&lt;br /&gt;
some evolution has to be postulated. For example, this evolution will conserve&lt;br /&gt;
the number of particles:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{\partial\rho}{\partial t}=  - \nabla \mu \nabla \frac{\delta A}{\delta\rho}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The later sort of expressions are called ''non-conserved dynamics''.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Brownian dynamics]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Interesting reading==&lt;br /&gt;
*[http://dx.doi.org/10.1088/0953-8984/12/8A/356 Umberto Marini Bettolo Marconi and Pedro Tarazona &amp;quot;Dynamic density functional theory of fluids&amp;quot;,  J. Phys.: Condens. Matter '''12''' A413(2000)]&lt;br /&gt;
&lt;br /&gt;
[[category: Density-functional theory]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Cole_equation_of_state</id>
		<title>Cole equation of state</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Cole_equation_of_state"/>
				<updated>2011-08-23T13:52:27Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: New eos&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The '''Cole equation of state''' &amp;lt;ref&amp;gt;R.H. Cole, Underwater Explosions. Princeton University Press 1948&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;&lt;br /&gt;
G.K. Batchelor, An introduction to ﬂuid mechanics. Cambridge University Press 1974 &amp;lt;/ref&amp;gt;&lt;br /&gt;
can be written, when atmospheric pressure is negligible, has the form&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;p = B \left[ \left( \frac{\rho}{\rho_0} \right)^\gamma  -1 \right]&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
In it, &amp;lt;math&amp;gt;\rho_0&amp;lt;/math&amp;gt; is a reference density around which the density varies&lt;br /&gt;
&amp;lt;math&amp;gt;\gamma&amp;lt;/math&amp;gt; is an exponent  and &amp;lt;math&amp;gt;B&amp;lt;/math&amp;gt; is a pressure parameter.&lt;br /&gt;
&lt;br /&gt;
Usually, the equation is used to model a nearly incompressible system. In this case,&lt;br /&gt;
the exponent is often set to a value of 7, and &amp;lt;math&amp;gt;B&amp;lt;/math&amp;gt; is large, in the following&lt;br /&gt;
sense. The fluctuations of the density are related to the speed of sound as&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\delta \rho}{\rho} = \frac{v^2}{c^2} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;v&amp;lt;/math&amp;gt; is the largest velocity, and &amp;lt;math&amp;gt;c&amp;lt;/math&amp;gt; is the speed of&lt;br /&gt;
sound (the ratio &amp;lt;math&amp;gt;v/c&amp;lt;/math&amp;gt; is [[Mach's number]]). The speed of sound can&lt;br /&gt;
be seen to be&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;c^2 = \frac{\gamma B}{\rho_0}. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Therefore, if &amp;lt;math&amp;gt;B=100 \rho_0 v^2 / \gamma&amp;lt;/math&amp;gt;, the relative density fluctuations&lt;br /&gt;
will be of about 0.01.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[category: equations of state]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Equations_of_state</id>
		<title>Equations of state</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Equations_of_state"/>
				<updated>2011-08-23T13:37:59Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added Cole&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Equations of state''' are generally expressions that relate the macroscopic observables, or ''state variables'', such as  [[pressure]], &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt;, volume, &amp;lt;math&amp;gt;V&amp;lt;/math&amp;gt;, and [[temperature]], &amp;lt;math&amp;gt;T&amp;lt;/math&amp;gt;. &lt;br /&gt;
==General==&lt;br /&gt;
*[[Common bulk modulus point]]&lt;br /&gt;
*[[Law of corresponding states]]&lt;br /&gt;
*[[Linear isothermal regularity]]&lt;br /&gt;
*[[Maxwell's equal area construction]]&lt;br /&gt;
*[[Tait-Murnaghan relation]]&lt;br /&gt;
*[[Zeno line]]&lt;br /&gt;
&lt;br /&gt;
==Virial equations of state==&lt;br /&gt;
*[[Virial equation of state]]&lt;br /&gt;
*[[Second virial coefficient]]&lt;br /&gt;
*[[Virial coefficients of model systems]]&lt;br /&gt;
==Semi-empirical equations of state==&lt;br /&gt;
Naturally there is the [[Equation of State: Ideal Gas|ideal gas equation of state]]. However, one of the first steps towards a description of realistic substances was the famous [[van der Waals equation of state]]. Since then a plethora of semi-empirical equations have been developed, often in a similar vein to the van der Waals equation of state, each trying to better reproduce the foibles of the many &lt;br /&gt;
gasses and/or liquids that are often of industrial interest.&lt;br /&gt;
{{columns-list|3|&lt;br /&gt;
*[[Amagat equation of state | Amagat]]&lt;br /&gt;
*[[Antoine equation of state | Antoine]]&lt;br /&gt;
*[[Battelli equation of state |Battelli]]&lt;br /&gt;
*[[Beattie-Bridgeman equation of state | Beattie-Bridgeman]]&lt;br /&gt;
*[[Benedict, Webb and Rubin equation of state |Benedict, Webb and Rubin ]]&lt;br /&gt;
*[[Berthelot equation of state | Berthelot]]&lt;br /&gt;
*[[Boltzmann equation of state | Boltzmann]]&lt;br /&gt;
*[[Boynton and Bramley equation of state | Boynton and Bramley]]&lt;br /&gt;
*[[Brillouin equation of state | Brillouin]]&lt;br /&gt;
*[[Clausius equation of state | Clausius]]&lt;br /&gt;
*[[Cole equation of state | Cole]]&lt;br /&gt;
*[[Dieterici equation of state | Dieterici]]&lt;br /&gt;
*[[Dupré equation of state |Dupré]]&lt;br /&gt;
*[[Elliott, Suresh, and Donohue  equation of state |Elliott, Suresh, and Donohue]]&lt;br /&gt;
*[[Fouché equation of state | Fouché]]&lt;br /&gt;
*[[Goebel equation of state | Goebel]]&lt;br /&gt;
*[[Hirn equation of state |Hirn]]&lt;br /&gt;
*[[Jäger equation of state | Jäger]]&lt;br /&gt;
*[[Kam equation of state | Kam]]&lt;br /&gt;
*[[Lagrange equation of state | Lagrange]]&lt;br /&gt;
*[[Leduc equation of state | Leduc]]&lt;br /&gt;
*[[Linear isothermal regularity]]&lt;br /&gt;
*[[Lorentz equation of state |Lorenz]]&lt;br /&gt;
*[[Mie equation of state | Mie]] &lt;br /&gt;
*[[Murnaghan equation of state | Murnaghan]]&lt;br /&gt;
*[[Natanson equation of state | Natanson]]&lt;br /&gt;
*[[Onnes equation of state | Onnes]]&lt;br /&gt;
*[[Peczalski equation of state |Peczalski]]&lt;br /&gt;
*[[Peng and Robinson equation of state |Peng and Robinson]]&lt;br /&gt;
*[[Planck equation of state |Planck]]&lt;br /&gt;
*[[Porter equation of state | Porter]]&lt;br /&gt;
*[[Rankine equation of state |Rankine]]&lt;br /&gt;
*[[Recknagel equation of state | Recknagel]]&lt;br /&gt;
*[[Redlich-Kwong equation of state | Redlich-Kwong]]&lt;br /&gt;
*[[Reinganum equation of state | Reinganum]]&lt;br /&gt;
*[[Sarrau equation of state | Sarrau]]&lt;br /&gt;
*[[Schiller equation of state | Schiller]]&lt;br /&gt;
*[[Schrieber equation of state | Schrieber]]&lt;br /&gt;
*[[Smoluchowski equation of state | Smoluchowski]]&lt;br /&gt;
*[[Starkweather equation of state |Starkweather ]]&lt;br /&gt;
*[[Tait equation of state | Tait]]&lt;br /&gt;
*[[Thiesen equation of state |Thiesen]]&lt;br /&gt;
*[[Tumlirz equation of state | Tumlirz]]&lt;br /&gt;
*[[van der Waals equation of state | van der Waals]]&lt;br /&gt;
*[[Walter equation of state | Walter]]&lt;br /&gt;
*[[Wohl equation of state | Wohl]]&lt;br /&gt;
*[[Phase diagrams of water | Water equation of state]]&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
==Other methods==&lt;br /&gt;
*[[ASOG (Analytical Solution of Groups)]]&lt;br /&gt;
*[[UNIFAC (Universal Functional Activity Coefficient)]]&lt;br /&gt;
==Model systems==&lt;br /&gt;
Equations of state for [[idealised models]]:&lt;br /&gt;
*[[Equation of State: three-dimensional hard dumbbells | Three-dimensional hard dumbbells]]&lt;br /&gt;
*[[Equations of state for hard convex bodies| Hard convex bodies]] &lt;br /&gt;
*[[Equations of state for hard rods | Hard rods]]&lt;br /&gt;
*[[Equations of state for the Gaussian overlap model | Gaussian overlap model]]&lt;br /&gt;
*[[Equations of state for the square shoulder model | Square shoulder model]]&lt;br /&gt;
*[[Equations of state for the square well model | Square well model]]&lt;br /&gt;
*[[Equations of state for the triangular well model | Triangular well model]]&lt;br /&gt;
*[[Equations of state for hard spheres]]&lt;br /&gt;
*[[Equations of state for crystals of hard spheres]]&lt;br /&gt;
*[[Equations of state for hard sphere mixtures]]&lt;br /&gt;
*[[Equations of state for hard disks]]&lt;br /&gt;
*[[Hard ellipsoid equation of state]]&lt;br /&gt;
*[[Lennard-Jones equation of state]]&lt;br /&gt;
*[[Fused hard sphere chains#Equation of state | Fused hard sphere chains]]&lt;br /&gt;
*[[Tetrahedral hard sphere model#Equation of state|Tetrahedral hard sphere model]]&lt;br /&gt;
==Interesting reading==&lt;br /&gt;
*[http://dx.doi.org/10.1088/0034-4885/7/1/312 James A. Beattie and Walter H. Stockmayer &amp;quot;Equations of state&amp;quot;, Reports on Progress in Physics '''7''' pp. 195-229 (1940)]&lt;br /&gt;
*[http://dx.doi.org/10.1021/ie50663a005 K. K. Shah and G. Thodos &amp;quot;A Comparison of Equations of State&amp;quot;, Industrial &amp;amp; Engineering Chemistry '''57''' pp. 30-37 (1965)]&lt;br /&gt;
*[http://dx.doi.org/10.1088/0034-4885/28/1/306 J. S. Rowlinson &amp;quot;The equation of state of dense systems&amp;quot;, Reports on Progress in Physics '''28''' pp. 169-199  (1965)]&lt;br /&gt;
'''Books'''&lt;br /&gt;
*&amp;quot;Equations of State for Fluids and Fluid Mixtures&amp;quot;, Eds. J. V. Sengers, R. F. Kayser, C. J. Peters, and H. J. White Jr., Elsevier (2000) ISBN 0-444-50384-6&lt;br /&gt;
[[Category: Results]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Lees-Edwards_boundary_conditions</id>
		<title>Lees-Edwards boundary conditions</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Lees-Edwards_boundary_conditions"/>
				<updated>2011-03-10T20:40:03Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: cat. added&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;These conditions are an adaption of standard [[periodic boundary conditions]] to simulations of shear flow (Lees and Edwards, 1972). They are convenient for e.g. simulations of [[Couette flow]].&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
'''Related reading'''&lt;br /&gt;
*[http://epress.anu.edu.au/sm/html/ch06s03.html Couette Flow and Shear Viscosity], in  [http://epress.anu.edu.au/sm_citation.html Denis J. Evans and Gary P. Morriss &amp;quot;Statistical Mechanics of Nonequilibrium Liquids&amp;quot; ANU E Press (2007)]&lt;br /&gt;
[[category: Computer simulation techniques]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Lees-Edwards_boundary_conditions</id>
		<title>Lees-Edwards boundary conditions</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Lees-Edwards_boundary_conditions"/>
				<updated>2011-03-10T20:39:31Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Created page with &amp;quot;These conditions are an adaption of standard periodic boundary conditions to simulations of shear flow (Lees and Edwards, 1972). They are convenient for e.g. simulations of [...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;These conditions are an adaption of standard [[periodic boundary conditions]] to simulations of shear flow (Lees and Edwards, 1972). They are convenient for e.g. simulations of [[Couette flow]].&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
'''Related reading'''&lt;br /&gt;
*[http://epress.anu.edu.au/sm/html/ch06s03.html Couette Flow and Shear Viscosity], in  [http://epress.anu.edu.au/sm_citation.html Denis J. Evans and Gary P. Morriss &amp;quot;Statistical Mechanics of Nonequilibrium Liquids&amp;quot; ANU E Press (2007)]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/User:Ddcampayo/Sandbox</id>
		<title>User:Ddcampayo/Sandbox</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/User:Ddcampayo/Sandbox"/>
				<updated>2010-09-08T20:53:41Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Hi world. --[[User:Dduque|Dduque]] 14:18, 23 April 2008 (CEST)&lt;br /&gt;
&lt;br /&gt;
{{user degree/PhD}}&lt;br /&gt;
&lt;br /&gt;
{{user DDcampayo/Sandbox/fortran66}}&lt;br /&gt;
&lt;br /&gt;
{{user DDcampayo/Sandbox/cplusplus}}&lt;br /&gt;
&lt;br /&gt;
{{popular}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;div style=&amp;quot;border:1px solid #f3f3ff; padding-left: 0.5em !important; background-color: #f3f3ff; border-width: 0 0 0 1.4em; clear:right; float:right;&amp;quot;&amp;gt;&lt;br /&gt;
Notation used:&lt;br /&gt;
*&amp;lt;math&amp;gt;g(r)&amp;lt;/math&amp;gt; is the [[Pair distribution function | pair distribution function]].&lt;br /&gt;
*&amp;lt;math&amp;gt;\Phi(r)&amp;lt;/math&amp;gt; is the [[Intermolecular pair potential  | pair potential]] acting between pairs.&lt;br /&gt;
*&amp;lt;math&amp;gt;h(1,2)&amp;lt;/math&amp;gt; is the [[Total correlation function | total correlation function]].&lt;br /&gt;
*&amp;lt;math&amp;gt;c(1,2)&amp;lt;/math&amp;gt; is the [[Direct correlation function | direct correlation function]].&lt;br /&gt;
*&amp;lt;math&amp;gt;\gamma (r)&amp;lt;/math&amp;gt; is the [[Indirect correlation function | indirect]] (or ''series'' or  ''chain'') correlation function.&lt;br /&gt;
*&amp;lt;math&amp;gt;y(r_{12})&amp;lt;/math&amp;gt; is the [[Cavity correlation function | cavity correlation function]].&lt;br /&gt;
*&amp;lt;math&amp;gt;B(r)&amp;lt;/math&amp;gt; is the [[ bridge function]].&lt;br /&gt;
*&amp;lt;math&amp;gt;\omega(r)&amp;lt;/math&amp;gt; is the [[Thermal potential | thermal potential]].&lt;br /&gt;
*&amp;lt;math&amp;gt;f(r)&amp;lt;/math&amp;gt; is the [[Mayer f-function]].&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Substantive_derivative</id>
		<title>Substantive derivative</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Substantive_derivative"/>
				<updated>2010-05-21T10:45:07Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: /* Alternative names */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The '''substantive derivative''' is a derivative taken along a path moving with velocity v, and is often used in fluid mechanics and [[classical mechanics]]. It describes the time rate of change of some quantity (such as [[heat]] or momentum) by following it, while moving with a – space and time dependent – velocity field. Note that the familiar &amp;lt;math&amp;gt;d&amp;lt;/math&amp;gt; now becomes &amp;lt;math&amp;gt;D&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The material derivative of a scalar field &amp;lt;math&amp;gt;\phi( x, t )&amp;lt;/math&amp;gt; is:&lt;br /&gt;
:&amp;lt;math&amp;gt;    \frac{D\varphi}{Dt} = \frac{\partial \varphi}{\partial t} + \mathbf{v}\cdot\nabla \varphi,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt; \nabla \varphi&amp;lt;/math&amp;gt; is the gradient of the scalar.&lt;br /&gt;
&lt;br /&gt;
For a vector field &amp;lt;math&amp;gt;u( x, t )&amp;lt;/math&amp;gt; it is defined as:&lt;br /&gt;
:&amp;lt;math&amp;gt;    \frac{D\mathbf{u}}{Dt} = \frac{\partial \mathbf{u}}{\partial t} + \mathbf{v}\cdot\nabla \mathbf{u},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\nabla \mathbf{u}&amp;lt;/math&amp;gt; is the covariant derivative of a vector.&lt;br /&gt;
&lt;br /&gt;
In case of the material derivative of a vector field, the term &amp;lt;math&amp;gt;\mathbf{v} \cdot \nabla \mathbf{u}&amp;lt;/math&amp;gt; can both be interpreted as &amp;lt;math&amp;gt;\mathbf{v} \cdot (\nabla \mathbf{u})&amp;lt;/math&amp;gt;, involving the tensor derivative of u, or as &amp;lt;math&amp;gt;(\mathbf{v} \cdot \nabla) \mathbf{u}&amp;lt;/math&amp;gt;, leading to the same result.&lt;br /&gt;
&lt;br /&gt;
==Alternative names==&lt;br /&gt;
There are many other names for this operator, including:&lt;br /&gt;
*'''material derivative'''&lt;br /&gt;
*'''convective derivative'''&lt;br /&gt;
*'''advective derivative'''&lt;br /&gt;
*'''substantive derivative'''&lt;br /&gt;
*'''substantial derivative'''&lt;br /&gt;
*'''Lagrangian derivative'''&lt;br /&gt;
*'''Stokes derivative'''&lt;br /&gt;
*'''particle derivative'''&lt;br /&gt;
*'''hydrodynamic derivative'''&lt;br /&gt;
*'''derivative following the motion'''&lt;br /&gt;
*'''total derivative'''&lt;br /&gt;
&lt;br /&gt;
The notation varies likewise, with some authors retaining the usual ''d'' instead of ''D''.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[Category: mathematics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Substantive_derivative</id>
		<title>Substantive derivative</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Substantive_derivative"/>
				<updated>2010-05-19T11:12:27Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Formulas added&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The '''substantive derivative''' is a derivative taken along a path moving with velocity v, and is often used in fluid mechanics and classical mechanics. It describes the time rate of change of some quantity (such as heat or momentum) by following it, while moving with a – space and time dependent – velocity field.&lt;br /&gt;
&lt;br /&gt;
The material derivative of a scalar field &amp;lt;math&amp;gt;\phi( x, t )&amp;lt;/math&amp;gt; is:&lt;br /&gt;
:&amp;lt;math&amp;gt;    \frac{D\varphi}{Dt} = \frac{\partial \varphi}{\partial t} + \mathbf{v}\cdot\nabla \varphi,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt; \nabla \varphi&amp;lt;/math&amp;gt; is the gradient of the scalar.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For a vector field &amp;lt;math&amp;gt;u( x, t )&amp;lt;/math&amp;gt; it is defined as:&lt;br /&gt;
:&amp;lt;math&amp;gt;    \frac{D\mathbf{u}}{Dt} = \frac{\partial \mathbf{u}}{\partial t} + \mathbf{v}\cdot\nabla \mathbf{u},&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\nabla \mathbf{u}&amp;lt;/math&amp;gt; is the covariant derivative of a vector.&lt;br /&gt;
&lt;br /&gt;
In case of the material derivative of a vector field, the term &amp;lt;math&amp;gt;\mathbf{v} \cdot \nabla \mathbf{u}&amp;lt;/math&amp;gt; can both be interpreted as &amp;lt;math&amp;gt;\mathbf{v} \cdot (\nabla \mathbf{u})&amp;lt;/math&amp;gt;, involving the tensor derivative of u, or as &amp;lt;math&amp;gt;(\mathbf{v} \cdot \nabla) \mathbf{u}&amp;lt;/math&amp;gt;, leading to the same result.[7]&lt;br /&gt;
&lt;br /&gt;
==Names==&lt;br /&gt;
There are many other names for this operator, including:&lt;br /&gt;
*'''material derivative'''&lt;br /&gt;
*'''convective derivative'''&lt;br /&gt;
*'''advective derivative'''&lt;br /&gt;
*'''substantive derivative'''&lt;br /&gt;
*'''substantial derivative'''&lt;br /&gt;
*'''Lagrangian derivative'''&lt;br /&gt;
*'''Stokes derivative'''&lt;br /&gt;
*'''particle derivative'''&lt;br /&gt;
*'''hydrodynamic derivative'''&lt;br /&gt;
*'''derivative following the motion'''&lt;br /&gt;
*'''total derivative'''&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[Category: classical mechanics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Substantive_derivative</id>
		<title>Substantive derivative</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Substantive_derivative"/>
				<updated>2010-05-19T11:07:08Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: new page. Some names&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;There are many other names for this operator, including:&lt;br /&gt;
*'''material derivative'''&lt;br /&gt;
*'''convective derivative'''&lt;br /&gt;
*'''advective derivative'''&lt;br /&gt;
*'''substantive derivative'''&lt;br /&gt;
*'''substantial derivative'''&lt;br /&gt;
*'''Lagrangian derivative'''&lt;br /&gt;
*'''Stokes derivative'''&lt;br /&gt;
*'''particle derivative'''&lt;br /&gt;
*'''hydrodynamic derivative'''&lt;br /&gt;
*'''derivative following the motion'''&lt;br /&gt;
*'''total derivative'''&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Navier-Stokes_equations</id>
		<title>Navier-Stokes equations</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Navier-Stokes_equations"/>
				<updated>2010-05-17T15:32:36Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Other form for the mom. eq.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Continuity ==&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{v}) = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
or, using the [[substantive derivative]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{D\rho}{Dt} + \rho (\nabla \cdot \mathbf{v}) = 0. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For an incompressible fluid, &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; is constant, hence the velocity field must be divergence-free:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \nabla \cdot \mathbf{v} =0. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Momentum ==&lt;br /&gt;
&lt;br /&gt;
(Also known as ''the'' Navier-Stokes equation.)&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \rho \left(\frac{\partial \mathbf{v}}{\partial t} + \mathbf{v} \cdot \nabla \mathbf{v} \right) = -\nabla p + \nabla \cdot\mathbb{T} + \mathbf{f}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
or, using the [[substantive derivative]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \rho \left(\frac{D \mathbf{v}}{D t}  \right) = -\nabla p + \nabla \cdot\mathbb{T} + \mathbf{f},  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\mathbf{f} &amp;lt;/math&amp;gt; is a volumetric force (e.g. &amp;lt;math&amp;gt;\rho g&amp;lt;/math&amp;gt; for gravity), and &amp;lt;math&amp;gt;\mathbb{T} &amp;lt;/math&amp;gt; is the stress tensor.&lt;br /&gt;
&lt;br /&gt;
Another form of the equation, more similar in form to the continuity equation, stresses the fact that the '''momentum density''' is conserved. For each of the three Cartesian coordinates &amp;lt;math&amp;gt;\alpha=1,2,3&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \frac{\partial \rho v_\alpha}{\partial t}  +&lt;br /&gt;
    \nabla \cdot {\rho v_\alpha \mathbf{v}} =&lt;br /&gt;
   -\frac{\partial p}{\partial x_\alpha} +&lt;br /&gt;
 \sum_\beta \frac{\partial }{\partial x_\beta}  \mathbb{T}_{\beta\alpha} + f_\alpha. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In vector form:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \frac{\partial \rho v_\alpha}{\partial t}  +&lt;br /&gt;
    \nabla \cdot {\rho \mathbf{v} \mathbf{v}} =&lt;br /&gt;
   -\nabla p + \nabla\cdot\mathbb{T} + \mathbf{f}. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The term &amp;lt;math&amp;gt; \mathbf{v} \mathbf{v} &amp;lt;/math&amp;gt; is a dyad (direct tensor product).&lt;br /&gt;
&lt;br /&gt;
==Stress==&lt;br /&gt;
&lt;br /&gt;
The vector quantity &amp;lt;math&amp;gt; \nabla \cdot\mathbb{T} &amp;lt;/math&amp;gt; is the ''shear stress''. For a Newtonian incompressible fluid,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \nabla \mathbb{T} = \mu \nabla^2 \mathbf{v}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with &amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt; being the (dynamic) viscosity.&lt;br /&gt;
&lt;br /&gt;
For an inviscid fluid, the momentum equation becomes Euler's equation for ideal fluids:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \rho \left(\frac{D \mathbf{v}}{D t}  \right) = -\nabla p + \mathbf{f} . &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[Category: classical mechanics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Navier-Stokes_equations</id>
		<title>Navier-Stokes equations</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Navier-Stokes_equations"/>
				<updated>2010-05-17T15:25:48Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: New section&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Continuity ==&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{v}) = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
or, using the [[substantive derivative]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{D\rho}{Dt} + \rho (\nabla \cdot \mathbf{v}) = 0. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For an incompressible fluid, &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; is constant, hence the velocity field must be divergence-free:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \nabla \cdot \mathbf{v} =0. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Momentum ==&lt;br /&gt;
&lt;br /&gt;
(Also known as ''the'' Navier-Stokes equation.)&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \rho \left(\frac{\partial \mathbf{v}}{\partial t} + \mathbf{v} \cdot \nabla \mathbf{v} \right) = -\nabla p + \nabla \cdot\mathbb{T} + \mathbf{f}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
or, using the [[substantive derivative]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \rho \left(\frac{D \mathbf{v}}{D t}  \right) = -\nabla p + \nabla \cdot\mathbb{T} + \mathbf{f},  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\mathbf{f} &amp;lt;/math&amp;gt; is a volumetric force (e.g. &amp;lt;math&amp;gt;\rho g&amp;lt;/math&amp;gt; for gravity), and &amp;lt;math&amp;gt;\mathbb{T} &amp;lt;/math&amp;gt; is the stress tensor.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Stress==&lt;br /&gt;
&lt;br /&gt;
The vector quantity &amp;lt;math&amp;gt; \nabla \cdot\mathbb{T} &amp;lt;/math&amp;gt; is the ''shear stress''. For a Newtonian incompressible fluid,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \nabla \mathbb{T} = \mu \nabla^2 \mathbf{v}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with &amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt; being the (dynamic) viscosity.&lt;br /&gt;
&lt;br /&gt;
For an inviscid fluid, the momentum equation becomes Euler's equation for ideal fluids:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \rho \left(\frac{D \mathbf{v}}{D t}  \right) = -\nabla p + \mathbf{f} . &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[Category: classical mechanics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Navier-Stokes_equations</id>
		<title>Navier-Stokes equations</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Navier-Stokes_equations"/>
				<updated>2010-05-13T09:54:14Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: New page with NS equations&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Continuity ==&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{v}) = 0 &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
or, using the [[substantive derivative]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{D\rho}{Dt} + \rho (\nabla \cdot \mathbf{v}) = 0. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For an incompressible fluid, &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; is constant, hence the velocity field must be divergence-free:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \nabla \cdot \mathbf{v} =0. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Momentum ==&lt;br /&gt;
&lt;br /&gt;
(Also known as ''the'' Navier-Stokes equation.)&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;  \rho \left(\frac{\partial \mathbf{v}}{\partial t} + \mathbf{v} \cdot \nabla \mathbf{v} \right) = -\nabla p + \nabla \cdot\mathbb{T} + \mathbf{f}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
or, using the [[substantive derivative]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \rho \left(\frac{D \mathbf{v}}{D t}  \right) = -\nabla p + \nabla \cdot\mathbb{T} + \mathbf{f},  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\mathbf{f} &amp;lt;/math&amp;gt; is a volumetric force (e.g. &amp;lt;math&amp;gt;\rho g&amp;lt;/math&amp;gt; for gravity), and &amp;lt;math&amp;gt;\mathbb{T} &amp;lt;/math&amp;gt; is the stress tensor.&lt;br /&gt;
&lt;br /&gt;
The vector quantity &amp;lt;math&amp;gt; \nabla \cdot\mathbb{T} &amp;lt;/math&amp;gt; is the ''shear stress''. For a Newtonian incompressible fluid,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \nabla \mathbb{T} = \mu \nabla^2 \mathbf{v}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with &amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt; being the (dynamic) viscosity.&lt;br /&gt;
&lt;br /&gt;
For an inviscid fluid, the momentum equation becomes Euler's equation for ideal fluids:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \rho \left(\frac{D \mathbf{v}}{D t}  \right) = -\nabla p + \mathbf{f} . &amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Hydrodynamics</id>
		<title>Hydrodynamics</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Hydrodynamics"/>
				<updated>2010-05-13T09:42:52Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: New page: '''Hydrodynamics''' is the science of the macroscopic motion of fluid bodies. It is a field theory, relating scalar fields (such as the density and the pressure) with vector fields (such a...&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Hydrodynamics''' is the science of the macroscopic motion of fluid bodies. It is a field theory, relating scalar fields (such as the density and the pressure) with vector fields (such as the velocity field) and tensor fields (stress tensor field).&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
[[Navier-Stokes equations]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Capillary_waves</id>
		<title>Capillary waves</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Capillary_waves"/>
				<updated>2010-05-13T09:40:59Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Link to (new) hydrodynamics&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==Thermal capillary waves==&lt;br /&gt;
Thermal '''capillary waves''' are oscillations of an [[interface]] which are thermal in origin. These take place at the molecular level, where only the  contribution due to [[surface tension]] is relevant.&lt;br /&gt;
Capillary wave theory  is a classic account of how thermal fluctuations distort an interface (Ref. 1). It starts from some [[intrinsic surface]] that is distorted. In the Monge representation, the surface is given as &amp;lt;math&amp;gt;z=h(x,y)&amp;lt;/math&amp;gt;. An increase in area of the surface causes a proportional increase of energy:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
    E_\mathrm{st}= \sigma \iint dx\, dy\ \sqrt{1+\left( \frac{dh}{dx} \right)^2+\left( \frac{dh}{dy} \right)^2} -1&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for small values of the derivatives (surfaces not too rough): &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
    E_\mathrm{st} \approx \frac{\sigma}{2} \iint dx\, dy\ \left[ \left( \frac{dh}{dx} \right)^2+\left( \frac{dh}{dy} \right)^2 \right].&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
A [[Fourier analysis]] treatment begins by writing the intrinsic surface as an infinite sum of normal modes:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;h(x,y)= \sum_\vec{q} a_\vec{q} e^{i\vec{q}\vec{r}}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Since normal modes are orthogonal, the energy is easily expressible as a sum of terms &amp;lt;math&amp;gt;\propto q^2 |a_\vec{q}|^2&amp;lt;/math&amp;gt;. Each term of the sum is quadratic in the amplitude; hence [[equipartition]] holds, according to standard [[statistical mechanics | classical statistical mechanics]], and the mean energy of each mode will be &amp;lt;math&amp;gt;k_B T/2&amp;lt;/math&amp;gt;. Surprisingly, this result leads to a '''divergent''' surface (the width of the interface is bound to diverge with its area) (Ref 2). This divergence is nevertheless very mild; even for displacements on the order of meters, the deviation of the surface is comparable to the size of the molecules.&lt;br /&gt;
Moreover, the introduction of an external field removes this divergence: the action of gravity is sufficient to keep the width fluctuation on the order&lt;br /&gt;
of one molecular diameter for areas larger than about 1 mm&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; (Ref. 2).&lt;br /&gt;
The action of gravity is taken into account by integrating the potential energy density due to gravity, &amp;lt;math&amp;gt;\rho g z&amp;lt;/math&amp;gt; from a reference height to the position of the surface, &amp;lt;math&amp;gt;z=h(x,y)&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;E_\mathrm{g}=  \iint dx\, dy\, \int_0^h dz \rho g z = \frac{\rho g}{2} \int dx\, dy\, h^2.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
(For simplicity, one neglects the density of the gas above, which is often acceptable; otherwise, instead of the density the difference in densities appears).&lt;br /&gt;
&lt;br /&gt;
Recently, a procedure has been proposed to obtain a molecular intrinsic&lt;br /&gt;
surface from simulation data (Ref. 3), the [[intrinsic sampling method]]. The density profiles obtained&lt;br /&gt;
from this surface are, in general, quite different from the usual&lt;br /&gt;
''mean density profiles''.&lt;br /&gt;
&lt;br /&gt;
==Gravity-capillary waves==&lt;br /&gt;
These are ordinary waves excited in an interface, such as ripples on&lt;br /&gt;
a water surface. Their dispersion relation reads, for waves on the interface between two fluids of infinite depth:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\omega^2=\frac{\rho-\rho'}{\rho+\rho'}gk+\frac{\sigma}{\rho+\rho'}k^3,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\omega&amp;lt;/math&amp;gt; is the angular frequency, &amp;lt;math&amp;gt;g&amp;lt;/math&amp;gt; the acceleration due to gravity, &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt; the [[surface tension]], &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\rho^'&amp;lt;/math&amp;gt; the mass density of the two fluids (&amp;lt;math&amp;gt;\rho &amp;gt; \rho^'&amp;lt;/math&amp;gt;) and &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt; the is wavenumber.&lt;br /&gt;
===Derivation===&lt;br /&gt;
This is a sketch of the derivation of the general dispersion relation, see Ref. 4 for a more detailed description. The problem is unfortunately a bit complex. As Richard Feynman put it (Ref. 6):&lt;br /&gt;
&amp;lt;blockquote&amp;gt;&lt;br /&gt;
&amp;quot;''...[water waves], which are easily seen by everyone and which are used as an example of waves in elementary courses... are the worst possible example... they have all the complications that waves can have''&amp;quot;&lt;br /&gt;
&amp;lt;/blockquote&amp;gt;&lt;br /&gt;
====Defining the problem====&lt;br /&gt;
Three contributions to the energy are involved: the [[surface tension]], gravity, and [[hydrodynamics]]. The parts due to surface tension (again the derivatives are taken to be small) and gravity are exactly as above.&lt;br /&gt;
The new contribution involves the [[kinetic energy]] of the fluid:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;T= \frac{\rho}{2}  \iint dx\, dy\, \int_{-\infty}^h dz v^2,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;v&amp;lt;/math&amp;gt; is the module of the velocity field &amp;lt;math&amp;gt;\vec{v}&amp;lt;/math&amp;gt;.&lt;br /&gt;
(Again, we are neglecting the flow of the gas above for simplicity.)&lt;br /&gt;
&lt;br /&gt;
====Wave solutions====&lt;br /&gt;
Let us suppose the surface of the liquid is described by a traveling plane wave:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;h(x,y,t)=\eta(t)e^{i\vec{q}\vec{r}},&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\eta(t)=\exp[i\omega t]&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\vec{q}=(q_x,q_y)&amp;lt;/math&amp;gt; is a two dimensional wave number vector, &amp;lt;math&amp;gt;\vec{r}=(x,y)&amp;lt;/math&amp;gt; being the horizontal position. We may take &amp;lt;math&amp;gt;\vec{q}=(q,0)&amp;lt;/math&amp;gt; without loss of generality:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;h(x,y,t)=\eta(t)e^{i q x}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In this case it is easy to perform the integrations involved in the expressions for the energies. The&lt;br /&gt;
integration over &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; can taken over a period of oscillation &amp;lt;math&amp;gt;\lambda=2\pi/q&amp;lt;/math&amp;gt;, then&lt;br /&gt;
multiplied by the number of oscillations in our very large (in principle, infinite) system: &amp;lt;math&amp;gt;L_x / \lambda&amp;lt;/math&amp;gt;. The integration over &amp;lt;math&amp;gt;y&amp;lt;/math&amp;gt; trivially yields &amp;lt;math&amp;gt;L_y&amp;lt;/math&amp;gt;. Performing the integrations, keeping in mind that only the real part of complex numbers is to be taken as physical, one finds:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;E_\mathrm{g}  = \frac{A}{2} \frac{\rho g}{2} \eta^2,&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;E_\mathrm{st} = \frac{A}{2} \frac{\sigma}{2} q^2 \eta^2,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;A=L_x\times L_y&amp;lt;/math&amp;gt; is the area of the system.&lt;br /&gt;
&lt;br /&gt;
To tackle the kinetic energy, suppose the fluid is incompressible and its flow is irrotational (often, sensible approximations) - the flow will then be [[potential flow|potential]]: &amp;lt;math&amp;gt;\vec{v}=\nabla\phi&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; is a potential (scalar field) which must satisfy [[Laplace's equation]] &amp;lt;math&amp;gt;\nabla^2\phi=0&amp;lt;/math&amp;gt;. &lt;br /&gt;
If we try try separation of variables with the potential:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi(x,y,z,t)=\xi(t) f(z) e^{i q x},&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with some function of time &amp;lt;math&amp;gt;\xi(t)&amp;lt;/math&amp;gt;, and some function of vertical component (height) &amp;lt;math&amp;gt;f(z)&amp;lt;/math&amp;gt;.&lt;br /&gt;
Laplace's equation then requires on the later&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;f''(z)= q^2 f(z) .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This equation can be solved with the proper boundary conditions: first, &amp;lt;math&amp;gt;\vec{v}&amp;lt;/math&amp;gt; must vanish well below the surface (in the &amp;quot;deep water&amp;quot; case, which is the one we consider, otherwise a more general relation holds, which is also well known in oceanography). Therefore &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;f(z) = a \, \exp(|q| z) &amp;lt;/math&amp;gt;, &lt;br /&gt;
&lt;br /&gt;
with some constant &amp;lt;math&amp;gt;a&amp;lt;/math&amp;gt;. The less trivial condition is the proper matching between &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;h&amp;lt;/math&amp;gt;: the potential field must correspond to a velocity field that is adjusted to the movement of the surface: &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;v_z (z=h) =\partial h/\partial t&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
(Actually, this is the linearized version of a more general expression, see below.)&lt;br /&gt;
&lt;br /&gt;
This implies that:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\xi(t)=\eta(t)'&amp;lt;/math&amp;gt;, and  &amp;lt;math&amp;gt;f'(z=h) = 1, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
so that &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;f(z) = \exp( -|q|(h-z))/|q| &amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
We may now find the velocity field, &amp;lt;math&amp;gt;\vec{v}=\nabla\phi&amp;lt;/math&amp;gt;, which shows the well-known circles: the elements of fluid undergo circular motion in the &amp;lt;math&amp;gt;x,z&amp;lt;/math&amp;gt; plane, with the circles getting smaller at deeper levels. The displacement of a fluid element is given by &amp;lt;math&amp;gt;\partial\vec{\psi}/\partial t= \vec{v}&amp;lt;/math&amp;gt;, and is plotted in Figure 1.&lt;br /&gt;
&lt;br /&gt;
[[Image:Wave_v_field.jpg|300px|thumb|right|Figure 1. Displacement of particle (snapshot)]]&lt;br /&gt;
&lt;br /&gt;
For the kinetic energy, we need&lt;br /&gt;
&amp;lt;math&amp;gt;v^2=|\nabla\phi|^2&amp;lt;/math&amp;gt;, which is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;v^2=  (\eta')^2 e^{ -2 |q|(h-z)}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with no dependence on &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;y&amp;lt;/math&amp;gt;; the other integration provides:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;T= \frac{\rho A }{2|q|} ( \eta' )^2 \int_{-\infty}^h e^{ -2 |q|(h-z)} = \frac{A}{2}  \frac{\rho }{2|q|} ( \eta' )^2 .&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The problem is thus specified by just a potential energy involving the square of &amp;lt;math&amp;gt;\eta(t)&amp;lt;/math&amp;gt; and a kinetic energy involving the square of its time derivative: a regular [[Harmonic spring approximation|harmonic oscillator]]. In particular:&lt;br /&gt;
:&amp;lt;math&amp;gt;E= \frac{A}{2}&lt;br /&gt;
\left[&lt;br /&gt;
\left( \rho g + {\sigma} q^2 \right) \frac{\eta^2}{2}+&lt;br /&gt;
\frac{\rho}{q} \frac{(\eta')^2}{2}&lt;br /&gt;
\right].&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
Identifying the oscillator's &amp;quot;spring constant&amp;quot; &amp;lt;math&amp;gt;\kappa = \rho g + {\sigma} q^2  &amp;lt;/math&amp;gt;, and its &amp;quot;mass&amp;quot;&lt;br /&gt;
&amp;lt;math&amp;gt;m= \rho / q&amp;lt;/math&amp;gt;, the oscillation frequency must be given by &amp;lt;math&amp;gt;\omega^2=\kappa/m&amp;lt;/math&amp;gt;, which results in:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\omega^2=g q+\frac{\sigma}{\rho} q^3,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
the same dispersion as above if &amp;lt;math&amp;gt;\rho'&amp;lt;/math&amp;gt; is neglected.&lt;br /&gt;
&lt;br /&gt;
====Alternative derivation====&lt;br /&gt;
&lt;br /&gt;
In Reference 7 the dispersion relation is derived in a somewhat different manner. The same assumptions are made regarding the fluid (it is inviscid, irrotational, and incompressible), so Laplace's Equation is to be satisfied: &amp;lt;math&amp;gt;\nabla^2\phi=0&amp;lt;/math&amp;gt;, with &amp;lt;math&amp;gt;\vec{v}=\nabla\phi&amp;lt;/math&amp;gt;. The boundary conditions, on the other hand, are sufficient to solve the problem.&lt;br /&gt;
&lt;br /&gt;
One boundary condition is the requirement that the surface of the liquid, defined by &amp;lt;math&amp;gt;z=h(x,y;t)&amp;lt;/math&amp;gt; follows the velocity field:&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\frac{\partial h}{\partial t}+v_x \frac{\partial h}{\partial x}+v_y \frac{\partial h}{\partial y}= v_z .&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
A simpler condition follows from linearization: &amp;lt;math&amp;gt; \partial h /\partial t =v_z  &amp;lt;/math&amp;gt;, as in the previous derivation. There is an additional boundary condition at the bottom of the fluid, which we take here as &amp;lt;math&amp;gt;v_z=0&amp;lt;/math&amp;gt; when &amp;lt;math&amp;gt;z\rightarrow -\infty&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
In the same fashion as above, we seek surface wave solutions, of the form &amp;lt;math&amp;gt;h(x,y,t)=a e^{i (qx-\omega t)}&amp;lt;/math&amp;gt;. We may guess a solution of the form&lt;br /&gt;
:&amp;lt;math&amp;gt;\phi=-i\omega h(x,y;t) f(z).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This first condition implies &amp;lt;math&amp;gt;f'(z=h)=1&amp;lt;/math&amp;gt;. Together with Laplace's equation, this leads to a function&lt;br /&gt;
:&amp;lt;math&amp;gt;f=(1/q) \exp(q(z-h)). &amp;lt;/math&amp;gt;&lt;br /&gt;
(see Ref 8 for a discussion on when Laplace's equation admits wave solutions.)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The other surface boundary condition is a [[Bernoulli equation]], stating that the pressure just below the surface, &amp;lt;math&amp;gt;p_-&amp;lt;/math&amp;gt;, must equal the [[saturation pressure]] of coexistence, minus a contribution due to the surface:&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
p_-=p -&lt;br /&gt;
\rho\left[&lt;br /&gt;
   \frac{\partial \phi}{\partial t}+&lt;br /&gt;
   \frac{1}{2} v^2+ gh&lt;br /&gt;
   \right] .&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
The linearized condition is&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\frac{\partial \phi}{\partial t}+gh = \frac{p-p_-}{\rho}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The connection with the curvature of the surface can be introduced by [[Young's equation]] for the pressure drop across a curved interface, whose linearized form is:&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
p-p_-=\sigma\left(\frac{\partial^2 h}{\partial x^2}+\frac{\partial^2 h}{\partial y^2}\right),&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt; is the surface tension.&lt;br /&gt;
The linearized condition is finally&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\frac{\partial \phi}{\partial t}+gh = \frac{\sigma}{\rho} \left(\frac{\partial^2 h}{\partial x^2}+\frac{\partial^2 h}{\partial y^2}\right).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This second condition, when applied to the surface wave above, establishes that &amp;lt;math&amp;gt;f(z=h)=(g+\sigma/\rho q^2)/\omega^2&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
For the two conditions to hold, &amp;lt;math&amp;gt;1/q&amp;lt;/math&amp;gt; must equal &amp;lt;math&amp;gt;(g+\sigma/\rho q^2)/\omega^2&amp;lt;/math&amp;gt;, which is precisely the same dispersion relation as the one above.&lt;br /&gt;
&lt;br /&gt;
This derivation makes clear the assumptions introduced. In particular, the linearization will only hold for smooth waves, the ones for which the wave amplitude, &amp;lt;math&amp;gt;a&amp;lt;/math&amp;gt; is smaller than the wavelength. Mathematically, the limit is &amp;lt;math&amp;gt;q a \ll 1&amp;lt;/math&amp;gt;. For ocean waves, this happens when waves approach the shore and the amplitude grows (in this limit, a bottom boundary condition &amp;lt;math&amp;gt;v_z (z=-H) =0&amp;lt;/math&amp;gt; must be employed, and waves are not dispersive, see Ref 7.)&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1103/PhysRevLett.15.621 F. P. Buff, R. A. Lovett, and F. H. Stillinger, Jr. &amp;quot;Interfacial density profile for fluids in the critical region&amp;quot; Physical Review Letters '''15''' pp. 621-623 (1965)]&lt;br /&gt;
#J. S. Rowlinson and B. Widom &amp;quot;Molecular Theory of Capillarity&amp;quot;. Dover 2002 (originally: Oxford University Press 1982) ISBN 0486425444&lt;br /&gt;
#[http://dx.doi.org/10.1103/PhysRevLett.91.166103 E. Chacón and P. Tarazona  &amp;quot;Intrinsic profiles beyond the capillary wave theory: A Monte Carlo study&amp;quot;, Physical Review Letters '''91'''  166103 (2003)]&lt;br /&gt;
#Samuel A. Safran &amp;quot;Statistical thermodynamics of surfaces, interfaces, and membranes&amp;quot; Addison-Wesley 1994 ISBN 9780813340791&lt;br /&gt;
#[http://dx.doi.org/10.1103/PhysRevLett.99.196101 P. Tarazona, R. Checa, and E. Chacón &amp;quot;Critical Analysis of the Density Functional Theory Prediction of Enhanced Capillary Waves&amp;quot;, Physical Review Letters '''99''' 196101 (2007)]&lt;br /&gt;
#R.P. Feynman, R.B. Leighton, and M. Sands &amp;quot;The Feynman lectures on physics&amp;quot; Addison-Wesley 1963. Section 51-4. ISBN 0201021153&lt;br /&gt;
#[http://dx.doi.org/10.1006/rwos.2001.0129  W.K. Melville &amp;quot;Surface, gravity and capillary waves&amp;quot;], in [http://www.sciencedirect.com/science/referenceworks/9780122274305  &amp;quot;Encyclopedia of Ocean Sciences&amp;quot;], Eds:  Steve A. Thorpe and Karl K. Turekian. Elsevier 2001, page 2916. ISBN 978-0-12-227430-5 &lt;br /&gt;
#[http://dx.doi.org/10.1088/0143-0807/25/1/014 F Behroozi &amp;quot;Fluid viscosity and the attenuation of surface waves: a derivation based on conservation of energy&amp;quot;,  European Journal of Physics '''25''' 115 (2004)]&lt;br /&gt;
==External links==&lt;br /&gt;
*[http://en.wikipedia.org/wiki/Capillary_wave Capillary wave entry in Wikipedia]&lt;br /&gt;
*[http://en.wikipedia.org/wiki/Thermal_capillary_wave Thermal capillary wave entry in Wikipedia]&lt;br /&gt;
[[Category: Classical thermodynamics ]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models</id>
		<title>Mean field models</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models"/>
				<updated>2010-05-03T14:28:10Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added link to Curie's_law&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A '''mean field model''', or a '''mean field solution''' of a model, is an approximation to the actual solution of a model in statistical physics. The model is made exactly solvable by treating the effect of all other particles on a given one as a ''mean field'' (hence its name). It appear in different forms and different contexts, but all mean field models have this feature in common.&lt;br /&gt;
&lt;br /&gt;
==Mean field solution of the Ising model==&lt;br /&gt;
&lt;br /&gt;
A well-known mean field solution of the [[Ising model]], known as the ''Bragg-Williams approximation'' goes as follows.&lt;br /&gt;
From the original Hamiltonian,&lt;br /&gt;
:&amp;lt;math&amp;gt; U = - J \sum_i^N S_i \sum_{&amp;lt;j&amp;gt;} S_j , &amp;lt;/math&amp;gt;&lt;br /&gt;
suppose we may approximate&lt;br /&gt;
:&amp;lt;math&amp;gt; \sum_{&amp;lt;j&amp;gt;} S_j \approx n \bar{s}, &amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; is the number of neighbors of site &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt; (e.g. 4 in a 2-D square lattice), and &amp;lt;math&amp;gt;\bar{s}&amp;lt;/math&amp;gt; is the (unknown) magnetization:&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar{s}=\frac{1}{N} \sum_i S_i . &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Therefore, the Hamiltonian turns to&lt;br /&gt;
:&amp;lt;math&amp;gt; U = - J n \sum_i^N S_i \bar{s} , &amp;lt;/math&amp;gt;&lt;br /&gt;
as in the regular Langevin theory of magnetism (see  [[Curie's_law]]): the spins are independent, but coupled to a constant field of strength&lt;br /&gt;
:&amp;lt;math&amp;gt;H= J n \bar{s}.&amp;lt;/math&amp;gt;&lt;br /&gt;
The magnetization of the Langevin theory is&lt;br /&gt;
:&amp;lt;math&amp;gt;  \bar{s} = \tanh( H/k_B T ). &amp;lt;/math&amp;gt;&lt;br /&gt;
Therefore:&lt;br /&gt;
:&amp;lt;math&amp;gt;  \bar{s} = \tanh(J n\bar{s}/k_B T). &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This is a '''self-consistent''' expression for &amp;lt;math&amp;gt;\bar{s}&amp;lt;/math&amp;gt;. There exists a critical temperature, defined by&lt;br /&gt;
:&amp;lt;math&amp;gt;k_B T_c= J n .&amp;lt;/math&amp;gt;&lt;br /&gt;
At temperatures higher than this value the only solution is &amp;lt;math&amp;gt;\bar{s}=0&amp;lt;/math&amp;gt;. Below it, however, this solution becomes unstable&lt;br /&gt;
(it corresponds to a maximum in energy), whereas two others are stable. Slightly below &amp;lt;math&amp;gt;T_c&amp;lt;/math&amp;gt;,&lt;br /&gt;
:&amp;lt;math&amp;gt;\bar{s} =\pm\sqrt{3\left(1 - \frac{T}{T_c}\right)}. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==General discussion==&lt;br /&gt;
The solution obtained shares a number of features with any other mean field approximation:&lt;br /&gt;
*It largely ignores geometry, which may be important in some cases. In particular, it reduces the lattice details to just the number of neighbours.&lt;br /&gt;
*As a consequence, it may predict phase transitions where none are found: the [[1-dimensional_Ising_model|1-D ising model]] &amp;lt;math&amp;gt;n=2&amp;lt;/math&amp;gt; is known to lack any phase transition (at finite temperature)&lt;br /&gt;
*In general, the theory ''underestimates fluctuations''&lt;br /&gt;
*It also leads to ''classical critical exponents'', like the &amp;lt;math&amp;gt;\left(1 - \frac{T}{T_c}\right)^{1/2}&amp;lt;/math&amp;gt; decay above. In 3-D, the magnetization follows a power law with a different exponent.&lt;br /&gt;
*Nevertheless, above a certain space dimension the critical exponents are correct. This dimension is 4 for the Ising model, as predicted by a self-consistency requirement due to E.M. Lipfshitz (similar ones are due to Peierls and L.D. Landau)&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models</id>
		<title>Mean field models</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models"/>
				<updated>2010-05-03T14:26:32Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Completed solution, section added.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A '''mean field model''', or a '''mean field solution''' of a model, is an approximation to the actual solution of a model in statistical physics. The model is made exactly solvable by treating the effect of all other particles on a given one as a ''mean field'' (hence its name). It appear in different forms and different contexts, but all mean field models have this feature in common.&lt;br /&gt;
&lt;br /&gt;
==Mean field solution of the Ising model==&lt;br /&gt;
&lt;br /&gt;
A well-known mean field solution of the [[Ising model]], known as the ''Bragg-Williams approximation'' goes as follows.&lt;br /&gt;
From the original Hamiltonian,&lt;br /&gt;
:&amp;lt;math&amp;gt; U = - J \sum_i^N S_i \sum_{&amp;lt;j&amp;gt;} S_j , &amp;lt;/math&amp;gt;&lt;br /&gt;
suppose we may approximate&lt;br /&gt;
:&amp;lt;math&amp;gt; \sum_{&amp;lt;j&amp;gt;} S_j \approx n \bar{s}, &amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; is the number of neighbors of site &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt; (e.g. 4 in a 2-D square lattice), and &amp;lt;math&amp;gt;\bar{s}&amp;lt;/math&amp;gt; is the (unknown) magnetization:&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar{s}=\frac{1}{N} \sum_i S_i . &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Therefore, the Hamiltonian turns to&lt;br /&gt;
:&amp;lt;math&amp;gt; U = - J n \sum_i^N S_i \bar{s} , &amp;lt;/math&amp;gt;&lt;br /&gt;
as in the regular Langevin theory of magnetism: the spins are independent, but coupled to a constant field of strength&lt;br /&gt;
:&amp;lt;math&amp;gt;H= J n \bar{s}.&amp;lt;/math&amp;gt;&lt;br /&gt;
The magnetization of the Langevin theory is&lt;br /&gt;
:&amp;lt;math&amp;gt;  \bar{s} = \tanh( H/k_B T ). &amp;lt;/math&amp;gt;&lt;br /&gt;
Therefore:&lt;br /&gt;
:&amp;lt;math&amp;gt;  \bar{s} = \tanh(J n\bar{s}/k_B T). &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This is a '''self-consistent''' expression for &amp;lt;math&amp;gt;\bar{s}&amp;lt;/math&amp;gt;. There exists a critical temperature, defined by&lt;br /&gt;
:&amp;lt;math&amp;gt;k_B T_c= J n .&amp;lt;/math&amp;gt;&lt;br /&gt;
At temperatures higher than this value the only solution is &amp;lt;math&amp;gt;\bar{s}=0&amp;lt;/math&amp;gt;. Below it, however, this solution becomes unstable&lt;br /&gt;
(it corresponds to a maximum in energy), whereas two others are stable. Slightly below &amp;lt;math&amp;gt;T_c&amp;lt;/math&amp;gt;,&lt;br /&gt;
:&amp;lt;math&amp;gt;\bar{s} =\pm\sqrt{3\left(1 - \frac{T}{T_c}\right)}. &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==General discussion==&lt;br /&gt;
The solution obtained shares a number of features with any other mean field approximation:&lt;br /&gt;
*It largely ignores geometry, which may be important in some cases. In particular, it reduces the lattice details to just the number of neighbours.&lt;br /&gt;
*As a consequence, it may predict phase transitions where none are found: the [[1-dimensional_Ising_model|1-D ising model]] &amp;lt;math&amp;gt;n=2&amp;lt;/math&amp;gt; is known to lack any phase transition (at finite temperature)&lt;br /&gt;
*In general, the theory ''underestimates fluctuations''&lt;br /&gt;
*It also leads to ''classical critical exponents'', like the &amp;lt;math&amp;gt;\left(1 - \frac{T}{T_c}\right)^{1/2}&amp;lt;/math&amp;gt; decay above. In 3-D, the magnetization follows a power law with a different exponent.&lt;br /&gt;
*Nevertheless, above a certain space dimension the critical exponents are correct. This dimension is 4 for the Ising model, as predicted by a self-consistency requirement due to E.M. Lipfshitz (similar ones are due to Peierls and L.D. Landau)&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models</id>
		<title>Mean field models</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models"/>
				<updated>2010-05-03T14:17:02Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: /* Mean field solution of the Ising model */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A '''mean field model''', or a '''mean field solution''' of a model, is an approximation to the actual solution of a model in statistical physics. The model is made exactly solvable by treating the effect of all other particles on a given one as a ''mean field'' (hence its name). It appear in different forms and different contexts, but all mean field models have this feature in common.&lt;br /&gt;
&lt;br /&gt;
==Mean field solution of the Ising model==&lt;br /&gt;
&lt;br /&gt;
A well-known mean field solution of the [[Ising model]], known as the ''Bragg-Williams approximation'' goes as follows.&lt;br /&gt;
From the original Hamiltonian,&lt;br /&gt;
:&amp;lt;math&amp;gt; U = - J \sum_i^N S_i \sum_{&amp;lt;j&amp;gt;} S_j , &amp;lt;/math&amp;gt;&lt;br /&gt;
suppose we may approximate&lt;br /&gt;
:&amp;lt;math&amp;gt; \sum_{&amp;lt;j&amp;gt;} S_j \approx n \bar{s}, &amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; is the number of neighbors of site &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt; (e.g. 4 in a 2-D square lattice), and &amp;lt;math&amp;gt;\bar{s}&amp;lt;/math&amp;gt; is the (unknown) magnetization:&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar{s}=\frac{1}{N} \sum_i S_i . &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Therefore, the Hamiltonian turns to&lt;br /&gt;
:&amp;lt;math&amp;gt; U = - J n \sum_i^N S_i \bar{s} , &amp;lt;/math&amp;gt;&lt;br /&gt;
as in the regular Langevin theory of magnetism: the spins are independent, but coupled to a constant field of strength&lt;br /&gt;
:&amp;lt;math&amp;gt;H= J n \bar{s}.&amp;lt;/math&amp;gt;&lt;br /&gt;
The magnetization of the Langevin theory is&lt;br /&gt;
:&amp;lt;math&amp;gt;  \bar{s} = \tanh( H/k_B T ). &amp;lt;/math&amp;gt;&lt;br /&gt;
Therefore:&lt;br /&gt;
:&amp;lt;math&amp;gt;  \bar{s} = \tanh(J n\bar{s}/k_B T). &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This is a '''self-consistent''' expression for &amp;lt;math&amp;gt;\bar{s}&amp;lt;/math&amp;gt;. There exists a critical temperature, defined by&lt;br /&gt;
:&amp;lt;math&amp;gt;k_B T_c= J n .&amp;lt;/math&amp;gt;&lt;br /&gt;
At temperatures higher than this value the only solution is &amp;lt;math&amp;gt;\bar{s}=0&amp;lt;/math&amp;gt;. Below it, however, this solution becomes unstable&lt;br /&gt;
(it corresponds to a maximum in energy), whereas two others are stable. Slightly below &amp;lt;math&amp;gt;T_c&amp;lt;/math&amp;gt;,&lt;br /&gt;
:&amp;lt;math&amp;gt;\bar{s} =\pm\sqrt{3\left(1 - \frac{T}{T_c}\right)}. &amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models</id>
		<title>Mean field models</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Mean_field_models"/>
				<updated>2010-04-29T10:34:36Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: I can't believe there was not an entry about this... work in progress&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A '''mean field model''', or a '''mean field solution''' of a model, is an approximation to the actual solution of a model in statistical physics. The model is made exactly solvable by treating the effect of all other particles on a given one as a ''mean field'' (hence its name). It appear in different forms and different contexts, but all mean field models have this feature in common.&lt;br /&gt;
&lt;br /&gt;
==Mean field solution of the Ising model==&lt;br /&gt;
&lt;br /&gt;
A well-known mean field solution of the [[Ising model]] goes as follows. From the original hamiltonian,&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{U}{k_B T} = - K \sum_i S_i \sum_j S_j , &amp;lt;/math&amp;gt;&lt;br /&gt;
suppose we may approximate&lt;br /&gt;
:&amp;lt;math&amp;gt; \sum_j S_j \approx N \bar{s}, &amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;N&amp;lt;/math&amp;gt; is the number of neighbors of site &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt; (e.g. 4 in a 2-D squate lattice), and &amp;lt;math&amp;gt;\bar{s}&amp;lt;/math&amp;gt; is the (unknown) magnetization:&lt;br /&gt;
:&amp;lt;math&amp;gt; \bar{s}=\frac{1}{N} \sum_i S_i . &amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Ising_model</id>
		<title>Ising model</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Ising_model"/>
				<updated>2010-04-29T10:26:30Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added link to Mean field models&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The '''Ising model''' &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/BF02980577 Ernst Ising &amp;quot;Beitrag zur Theorie des Ferromagnetismus&amp;quot;, 	Zeitschrift für Physik A Hadrons and Nuclei '''31''' pp. 253-258 (1925)]&amp;lt;/ref&amp;gt; (also known as the '''Lenz-Ising''' model) is commonly defined over an ordered lattice. &lt;br /&gt;
Each site of the lattice can adopt two states, &amp;lt;math&amp;gt;S \in \{-1, +1 \}&amp;lt;/math&amp;gt;. Note that sometimes these states are referred to as ''spins'' and the values are referred to as ''down'' and ''up'' respectively. &lt;br /&gt;
The energy of the system is the sum of pair interactions&lt;br /&gt;
between nearest neighbors.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{U}{k_B T} = - K \sum_{\langle ij \rangle} S_i S_j &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;k_B&amp;lt;/math&amp;gt; is the [[Boltzmann constant]], &amp;lt;math&amp;gt;T&amp;lt;/math&amp;gt; is the [[temperature]],  &amp;lt;math&amp;gt; \langle ij \rangle &amp;lt;/math&amp;gt; indicates that the sum is performed over nearest neighbors, and&lt;br /&gt;
&amp;lt;math&amp;gt; S_i &amp;lt;/math&amp;gt; indicates the state of the i-th site, and &amp;lt;math&amp;gt; K &amp;lt;/math&amp;gt; is the coupling constant. &lt;br /&gt;
&lt;br /&gt;
For a detailed and very readable history of the Lenz-Ising model see the following references:&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/RevModPhys.39.883  S. G. Brush &amp;quot;History of the Lenz-Ising Model&amp;quot;, Reviews of Modern Physics '''39''' pp. 883-893 (1967)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/s00407-004-0088-3 Martin Niss &amp;quot;History of the Lenz-Ising Model 1920-1950: From Ferromagnetic to Cooperative Phenomena&amp;quot;, Archive for History of Exact Sciences '''59''' pp. 267-318 (2005)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/s00407-008-0039-5 Martin Niss &amp;quot;History of the Lenz–Ising Model 1950–1965: from irrelevance to relevance&amp;quot;, Archive for History of Exact Sciences '''63''' pp. 243-287 (2009)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
==1-dimensional Ising model==&lt;br /&gt;
:''Main article: [[1-dimensional Ising model]]''&lt;br /&gt;
The 1-dimensional Ising model has an exact solution.&lt;br /&gt;
&lt;br /&gt;
==2-dimensional Ising model==&lt;br /&gt;
The 2-dimensional Ising model was solved by [[Lars Onsager]] in 1944&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRev.65.117 Lars Onsager &amp;quot;Crystal Statistics. I. A Two-Dimensional Model with an Order-Disorder Transition&amp;quot;, Physical Review '''65''' pp. 117 - 149 (1944)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRev.88.1332 M. Kac and J. C. Ward &amp;quot;A Combinatorial Solution of the Two-Dimensional Ising Model&amp;quot;, Physical Review '''88''' pp. 1332-1337 (1952)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;Rodney J. Baxter  &amp;quot;Exactly Solved Models in Statistical Mechanics&amp;quot;, Academic Press (1982)  ISBN 0120831821 Chapter 7 (freely available [http://tpsrv.anu.edu.au/Members/baxter/book/Exactly.pdf pdf])&amp;lt;/ref&amp;gt;&lt;br /&gt;
after [[Rudolf Peierls]] had previously shown  that, contrary to the one-dimensional case, the two-dimensional model must have a phase transition&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1017/S0305004100019174 Rudolf Peierls &amp;quot;On Ising's model of ferromagnetism&amp;quot;, Mathematical Proceedings of the Cambridge Philosophical Society '''32''' pp. 477-481 (1936)]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRev.136.A437 Robert B. Griffiths &amp;quot;Peierls Proof of Spontaneous Magnetization in a Two-Dimensional Ising Ferromagnet&amp;quot;, Physical Review A '''136''' pp. 437-439 (1964)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==3-dimensional Ising model==&lt;br /&gt;
Sorin Istrail has shown that the solution of Ising's model cannot be extended into three dimensions for any lattice&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://www.sandia.gov/LabNews/LN04-21-00/sorin_story.html Three-dimensional proof for Ising model impossible, Sandia researcher claims to have shown]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1145/335305.335316    	Sorin Istrail 	 &amp;quot;Statistical mechanics, three-dimensionality and NP-completeness: I. Universality of intracatability for the partition function of the Ising model across non-planar surfaces&amp;quot;, Proceedings of the thirty-second annual ACM symposium on Theory of computing pp. 87-96   (2000)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
==ANNNI model==&lt;br /&gt;
The '''axial next-nearest neighbour Ising''' (ANNNI) model &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0370-1573(88)90140-8  Walter Selke &amp;quot;The ANNNI model — Theoretical analysis and experimental application&amp;quot;, Physics Reports  '''170''' pp. 213-264 (1988)]&amp;lt;/ref&amp;gt; is used to study alloys, adsorbates, ferroelectrics, magnetic systems, and polytypes.&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Critical exponents]]&lt;br /&gt;
*[[Potts model]]&lt;br /&gt;
*[[Mean field models]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[Category: Models]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Statistical_mechanics</id>
		<title>Statistical mechanics</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Statistical_mechanics"/>
				<updated>2010-04-29T10:25:24Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added link to Mean field models&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{columns-list|3|&lt;br /&gt;
==B==&lt;br /&gt;
*[[BBGKY hierarchy]]&lt;br /&gt;
*[[Boltzmann average]]&lt;br /&gt;
*[[Boltzmann constant]]&lt;br /&gt;
*[[Boltzmann distribution]]&lt;br /&gt;
*[[Boltzmann factor]]&lt;br /&gt;
*[[Born-Green equation]]&lt;br /&gt;
*[[Brownian motion]]&lt;br /&gt;
&lt;br /&gt;
==C==&lt;br /&gt;
*[[Canonical ensemble]]&lt;br /&gt;
*[[Chemical potential]]&lt;br /&gt;
*[[Compressibility equation]]&lt;br /&gt;
*[[Critical exponents]]&lt;br /&gt;
*[[Critical points]]&lt;br /&gt;
*[[Curie's law]]&lt;br /&gt;
&lt;br /&gt;
==D==&lt;br /&gt;
*[[Darwin-Fowler method]]&lt;br /&gt;
*[[de Broglie thermal wavelength]]&lt;br /&gt;
&lt;br /&gt;
==E==&lt;br /&gt;
*[[Energy equation]]&lt;br /&gt;
*[[Entropy]]&lt;br /&gt;
*[[Ensembles in thermostatistics]]&lt;br /&gt;
*[[Ergodic hypothesis]]&lt;br /&gt;
&lt;br /&gt;
==F==&lt;br /&gt;
*[[Fermi-Pasta-Ulam experiment]]&lt;br /&gt;
*[[Fisher–Ruelle stability criteria]]&lt;br /&gt;
*[[Fisher-Widom line]]&lt;br /&gt;
*[[Four-body function]]&lt;br /&gt;
&lt;br /&gt;
==G==&lt;br /&gt;
*[[Gibbs distribution]]&lt;br /&gt;
*[[Gibbs ensemble]]&lt;br /&gt;
*[[Gibbs measures]]&lt;br /&gt;
*[[Gibbs paradox]]&lt;br /&gt;
*[[Goldstone modes]]&lt;br /&gt;
*[[Grand canonical ensemble]]&lt;br /&gt;
&lt;br /&gt;
==I==&lt;br /&gt;
*[[Information theory]]&lt;br /&gt;
*[[Internal energy]]&lt;br /&gt;
*[[Intermolecular pair potential]]&lt;br /&gt;
*[[Isoenthalpic–isobaric ensemble]]&lt;br /&gt;
*[[Isothermal-isobaric ensemble]]&lt;br /&gt;
==J==&lt;br /&gt;
*[[Joule-Thomson effect]]&lt;br /&gt;
==K==&lt;br /&gt;
*[[Kirkwood superposition approximation]]&lt;br /&gt;
*[[Kolmogorov–Arnold–Moser theorem]]&lt;br /&gt;
&lt;br /&gt;
==L==&lt;br /&gt;
*[[Law of corresponding states]]&lt;br /&gt;
*[[Liouville's theorem]]&lt;br /&gt;
*[[Loschmidt's paradox]] (Umkehreinwand)&lt;br /&gt;
*[[Lyapunov exponents]]&lt;br /&gt;
&lt;br /&gt;
==M==&lt;br /&gt;
*[[Maxwell velocity distribution]]&lt;br /&gt;
*[[Maxwell's demon]]&lt;br /&gt;
*[[Mean field models]]&lt;br /&gt;
*[[Microcanonical ensemble]]&lt;br /&gt;
*[[Microstate]]&lt;br /&gt;
*[[Mixing systems]]&lt;br /&gt;
&lt;br /&gt;
==P==&lt;br /&gt;
*[[Pair distribution function]]&lt;br /&gt;
*[[Parrondo's paradox]]&lt;br /&gt;
*[[Partition function]]&lt;br /&gt;
*[[Phase space]]&lt;br /&gt;
*[[Phase transitions]]&lt;br /&gt;
*[[Poincaré theorem]] &lt;br /&gt;
*[[Pressure]]&lt;br /&gt;
*[[Pressure equation]] (aka. virial equation)&lt;br /&gt;
&lt;br /&gt;
==Q==&lt;br /&gt;
*[[Quantum statistics]]&lt;br /&gt;
==R==&lt;br /&gt;
*[[Radial distribution function]]&lt;br /&gt;
==S==&lt;br /&gt;
*[[Semi-grand ensembles]]&lt;br /&gt;
*[[Stochastic transition]]&lt;br /&gt;
*[[Structure factor]]&lt;br /&gt;
*[[Surface tension]]&lt;br /&gt;
&lt;br /&gt;
==T==&lt;br /&gt;
*[[Temperature]]&lt;br /&gt;
*[[Thermodynamic limit]]&lt;br /&gt;
*[[Transfer matrices]] &lt;br /&gt;
==Y==&lt;br /&gt;
*[[Yang-Yang anomaly]]&lt;br /&gt;
==Z==&lt;br /&gt;
*[[Zermelo’s paradox]] (Wiederkehreinwand)&lt;br /&gt;
}}&lt;br /&gt;
==General reading==&lt;br /&gt;
'''Books'''&lt;br /&gt;
* Donald A. McQuarrie &amp;quot;Statistical Mechanics&amp;quot;, University Science Books (1984) (Re-published 2000) ISBN 978-1-891389-15-3&lt;br /&gt;
* L. D. Landau and E. M. Lifshitz &amp;quot;Statistical Physics&amp;quot;, Course of Theoretical Physics volume 5 Part 1 3rd Edition (1984) ISBN 0750633727&lt;br /&gt;
* Terrell L. Hill &amp;quot;Statistical Mechanics: Principles and Selected Applications&amp;quot; (1956) ISBN 0486653900&lt;br /&gt;
* Terrell L. Hill &amp;quot;An Introduction to Statistical Thermodynamics&amp;quot; (1986) ISBN 0486652424&lt;br /&gt;
'''Papers'''&lt;br /&gt;
*[http://dx.doi.org/10.1103/RevModPhys.27.289  D. Ter Haar &amp;quot;Foundations of Statistical Mechanics&amp;quot;, Reviews of Modern Physics '''27''' pp. 289 - 338 (1955)]&lt;br /&gt;
*[http://dx.doi.org/10.1088/0034-4885/42/12/002 O. Penrose &amp;quot;Foundations of statistical mechanics&amp;quot;, Reports on Progress in Physics '''42''' pp. 1937-2006 (1979)]&lt;br /&gt;
*[http://dx.doi.org/10.1126/science.177.4047.393 P. W. Anderson &amp;quot;More Is Different&amp;quot;, Science '''177''' pp. 393-396 (1972)]&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268970600965835 J. S. Rowlinson &amp;quot;The evolution of some statistical mechanical ideas&amp;quot;, Molecular Physics '''104''' pp. 3399 - 3410 (2006)]&lt;br /&gt;
*[http://dx.doi.org/10.1016/S0378-4371(98)00517-2 Elliott H. Lieb  &amp;quot;Some problems in statistical mechanics that I would like to see solved&amp;quot;, Physica A '''263''' pp. 491-499 (1999)]&lt;br /&gt;
*[http://www.pro-physik.de/Phy/pdfstart.do?mid=3&amp;amp;articleid=25753&amp;amp;recordid=25793 Joel L. Lebowitz  &amp;quot;Emergent Phenomena&amp;quot;, Physik Journal '''6''' #9 pp. 41-46 (2007)]&lt;br /&gt;
[[category: statistical mechanics]]&lt;br /&gt;
__NOTOC__&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm</id>
		<title>Beeman's algorithm</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm"/>
				<updated>2010-04-19T11:01:10Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Interesting: same positions as Verlet&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Beeman's algorithm''' &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0021-9991(76)90059-0 D. Beeman &amp;quot;Some multistep methods for use in molecular dynamics calculations&amp;quot;, Journal of Computational Physics '''20''' pp. 130-139 (1976)]&amp;lt;/ref&amp;gt;  is is a method for [[Integrators for molecular dynamics |numerically integrating ordinary differential equations]], generally position and velocity, which is closely related to Verlet integration.&lt;br /&gt;
&lt;br /&gt;
In its standard form, it produces the same trajectories as the Verlet algorithm, but the velocities are more accurate:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;x(t+\Delta t) = x(t) + v(t) \Delta t + \left(\frac{2}{3}a(t)  - \frac{1}{6} a(t - \Delta t) \right)\Delta t^2 + O( \Delta t^4) &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;v(t + \Delta t) = v(t) + \left(\frac{1}{3}a(t + \Delta t)  + \frac{5}{6}a(t)  - \frac{1}{6}a(t - \Delta t) \right) \Delta t + O(\Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where ''x'' is the position, ''v'' is the velocity, ''a'' is the acceleration, ''t'' is time, and &amp;lt;math&amp;gt;\Delta t&amp;lt;/math&amp;gt; is the [[Time step|time-step]].&lt;br /&gt;
&lt;br /&gt;
A predictor-corrector variant is useful when the forces are velocity-dependent:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    x(t+\Delta t) = x(t) + v(t) \Delta t + \frac{2}{3}a(t) \Delta t^2 - \frac{1}{6} a(t - \Delta t) \Delta t^2 + O( \Delta t^4).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The velocities at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t)_{(\mathrm{predicted})} = v(t) + \frac{3}{2}a(t) \Delta t - \frac{1}{2}a(t - \Delta t) \Delta t + O( \Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The accelerations at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions and predicted velocities.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t)_{(\mathrm{corrected})} = v(t) + \frac{1}{3}a(t + \Delta t) \Delta t + \frac{5}{6}a(t) \Delta t - \frac{1}{6}a(t - \Delta t) \Delta t + O( \Delta t^3) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Velocity Verlet algorithm]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
==External links==&lt;br /&gt;
*[http://en.wikipedia.org/wiki/Beeman%27s_algorithm Beeman's algorithm entry on wikipedia]&lt;br /&gt;
[[category: Molecular dynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm</id>
		<title>Beeman's algorithm</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm"/>
				<updated>2010-04-17T13:35:31Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Link to wikipedia&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Beeman's algorithm''' is is a method for numerically integrating ordinary differential equations, generally position and velocity, which is closely related to Verlet integration.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;x(t+\Delta t) = x(t) + v(t) \Delta t + (\frac{2}{3}a(t)  - \frac{1}{6} a(t - \Delta t) )\Delta t^2 + O( \Delta t^4) &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;v(t + \Delta t) = v(t) + (\frac{1}{3}a(t + \Delta t)  + \frac{5}{6}a(t)  - \frac{1}{6}a(t - \Delta t)) \Delta t + O(\Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where ''x'' is the position, ''v'' is the velocity, ''a'' is the acceleration, ''t'' is time, and ''\Delta t'' is the time-step.&lt;br /&gt;
&lt;br /&gt;
A predictor-corrector variant is useful when the forces are velocity-dependent:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    x(t+\Delta t) = x(t) + v(t) \Delta t + \frac{2}{3}a(t) \Delta t^2 - \frac{1}{6} a(t - \Delta t) \Delta t^2 + O( \Delta t^4).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The velocities at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t) (predicted) = v(t) + \frac{3}{2}a(t) \Delta t - \frac{1}{2}a(t - \Delta t) \Delta t + O( \Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The accelerations at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions and predicted velocities.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t) (corrected) = v(t) + \frac{1}{3}a(t + \Delta t) \Delta t + \frac{5}{6}a(t) \Delta t - \frac{1}{6}a(t - \Delta t) \Delta t + O( \Delta t^3) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Velocity Verlet algorithm]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*[http://en.wikipedia.org/wiki/Beeman%27s_algorithm Beeman's algorithm entry on wikipedia]&lt;br /&gt;
[[category: Molecular dynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm</id>
		<title>Beeman's algorithm</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm"/>
				<updated>2010-04-17T13:07:22Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: common factor&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Beeman's algorithm''' is is a method for numerically integrating ordinary differential equations, generally position and velocity, which is closely related to Verlet integration.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;x(t+\Delta t) = x(t) + v(t) \Delta t + (\frac{2}{3}a(t)  - \frac{1}{6} a(t - \Delta t) )\Delta t^2 + O( \Delta t^4) &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;v(t + \Delta t) = v(t) + (\frac{1}{3}a(t + \Delta t)  + \frac{5}{6}a(t)  - \frac{1}{6}a(t - \Delta t)) \Delta t + O(\Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where ''x'' is the position, ''v'' is the velocity, ''a'' is the acceleration, ''t'' is time, and ''\Delta t'' is the time-step.&lt;br /&gt;
&lt;br /&gt;
A predictor-corrector variant is useful when the forces are velocity-dependent:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    x(t+\Delta t) = x(t) + v(t) \Delta t + \frac{2}{3}a(t) \Delta t^2 - \frac{1}{6} a(t - \Delta t) \Delta t^2 + O( \Delta t^4).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The velocities at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t) (predicted) = v(t) + \frac{3}{2}a(t) \Delta t - \frac{1}{2}a(t - \Delta t) \Delta t + O( \Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The accelerations at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions and predicted velocities.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t) (corrected) = v(t) + \frac{1}{3}a(t + \Delta t) \Delta t + \frac{5}{6}a(t) \Delta t - \frac{1}{6}a(t - \Delta t) \Delta t + O( \Delta t^3) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Velocity Verlet algorithm]]&lt;br /&gt;
[[category: Molecular dynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm</id>
		<title>Beeman's algorithm</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Beeman%27s_algorithm"/>
				<updated>2010-04-17T10:16:17Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: New page: '''Beeman's algorithm''' is is a method for numerically integrating ordinary differential equations, generally position and velocity, which is closely related to Verlet integration.  :&amp;lt;mat...&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Beeman's algorithm''' is is a method for numerically integrating ordinary differential equations, generally position and velocity, which is closely related to Verlet integration.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;x(t+\Delta t) = x(t) + v(t) \Delta t + \frac{2}{3}a(t) \Delta t^2 - \frac{1}{6} a(t - \Delta t) \Delta t^2 + O( \Delta t^4) &amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;v(t + \Delta t) = v(t) + \frac{1}{3}a(t + \Delta t) \Delta t + \frac{5}{6}a(t) \Delta t - \frac{1}{6}a(t - \Delta t) \Delta t + O(\Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where ''x'' is the position, ''v'' is the velocity, ''a'' is the acceleration, ''t'' is time, and ''\Delta t'' is the time-step.&lt;br /&gt;
&lt;br /&gt;
A predictor-corrector variant is useful when the forces are velocity-dependent:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    x(t+\Delta t) = x(t) + v(t) \Delta t + \frac{2}{3}a(t) \Delta t^2 - \frac{1}{6} a(t - \Delta t) \Delta t^2 + O( \Delta t^4).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The velocities at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t) (predicted) = v(t) + \frac{3}{2}a(t) \Delta t - \frac{1}{2}a(t - \Delta t) \Delta t + O( \Delta t^3)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The accelerations at time &amp;lt;math&amp;gt;t =t + \Delta t&amp;lt;/math&amp;gt; are then calculated from the positions and predicted velocities.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;    v(t + \Delta t) (corrected) = v(t) + \frac{1}{3}a(t + \Delta t) \Delta t + \frac{5}{6}a(t) \Delta t - \frac{1}{6}a(t - \Delta t) \Delta t + O( \Delta t^3) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Velocity Verlet algorithm]]&lt;br /&gt;
[[category: Molecular dynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Conferences</id>
		<title>Conferences</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Conferences"/>
				<updated>2010-04-09T09:25:19Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added 2011 conference&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The following is a chronological list of conferences, seminars, or meetings related to thermodynamics, statistical mechanics, soft condensed matter, many-body problems, complex fluids etc. &lt;br /&gt;
===2011===&lt;br /&gt;
====March====&lt;br /&gt;
*[http://19ectp.cheng.auth.gr  19th European Conference on Thermophysical Properties]  August 28 - September 1 2011 Thessaloniki (Greece)&lt;br /&gt;
===2010===&lt;br /&gt;
====April====&lt;br /&gt;
*[https://www.cecam.org/workshop-445.html Interatomic potentials for transition metals and their compounds]  April 12-14 2010  CECAM-ETHZ, Zurich, (Switzerland)&lt;br /&gt;
*[https://www.cecam.org/workshop-442.html Materials Informatics: Tools for Design and Discovery] April 19-21 2010  CECAM-HQ-EPFL, Lausanne, (Switzerland)&lt;br /&gt;
====May====&lt;br /&gt;
*[https://www.cecam.org/workshop-413.html Molecular Simulation of Clathrate Hydrates]  May 6-8 2010 ACAM, Dublin, (Ireland)&lt;br /&gt;
*[http://www.ppeppd2010.cn/ Properties and Phase Equilibria for Product and Process Design] May 16-21, 2010 Suzhou, Jiangsu (China)&lt;br /&gt;
*[https://www.cecam.org/workshop-458.html Dynamic coarse-graining: Towards quantitative mesoscale modeling of complex fluids]  May 19-21 2010 ACAM, Dublin, (Ireland)&lt;br /&gt;
====June====&lt;br /&gt;
*[https://www.cecam.org/workshop-382.html Advances in the Implementation of Polarizable Force Fields for Molecular Simulations]  June 7-9, 2010 CECAM-HQ-EPFL, Lausanne,(Switzerland)&lt;br /&gt;
*[http://liblice.icpf.cas.cz/2010/2010.php Eighth  Liblice Conference on the Statistical Mechanics of Liquids] June 13-18, 2010 Brno (Czech Republic)&lt;br /&gt;
*[http://www.mace.manchester.ac.uk/5thspheric 5th International SPHERIC SPH Workshop] June 23-25, 2010 Manchester (UK)&lt;br /&gt;
&lt;br /&gt;
====July====&lt;br /&gt;
*[http://ismc2010.ugr.es International Soft Matter Conference 2010] 5th-8th July 2010, Granada, Spain&lt;br /&gt;
*[http://www.statphys.org.au StatPhys 24: XXIV International Conference on Statistical Physics of the International Union for Pure and Applied Physics (IUPAP)] 19-23 July, (2010). Cairns (Australia)&lt;br /&gt;
*[https://www.cecam.org/workshop-472.html Crystallisation: from colloids to pharmaceuticals]  July 22-24, 2010 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo in the Apuan Alps VI] 24th-31st July 2010, Vallico Sotto, Italy&lt;br /&gt;
====August====&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program V] 1st-8th August 2010, Vallico Sotto (Italy)&lt;br /&gt;
*[http://ipht.cea.fr/Meetings/BegRohu2010/ Concepts and Methods of Statistical Mechanics] 23 August - 4 September 2010 Saint Pierre Quiberon (France)&lt;br /&gt;
&lt;br /&gt;
====September====&lt;br /&gt;
*[http://ergodic.ugr.es/cp 11th Granada Seminar: Foundations of Nonequilibrium Statistical Physics — From Basic Science to Future Challenges] 13-17  September, (2010). La Herradura, Granada (Spain)&lt;br /&gt;
*[http://tnt.phys.uniroma1.it/~transport/ Anomalous Transport: from Billiards to Nanosystems] 20-24 September 2010 Sperlonga (Italy)&lt;br /&gt;
====October====&lt;br /&gt;
*[http://www.pks.mpg.de/~fifcm10/ Fluctuation-Induced Forces in Condensed Matter] 11-15 October 2010 Dresden (Germany)&lt;br /&gt;
==Previous conferences==&lt;br /&gt;
Note: over time it is natural that more and more of these links will become broken. &lt;br /&gt;
=====2007=====&lt;br /&gt;
*[http://www.simbioma.cecam.org/ Simulation of Hard Bodies] April 16 to April 19 2007 in Lyon.&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 97th Statistical Mechanics Conference] May 6-8, 2007 Rutgers University&lt;br /&gt;
*[http://www.ucm.es/info/molecsim/luis/workshop.htm Workshop on Theory and Computer Simulations of Inhomogenoeus Fluids] May 16-18, 2007, Universidad Complutense, Madrid.&lt;br /&gt;
*[http://www-thphys.physics.ox.ac.uk/users/JuliaYeomans/OxfordWorkshop/home.php Mesoscale Modelling for Complex Fluids and Flows] June 25--27, 2007 University of Oxford, UK.&lt;br /&gt;
*[http://www.ecns2007.org 4th European Conference on Neutron Scattering] Lund, Sweden 25-29 June 2007&lt;br /&gt;
*[http://www.realitygrid.org/CompSci07 Computational Science 2007] 25-26 June 2007  The Royal Society, London&lt;br /&gt;
*[https://www.cecam.fr/index.php?content=activities/workshop New directions in liquid state theory] CECAM workshop, 2 - 4 July, 2007 at ENS, Lyon, France.&lt;br /&gt;
*[http://www.cecam.fr/index.php?content=activities/workshop&amp;amp;action=details&amp;amp;wid=157 Fluid phase behaviour and critical phenomena from liquid state theories and simulations] 5-7 July  2007 CECAM workshop, Lyon, France.&lt;br /&gt;
*[http://www.statphys23.org/ STATPHYS 23] Genova, Italy, from July 9 to 13, 2007.&lt;br /&gt;
*[http://www.iupac2007.org/ 41st IUPAC World Chemistry Conference] Turin, Italy, August 5-11th&lt;br /&gt;
*[http://www.srcf.ucam.org/~jae1001/ccp5_2007 CCP5 Annual Conference] 29th-31st August 2007 New Hall, Cambridge, UK&lt;br /&gt;
*[http://ccp2007.ulb.ac.be CCP 2007] Brussels  5-8 September  2007&lt;br /&gt;
*[http://www.castep.org CASTEP Workshop] 17th - 21st September 2007 University of York, UK&lt;br /&gt;
*[http://thermo2007.ifp.fr Thermodynamics 2007] 26-28 September 2007, IFP - Rueil-Malmaison (France)&lt;br /&gt;
*[http://www.iccmse.org/  International Conference of Computational Methods in Sciences and Engineering 2007] Corfu, Greece, 25-30 September 2007&lt;br /&gt;
*[http://www.chem.unisa.it/polnan/index.html Polymers in Nanotechnology] 27-28th September 2007, Salerno, Italy.&lt;br /&gt;
*[http://www.fz-juelich.de/iff/ismc2007/  International Soft Matter Conference 2007] 1 - 4 October 2007, Eurogress, Aachen (Germany)&lt;br /&gt;
*[http://www.escet.urjc.es/~fisica/encuentro_complejos/index.html II Meeting on Modelling of Complex Systems]  Universidad Rey Juan Carlos, Mostoles (Madrid), October 25-26 2007&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/SCD/event_22663.html Structuring Colloidal Dispersions by External Fields] 21 November 2007, Institute of Physics, London, United Kingdom&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 98th Statistical Mechanics Conference] December 16-18, 2007, Rutgers University, New Jersey, USA.&lt;br /&gt;
&lt;br /&gt;
=====2008=====&lt;br /&gt;
*[http://www.iop.org/activity/groups/subject/lcf/Events/file_25833.pdf Recent Advances in the Understanding of Confined Fluids: from Superfluids to Oil Reservoirs] 9-11 January, Cosener's House, Abingdon UK&lt;br /&gt;
*[http://academic.sun.ac.za/summerschool/2008.html  Workshop on Soft Condensed Matter and Physics of Biological Systems - Perspectives and topics for South Africa]  23 Jan 2008 - 1 Feb 2008 National Institute for Theoretical Physics at Stellenbosch Institute of Advanced Study, Stellenbosch, Western Cape, South Africa&lt;br /&gt;
*[http://bifi.unizar.es/events/bifi2008/main.htm Bifi 2008 Large Scale Simulations of Complex Systems, Condensed Matter and Fusion Plasma] 6–8 February 2008, Zaragoza, Spain&lt;br /&gt;
*[http://events.dechema.de/Tagungen/MolMod+Workshop.html International Workshop Molecular Modeling and Simulation in Applied Material Science] March 10-11,  DECHEMA-Haus, Frankfurt am Main, Germany&lt;br /&gt;
*[http://www.aps.org/meetings/march/index.cfm APS March Meeting] March 10-14, 2008. New Orleans, Louisiana, USA&lt;br /&gt;
*[http://users.physik.tu-muenchen.de/metz/jerusalem.html Modelling anomalous diffusion and relaxation]  23–28 March 2008, Jerusalem, Israel&lt;br /&gt;
*[http://www.newton.cam.ac.uk/programmes/CSM/csmw02.html Markov-Chain Monte Carlo Methods] 25 March to 28 March 2008 Isaac Newton Institute for Mathematical Sciences, Cambridge, UK &lt;br /&gt;
*[http://www.usal.es/~fises/ XV Congreso de Física Estadística (Fises' 08)] 27-29 March 2008, Salamanca, Spain&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/CMMP08/event_26545.html Condensed Matter and Materials Physics (CMMP)]  26-28 March 2008 Royal Holloway, University of London, UK&lt;br /&gt;
*[http://www.icmab.es/softmatter2008/index.html SoftMatter 2008] &amp;quot;Workshop on Electrostatic Effects in Soft Matter: Bringing Experiments, Theory and Simulation Together&amp;quot; 10 – 11 April ICMAB-CSIC, Barcelona, Spain.&lt;br /&gt;
*[http://www.icmab.es/11emscf/index.html 11th European Meeting on Supercritical Fluids] &amp;quot;New Perspectives in Supercritical Fluids: Nanoscience, Materials and Processing&amp;quot; 4-7 May 2008, ICMAB-CSIC, Barcelona, Spain&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 99th Statistical Mechanics Conference] May 11-13, 2008 Rutgers University,  USA&lt;br /&gt;
*[http://www.fondation-pgg.org/events/degennesdays/ DeGennesDays] 15-17 May 2008 Collège de France, Paris.&lt;br /&gt;
*[http://www.ill.fr/Events/rktsymposium/  Surfaces and Interfaces in Soft Matter and Biology SISMB 2008] &amp;quot;The impact and future of neutron reflectivity - A Symposium in Honor of Robert K. Thomas&amp;quot; 21-23 May 2008, Institut Laue-Langevin (Grenoble, France).&lt;br /&gt;
*[http://www.plmmp.univ.kiev.ua/ Physics of Liquid Matter: Modern Problems] May 23-26, 2008, Kyiv National Taras Shevchenko University, Ukraine&lt;br /&gt;
*[http://www.ffn.ub.es/sitges/ XXI Sitges Conference] XXI Sitges Conference on Statistical Mechanics. Statistical Mechanics of Molecular Biophysics  2nd-6th June 2008, Sitges, Spain&lt;br /&gt;
*[http://www1.ci.uc.pt/gcpi/poly2008 Polyelectrolytes 2008]  16th-19th June 2008, Coimbra, Portugal&lt;br /&gt;
*[http://www-spht.cea.fr/Meetings/BegRohu2008/index.html The Beg Rohu Summer School: Manifolds in random media, random matrices and extreme value statistics] 16th - 28th June 2008, French National Sailing School, Quiberon peninsula, France.&lt;br /&gt;
*[http://www.chm.bris.ac.uk/cms/ Computational Molecular Science 2008] 22nd – 25th June 2008, Cirencester, UK.&lt;br /&gt;
*[http://www.liquids2008.se/ 7th Liquid Matter Conference] 27 June - 1 July 2008  Lund, Sweden&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School 2008] University of Sheffield, England July 6 - July 15 2008.&lt;br /&gt;
*Potentials Workshop: Recent developments in interatomic potentials 7-8 July 2008  Oxford, UK&lt;br /&gt;
*[http://www.lcc-toulouse.fr/molmat2008/ MOLMAT2008 International Symposium on Molecular Materials based on Chemistry, Solid State Physics, Theory and Nanotechnology]   July 8-11th  2008 Toulouse, France&lt;br /&gt;
*[http://www2.polito.it/eventi/sigmaphi2008/ SigmaPhi2008] 14th -18th July 2008 Kolympari, Crete, Greece&lt;br /&gt;
*[http://www.cecam.org/workshop-188.html Dissipative Particle Dynamics: Addressing deficiencies and establishing new frontiers] July, 16th-18th 2008  CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/event_22243.html Molecular Dynamics for Non-Adiabatic Processes] 21 July 2008 to 22 July 2008 Institute of Physics, London&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcitaa_08/announcement.html Quantum Monte Carlo in the Apuan Alps IV] 26th July - Sat 2nd August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.cecam.org/workshop-215.html New directions in the theory and modelling of liquid crystals] July, 28th 2008 to July, 30th 2008, CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcatcp_08/announcement.html Quantum Monte Carlo and the CASINO program III] 3rd August - Sun 10th August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.icct2008.org/ 20th International Conference on Chemical Thermodynamics] August 3-8, 2008, Warsaw, Poland.&lt;br /&gt;
*[http://perso.ens-lyon.fr/thierry.dauxois/LORIS/LesHouchesSummerSchool2008.html Long-Range Interacting Systems] Summer School in Les Houches (France), 4-29 August 2008&lt;br /&gt;
*[http://ctbp.ucsd.edu/summer_school08/apply2008.html Coarse-Grained Physical Modeling of Biological Systems: Advanced Theory and Methods] August 11-15, 2008 University of California San Diego&lt;br /&gt;
*[http://www.chem.ucl.ac.uk/astrosurf/SIPML.html Surface and Interface Processes at the Molecular Level]  17 - 23 August 2008, Lucca, Italy&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD141/index.asp  Faraday Discussion 141: Water - From Interfaces to the Bulk] 27 - 29 August 2008 Heriot-Watt University, Edinburgh, United Kingdom&lt;br /&gt;
*[http://ectp18.conforganizer.net   18th European Conference on Thermophysical Properties]  31 Aug-4 Sep 2008 Pau, France&lt;br /&gt;
*[http://iber2008.df.fct.unl.pt/  9th Iberian Joint Meeting on Atomic and Molecular Physics - IBER 2008]  7-9th September,  Capuchos, Portugal&lt;br /&gt;
*[http://www.cmmp.ucl.ac.uk/~dmd/ccp5.htm  CCP5 Annual Meeting: Surfaces and Interfaces] 8-10th September, London, UK&lt;br /&gt;
*[http://ergodic.ugr.es/cp/ 10th  Granada  Seminar on Computational and Statistical Physics: Modeling and Simulation of New Materials] September 15-19, 2008 Granada, Spain&lt;br /&gt;
*[http://www.cecam.org/workshop-222.html Standardisation and databasing of ab-initio and classical simulations] September, 18th 2008 to September, 19th 2008  CECAM-ETHZ, Zurich, Switzerland&lt;br /&gt;
*[http://www.iccmse.org/ International Conference of Computational Methods in Sciences and Engineering 2008 (ICCMSE 2008)]  25-30 September, Crete, Greece&lt;br /&gt;
*[http://www.mmm2008.org/bin/view.pl/Main/WebHome Multscale Materials Modeling] 27–31 October 2008, Tallahassee, Florida USA&lt;br /&gt;
*[http://www.aiche.org/Conferences/AnnualMeeting/index.aspx 2008 AIChE Annual Meeting] November 16-21 2008 Philadelphia, Pennsylvania USA&lt;br /&gt;
*[http://www.ihp.jussieu.fr/ceb/Trimestres/T08-4/C3/index.html Statistical mechanics] Paris (France) 8-12 December 2008&lt;br /&gt;
*[http://complex.ffn.ub.es/bcnetworkshop BCNet Workshop] Trends and perspectives in complex networks. Barcelona (Spain) 10-12 December 2008&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 100th Statistical Mechanics Conference]  Rutgers University, (USA) 13-18 December 2008&lt;br /&gt;
=====2009=====&lt;br /&gt;
*[http://www.ccpb.ac.uk/events/conference/2009/ Biomolecular Simulation 2009] 6-8 January, Yorkshire Museum and Gardens, York, United Kingdom 2009&lt;br /&gt;
*[http://www.fisica.unam.mx/externos/wintermeeting/ XXXVIII edition of the Winter Meeting on Statistical Physics] Taxco, Guerrero (Mexico) 6th - 9th January, 2009.&lt;br /&gt;
*[http://www.ucl.ac.uk/msl/events/2009/workshop09.htm 2009 MSL Workshop: Accessing large length and time scales with accurate quantum methods]  12th - 13th January 2009 University College London (United Kingdom)&lt;br /&gt;
*[http://euler.us.es/%7Eopap/stochgame/index-en.html Stochastic Models in Physics, Biology, and Social Sciences] Carmona (Sevilla), Spain February 12-14 (2009)&lt;br /&gt;
*[http://hera.physik.uni-konstanz.de/igk/news/workshops/homepage/index.html Frontiers of Soft Condensed Matter 2009]  Les Houches () 15-20 February  2009&lt;br /&gt;
*[http://www.mpipks-dresden.mpg.de/~mbsffe09/ Many-body systems far from equilibrium: Fluctuations, slow dynamics and long-range interactions] Max Planck Institute for the Physics of Complex Systems Dresden, Germany February 16 - 27 (2009)&lt;br /&gt;
*[http://www.formulation.org.uk/Conference_flyers_Sept2007_on/Flyer-sims.pdf Workshop on advances in modelling for formulations]  25th of March 2009 at GSK Waybridge (United Kingdom)&lt;br /&gt;
*[http://www.physik.uni-leipzig.de/~janke/meco34/ 34th Conference of the Middle European Cooperation in Statistical Physics] 30 March - 01 April 2009 Universität Leipzig (Germany)&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws2/ Workshop II: The Boltzmann Equation: DiPerna-Lions Plus 20 Years] April 15-17 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-313.html Computational Studies of Defects in Nanoscale Carbon Materials]  May 11, 2009 to May 13, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.cecam.org/workshop-320.html Modeling of Carbon and Inorganic Nanotubes and Nanostructures]  May 13, 2009 to May 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ima.umn.edu/2008-2009/W5.18-22.09/ Molecular Simulations: Algorithms, Analysis, and Applications] Institute for Mathematics and its Applications, University of Minnesota (USA), May 18-22, 2009&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws4/ Workshop IV: Asymptotic Methods for Dissipative Particle Systems] May 18-22 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-310.html Computer Simulation in Food Science: CFD meets Soft Matter]  May 25, 2009 to May 27, 2009 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://complenet09.diit.unict.it  CompleNet 2009] International Workshop on Complex Networks. Catania (Italy),  May 26-28, 2009&lt;br /&gt;
*[http://go.warwick.ac.uk/maths/research/events/2008_2009/symposium/wks5/ EPSRC Symposium Workshop on Molecular Dynamics] Monday 1 – Friday 5 June (2009) Warwick (United Kingdom)&lt;br /&gt;
*[http://www.cecam.org/workshop-272.html Theoretical Modeling of Transport in Nanostructures]  June 2, 2009 to June 5, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland) &lt;br /&gt;
*[http://www.mpip-mainz.mpg.de/mmsd/ Mainz Materials Simulation Days] 3-5 June 2009 Max Planck Institute for Polymer Research (Germany)&lt;br /&gt;
*[http://www.soms.ethz.ch/workshop2009 Coping with Crises in Complex Socio-Economic Systems] ETH Zurich (Switzerland), June 8-13, 2009&lt;br /&gt;
*[[MOSSNOHO Workshop 2009]] 16 of June 2009, Universidad Complutense de Madrid (Spain)&lt;br /&gt;
*[http://cftc.cii.fc.ul.pt/Workshops/flowNjam/index.html Flow(ers) and jam(mers): from liquid crystals to grains] Lisbon (Portugal) 17-19 June 2009&lt;br /&gt;
*[http://ipht.cea.fr/Meetings/BegRohu2009/ Beg Rohu Summer School: Quantum Physics Out of Equilibrium] Ecole Nationale de Voile (France) 15-27 June 2009&lt;br /&gt;
*[http://symp17.boulder.nist.gov  Seventeenth Symposium on Thermophysical Properties] Boulder, Colorado (USA), June 21-26, 2009&lt;br /&gt;
*[http://www.fhi-berlin.mpg.de/th/Meetings/DFT-workshop-Berlin2009/ Hands-on Tutorial on Ab Initio Molecular Simulations: Toward a First-Principles Understanding of Materials Properties and Functions] Berlin (Germany) June 22-July 1 2009&lt;br /&gt;
*[https://www.irphe.univ-mrs.fr/~fe09 Fluid and Elasticity] Carry-le-Rouet, near Marseilles (France) June 23-26, 2009&lt;br /&gt;
*[http://www.icmp.lviv.ua/statphys2009/ Statistical Physics: Modern Trends and Applications] June 23-25, 2009 Lviv, (Ukraine)&lt;br /&gt;
*[http://www.fuw.edu.pl/~wssph/ 3rd Warsaw School of Statistical Physics] Kazimierz Dolny (Poland), 27 June - 4 July, 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-298.html Modeling and Simulation of Water at Interfaces from Ambient to Supercooled Conditions] June 29, 2009 to July 1, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School] University of Sheffield  (England) July 5 - July 14 2009 &lt;br /&gt;
*[http://math.arizona.edu/~goriely/leshouches/home.html  New trends in the Physics and Mechanics of Biological Systems&amp;quot;]  Les Houches (France), 6-31 July 2009&lt;br /&gt;
*[http://research.yale.edu/boulder/Boulder-2009/index.html Nonequilibrium Statistical Mechanics: Fundamental Problems and Applications] July 6-24  2009 Boulder (USA)&lt;br /&gt;
*[http://www.xrqtc.cat/index.php/ca/homew New trends in Computational Chemistry for Industry Applications] July 6-7 Barcelona (Spain)&lt;br /&gt;
*[http://www.frias.uni-freiburg.de/BFF Computational Methods for Soft Matter and Biological Systems] July 8-11, 2009, FRIAS, Freiburg (Germany)&lt;br /&gt;
*[http://www.cecam.org/workshop-286.html Structural Transitions in Solids: Theory, Simulations, Experiments and Visualization Techniques] July 8, 2009 to July 11, 2009 CECAM-USI, Lugano (Switzerland)&lt;br /&gt;
*[http://fomms.org FOMMS 2009, Fourth International Conference Foundations of Molecular Modeling and Simulation] Semiahmoo Resort, Blaine, WA (USA)  12-16 July 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-308.html Computer Simulation Approaches to Study Self-Assembly: From Patchy Nano-Colloids to Virus Capsids]  July 13, 2009 to July 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.md-net.org.uk/events/bath_jul_2009.htm EPSRC Network Mathematical Challenges of Molecular Dynamics] 13-15 July (2009) Bath, United Kingdom.&lt;br /&gt;
*[http://www.cecam.org/workshop-279.html New Trends in Simulating Colloids: from Models to Applications] July 15, 2009 to July 18, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD144/index.asp Faraday Discussion 144: Multiscale Modelling of Soft Matter] University of Groningen (The Netherlands) 20 - 22 July 2009&lt;br /&gt;
*[http://www2.yukawa.kyoto-u.ac.jp/~ykis2009/Welcome.html Frontiers in Nonequilibrium Physics: Fundamental Theory, Glassy &amp;amp; Granular Materials, and Computational Physics] July 21 - August 21, 2009  Kyoto (Japan)&lt;br /&gt;
*[http://www.cecam.org/workshop-293.html Fundamental Aspects of Deterministic Thermostats] July 27, 2009 to July 29, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program IV]  2nd-9th August 2009 Towler Institute, Tuscany, (Italy)&lt;br /&gt;
*[http://www.warwick.ac.uk/go/quantsim09  EPSRC Symposium Workshop on Quantum Simulations] 24th-28th August 2009 University of Warwick (United Kingdom)&lt;br /&gt;
*[http://itf.fys.kuleuven.be/~fpspXII/ Fundamental Problems in Statistical Physics XII] August 31 - September 11, 2009 Leuven (Belgium)&lt;br /&gt;
*[http://denali.phys.uniroma1.it/~idmrcs6/ 6th International Discussion Meeting on Relaxations in Complex Systems] August 31- September 5, 2009, Roma (Italy)&lt;br /&gt;
*[http://www.dft09.org/ International Conference on the Applications of Density Functional Theory in Chemistry and Physics] August 31st to September 4th 2009  Lyon (France)&lt;br /&gt;
*[http://www.dfrl.ucl.ac.uk/CCP5/ccp5.htm CCP5 Annual Meeting 2009 Structure Prediction]  7th to  9th, September 2009 London (United Kingdom)&lt;br /&gt;
*[http://fises.dfa.uhu.es/fises09/ XVI Congreso de Física Estadística] Huelva, 10-12  September  2009, Spain&lt;br /&gt;
*[http://th-www.if.uj.edu.pl/zfs/smoluchowski/ 22nd Marian Smoluchowski Symposium On Statistical Physics] 12-17 September 2009 Zakopane (Poland)&lt;br /&gt;
*[http://www.isis.rl.ac.uk/largescale/loq/SAS2009/SAS2009.htm SAS-2009] XIV International Conference on Small-Angle Scattering, Sunday 13 - Friday 18 September, 2009, Oxford (UK)&lt;br /&gt;
*[http://www.esc.sandia.gov/dsmc09/dsmc09.html Direct Simulation Monte Carlo workshop] September 13-16, 2009 Santa Fe, New Mexico, USA,&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/PHYSASPECTS_09/index.html Physical Aspects of Polymer Science] 14-16 September 2009 Bristol (United Kingdom)&lt;br /&gt;
*[http://www.thermodynamics2009.org/ Thermodynamics 2009] September 23-25  Imperial College London , U.K. (2009)&lt;br /&gt;
*[http://www.crm.cat/wkstatisticalphysics/ Techniques and Challenges from Statistical Physics] October 14 to 16, 2009 Barcelona, (Spain)&lt;br /&gt;
*[http://paginas.fe.up.pt/~equifase/ EQUIFASE 2009] VIII Iberoamerican Conference on Phase Equilibria and Fluid Properties for Process Design, Praia da Rocha, Portugal 17-21 October 2009&lt;br /&gt;
*[http://cint.lanl.gov/workshop2009/ Multiple Length Scales in Polymers and Complex Fluids] October 18-21, 2009 Bishop's Lodge, Santa Fe (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-290.html Classical Density Functional Theory Methods in Soft and Hard Matter] October 21, 2009 to October 23, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://seneca.fis.ucm.es/parr/ktlog2_09 kTlog2 '09: Computing Matters Workshop] 22-24 October, 2009, Toledo (Spain)&lt;br /&gt;
*[https://www.cecam.org/workshop-325.html Linking Systems Biology and Biomolecular Simulations]  November 16-19 2009 CECAM Lausanne, (Switzerland) &lt;br /&gt;
*[http://www.lorentzcenter.nl/lc/web/2009/357/info.php3?wsid=357 Subdivide and Tile: Triangulating spaces for understanding the world] November 16 to 20 2009, Leiden (Netherlands)&lt;br /&gt;
*[http://www.dfi.uchile.cl/~granular09/Welcome.html Southern Workshop on Granular Materials 2009 - SWGM09] November 30 to December 4 2009, Viña del Mar (Chile)&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 102nd Statistical Mechanics Conference]  Rutgers University, December 13-15, 2009 (USA)&lt;br /&gt;
*[http://www.cmmp.org.uk/ Condensed Matter and Materials Physics (CMMP)] 15-17 December 2009 Warwick University (United Kingdom)&lt;br /&gt;
=====2010=====&lt;br /&gt;
*[http://ddays2010.northwestern.edu Dynamics Days] January 4-7, 2010 Evanston Illinois (USA)&lt;br /&gt;
*[http://www2.surrey.ac.uk/maths/news/events/2010/emerging_interfaces_workshop.htm Emerging Interfacial Dynamics] January 6-8 University of Surrey (UK)&lt;br /&gt;
*[http://www.comphys.ethz.ch/jstat/    Journées de Physique Statistique 2010] 28-29 January 2010 Paris (France)&lt;br /&gt;
*[http://www.theory.caltech.edu/~ooguri/CMP-HEP/CMP-HEP.htm Condensed Matter Physics Meets High Energy Physics] University of Tokyo, February 8-12, 2010 (Japan)&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/2010/CFFI10/index.html Complex Fluid-Fluid Interfaces] 25 February 2010 Institute of Physics, London (UK)&lt;br /&gt;
*[http://tfy.tkk.fi/soft/levi2010/ International Workshop on Coarse-Grained Biomolecular Modeling] 7-12 March, Levi, (Finland)&lt;br /&gt;
*[http://www.lpm.u-nancy.fr/webperso/chatelain.c/GrpPhysStat/Meco35/index.php 35th Conference of the Middle European Cooperation in Statistical Physics] March 15th - 19th, 2010 Pont-à-Mousson (France)&lt;br /&gt;
&lt;br /&gt;
__NOTOC__&lt;br /&gt;
[[category: Miscellaneous]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature</id>
		<title>Inverse temperature</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature"/>
				<updated>2010-03-04T11:15:36Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: cleaned a bit, added reference to quantum stat. mech.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;It is often convenient to define a dimensionless ''inverse'' temperature, &amp;lt;math&amp;gt;\beta&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This notation likely comes from its origin as a Lagrangian multiplier, for which Greek letters are customarily written.&lt;br /&gt;
&lt;br /&gt;
Indeed, it shown in Ref. 1 (pp. 79-85) that this is the way it enters. The task is to maximize number of ways $N$ particles may be asigned to $K$ space-momentum cells, such that one has a set of occupation numbers &amp;lt;math&amp;gt;n_i&amp;lt;/math&amp;gt;. Introducing the  [[partition function]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Omega\propto\frac{N!}{n_1! n_2! \ldots n_K!} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
one could maximize its logarithm (a monotonous function):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\log \Omega \approx \log N -N - \sum_ i ( \log n_i + n_i) + \mathrm{consts} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where [[Stirling's approximation]] for large numbers has been used. The maximization must be performed subject to the constraint:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_i n_i=N&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
An additional constraint, which applies only to dilute gases, is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_i n_i e_i=E, &amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;E&amp;lt;/math&amp;gt; is the total energy and &amp;lt;math&amp;gt;e_i=p_i^2/2m&amp;lt;/math&amp;gt; is the energy of cell &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The method of [[Lagrange multipliers]] entails finding the extremum of the function&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;L=\log\Omega - \alpha (\sum_i n_i - N ) - \beta ( \sum_i n_i e_i - E  ),&amp;lt;/math&amp;gt;&lt;br /&gt;
where the two Lagrange multipliers enforce the two conditions and permit the treatment of&lt;br /&gt;
the occupations as independent variables. The minimization leads to&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;n_i=C e^{-\beta e_i}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and an application to the case of an ideal gas reveals the connection with the temperature,&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT} .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Similar methods are used for [[quantum statistics]] of dilute gases (Ref. 1, pp. 179-185).&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
#Kerson Huang, &amp;quot;Statistical Physics&amp;quot; John Wiley and Sons, second edition (1987)&lt;br /&gt;
[[category: Classical thermodynamics]]&lt;br /&gt;
[[category: statistical mechanics]]&lt;br /&gt;
[[category: Non-equilibrium thermodynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature</id>
		<title>Inverse temperature</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature"/>
				<updated>2010-03-04T11:07:18Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Eqn fixed&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;It is often convenient to define a dimensionless ''inverse'' temperature, &amp;lt;math&amp;gt;\beta&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This notation likely comes from its origin as a Lagrangian multiplier, for which Greek letters are customarily written.&lt;br /&gt;
&lt;br /&gt;
Indeed, it shown in Ref. 1 that this is the way it enters. The task is to maximize number of ways $N$ particles may be asigned to $K$ space-momentum cells, such that one has a set of occupation numbers &amp;lt;math&amp;gt;n_i&amp;lt;/math&amp;gt;. Introducing the  [[partition function]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Omega\propto\frac{N!}{n_1! n_2! \ldots n_K!} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
one could maximize its logarithm (a monotonous function):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\log \Omega \approx \log N -N - \sum_ i ( \log n_i + n_i) + \mathrm{consts} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where [[Stirling's approximation]] for large numbers has been used. The maximization must be performed subject to the constraint:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_i n_i=N&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
An additional constraint, which applies only to dilute gases, is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_i n_i e_i=E&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;E&amp;lt;/math&amp;gt; is the total energy and &amp;lt;math&amp;gt;e_i=p_i^2/2m&amp;lt;/math&amp;gt; is the energy of cell &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The method of [[Lagrange multipliers]] entail finding the extremum of the function&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;L=\log\Omega - \alpha (\sum_i n_i - N ) - \beta ( \sum_i n_i e_i - E  )&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where the two Lagrange multipliers enforce the two conditions and permit the treatment of&lt;br /&gt;
the occupations as independent variables. The minimization leads to&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;n_i=C e^{-\beta e_i}, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and an application to the case of an ideal gas reveals the connection with the temperature,&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT} .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
#Kerson Huang, &amp;quot;Statistical Physics&amp;quot; John Wiley and Sons, second edition, pp. 79-85  (1987)&lt;br /&gt;
[[category: Classical thermodynamics]]&lt;br /&gt;
[[category: statistical mechanics]]&lt;br /&gt;
[[category: Non-equilibrium thermodynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature</id>
		<title>Inverse temperature</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature"/>
				<updated>2010-03-04T11:04:25Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;It is often convenient to define a dimensionless ''inverse'' temperature, &amp;lt;math&amp;gt;\beta&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This notation likely comes from its origin as a Lagrangian multiplier, for which Greek letters are customarily written.&lt;br /&gt;
&lt;br /&gt;
Indeed, it shown in Ref. 1 that this is the way it enters. The task is to maximize number of ways $N$ particles may be asigned to $K$ space-momentum cells, such that one has a set of occupation numbers &amp;lt;math&amp;gt;n_i&amp;lt;/math&amp;gt;. Introducing the  [[partition function]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Omega\propto\frac{N!}{n_1! n_2! \ldots n_K!} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
one could maximize its logarithm (a monotonous function):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\log \Omega \approx \log N -N - \sum_ i ( \log n_i + n_i) + \mathrm{consts} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where [[Stirling's approximation]] for large numbers has been used. The maximization must be performed subject to the constraint:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_i n_i=N&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
An additional constraint, which applies only to dilute gases, is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_i n_i e_i=E&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;E&amp;lt;/math&amp;gt; is the total energy and &amp;lt;math&amp;gt;e_i=p_i^2/2m&amp;lt;/math&amp;gt; is the energy of cell &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The method of [[Lagrange multipliers]] entail finding the extremum of the function&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;L=\log\Omega - \alpha (\sum_i n_i - N ) - \beta ( \sum_i n_i e_i - E  )&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
where the two Lagrange multipliers enforce the two conditions and permit the treatment of&lt;br /&gt;
the occupations as independent variables. The minimization leads to&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;n_i=Ce^{-\beta e_i), &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and an application to the case of an ideal gas reveals the connection with the temperature,&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT} .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
#Kerson Huang, &amp;quot;Statistical Physics&amp;quot; John Wiley and Sons, second edition, pp. 79-85  (1987)&lt;br /&gt;
[[category: Classical thermodynamics]]&lt;br /&gt;
[[category: statistical mechanics]]&lt;br /&gt;
[[category: Non-equilibrium thermodynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature</id>
		<title>Inverse temperature</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Inverse_temperature"/>
				<updated>2010-03-04T10:56:28Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: temp save&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;It is often convenient to define a dimensionless ''inverse'' temperature, &amp;lt;math&amp;gt;\beta&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This notation likely comes from its origin as a Lagrangian multiplier, for which Greek letters are customarily written.&lt;br /&gt;
&lt;br /&gt;
Indeed, it shown in Ref. 1 that this is the way it enters. The task is to maximize number of ways $N$ particles may be asigned to $K$ space-momentum cells. Introducing the  [[partition function]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Omega\propto\frac{N!}{n_1! n_2! \ldots n_K!} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
one could maximize its logarithm (a monotonous function):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\log \Omega \approx \log N -N - \sum_ i ( \log n_i + n_i) + \mathrm{consts} ,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where [[Stirling's approximation]] for large numbers has been used.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
#Kerson Huang, &amp;quot;Statistical Physics&amp;quot; John Wiley and Sons, second edition, pp. 79-85  (1987)&lt;br /&gt;
[[category: Classical thermodynamics]]&lt;br /&gt;
[[category: statistical mechanics]]&lt;br /&gt;
[[category: Non-equilibrium thermodynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Temperature</id>
		<title>Temperature</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Temperature"/>
				<updated>2010-03-04T10:28:06Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Link to (new) inverse T&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The '''temperature''' of a system in [[classical thermodynamics]] is  intimately related to the [[zeroth law of thermodynamics]]; two systems having to have the same temperature if they are to be in thermal equilibrium (i.e. there is no net [[heat]] flow between them).&lt;br /&gt;
However, it is most useful to have a temperature scale.&lt;br /&gt;
By making use of the [[Equation of State: Ideal Gas |ideal gas law]] one can define an absolute temperature&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;T = \frac{pV}{Nk_B}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
however, perhaps a better definition of temperature is &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{1}{T(E,V,N)} = \left. \frac{\partial S}{\partial E}\right\vert_{V,N}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; is the [[entropy]].&lt;br /&gt;
==Units==&lt;br /&gt;
Temperature has the SI units of ''kelvin'' (K) (named in honour of [[William Thomson]]) The kelvin is the fraction 1/273.16 of the thermodynamic temperature of the [[triple point]] of [[water]].&lt;br /&gt;
====External links====&lt;br /&gt;
*[http://physics.nist.gov/cuu/Units/kelvin.html NIST reference page]&lt;br /&gt;
&lt;br /&gt;
==Kinetic temperature==&lt;br /&gt;
:&amp;lt;math&amp;gt;T = \frac{2}{3} \frac{1}{k_B} \overline {\left(\frac{1}{2}m_i v_i^2\right)}&amp;lt;/math&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
where &amp;lt;math&amp;gt;k_B&amp;lt;/math&amp;gt; is the [[Boltzmann constant]].  The kinematic temperature so defined is related to the [[equipartition]] theorem; for more details, see [http://clesm.mae.ufl.edu/wiki.pub/index.php/Configuration_integral_%28statistical_mechanics%29 Configuration integral].&lt;br /&gt;
&lt;br /&gt;
==Configurational temperature==&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevLett.78.772 Hans Henrik Rugh &amp;quot;Dynamical Approach to Temperature&amp;quot;, Physical Review Letters ''' 78''' pp. 772-774 (1997)]&lt;br /&gt;
*[http://dx.doi.org/10.1063/1.480995 András Baranyai &amp;quot;On the configurational temperature of simple fluids&amp;quot;, Journal of Chemical Physics '''112''' pp. 3964-3966 (2000)]&lt;br /&gt;
&lt;br /&gt;
==Non-equilibrium temperature==&lt;br /&gt;
*[http://dx.doi.org/10.1063/1.2743032     Alexander V. Popov and Rigoberto Hernandez &amp;quot;Ontology of temperature in nonequilibrium systems&amp;quot;, Journal of Chemical Physics '''126''' 244506 (2007)]&lt;br /&gt;
*[http://dx.doi.org/10.1063/1.2958913  J.-L. Garden, J. Richard, and H. Guillou &amp;quot;Temperature of systems out of thermodynamic equilibrium&amp;quot;, Journal of Chemical Physics '''129''' 044508 (2008)]&lt;br /&gt;
&lt;br /&gt;
==Inverse temperature==&lt;br /&gt;
It is frequently convenient to define a so-called [[inverse temperature]], &amp;lt;math&amp;gt;\beta&amp;lt;/math&amp;gt;, such that&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\beta := \frac{1}{k_BT}&amp;lt;/math&amp;gt;&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Thermostats | Thermostats in molecular dynamics]]&lt;br /&gt;
==References==&lt;br /&gt;
#William Thomson &amp;quot;On an Absolute Thermometric Scale, founded on Carnot's Theory of the Motive Power of Heat, and calculated from the Results of Regnault's Experiments on the Pressure and Latent Heat of Steam&amp;quot;, Philosophical Magazine '''October''' pp.  (1848)&lt;br /&gt;
#[http://dx.doi.org/10.1088/0026-1394/27/1/002 H. Preston-Thomas &amp;quot;The International Temperature Scale of 1990 (ITS-90)&amp;quot;, Metrologia '''27''' pp. 3-10  (1990)]&lt;br /&gt;
#[http://dx.doi.org/10.1088/0026-1394/27/2/010 H. Preston-Thomas &amp;quot;ERRATUM: The International Temperature Scale of 1990 (ITS-90)&amp;quot;, Metrologia '''27''' p. 107 (1990)]&lt;br /&gt;
[[category: Classical thermodynamics]]&lt;br /&gt;
[[category: statistical mechanics]]&lt;br /&gt;
[[category: Non-equilibrium thermodynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Gauss_theorem</id>
		<title>Gauss theorem</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Gauss_theorem"/>
				<updated>2010-02-05T14:35:24Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Some math...&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{stub-general}}&lt;br /&gt;
Also known as '''divergence theorem'''. For a scalar field &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt;:&lt;br /&gt;
:&amp;lt;math&amp;gt;    \int_{\partial\Omega} A \cdot d\vec{S} = \int_\Omega \nabla A dV .&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
It trivialy generalizes to vector fields, by applying it to each Cartesian component.&lt;br /&gt;
&lt;br /&gt;
[[category: mathematics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Continuity_equation</id>
		<title>Continuity equation</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Continuity_equation"/>
				<updated>2010-02-05T14:32:53Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Some hydrodynamics ...&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Stub-general}}&lt;br /&gt;
The '''continuity equation''' expresses the conservation of mass. It is a direct consequence of [[Gauss theorem]].&lt;br /&gt;
&lt;br /&gt;
If the mass enclosed in a region &amp;lt;math&amp;gt;\Omega&amp;lt;/math&amp;gt; is &amp;lt;math&amp;gt;M&amp;lt;/math&amp;gt;, by definition of mass density &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;M=\int_\Omega \rho dV .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The net loss of matter in this region must be caused by an outward flow &amp;lt;math&amp;gt;\rho \vec{v}&amp;lt;/math&amp;gt; across its boundary:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\partial M}{\partial t}= - \int_{\partial\Omega} \rho \vec{v} \cdot d\vec{S} .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
According to [[Gauss theorem]],&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\int_{\partial\Omega} \rho \vec{v} \cdot d\vec{S} = \int_\Omega \nabla( \rho \vec{v} ) dV  .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Since the region is a general one, and it does not change with time, the resulting equation is&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{\partial \rho}{\partial t} + \nabla (\rho \vec{v}) =0 .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
As a direct consequence an incompressible fluid, with constant &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt;, implies a [[solenoidal]] velocity field: &lt;br /&gt;
&amp;lt;math&amp;gt; \nabla \vec{v} =0 &amp;lt;/math&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Conferences</id>
		<title>Conferences</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Conferences"/>
				<updated>2010-02-05T14:20:24Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added SPH conference&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The following is a chronological list of conferences, seminars, or meetings related to thermodynamics, statistical mechanics, soft condensed matter, many-body problems, complex fluids etc. &lt;br /&gt;
===2010===&lt;br /&gt;
====February====&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/2010/CFFI10/index.html Complex Fluid-Fluid Interfaces] 25 February 2010 Institute of Physics, London (UK)&lt;br /&gt;
*[http://www.theory.caltech.edu/~ooguri/CMP-HEP/CMP-HEP.htm Condensed Matter Physics Meets High Energy Physics] University of Tokyo, February 8-12, 2010 (Japan)&lt;br /&gt;
====March====&lt;br /&gt;
*[http://tfy.tkk.fi/soft/levi2010/ International Workshop on Coarse-Grained Biomolecular Modeling] 7-12 March, Levi, (Finland)&lt;br /&gt;
*[http://www.lpm.u-nancy.fr/webperso/chatelain.c/GrpPhysStat/Meco35/index.php 35th Conference of the Middle European Cooperation in Statistical Physics] March 15th - 19th, 2010 Pont-à-Mousson (France)&lt;br /&gt;
====April====&lt;br /&gt;
*[https://www.cecam.org/workshop-445.html Interatomic potentials for transition metals and their compounds]  April 12-14 2010  CECAM-ETHZ, Zurich, (Switzerland)&lt;br /&gt;
*[https://www.cecam.org/workshop-442.html Materials Informatics: Tools for Design and Discovery] April 19-21 2010  CECAM-HQ-EPFL, Lausanne, (Switzerland)&lt;br /&gt;
====May====&lt;br /&gt;
*[https://www.cecam.org/workshop-413.html Molecular Simulation of Clathrate Hydrates]  May 6-8 2010 ACAM, Dublin, (Ireland)&lt;br /&gt;
*[http://www.ppeppd2010.cn/ Properties and Phase Equilibria for Product and Process Design] May 16-21, 2010 Suzhou, Jiangsu (China)&lt;br /&gt;
*[https://www.cecam.org/workshop-458.html Dynamic coarse-graining: Towards quantitative mesoscale modeling of complex fluids]  May 19-21 2010 ACAM, Dublin, (Ireland)&lt;br /&gt;
====June====&lt;br /&gt;
*[https://www.cecam.org/workshop-382.html Advances in the Implementation of Polarizable Force Fields for Molecular Simulations]  June 7-9, 2010 CECAM-HQ-EPFL, Lausanne,(Switzerland)&lt;br /&gt;
*[http://liblice.icpf.cas.cz/2010/2010.php Eighth  Liblice Conference on the Statistical Mechanics of Liquids] June 13-18, 2010 Brno (Czech Republic)&lt;br /&gt;
*[http://www.mace.manchester.ac.uk/5thspheric 5th International SPHERIC SPH Workshop] June 23-25, 2010 Manchester (UK)&lt;br /&gt;
&lt;br /&gt;
====July====&lt;br /&gt;
*[http://ismc2010.ugr.es International Soft Matter Conference 2010] 5th-8th July 2010, Granada, Spain&lt;br /&gt;
*[http://www.statphys.org.au StatPhys 24: XXIV International Conference on Statistical Physics of the International Union for Pure and Applied Physics (IUPAP)] 19-23 July, (2010). Cairns (Australia)&lt;br /&gt;
*[https://www.cecam.org/workshop-472.html Crystallisation: from colloids to pharmaceuticals]  July 22-24, 2010 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo in the Apuan Alps VI] 24th-31st July 2010, Vallico Sotto, Italy&lt;br /&gt;
====August====&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program V] 1st-8th August 2010, Vallico Sotto, Italy&lt;br /&gt;
====September====&lt;br /&gt;
*[http://ergodic.ugr.es/cp 11th Granada Seminar: Foundations of Nonequilibrium Statistical Physics — From Basic Science to Future Challenges] 13-17  September, (2010). La Herradura, Granada (Spain)&lt;br /&gt;
&lt;br /&gt;
==Previous conferences==&lt;br /&gt;
Note: over time it is natural that more and more of these links will become broken. &lt;br /&gt;
=====2007=====&lt;br /&gt;
*[http://www.simbioma.cecam.org/ Simulation of Hard Bodies] April 16 to April 19 2007 in Lyon.&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 97th Statistical Mechanics Conference] May 6-8, 2007 Rutgers University&lt;br /&gt;
*[http://www.ucm.es/info/molecsim/luis/workshop.htm Workshop on Theory and Computer Simulations of Inhomogenoeus Fluids] May 16-18, 2007, Universidad Complutense, Madrid.&lt;br /&gt;
*[http://www-thphys.physics.ox.ac.uk/users/JuliaYeomans/OxfordWorkshop/home.php Mesoscale Modelling for Complex Fluids and Flows] June 25--27, 2007 University of Oxford, UK.&lt;br /&gt;
*[http://www.ecns2007.org 4th European Conference on Neutron Scattering] Lund, Sweden 25-29 June 2007&lt;br /&gt;
*[http://www.realitygrid.org/CompSci07 Computational Science 2007] 25-26 June 2007  The Royal Society, London&lt;br /&gt;
*[https://www.cecam.fr/index.php?content=activities/workshop New directions in liquid state theory] CECAM workshop, 2 - 4 July, 2007 at ENS, Lyon, France.&lt;br /&gt;
*[http://www.cecam.fr/index.php?content=activities/workshop&amp;amp;action=details&amp;amp;wid=157 Fluid phase behaviour and critical phenomena from liquid state theories and simulations] 5-7 July  2007 CECAM workshop, Lyon, France.&lt;br /&gt;
*[http://www.statphys23.org/ STATPHYS 23] Genova, Italy, from July 9 to 13, 2007.&lt;br /&gt;
*[http://www.iupac2007.org/ 41st IUPAC World Chemistry Conference] Turin, Italy, August 5-11th&lt;br /&gt;
*[http://www.srcf.ucam.org/~jae1001/ccp5_2007 CCP5 Annual Conference] 29th-31st August 2007 New Hall, Cambridge, UK&lt;br /&gt;
*[http://ccp2007.ulb.ac.be CCP 2007] Brussels  5-8 September  2007&lt;br /&gt;
*[http://www.castep.org CASTEP Workshop] 17th - 21st September 2007 University of York, UK&lt;br /&gt;
*[http://thermo2007.ifp.fr Thermodynamics 2007] 26-28 September 2007, IFP - Rueil-Malmaison (France)&lt;br /&gt;
*[http://www.iccmse.org/  International Conference of Computational Methods in Sciences and Engineering 2007] Corfu, Greece, 25-30 September 2007&lt;br /&gt;
*[http://www.chem.unisa.it/polnan/index.html Polymers in Nanotechnology] 27-28th September 2007, Salerno, Italy.&lt;br /&gt;
*[http://www.fz-juelich.de/iff/ismc2007/  International Soft Matter Conference 2007] 1 - 4 October 2007, Eurogress, Aachen (Germany)&lt;br /&gt;
*[http://www.escet.urjc.es/~fisica/encuentro_complejos/index.html II Meeting on Modelling of Complex Systems]  Universidad Rey Juan Carlos, Mostoles (Madrid), October 25-26 2007&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/SCD/event_22663.html Structuring Colloidal Dispersions by External Fields] 21 November 2007, Institute of Physics, London, United Kingdom&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 98th Statistical Mechanics Conference] December 16-18, 2007, Rutgers University, New Jersey, USA.&lt;br /&gt;
&lt;br /&gt;
=====2008=====&lt;br /&gt;
*[http://www.iop.org/activity/groups/subject/lcf/Events/file_25833.pdf Recent Advances in the Understanding of Confined Fluids: from Superfluids to Oil Reservoirs] 9-11 January, Cosener's House, Abingdon UK&lt;br /&gt;
*[http://academic.sun.ac.za/summerschool/2008.html  Workshop on Soft Condensed Matter and Physics of Biological Systems - Perspectives and topics for South Africa]  23 Jan 2008 - 1 Feb 2008 National Institute for Theoretical Physics at Stellenbosch Institute of Advanced Study, Stellenbosch, Western Cape, South Africa&lt;br /&gt;
*[http://bifi.unizar.es/events/bifi2008/main.htm Bifi 2008 Large Scale Simulations of Complex Systems, Condensed Matter and Fusion Plasma] 6–8 February 2008, Zaragoza, Spain&lt;br /&gt;
*[http://events.dechema.de/Tagungen/MolMod+Workshop.html International Workshop Molecular Modeling and Simulation in Applied Material Science] March 10-11,  DECHEMA-Haus, Frankfurt am Main, Germany&lt;br /&gt;
*[http://www.aps.org/meetings/march/index.cfm APS March Meeting] March 10-14, 2008. New Orleans, Louisiana, USA&lt;br /&gt;
*[http://users.physik.tu-muenchen.de/metz/jerusalem.html Modelling anomalous diffusion and relaxation]  23–28 March 2008, Jerusalem, Israel&lt;br /&gt;
*[http://www.newton.cam.ac.uk/programmes/CSM/csmw02.html Markov-Chain Monte Carlo Methods] 25 March to 28 March 2008 Isaac Newton Institute for Mathematical Sciences, Cambridge, UK &lt;br /&gt;
*[http://www.usal.es/~fises/ XV Congreso de Física Estadística (Fises' 08)] 27-29 March 2008, Salamanca, Spain&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/CMMP08/event_26545.html Condensed Matter and Materials Physics (CMMP)]  26-28 March 2008 Royal Holloway, University of London, UK&lt;br /&gt;
*[http://www.icmab.es/softmatter2008/index.html SoftMatter 2008] &amp;quot;Workshop on Electrostatic Effects in Soft Matter: Bringing Experiments, Theory and Simulation Together&amp;quot; 10 – 11 April ICMAB-CSIC, Barcelona, Spain.&lt;br /&gt;
*[http://www.icmab.es/11emscf/index.html 11th European Meeting on Supercritical Fluids] &amp;quot;New Perspectives in Supercritical Fluids: Nanoscience, Materials and Processing&amp;quot; 4-7 May 2008, ICMAB-CSIC, Barcelona, Spain&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 99th Statistical Mechanics Conference] May 11-13, 2008 Rutgers University,  USA&lt;br /&gt;
*[http://www.fondation-pgg.org/events/degennesdays/ DeGennesDays] 15-17 May 2008 Collège de France, Paris.&lt;br /&gt;
*[http://www.ill.fr/Events/rktsymposium/  Surfaces and Interfaces in Soft Matter and Biology SISMB 2008] &amp;quot;The impact and future of neutron reflectivity - A Symposium in Honor of Robert K. Thomas&amp;quot; 21-23 May 2008, Institut Laue-Langevin (Grenoble, France).&lt;br /&gt;
*[http://www.plmmp.univ.kiev.ua/ Physics of Liquid Matter: Modern Problems] May 23-26, 2008, Kyiv National Taras Shevchenko University, Ukraine&lt;br /&gt;
*[http://www.ffn.ub.es/sitges/ XXI Sitges Conference] XXI Sitges Conference on Statistical Mechanics. Statistical Mechanics of Molecular Biophysics  2nd-6th June 2008, Sitges, Spain&lt;br /&gt;
*[http://www1.ci.uc.pt/gcpi/poly2008 Polyelectrolytes 2008]  16th-19th June 2008, Coimbra, Portugal&lt;br /&gt;
*[http://www-spht.cea.fr/Meetings/BegRohu2008/index.html The Beg Rohu Summer School: Manifolds in random media, random matrices and extreme value statistics] 16th - 28th June 2008, French National Sailing School, Quiberon peninsula, France.&lt;br /&gt;
*[http://www.chm.bris.ac.uk/cms/ Computational Molecular Science 2008] 22nd – 25th June 2008, Cirencester, UK.&lt;br /&gt;
*[http://www.liquids2008.se/ 7th Liquid Matter Conference] 27 June - 1 July 2008  Lund, Sweden&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School 2008] University of Sheffield, England July 6 - July 15 2008.&lt;br /&gt;
*Potentials Workshop: Recent developments in interatomic potentials 7-8 July 2008  Oxford, UK&lt;br /&gt;
*[http://www.lcc-toulouse.fr/molmat2008/ MOLMAT2008 International Symposium on Molecular Materials based on Chemistry, Solid State Physics, Theory and Nanotechnology]   July 8-11th  2008 Toulouse, France&lt;br /&gt;
*[http://www2.polito.it/eventi/sigmaphi2008/ SigmaPhi2008] 14th -18th July 2008 Kolympari, Crete, Greece&lt;br /&gt;
*[http://www.cecam.org/workshop-188.html Dissipative Particle Dynamics: Addressing deficiencies and establishing new frontiers] July, 16th-18th 2008  CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/event_22243.html Molecular Dynamics for Non-Adiabatic Processes] 21 July 2008 to 22 July 2008 Institute of Physics, London&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcitaa_08/announcement.html Quantum Monte Carlo in the Apuan Alps IV] 26th July - Sat 2nd August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.cecam.org/workshop-215.html New directions in the theory and modelling of liquid crystals] July, 28th 2008 to July, 30th 2008, CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcatcp_08/announcement.html Quantum Monte Carlo and the CASINO program III] 3rd August - Sun 10th August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.icct2008.org/ 20th International Conference on Chemical Thermodynamics] August 3-8, 2008, Warsaw, Poland.&lt;br /&gt;
*[http://perso.ens-lyon.fr/thierry.dauxois/LORIS/LesHouchesSummerSchool2008.html Long-Range Interacting Systems] Summer School in Les Houches (France), 4-29 August 2008&lt;br /&gt;
*[http://ctbp.ucsd.edu/summer_school08/apply2008.html Coarse-Grained Physical Modeling of Biological Systems: Advanced Theory and Methods] August 11-15, 2008 University of California San Diego&lt;br /&gt;
*[http://www.chem.ucl.ac.uk/astrosurf/SIPML.html Surface and Interface Processes at the Molecular Level]  17 - 23 August 2008, Lucca, Italy&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD141/index.asp  Faraday Discussion 141: Water - From Interfaces to the Bulk] 27 - 29 August 2008 Heriot-Watt University, Edinburgh, United Kingdom&lt;br /&gt;
*[http://ectp18.conforganizer.net   18th European Conference on Thermophysical Properties]  31 Aug-4 Sep 2008 Pau, France&lt;br /&gt;
*[http://iber2008.df.fct.unl.pt/  9th Iberian Joint Meeting on Atomic and Molecular Physics - IBER 2008]  7-9th September,  Capuchos, Portugal&lt;br /&gt;
*[http://www.cmmp.ucl.ac.uk/~dmd/ccp5.htm  CCP5 Annual Meeting: Surfaces and Interfaces] 8-10th September, London, UK&lt;br /&gt;
*[http://ergodic.ugr.es/cp/ 10th  Granada  Seminar on Computational and Statistical Physics: Modeling and Simulation of New Materials] September 15-19, 2008 Granada, Spain&lt;br /&gt;
*[http://www.cecam.org/workshop-222.html Standardisation and databasing of ab-initio and classical simulations] September, 18th 2008 to September, 19th 2008  CECAM-ETHZ, Zurich, Switzerland&lt;br /&gt;
*[http://www.iccmse.org/ International Conference of Computational Methods in Sciences and Engineering 2008 (ICCMSE 2008)]  25-30 September, Crete, Greece&lt;br /&gt;
*[http://www.mmm2008.org/bin/view.pl/Main/WebHome Multscale Materials Modeling] 27–31 October 2008, Tallahassee, Florida USA&lt;br /&gt;
*[http://www.aiche.org/Conferences/AnnualMeeting/index.aspx 2008 AIChE Annual Meeting] November 16-21 2008 Philadelphia, Pennsylvania USA&lt;br /&gt;
*[http://www.ihp.jussieu.fr/ceb/Trimestres/T08-4/C3/index.html Statistical mechanics] Paris (France) 8-12 December 2008&lt;br /&gt;
*[http://complex.ffn.ub.es/bcnetworkshop BCNet Workshop] Trends and perspectives in complex networks. Barcelona (Spain) 10-12 December 2008&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 100th Statistical Mechanics Conference]  Rutgers University, (USA) 13-18 December 2008&lt;br /&gt;
=====2009=====&lt;br /&gt;
*[http://www.ccpb.ac.uk/events/conference/2009/ Biomolecular Simulation 2009] 6-8 January, Yorkshire Museum and Gardens, York, United Kingdom 2009&lt;br /&gt;
*[http://www.fisica.unam.mx/externos/wintermeeting/ XXXVIII edition of the Winter Meeting on Statistical Physics] Taxco, Guerrero (Mexico) 6th - 9th January, 2009.&lt;br /&gt;
*[http://www.ucl.ac.uk/msl/events/2009/workshop09.htm 2009 MSL Workshop: Accessing large length and time scales with accurate quantum methods]  12th - 13th January 2009 University College London (United Kingdom)&lt;br /&gt;
*[http://euler.us.es/%7Eopap/stochgame/index-en.html Stochastic Models in Physics, Biology, and Social Sciences] Carmona (Sevilla), Spain February 12-14 (2009)&lt;br /&gt;
*[http://hera.physik.uni-konstanz.de/igk/news/workshops/homepage/index.html Frontiers of Soft Condensed Matter 2009]  Les Houches () 15-20 February  2009&lt;br /&gt;
*[http://www.mpipks-dresden.mpg.de/~mbsffe09/ Many-body systems far from equilibrium: Fluctuations, slow dynamics and long-range interactions] Max Planck Institute for the Physics of Complex Systems Dresden, Germany February 16 - 27 (2009)&lt;br /&gt;
*[http://www.formulation.org.uk/Conference_flyers_Sept2007_on/Flyer-sims.pdf Workshop on advances in modelling for formulations]  25th of March 2009 at GSK Waybridge (United Kingdom)&lt;br /&gt;
*[http://www.physik.uni-leipzig.de/~janke/meco34/ 34th Conference of the Middle European Cooperation in Statistical Physics] 30 March - 01 April 2009 Universität Leipzig (Germany)&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws2/ Workshop II: The Boltzmann Equation: DiPerna-Lions Plus 20 Years] April 15-17 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-313.html Computational Studies of Defects in Nanoscale Carbon Materials]  May 11, 2009 to May 13, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.cecam.org/workshop-320.html Modeling of Carbon and Inorganic Nanotubes and Nanostructures]  May 13, 2009 to May 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ima.umn.edu/2008-2009/W5.18-22.09/ Molecular Simulations: Algorithms, Analysis, and Applications] Institute for Mathematics and its Applications, University of Minnesota (USA), May 18-22, 2009&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws4/ Workshop IV: Asymptotic Methods for Dissipative Particle Systems] May 18-22 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-310.html Computer Simulation in Food Science: CFD meets Soft Matter]  May 25, 2009 to May 27, 2009 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://complenet09.diit.unict.it  CompleNet 2009] International Workshop on Complex Networks. Catania (Italy),  May 26-28, 2009&lt;br /&gt;
*[http://go.warwick.ac.uk/maths/research/events/2008_2009/symposium/wks5/ EPSRC Symposium Workshop on Molecular Dynamics] Monday 1 – Friday 5 June (2009) Warwick (United Kingdom)&lt;br /&gt;
*[http://www.cecam.org/workshop-272.html Theoretical Modeling of Transport in Nanostructures]  June 2, 2009 to June 5, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland) &lt;br /&gt;
*[http://www.mpip-mainz.mpg.de/mmsd/ Mainz Materials Simulation Days] 3-5 June 2009 Max Planck Institute for Polymer Research (Germany)&lt;br /&gt;
*[http://www.soms.ethz.ch/workshop2009 Coping with Crises in Complex Socio-Economic Systems] ETH Zurich (Switzerland), June 8-13, 2009&lt;br /&gt;
*[[MOSSNOHO Workshop 2009]] 16 of June 2009, Universidad Complutense de Madrid (Spain)&lt;br /&gt;
*[http://cftc.cii.fc.ul.pt/Workshops/flowNjam/index.html Flow(ers) and jam(mers): from liquid crystals to grains] Lisbon (Portugal) 17-19 June 2009&lt;br /&gt;
*[http://ipht.cea.fr/Meetings/BegRohu2009/ Beg Rohu Summer School: Quantum Physics Out of Equilibrium] Ecole Nationale de Voile (France) 15-27 June 2009&lt;br /&gt;
*[http://symp17.boulder.nist.gov  Seventeenth Symposium on Thermophysical Properties] Boulder, Colorado (USA), June 21-26, 2009&lt;br /&gt;
*[http://www.fhi-berlin.mpg.de/th/Meetings/DFT-workshop-Berlin2009/ Hands-on Tutorial on Ab Initio Molecular Simulations: Toward a First-Principles Understanding of Materials Properties and Functions] Berlin (Germany) June 22-July 1 2009&lt;br /&gt;
*[https://www.irphe.univ-mrs.fr/~fe09 Fluid and Elasticity] Carry-le-Rouet, near Marseilles (France) June 23-26, 2009&lt;br /&gt;
*[http://www.icmp.lviv.ua/statphys2009/ Statistical Physics: Modern Trends and Applications] June 23-25, 2009 Lviv, (Ukraine)&lt;br /&gt;
*[http://www.fuw.edu.pl/~wssph/ 3rd Warsaw School of Statistical Physics] Kazimierz Dolny (Poland), 27 June - 4 July, 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-298.html Modeling and Simulation of Water at Interfaces from Ambient to Supercooled Conditions] June 29, 2009 to July 1, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School] University of Sheffield  (England) July 5 - July 14 2009 &lt;br /&gt;
*[http://math.arizona.edu/~goriely/leshouches/home.html  New trends in the Physics and Mechanics of Biological Systems&amp;quot;]  Les Houches (France), 6-31 July 2009&lt;br /&gt;
*[http://research.yale.edu/boulder/Boulder-2009/index.html Nonequilibrium Statistical Mechanics: Fundamental Problems and Applications] July 6-24  2009 Boulder (USA)&lt;br /&gt;
*[http://www.xrqtc.cat/index.php/ca/homew New trends in Computational Chemistry for Industry Applications] July 6-7 Barcelona (Spain)&lt;br /&gt;
*[http://www.frias.uni-freiburg.de/BFF Computational Methods for Soft Matter and Biological Systems] July 8-11, 2009, FRIAS, Freiburg (Germany)&lt;br /&gt;
*[http://www.cecam.org/workshop-286.html Structural Transitions in Solids: Theory, Simulations, Experiments and Visualization Techniques] July 8, 2009 to July 11, 2009 CECAM-USI, Lugano (Switzerland)&lt;br /&gt;
*[http://fomms.org FOMMS 2009, Fourth International Conference Foundations of Molecular Modeling and Simulation] Semiahmoo Resort, Blaine, WA (USA)  12-16 July 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-308.html Computer Simulation Approaches to Study Self-Assembly: From Patchy Nano-Colloids to Virus Capsids]  July 13, 2009 to July 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.md-net.org.uk/events/bath_jul_2009.htm EPSRC Network Mathematical Challenges of Molecular Dynamics] 13-15 July (2009) Bath, United Kingdom.&lt;br /&gt;
*[http://www.cecam.org/workshop-279.html New Trends in Simulating Colloids: from Models to Applications] July 15, 2009 to July 18, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD144/index.asp Faraday Discussion 144: Multiscale Modelling of Soft Matter] University of Groningen (The Netherlands) 20 - 22 July 2009&lt;br /&gt;
*[http://www2.yukawa.kyoto-u.ac.jp/~ykis2009/Welcome.html Frontiers in Nonequilibrium Physics: Fundamental Theory, Glassy &amp;amp; Granular Materials, and Computational Physics] July 21 - August 21, 2009  Kyoto (Japan)&lt;br /&gt;
*[http://www.cecam.org/workshop-293.html Fundamental Aspects of Deterministic Thermostats] July 27, 2009 to July 29, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program IV]  2nd-9th August 2009 Towler Institute, Tuscany, (Italy)&lt;br /&gt;
*[http://www.warwick.ac.uk/go/quantsim09  EPSRC Symposium Workshop on Quantum Simulations] 24th-28th August 2009 University of Warwick (United Kingdom)&lt;br /&gt;
*[http://itf.fys.kuleuven.be/~fpspXII/ Fundamental Problems in Statistical Physics XII] August 31 - September 11, 2009 Leuven (Belgium)&lt;br /&gt;
*[http://denali.phys.uniroma1.it/~idmrcs6/ 6th International Discussion Meeting on Relaxations in Complex Systems] August 31- September 5, 2009, Roma (Italy)&lt;br /&gt;
*[http://www.dft09.org/ International Conference on the Applications of Density Functional Theory in Chemistry and Physics] August 31st to September 4th 2009  Lyon (France)&lt;br /&gt;
*[http://www.dfrl.ucl.ac.uk/CCP5/ccp5.htm CCP5 Annual Meeting 2009 Structure Prediction]  7th to  9th, September 2009 London (United Kingdom)&lt;br /&gt;
*[http://fises.dfa.uhu.es/fises09/ XVI Congreso de Física Estadística] Huelva, 10-12  September  2009, Spain&lt;br /&gt;
*[http://th-www.if.uj.edu.pl/zfs/smoluchowski/ 22nd Marian Smoluchowski Symposium On Statistical Physics] 12-17 September 2009 Zakopane (Poland)&lt;br /&gt;
*[http://www.isis.rl.ac.uk/largescale/loq/SAS2009/SAS2009.htm SAS-2009] XIV International Conference on Small-Angle Scattering, Sunday 13 - Friday 18 September, 2009, Oxford (UK)&lt;br /&gt;
*[http://www.esc.sandia.gov/dsmc09/dsmc09.html Direct Simulation Monte Carlo workshop] September 13-16, 2009 Santa Fe, New Mexico, USA,&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/PHYSASPECTS_09/index.html Physical Aspects of Polymer Science] 14-16 September 2009 Bristol (United Kingdom)&lt;br /&gt;
*[http://www.thermodynamics2009.org/ Thermodynamics 2009] September 23-25  Imperial College London , U.K. (2009)&lt;br /&gt;
*[http://www.crm.cat/wkstatisticalphysics/ Techniques and Challenges from Statistical Physics] October 14 to 16, 2009 Barcelona, (Spain)&lt;br /&gt;
*[http://paginas.fe.up.pt/~equifase/ EQUIFASE 2009] VIII Iberoamerican Conference on Phase Equilibria and Fluid Properties for Process Design, Praia da Rocha, Portugal 17-21 October 2009&lt;br /&gt;
*[http://cint.lanl.gov/workshop2009/ Multiple Length Scales in Polymers and Complex Fluids] October 18-21, 2009 Bishop's Lodge, Santa Fe (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-290.html Classical Density Functional Theory Methods in Soft and Hard Matter] October 21, 2009 to October 23, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://seneca.fis.ucm.es/parr/ktlog2_09 kTlog2 '09: Computing Matters Workshop] 22-24 October, 2009, Toledo (Spain)&lt;br /&gt;
*[https://www.cecam.org/workshop-325.html Linking Systems Biology and Biomolecular Simulations]  November 16-19 2009 CECAM Lausanne, (Switzerland) &lt;br /&gt;
*[http://www.lorentzcenter.nl/lc/web/2009/357/info.php3?wsid=357 Subdivide and Tile: Triangulating spaces for understanding the world] November 16 to 20 2009, Leiden (Netherlands)&lt;br /&gt;
*[http://www.dfi.uchile.cl/~granular09/Welcome.html Southern Workshop on Granular Materials 2009 - SWGM09] November 30 to December 4 2009, Viña del Mar (Chile)&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 102nd Statistical Mechanics Conference]  Rutgers University, December 13-15, 2009 (USA)&lt;br /&gt;
*[http://www.cmmp.org.uk/ Condensed Matter and Materials Physics (CMMP)] 15-17 December 2009 Warwick University (United Kingdom)&lt;br /&gt;
=====2010=====&lt;br /&gt;
*[http://ddays2010.northwestern.edu Dynamics Days] January 4-7, 2010 Evanston Illinois (USA)&lt;br /&gt;
*[http://www2.surrey.ac.uk/maths/news/events/2010/emerging_interfaces_workshop.htm Emerging Interfacial Dynamics] January 6-8 University of Surrey (UK)&lt;br /&gt;
*[http://www.comphys.ethz.ch/jstat/    Journées de Physique Statistique 2010] 28-29 January 2010 Paris (France)&lt;br /&gt;
&lt;br /&gt;
__NOTOC__&lt;br /&gt;
[[category: Miscellaneous]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Silicon</id>
		<title>Silicon</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Silicon"/>
				<updated>2009-12-16T11:58:57Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added a nice reference (a tight-binding quantum approax)&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Stub-general}}&lt;br /&gt;
'''Silicon''' (Si)&lt;br /&gt;
==Models of silicon==&lt;br /&gt;
====Stillinger-Weber model====&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevB.31.5262      Frank H. Stillinger and Thomas A. Weber &amp;quot;Computer simulation of local order in condensed phases of silicon&amp;quot;, Physical Review B '''31''' pp.  5262-5271 (1985)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
====Tersoff potential====&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevB.37.6991  J. Tersoff &amp;quot;New empirical approach for the structure and energy of covalent systems&amp;quot;, Physical Review B '''37''' pp. 6991-7000 (1988)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
====Quantum====&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevLett.94.095701  M. Kaczmarski, O.N. Bedoya-Martínez, and E.R. Hernández      &amp;quot;Phase Diagram of Silicon from Atomistic Simulations&amp;quot;, Physical Review Letters '''94''' p. 095701 (2005)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
==Melting point==&lt;br /&gt;
Yoo et al have calculated the melting point to be &amp;lt;math&amp;gt;T_m \approx1540 \pm 50 ~\mathrm{K}&amp;lt;/math&amp;gt; at zeo pressure&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/j.cplett.2009.09.075 Soohaeng Yoo, Sotiris S. Xantheas and Xiao Cheng Zeng &amp;quot;The melting temperature of bulk silicon from ab initio molecular dynamics simulations&amp;quot;, Chemical Physics Letters '''481''' pp. 88-90  (2009)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
==Polyamorphism in silicon==&lt;br /&gt;
Silicon is a [[Polyamorphic systems | polyamorphic system]].&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1038/35107036 Sudip K. Deb, Martin Wilding, Maddury Somayazulu and Paul F. McMillan &amp;quot;Pressure-induced amorphization and an amorphous–amorphous transition in densified porous silicon&amp;quot;, Nature '''414''' pp. 528-530 (2001)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1038/nmat994 Srikanth Sastry and  C. Austen Angell &amp;quot;Liquid–liquid phase transition in supercooled silicon&amp;quot;, Nature Materials '''2''' pp. 739 - 743 (2003)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0953-8984/17/15/002  Philippe Beaucage and Normand Mousseau &amp;quot;Liquid–liquid phase transition in Stillinger–Weber silicon&amp;quot;, Jorunal of Physics: Condensed Matter '''17''' pp.  2269-2279  (2005)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.2970084 N. Jakse and A. Pasturel &amp;quot;Dynamic aspects of the liquid-liquid phase transformation in silicon&amp;quot;, Journal of Chemical Physics '''129''' 104503 (2008)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
'''Related reading'''&lt;br /&gt;
*[http://dx.doi.org/10.1209/0295-5075/9/7/015  L. Goodwin, A. J. Skinner and D. G. Pettifor &amp;quot;Generating Transferable Tight-Binding Parameters: Application to Silicon&amp;quot;, Europhysics Letters '''9''' pp. 701-706 (1989)]&lt;br /&gt;
*[http://dx.doi.org/10.1063/1.3268346 Tianshu Li, Davide Donadio, and Giulia Galli &amp;quot;Nucleation of tetrahedral solids: A molecular dynamics study of supercooled liquid silicon&amp;quot;, Journal of Chemical Physics '''131''' 224519 (2009)]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[category: models]]&lt;br /&gt;
[[Category: Polyamorphic systems]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Talk:1-dimensional_hard_rods</id>
		<title>Talk:1-dimensional hard rods</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Talk:1-dimensional_hard_rods"/>
				<updated>2009-11-10T12:04:48Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;the derivation of the isobaric ensemble is mathematically WRONG!!!&lt;br /&gt;
:Could you provide details? --[[User:Carl McBride | &amp;lt;b&amp;gt;&amp;lt;FONT COLOR=&amp;quot;#8B3A3A&amp;quot;&amp;gt;Carl McBride&amp;lt;/FONT&amp;gt;&amp;lt;/b&amp;gt;]] ([[User_talk:Carl_McBride |talk]]) 15:11, 6 November 2009 (CET)&lt;br /&gt;
:The book by Ziman is quite readable, but please consider the following references: [http://arxiv.org/abs/cond-mat/9610062 A. Drory at arXiv], Kierlik and Rosinberg ''J Stat Phys'' '''68''' 1037 (1992), Percus ''J Stat Phys'' '''28''' 67 (1982). And, please don't shout. --[[User:Dduque|Dduque]] 13:04, 10 November 2009 (CET)&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Conferences</id>
		<title>Conferences</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Conferences"/>
				<updated>2009-10-27T09:30:23Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: /* January */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The following is a chronological list of conferences, seminars, or meetings related to thermodynamics, statistical mechanics, soft condensed matter, many-body problems, complex fluids etc. &lt;br /&gt;
===2009===&lt;br /&gt;
====November====&lt;br /&gt;
*[http://www.dfi.uchile.cl/~granular09/Welcome.html Southern Workshop on Granular Materials 2009 - SWGM09] November 30 to December 4 2009, Viña del Mar (Chile)&lt;br /&gt;
*[http://www.lorentzcenter.nl/lc/web/2009/357/info.php3?wsid=357 Subdivide and Tile: Triangulating spaces for understanding the world] Nov 16 to 20 Nov 20 2009, Leiden (Netherlands)&lt;br /&gt;
&lt;br /&gt;
====December====&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 102nd Statistical Mechanics Conference]  Rutgers University, December 13-15, 2009 (USA)&lt;br /&gt;
*[http://www.cmmp.org.uk/ Condensed Matter and Materials Physics (CMMP)] 15-17 December 2009 Warwick University (United Kingdom)&lt;br /&gt;
&lt;br /&gt;
===2010===&lt;br /&gt;
====January====&lt;br /&gt;
*[http://ddays2010.northwestern.edu Dynamics Days] January 4-7, 2010 Evanston Illinois (USA)&lt;br /&gt;
*[http://www2.surrey.ac.uk/maths/news/events/2010/emerging_interfaces_workshop.htm Emerging Interfacial Dynamics] January 6-8 University of Surrey (UK)&lt;br /&gt;
&lt;br /&gt;
====May====&lt;br /&gt;
*[http://www.ppeppd2010.cn/ Properties and Phase Equilibria for Product and Process Design] May 16-21, 2010 Suzhou, Jiangsu (China)&lt;br /&gt;
====June====&lt;br /&gt;
*[http://liblice.icpf.cas.cz/2010/2010.php Eighth  Liblice Conference on the Statistical Mechanics of Liquids] June 13-18, 2010 Brno (Czech Republic)&lt;br /&gt;
====July====&lt;br /&gt;
*[http://ismc2010.ugr.es International Soft Matter Conference 2010] 5th-8th July 2010, Granada, Spain&lt;br /&gt;
*[http://www.statphys.org.au StatPhys 24: XXIV International Conference on Statistical Physics of the International Union for Pure and Applied Physics (IUPAP)] 19-23 July, (2010). Cairns (Australia)&lt;br /&gt;
&lt;br /&gt;
====September====&lt;br /&gt;
*[http://ergodic.ugr.es/cp 11th Granada Seminar: Foundations of Nonequilibrium Statistical Physics — From Basic Science to Future Challenges] 13-17  September, (2010). La Herradura, Granada (Spain)&lt;br /&gt;
&lt;br /&gt;
==Previous conferences==&lt;br /&gt;
=====2007=====&lt;br /&gt;
*[http://www.simbioma.cecam.org/ Simulation of Hard Bodies] April 16 to April 19 2007 in Lyon.&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 97th Statistical Mechanics Conference] May 6-8, 2007 Rutgers University&lt;br /&gt;
*[http://www.ucm.es/info/molecsim/luis/workshop.htm Workshop on Theory and Computer Simulations of Inhomogenoeus Fluids] May 16-18, 2007, Universidad Complutense, Madrid.&lt;br /&gt;
*[http://www-thphys.physics.ox.ac.uk/users/JuliaYeomans/OxfordWorkshop/home.php Mesoscale Modelling for Complex Fluids and Flows] June 25--27, 2007 University of Oxford, UK.&lt;br /&gt;
*[http://www.ecns2007.org 4th European Conference on Neutron Scattering] Lund, Sweden 25-29 June 2007&lt;br /&gt;
*[http://www.realitygrid.org/CompSci07 Computational Science 2007] 25-26 June 2007  The Royal Society, London&lt;br /&gt;
*[https://www.cecam.fr/index.php?content=activities/workshop New directions in liquid state theory] CECAM workshop, 2 - 4 July, 2007 at ENS, Lyon, France.&lt;br /&gt;
*[http://www.cecam.fr/index.php?content=activities/workshop&amp;amp;action=details&amp;amp;wid=157 Fluid phase behaviour and critical phenomena from liquid state theories and simulations] 5-7 July  2007 CECAM workshop, Lyon, France.&lt;br /&gt;
*[http://www.statphys23.org/ STATPHYS 23] Genova, Italy, from July 9 to 13, 2007.&lt;br /&gt;
*[http://www.iupac2007.org/ 41st IUPAC World Chemistry Conference] Turin, Italy, August 5-11th&lt;br /&gt;
*[http://www.srcf.ucam.org/~jae1001/ccp5_2007 CCP5 Annual Conference] 29th-31st August 2007 New Hall, Cambridge, UK&lt;br /&gt;
*[http://ccp2007.ulb.ac.be CCP 2007] Brussels  5-8 September  2007&lt;br /&gt;
*[http://www.castep.org CASTEP Workshop] 17th - 21st September 2007 University of York, UK&lt;br /&gt;
*[http://thermo2007.ifp.fr Thermodynamics 2007] 26-28 September 2007, IFP - Rueil-Malmaison (France)&lt;br /&gt;
*[http://www.iccmse.org/  International Conference of Computational Methods in Sciences and Engineering 2007] Corfu, Greece, 25-30 September 2007&lt;br /&gt;
*[http://www.chem.unisa.it/polnan/index.html Polymers in Nanotechnology] 27-28th September 2007, Salerno, Italy.&lt;br /&gt;
*[http://www.fz-juelich.de/iff/ismc2007/  International Soft Matter Conference 2007] 1 - 4 October 2007, Eurogress, Aachen (Germany)&lt;br /&gt;
*[http://www.escet.urjc.es/~fisica/encuentro_complejos/index.html II Meeting on Modelling of Complex Systems]  Universidad Rey Juan Carlos, Mostoles (Madrid), October 25-26 2007&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/SCD/event_22663.html Structuring Colloidal Dispersions by External Fields] 21 November 2007, Institute of Physics, London, United Kingdom&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 98th Statistical Mechanics Conference] December 16-18, 2007, Rutgers University, New Jersey, USA.&lt;br /&gt;
=====2008=====&lt;br /&gt;
*[http://www.iop.org/activity/groups/subject/lcf/Events/file_25833.pdf Recent Advances in the Understanding of Confined Fluids: from Superfluids to Oil Reservoirs] 9-11 January, Cosener's House, Abingdon UK&lt;br /&gt;
*[http://academic.sun.ac.za/summerschool/2008.html  Workshop on Soft Condensed Matter and Physics of Biological Systems - Perspectives and topics for South Africa]  23 Jan 2008 - 1 Feb 2008 National Institute for Theoretical Physics at Stellenbosch Institute of Advanced Study, Stellenbosch, Western Cape, South Africa&lt;br /&gt;
*[http://bifi.unizar.es/events/bifi2008/main.htm Bifi 2008 Large Scale Simulations of Complex Systems, Condensed Matter and Fusion Plasma] 6–8 February 2008, Zaragoza, Spain&lt;br /&gt;
*[http://events.dechema.de/Tagungen/MolMod+Workshop.html International Workshop Molecular Modeling and Simulation in Applied Material Science] March 10-11,  DECHEMA-Haus, Frankfurt am Main, Germany&lt;br /&gt;
*[http://www.aps.org/meetings/march/index.cfm APS March Meeting] March 10-14, 2008. New Orleans, Louisiana, USA&lt;br /&gt;
*[http://users.physik.tu-muenchen.de/metz/jerusalem.html Modelling anomalous diffusion and relaxation]  23–28 March 2008, Jerusalem, Israel&lt;br /&gt;
*[http://www.newton.cam.ac.uk/programmes/CSM/csmw02.html Markov-Chain Monte Carlo Methods] 25 March to 28 March 2008 Isaac Newton Institute for Mathematical Sciences, Cambridge, UK &lt;br /&gt;
*[http://www.usal.es/~fises/ XV Congreso de Física Estadística (Fises' 08)] 27-29 March 2008, Salamanca, Spain&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/CMMP08/event_26545.html Condensed Matter and Materials Physics (CMMP)]  26-28 March 2008 Royal Holloway, University of London, UK&lt;br /&gt;
*[http://www.icmab.es/softmatter2008/index.html SoftMatter 2008] &amp;quot;Workshop on Electrostatic Effects in Soft Matter: Bringing Experiments, Theory and Simulation Together&amp;quot; 10 – 11 April ICMAB-CSIC, Barcelona, Spain.&lt;br /&gt;
*[http://www.icmab.es/11emscf/index.html 11th European Meeting on Supercritical Fluids] &amp;quot;New Perspectives in Supercritical Fluids: Nanoscience, Materials and Processing&amp;quot; 4-7 May 2008, ICMAB-CSIC, Barcelona, Spain&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 99th Statistical Mechanics Conference] May 11-13, 2008 Rutgers University,  USA&lt;br /&gt;
*[http://www.fondation-pgg.org/events/degennesdays/ DeGennesDays] 15-17 May 2008 Collège de France, Paris.&lt;br /&gt;
*[http://www.ill.fr/Events/rktsymposium/  Surfaces and Interfaces in Soft Matter and Biology SISMB 2008] &amp;quot;The impact and future of neutron reflectivity - A Symposium in Honor of Robert K. Thomas&amp;quot; 21-23 May 2008, Institut Laue-Langevin (Grenoble, France).&lt;br /&gt;
*[http://www.plmmp.univ.kiev.ua/ Physics of Liquid Matter: Modern Problems] May 23-26, 2008, Kyiv National Taras Shevchenko University, Ukraine&lt;br /&gt;
*[http://www.ffn.ub.es/sitges/ XXI Sitges Conference] XXI Sitges Conference on Statistical Mechanics. Statistical Mechanics of Molecular Biophysics  2nd-6th June 2008, Sitges, Spain&lt;br /&gt;
*[http://www1.ci.uc.pt/gcpi/poly2008 Polyelectrolytes 2008]  16th-19th June 2008, Coimbra, Portugal&lt;br /&gt;
*[http://www-spht.cea.fr/Meetings/BegRohu2008/index.html The Beg Rohu Summer School: Manifolds in random media, random matrices and extreme value statistics] 16th - 28th June 2008, French National Sailing School, Quiberon peninsula, France.&lt;br /&gt;
*[http://www.chm.bris.ac.uk/cms/ Computational Molecular Science 2008] 22nd – 25th June 2008, Cirencester, UK.&lt;br /&gt;
*[http://www.liquids2008.se/ 7th Liquid Matter Conference] 27 June - 1 July 2008  Lund, Sweden&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School 2008] University of Sheffield, England July 6 - July 15 2008.&lt;br /&gt;
*Potentials Workshop: Recent developments in interatomic potentials 7-8 July 2008  Oxford, UK&lt;br /&gt;
*[http://www.lcc-toulouse.fr/molmat2008/ MOLMAT2008 International Symposium on Molecular Materials based on Chemistry, Solid State Physics, Theory and Nanotechnology]   July 8-11th  2008 Toulouse, France&lt;br /&gt;
*[http://www2.polito.it/eventi/sigmaphi2008/ SigmaPhi2008] 14th -18th July 2008 Kolympari, Crete, Greece&lt;br /&gt;
*[http://www.cecam.org/workshop-188.html Dissipative Particle Dynamics: Addressing deficiencies and establishing new frontiers] July, 16th-18th 2008  CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/event_22243.html Molecular Dynamics for Non-Adiabatic Processes] 21 July 2008 to 22 July 2008 Institute of Physics, London&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcitaa_08/announcement.html Quantum Monte Carlo in the Apuan Alps IV] 26th July - Sat 2nd August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.cecam.org/workshop-215.html New directions in the theory and modelling of liquid crystals] July, 28th 2008 to July, 30th 2008, CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcatcp_08/announcement.html Quantum Monte Carlo and the CASINO program III] 3rd August - Sun 10th August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.icct2008.org/ 20th International Conference on Chemical Thermodynamics] August 3-8, 2008, Warsaw, Poland.&lt;br /&gt;
*[http://perso.ens-lyon.fr/thierry.dauxois/LORIS/LesHouchesSummerSchool2008.html Long-Range Interacting Systems] Summer School in Les Houches (France), 4-29 August 2008&lt;br /&gt;
*[http://ctbp.ucsd.edu/summer_school08/apply2008.html Coarse-Grained Physical Modeling of Biological Systems: Advanced Theory and Methods] August 11-15, 2008 University of California San Diego&lt;br /&gt;
*[http://www.chem.ucl.ac.uk/astrosurf/SIPML.html Surface and Interface Processes at the Molecular Level]  17 - 23 August 2008, Lucca, Italy&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD141/index.asp  Faraday Discussion 141: Water - From Interfaces to the Bulk] 27 - 29 August 2008 Heriot-Watt University, Edinburgh, United Kingdom&lt;br /&gt;
*[http://ectp18.conforganizer.net   18th European Conference on Thermophysical Properties]  31 Aug-4 Sep 2008 Pau, France&lt;br /&gt;
*[http://iber2008.df.fct.unl.pt/  9th Iberian Joint Meeting on Atomic and Molecular Physics - IBER 2008]  7-9th September,  Capuchos, Portugal&lt;br /&gt;
*[http://www.cmmp.ucl.ac.uk/~dmd/ccp5.htm  CCP5 Annual Meeting: Surfaces and Interfaces] 8-10th September, London, UK&lt;br /&gt;
*[http://ergodic.ugr.es/cp/ 10th  Granada  Seminar on Computational and Statistical Physics: Modeling and Simulation of New Materials] September 15-19, 2008 Granada, Spain&lt;br /&gt;
*[http://www.cecam.org/workshop-222.html Standardisation and databasing of ab-initio and classical simulations] September, 18th 2008 to September, 19th 2008  CECAM-ETHZ, Zurich, Switzerland&lt;br /&gt;
*[http://www.iccmse.org/ International Conference of Computational Methods in Sciences and Engineering 2008 (ICCMSE 2008)]  25-30 September, Crete, Greece&lt;br /&gt;
*[http://www.mmm2008.org/bin/view.pl/Main/WebHome Multscale Materials Modeling] 27–31 October 2008, Tallahassee, Florida USA&lt;br /&gt;
*[http://www.aiche.org/Conferences/AnnualMeeting/index.aspx 2008 AIChE Annual Meeting] November 16-21 2008 Philadelphia, Pennsylvania USA&lt;br /&gt;
*[http://www.ihp.jussieu.fr/ceb/Trimestres/T08-4/C3/index.html Statistical mechanics] Paris (France) 8-12 December 2008&lt;br /&gt;
*[http://complex.ffn.ub.es/bcnetworkshop BCNet Workshop] Trends and perspectives in complex networks. Barcelona (Spain) 10-12 December 2008&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 100th Statistical Mechanics Conference]  Rutgers University, (USA) 13-18 December 2008&lt;br /&gt;
=====2009=====&lt;br /&gt;
*[http://www.ccpb.ac.uk/events/conference/2009/ Biomolecular Simulation 2009] 6-8 January, Yorkshire Museum and Gardens, York, United Kingdom 2009&lt;br /&gt;
*[http://www.fisica.unam.mx/externos/wintermeeting/ XXXVIII edition of the Winter Meeting on Statistical Physics] Taxco, Guerrero (Mexico) 6th - 9th January, 2009.&lt;br /&gt;
*[http://www.ucl.ac.uk/msl/events/2009/workshop09.htm 2009 MSL Workshop: Accessing large length and time scales with accurate quantum methods]  12th - 13th January 2009 University College London (United Kingdom)&lt;br /&gt;
*[http://euler.us.es/%7Eopap/stochgame/index-en.html Stochastic Models in Physics, Biology, and Social Sciences] Carmona (Sevilla), Spain February 12-14 (2009)&lt;br /&gt;
*[http://hera.physik.uni-konstanz.de/igk/news/workshops/homepage/index.html Frontiers of Soft Condensed Matter 2009]  Les Houches () 15-20 February  2009&lt;br /&gt;
*[http://www.mpipks-dresden.mpg.de/~mbsffe09/ Many-body systems far from equilibrium: Fluctuations, slow dynamics and long-range interactions] Max Planck Institute for the Physics of Complex Systems Dresden, Germany February 16 - 27 (2009)&lt;br /&gt;
*[http://www.formulation.org.uk/Conference_flyers_Sept2007_on/Flyer-sims.pdf Workshop on advances in modelling for formulations]  25th of March 2009 at GSK Waybridge (United Kingdom)&lt;br /&gt;
*[http://www.physik.uni-leipzig.de/~janke/meco34/ 34th Conference of the Middle European Cooperation in Statistical Physics] 30 March - 01 April 2009 Universität Leipzig (Germany)&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws2/ Workshop II: The Boltzmann Equation: DiPerna-Lions Plus 20 Years] April 15-17 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-313.html Computational Studies of Defects in Nanoscale Carbon Materials]  May 11, 2009 to May 13, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.cecam.org/workshop-320.html Modeling of Carbon and Inorganic Nanotubes and Nanostructures]  May 13, 2009 to May 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ima.umn.edu/2008-2009/W5.18-22.09/ Molecular Simulations: Algorithms, Analysis, and Applications] Institute for Mathematics and its Applications, University of Minnesota (USA), May 18-22, 2009&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws4/ Workshop IV: Asymptotic Methods for Dissipative Particle Systems] May 18-22 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-310.html Computer Simulation in Food Science: CFD meets Soft Matter]  May 25, 2009 to May 27, 2009 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://complenet09.diit.unict.it  CompleNet 2009] International Workshop on Complex Networks. Catania (Italy),  May 26-28, 2009&lt;br /&gt;
*[http://go.warwick.ac.uk/maths/research/events/2008_2009/symposium/wks5/ EPSRC Symposium Workshop on Molecular Dynamics] Monday 1 – Friday 5 June (2009) Warwick (United Kingdom)&lt;br /&gt;
*[http://www.cecam.org/workshop-272.html Theoretical Modeling of Transport in Nanostructures]  June 2, 2009 to June 5, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland) &lt;br /&gt;
*[http://www.mpip-mainz.mpg.de/mmsd/ Mainz Materials Simulation Days] 3-5 June 2009 Max Planck Institute for Polymer Research (Germany)&lt;br /&gt;
*[http://www.soms.ethz.ch/workshop2009 Coping with Crises in Complex Socio-Economic Systems] ETH Zurich (Switzerland), June 8-13, 2009&lt;br /&gt;
*[[MOSSNOHO Workshop 2009]] 16 of June 2009, Universidad Complutense de Madrid (Spain)&lt;br /&gt;
*[http://cftc.cii.fc.ul.pt/Workshops/flowNjam/index.html Flow(ers) and jam(mers): from liquid crystals to grains] Lisbon (Portugal) 17-19 June 2009&lt;br /&gt;
*[http://ipht.cea.fr/Meetings/BegRohu2009/ Beg Rohu Summer School: Quantum Physics Out of Equilibrium] Ecole Nationale de Voile (France) 15-27 June 2009&lt;br /&gt;
*[http://symp17.boulder.nist.gov  Seventeenth Symposium on Thermophysical Properties] Boulder, Colorado (USA), June 21-26, 2009&lt;br /&gt;
*[http://www.fhi-berlin.mpg.de/th/Meetings/DFT-workshop-Berlin2009/ Hands-on Tutorial on Ab Initio Molecular Simulations: Toward a First-Principles Understanding of Materials Properties and Functions] Berlin (Germany) June 22-July 1 2009&lt;br /&gt;
*[https://www.irphe.univ-mrs.fr/~fe09 Fluid and Elasticity] Carry-le-Rouet, near Marseilles (France) June 23-26, 2009&lt;br /&gt;
*[http://www.icmp.lviv.ua/statphys2009/ Statistical Physics: Modern Trends and Applications] June 23-25, 2009 Lviv, (Ukraine)&lt;br /&gt;
*[http://www.fuw.edu.pl/~wssph/ 3rd Warsaw School of Statistical Physics] Kazimierz Dolny (Poland), 27 June - 4 July, 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-298.html Modeling and Simulation of Water at Interfaces from Ambient to Supercooled Conditions] June 29, 2009 to July 1, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School] University of Sheffield  (England) July 5 - July 14 2009 &lt;br /&gt;
*[http://math.arizona.edu/~goriely/leshouches/home.html  New trends in the Physics and Mechanics of Biological Systems&amp;quot;]  Les Houches (France), 6-31 July 2009&lt;br /&gt;
*[http://research.yale.edu/boulder/Boulder-2009/index.html Nonequilibrium Statistical Mechanics: Fundamental Problems and Applications] July 6-24  2009 Boulder (USA)&lt;br /&gt;
*[http://www.xrqtc.cat/index.php/ca/homew New trends in Computational Chemistry for Industry Applications] July 6-7 Barcelona (Spain)&lt;br /&gt;
*[http://www.frias.uni-freiburg.de/BFF Computational Methods for Soft Matter and Biological Systems] July 8-11, 2009, FRIAS, Freiburg (Germany)&lt;br /&gt;
*[http://www.cecam.org/workshop-286.html Structural Transitions in Solids: Theory, Simulations, Experiments and Visualization Techniques] July 8, 2009 to July 11, 2009 CECAM-USI, Lugano (Switzerland)&lt;br /&gt;
*[http://fomms.org FOMMS 2009, Fourth International Conference Foundations of Molecular Modeling and Simulation] Semiahmoo Resort, Blaine, WA (USA)  12-16 July 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-308.html Computer Simulation Approaches to Study Self-Assembly: From Patchy Nano-Colloids to Virus Capsids]  July 13, 2009 to July 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.md-net.org.uk/events/bath_jul_2009.htm EPSRC Network Mathematical Challenges of Molecular Dynamics] 13-15 July (2009) Bath, United Kingdom.&lt;br /&gt;
*[http://www.cecam.org/workshop-279.html New Trends in Simulating Colloids: from Models to Applications] July 15, 2009 to July 18, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD144/index.asp Faraday Discussion 144: Multiscale Modelling of Soft Matter] University of Groningen (The Netherlands) 20 - 22 July 2009&lt;br /&gt;
*[http://www2.yukawa.kyoto-u.ac.jp/~ykis2009/Welcome.html Frontiers in Nonequilibrium Physics: Fundamental Theory, Glassy &amp;amp; Granular Materials, and Computational Physics] July 21 - August 21, 2009  Kyoto (Japan)&lt;br /&gt;
*[http://www.cecam.org/workshop-293.html Fundamental Aspects of Deterministic Thermostats] July 27, 2009 to July 29, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program IV]  2nd-9th August 2009 Towler Institute, Tuscany, (Italy)&lt;br /&gt;
*[http://www.warwick.ac.uk/go/quantsim09  EPSRC Symposium Workshop on Quantum Simulations] 24th-28th August 2009 University of Warwick (United Kingdom)&lt;br /&gt;
*[http://itf.fys.kuleuven.be/~fpspXII/ Fundamental Problems in Statistical Physics XII] August 31 - September 11, 2009 Leuven (Belgium)&lt;br /&gt;
*[http://denali.phys.uniroma1.it/~idmrcs6/ 6th International Discussion Meeting on Relaxations in Complex Systems] August 31- September 5, 2009, Roma (Italy)&lt;br /&gt;
*[http://www.dft09.org/ International Conference on the Applications of Density Functional Theory in Chemistry and Physics] August 31st to September 4th 2009  Lyon (France)&lt;br /&gt;
*[http://www.dfrl.ucl.ac.uk/CCP5/ccp5.htm CCP5 Annual Meeting 2009 Structure Prediction]  7th to  9th, September 2009 London (United Kingdom)&lt;br /&gt;
*[http://fises.dfa.uhu.es/fises09/ XVI Congreso de Física Estadística] Huelva, 10-12  September  2009, Spain&lt;br /&gt;
*[http://th-www.if.uj.edu.pl/zfs/smoluchowski/ 22nd Marian Smoluchowski Symposium On Statistical Physics] 12-17 September 2009 Zakopane (Poland)&lt;br /&gt;
*[http://www.isis.rl.ac.uk/largescale/loq/SAS2009/SAS2009.htm SAS-2009] XIV International Conference on Small-Angle Scattering, Sunday 13 - Friday 18 September, 2009, Oxford (UK)&lt;br /&gt;
*[http://www.esc.sandia.gov/dsmc09/dsmc09.html Direct Simulation Monte Carlo workshop] September 13-16, 2009 Santa Fe, New Mexico, USA,&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/PHYSASPECTS_09/index.html Physical Aspects of Polymer Science] 14-16 September 2009 Bristol (United Kingdom)&lt;br /&gt;
*[http://www.thermodynamics2009.org/ Thermodynamics 2009] September 23-25  Imperial College London , U.K. (2009)&lt;br /&gt;
*[http://www.crm.cat/wkstatisticalphysics/ Techniques and Challenges from Statistical Physics] October 14 to 16, 2009 Barcelona, (Spain)&lt;br /&gt;
*[http://paginas.fe.up.pt/~equifase/ EQUIFASE 2009] VIII Iberoamerican Conference on Phase Equilibria and Fluid Properties for Process Design, Praia da Rocha, Portugal 17-21 October 2009&lt;br /&gt;
*[http://cint.lanl.gov/workshop2009/ Multiple Length Scales in Polymers and Complex Fluids] October 18-21, 2009 Bishop's Lodge, Santa Fe (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-290.html Classical Density Functional Theory Methods in Soft and Hard Matter] October 21, 2009 to October 23, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://seneca.fis.ucm.es/parr/ktlog2_09 kTlog2 '09: Computing Matters Workshop] 22-24 October, 2009, Toledo (Spain)&lt;br /&gt;
&lt;br /&gt;
__NOTOC__&lt;br /&gt;
[[category: Miscellaneous]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Conferences</id>
		<title>Conferences</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Conferences"/>
				<updated>2009-09-22T07:51:46Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Conf. added&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The following is a chronological list of conferences, seminars, or meetings related to thermodynamics, statistical mechanics, soft condensed matter, many-body problems, complex fluids etc. &lt;br /&gt;
===2009===&lt;br /&gt;
====September====&lt;br /&gt;
*[http://www.thermodynamics2009.org/ Thermodynamics 2009] September 23-25  Imperial College London , U.K. (2009)&lt;br /&gt;
====October====&lt;br /&gt;
*[http://paginas.fe.up.pt/~equifase/ EQUIFASE 2009] VIII Iberoamerican Conference on Phase Equilibria and Fluid Properties for Process Design, Praia da Rocha, Portugal 17-21 October 2009&lt;br /&gt;
*[http://cint.lanl.gov/workshop2009/ Multiple Length Scales in Polymers and Complex Fluids] October 18- 21, 2009 Bishop's Lodge, Santa Fe (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-290.html Classical Density Functional Theory Methods in Soft and Hard Matter] October 21, 2009 to October 23, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://seneca.fis.ucm.es/parr/ktlog2_09 kTlog2 '09: Computing Matters Workshop] 22-24 October, 2009, Toledo (Spain)&lt;br /&gt;
====November====&lt;br /&gt;
*[http://www.dfi.uchile.cl/~granular09/Welcome.html Southern Workshop on Granular Materials 2009 - SWGM09] November 30 to December 4 2009, Viña del Mar (Chile)&lt;br /&gt;
*[http://www.lorentzcenter.nl/lc/web/2009/357/info.php3?wsid=357 Subdivide and Tile: Triangulating spaces for understanding the world] Nov 16 to 20 Nov 20 2009, Leiden (Netherlands)&lt;br /&gt;
&lt;br /&gt;
====December====&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 102nd Statistical Mechanics Conference]  Rutgers University, December 13-15, 2009 (USA)&lt;br /&gt;
*[http://www.cmmp.org.uk/ Condensed Matter and Materials Physics (CMMP)] 15-17 December 2009 Warwick University (United Kingdom)&lt;br /&gt;
&lt;br /&gt;
===2010===&lt;br /&gt;
====January====&lt;br /&gt;
*[http://ddays2010.northwestern.edu Dynamics Days] January 4-7, 2010 Evanston Illinois (USA)&lt;br /&gt;
====May====&lt;br /&gt;
*[http://www.ppeppd2010.cn/ Properties and Phase Equilibria for Product and Process Design] May 16-21, 2010 Suzhou, Jiangsu (China)&lt;br /&gt;
====June====&lt;br /&gt;
*[http://liblice.icpf.cas.cz/2010/2010.php Eighth  Liblice Conference on the Statistical Mechanics of Liquids] June 13-18, 2010 Brno (Czech Republic)&lt;br /&gt;
====July====&lt;br /&gt;
*[http://ismc2010.ugr.es International Soft Matter Conference 2010] 5th-8th July 2010, Granada, Spain&lt;br /&gt;
*[http://www.statphys.org.au StatPhys 24: XXIV International Conference on Statistical Physics of the International Union for Pure and Applied Physics (IUPAP)] 19-23 July, (2010). Cairns (Australia)&lt;br /&gt;
&lt;br /&gt;
==Previous conferences==&lt;br /&gt;
=====2007=====&lt;br /&gt;
*[http://www.simbioma.cecam.org/ Simulation of Hard Bodies] April 16 to April 19 2007 in Lyon.&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 97th Statistical Mechanics Conference] May 6-8, 2007 Rutgers University&lt;br /&gt;
*[http://www.ucm.es/info/molecsim/luis/workshop.htm Workshop on Theory and Computer Simulations of Inhomogenoeus Fluids] May 16-18, 2007, Universidad Complutense, Madrid.&lt;br /&gt;
*[http://www-thphys.physics.ox.ac.uk/users/JuliaYeomans/OxfordWorkshop/home.php Mesoscale Modelling for Complex Fluids and Flows] June 25--27, 2007 University of Oxford, UK.&lt;br /&gt;
*[http://www.ecns2007.org 4th European Conference on Neutron Scattering] Lund, Sweden 25-29 June 2007&lt;br /&gt;
*[http://www.realitygrid.org/CompSci07 Computational Science 2007] 25-26 June 2007  The Royal Society, London&lt;br /&gt;
*[https://www.cecam.fr/index.php?content=activities/workshop New directions in liquid state theory] CECAM workshop, 2 - 4 July, 2007 at ENS, Lyon, France.&lt;br /&gt;
*[http://www.cecam.fr/index.php?content=activities/workshop&amp;amp;action=details&amp;amp;wid=157 Fluid phase behaviour and critical phenomena from liquid state theories and simulations] 5-7 July  2007 CECAM workshop, Lyon, France.&lt;br /&gt;
*[http://www.statphys23.org/ STATPHYS 23] Genova, Italy, from July 9 to 13, 2007.&lt;br /&gt;
*[http://www.iupac2007.org/ 41st IUPAC World Chemistry Conference] Turin, Italy, August 5-11th&lt;br /&gt;
*[http://www.srcf.ucam.org/~jae1001/ccp5_2007 CCP5 Annual Conference] 29th-31st August 2007 New Hall, Cambridge, UK&lt;br /&gt;
*[http://ccp2007.ulb.ac.be CCP 2007] Brussels  5-8 September  2007&lt;br /&gt;
*[http://www.castep.org CASTEP Workshop] 17th - 21st September 2007 University of York, UK&lt;br /&gt;
*[http://thermo2007.ifp.fr Thermodynamics 2007] 26-28 September 2007, IFP - Rueil-Malmaison (France)&lt;br /&gt;
*[http://www.iccmse.org/  International Conference of Computational Methods in Sciences and Engineering 2007] Corfu, Greece, 25-30 September 2007&lt;br /&gt;
*[http://www.chem.unisa.it/polnan/index.html Polymers in Nanotechnology] 27-28th September 2007, Salerno, Italy.&lt;br /&gt;
*[http://www.fz-juelich.de/iff/ismc2007/  International Soft Matter Conference 2007] 1 - 4 October 2007, Eurogress, Aachen (Germany)&lt;br /&gt;
*[http://www.escet.urjc.es/~fisica/encuentro_complejos/index.html II Meeting on Modelling of Complex Systems]  Universidad Rey Juan Carlos, Mostoles (Madrid), October 25-26 2007&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/SCD/event_22663.html Structuring Colloidal Dispersions by External Fields] 21 November 2007, Institute of Physics, London, United Kingdom&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 98th Statistical Mechanics Conference] December 16-18, 2007, Rutgers University, New Jersey, USA.&lt;br /&gt;
=====2008=====&lt;br /&gt;
*[http://www.iop.org/activity/groups/subject/lcf/Events/file_25833.pdf Recent Advances in the Understanding of Confined Fluids: from Superfluids to Oil Reservoirs] 9-11 January, Cosener's House, Abingdon UK&lt;br /&gt;
*[http://academic.sun.ac.za/summerschool/2008.html  Workshop on Soft Condensed Matter and Physics of Biological Systems - Perspectives and topics for South Africa]  23 Jan 2008 - 1 Feb 2008 National Institute for Theoretical Physics at Stellenbosch Institute of Advanced Study, Stellenbosch, Western Cape, South Africa&lt;br /&gt;
*[http://bifi.unizar.es/events/bifi2008/main.htm Bifi 2008 Large Scale Simulations of Complex Systems, Condensed Matter and Fusion Plasma] 6–8 February 2008, Zaragoza, Spain&lt;br /&gt;
*[http://events.dechema.de/Tagungen/MolMod+Workshop.html International Workshop Molecular Modeling and Simulation in Applied Material Science] March 10-11,  DECHEMA-Haus, Frankfurt am Main, Germany&lt;br /&gt;
*[http://www.aps.org/meetings/march/index.cfm APS March Meeting] March 10-14, 2008. New Orleans, Louisiana, USA&lt;br /&gt;
*[http://users.physik.tu-muenchen.de/metz/jerusalem.html Modelling anomalous diffusion and relaxation]  23–28 March 2008, Jerusalem, Israel&lt;br /&gt;
*[http://www.newton.cam.ac.uk/programmes/CSM/csmw02.html Markov-Chain Monte Carlo Methods] 25 March to 28 March 2008 Isaac Newton Institute for Mathematical Sciences, Cambridge, UK &lt;br /&gt;
*[http://www.usal.es/~fises/ XV Congreso de Física Estadística (Fises' 08)] 27-29 March 2008, Salamanca, Spain&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/CMMP08/event_26545.html Condensed Matter and Materials Physics (CMMP)]  26-28 March 2008 Royal Holloway, University of London, UK&lt;br /&gt;
*[http://www.icmab.es/softmatter2008/index.html SoftMatter 2008] &amp;quot;Workshop on Electrostatic Effects in Soft Matter: Bringing Experiments, Theory and Simulation Together&amp;quot; 10 – 11 April ICMAB-CSIC, Barcelona, Spain.&lt;br /&gt;
*[http://www.icmab.es/11emscf/index.html 11th European Meeting on Supercritical Fluids] &amp;quot;New Perspectives in Supercritical Fluids: Nanoscience, Materials and Processing&amp;quot; 4-7 May 2008, ICMAB-CSIC, Barcelona, Spain&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 99th Statistical Mechanics Conference] May 11-13, 2008 Rutgers University,  USA&lt;br /&gt;
*[http://www.fondation-pgg.org/events/degennesdays/ DeGennesDays] 15-17 May 2008 Collège de France, Paris.&lt;br /&gt;
*[http://www.ill.fr/Events/rktsymposium/  Surfaces and Interfaces in Soft Matter and Biology SISMB 2008] &amp;quot;The impact and future of neutron reflectivity - A Symposium in Honor of Robert K. Thomas&amp;quot; 21-23 May 2008, Institut Laue-Langevin (Grenoble, France).&lt;br /&gt;
*[http://www.plmmp.univ.kiev.ua/ Physics of Liquid Matter: Modern Problems] May 23-26, 2008, Kyiv National Taras Shevchenko University, Ukraine&lt;br /&gt;
*[http://www.ffn.ub.es/sitges/ XXI Sitges Conference] XXI Sitges Conference on Statistical Mechanics. Statistical Mechanics of Molecular Biophysics  2nd-6th June 2008, Sitges, Spain&lt;br /&gt;
*[http://www1.ci.uc.pt/gcpi/poly2008 Polyelectrolytes 2008]  16th-19th June 2008, Coimbra, Portugal&lt;br /&gt;
*[http://www-spht.cea.fr/Meetings/BegRohu2008/index.html The Beg Rohu Summer School: Manifolds in random media, random matrices and extreme value statistics] 16th - 28th June 2008, French National Sailing School, Quiberon peninsula, France.&lt;br /&gt;
*[http://www.chm.bris.ac.uk/cms/ Computational Molecular Science 2008] 22nd – 25th June 2008, Cirencester, UK.&lt;br /&gt;
*[http://www.liquids2008.se/ 7th Liquid Matter Conference] 27 June - 1 July 2008  Lund, Sweden&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School 2008] University of Sheffield, England July 6 - July 15 2008.&lt;br /&gt;
*Potentials Workshop: Recent developments in interatomic potentials 7-8 July 2008  Oxford, UK&lt;br /&gt;
*[http://www.lcc-toulouse.fr/molmat2008/ MOLMAT2008 International Symposium on Molecular Materials based on Chemistry, Solid State Physics, Theory and Nanotechnology]   July 8-11th  2008 Toulouse, France&lt;br /&gt;
*[http://www2.polito.it/eventi/sigmaphi2008/ SigmaPhi2008] 14th -18th July 2008 Kolympari, Crete, Greece&lt;br /&gt;
*[http://www.cecam.org/workshop-188.html Dissipative Particle Dynamics: Addressing deficiencies and establishing new frontiers] July, 16th-18th 2008  CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/event_22243.html Molecular Dynamics for Non-Adiabatic Processes] 21 July 2008 to 22 July 2008 Institute of Physics, London&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcitaa_08/announcement.html Quantum Monte Carlo in the Apuan Alps IV] 26th July - Sat 2nd August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.cecam.org/workshop-215.html New directions in the theory and modelling of liquid crystals] July, 28th 2008 to July, 30th 2008, CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcatcp_08/announcement.html Quantum Monte Carlo and the CASINO program III] 3rd August - Sun 10th August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.icct2008.org/ 20th International Conference on Chemical Thermodynamics] August 3-8, 2008, Warsaw, Poland.&lt;br /&gt;
*[http://perso.ens-lyon.fr/thierry.dauxois/LORIS/LesHouchesSummerSchool2008.html Long-Range Interacting Systems] Summer School in Les Houches (France), 4-29 August 2008&lt;br /&gt;
*[http://ctbp.ucsd.edu/summer_school08/apply2008.html Coarse-Grained Physical Modeling of Biological Systems: Advanced Theory and Methods] August 11-15, 2008 University of California San Diego&lt;br /&gt;
*[http://www.chem.ucl.ac.uk/astrosurf/SIPML.html Surface and Interface Processes at the Molecular Level]  17 - 23 August 2008, Lucca, Italy&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD141/index.asp  Faraday Discussion 141: Water - From Interfaces to the Bulk] 27 - 29 August 2008 Heriot-Watt University, Edinburgh, United Kingdom&lt;br /&gt;
*[http://ectp18.conforganizer.net   18th European Conference on Thermophysical Properties]  31 Aug-4 Sep 2008 Pau, France&lt;br /&gt;
*[http://iber2008.df.fct.unl.pt/  9th Iberian Joint Meeting on Atomic and Molecular Physics - IBER 2008]  7-9th September,  Capuchos, Portugal&lt;br /&gt;
*[http://www.cmmp.ucl.ac.uk/~dmd/ccp5.htm  CCP5 Annual Meeting: Surfaces and Interfaces] 8-10th September, London, UK&lt;br /&gt;
*[http://ergodic.ugr.es/cp/ 10th  Granada  Seminar on Computational and Statistical Physics: Modeling and Simulation of New Materials] September 15-19, 2008 Granada, Spain&lt;br /&gt;
*[http://www.cecam.org/workshop-222.html Standardisation and databasing of ab-initio and classical simulations] September, 18th 2008 to September, 19th 2008  CECAM-ETHZ, Zurich, Switzerland&lt;br /&gt;
*[http://www.iccmse.org/ International Conference of Computational Methods in Sciences and Engineering 2008 (ICCMSE 2008)]  25-30 September, Crete, Greece&lt;br /&gt;
*[http://www.mmm2008.org/bin/view.pl/Main/WebHome Multscale Materials Modeling] 27–31 October 2008, Tallahassee, Florida USA&lt;br /&gt;
*[http://www.aiche.org/Conferences/AnnualMeeting/index.aspx 2008 AIChE Annual Meeting] November 16-21 2008 Philadelphia, Pennsylvania USA&lt;br /&gt;
*[http://www.ihp.jussieu.fr/ceb/Trimestres/T08-4/C3/index.html Statistical mechanics] Paris (France) 8-12 December 2008&lt;br /&gt;
*[http://complex.ffn.ub.es/bcnetworkshop BCNet Workshop] Trends and perspectives in complex networks. Barcelona (Spain) 10-12 December 2008&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 100th Statistical Mechanics Conference]  Rutgers University, (USA) 13-18 December 2008&lt;br /&gt;
=====2009=====&lt;br /&gt;
*[http://www.ccpb.ac.uk/events/conference/2009/ Biomolecular Simulation 2009] 6-8 January, Yorkshire Museum and Gardens, York, United Kingdom 2009&lt;br /&gt;
*[http://www.fisica.unam.mx/externos/wintermeeting/ XXXVIII edition of the Winter Meeting on Statistical Physics] Taxco, Guerrero (Mexico) 6th - 9th January, 2009.&lt;br /&gt;
*[http://www.ucl.ac.uk/msl/events/2009/workshop09.htm 2009 MSL Workshop: Accessing large length and time scales with accurate quantum methods]  12th - 13th January 2009 University College London (United Kingdom)&lt;br /&gt;
*[http://euler.us.es/%7Eopap/stochgame/index-en.html Stochastic Models in Physics, Biology, and Social Sciences] Carmona (Sevilla), Spain February 12-14 (2009)&lt;br /&gt;
*[http://hera.physik.uni-konstanz.de/igk/news/workshops/homepage/index.html Frontiers of Soft Condensed Matter 2009]  Les Houches () 15-20 February  2009&lt;br /&gt;
*[http://www.mpipks-dresden.mpg.de/~mbsffe09/ Many-body systems far from equilibrium: Fluctuations, slow dynamics and long-range interactions] Max Planck Institute for the Physics of Complex Systems Dresden, Germany February 16 - 27 (2009)&lt;br /&gt;
*[http://www.formulation.org.uk/Conference_flyers_Sept2007_on/Flyer-sims.pdf Workshop on advances in modelling for formulations]  25th of March 2009 at GSK Waybridge (United Kingdom)&lt;br /&gt;
*[http://www.physik.uni-leipzig.de/~janke/meco34/ 34th Conference of the Middle European Cooperation in Statistical Physics] 30 March - 01 April 2009 Universität Leipzig (Germany)&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws2/ Workshop II: The Boltzmann Equation: DiPerna-Lions Plus 20 Years] April 15-17 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-313.html Computational Studies of Defects in Nanoscale Carbon Materials]  May 11, 2009 to May 13, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.cecam.org/workshop-320.html Modeling of Carbon and Inorganic Nanotubes and Nanostructures]  May 13, 2009 to May 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ima.umn.edu/2008-2009/W5.18-22.09/ Molecular Simulations: Algorithms, Analysis, and Applications] Institute for Mathematics and its Applications, University of Minnesota (USA), May 18-22, 2009&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws4/ Workshop IV: Asymptotic Methods for Dissipative Particle Systems] May 18-22 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-310.html Computer Simulation in Food Science: CFD meets Soft Matter]  May 25, 2009 to May 27, 2009 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://complenet09.diit.unict.it  CompleNet 2009] International Workshop on Complex Networks. Catania (Italy),  May 26-28, 2009&lt;br /&gt;
*[http://go.warwick.ac.uk/maths/research/events/2008_2009/symposium/wks5/ EPSRC Symposium Workshop on Molecular Dynamics] Monday 1 – Friday 5 June (2009) Warwick (United Kingdom)&lt;br /&gt;
*[http://www.cecam.org/workshop-272.html Theoretical Modeling of Transport in Nanostructures]  June 2, 2009 to June 5, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland) &lt;br /&gt;
*[http://www.mpip-mainz.mpg.de/mmsd/ Mainz Materials Simulation Days] 3-5 June 2009 Max Planck Institute for Polymer Research (Germany)&lt;br /&gt;
*[http://www.soms.ethz.ch/workshop2009 Coping with Crises in Complex Socio-Economic Systems] ETH Zurich (Switzerland), June 8-13, 2009&lt;br /&gt;
*[[MOSSNOHO Workshop 2009]] 16 of June 2009, Universidad Complutense de Madrid (Spain)&lt;br /&gt;
*[http://cftc.cii.fc.ul.pt/Workshops/flowNjam/index.html Flow(ers) and jam(mers): from liquid crystals to grains] Lisbon (Portugal) 17-19 June 2009&lt;br /&gt;
*[http://ipht.cea.fr/Meetings/BegRohu2009/ Beg Rohu Summer School: Quantum Physics Out of Equilibrium] Ecole Nationale de Voile (France) 15-27 June 2009&lt;br /&gt;
*[http://symp17.boulder.nist.gov  Seventeenth Symposium on Thermophysical Properties] Boulder, Colorado (USA), June 21-26, 2009&lt;br /&gt;
*[http://www.fhi-berlin.mpg.de/th/Meetings/DFT-workshop-Berlin2009/ Hands-on Tutorial on Ab Initio Molecular Simulations: Toward a First-Principles Understanding of Materials Properties and Functions] Berlin (Germany) June 22-July 1 2009&lt;br /&gt;
*[https://www.irphe.univ-mrs.fr/~fe09 Fluid and Elasticity] Carry-le-Rouet, near Marseilles (France) June 23-26, 2009&lt;br /&gt;
*[http://www.icmp.lviv.ua/statphys2009/ Statistical Physics: Modern Trends and Applications] June 23-25, 2009 Lviv, (Ukraine)&lt;br /&gt;
*[http://www.fuw.edu.pl/~wssph/ 3rd Warsaw School of Statistical Physics] Kazimierz Dolny (Poland), 27 June - 4 July, 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-298.html Modeling and Simulation of Water at Interfaces from Ambient to Supercooled Conditions] June 29, 2009 to July 1, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School] University of Sheffield  (England) July 5 - July 14 2009 &lt;br /&gt;
*[http://math.arizona.edu/~goriely/leshouches/home.html  New trends in the Physics and Mechanics of Biological Systems&amp;quot;]  Les Houches (France), 6-31 July 2009&lt;br /&gt;
*[http://research.yale.edu/boulder/Boulder-2009/index.html Nonequilibrium Statistical Mechanics: Fundamental Problems and Applications] July 6-24  2009 Boulder (USA)&lt;br /&gt;
*[http://www.xrqtc.cat/index.php/ca/homew New trends in Computational Chemistry for Industry Applications] July 6-7 Barcelona (Spain)&lt;br /&gt;
*[http://www.frias.uni-freiburg.de/BFF Computational Methods for Soft Matter and Biological Systems] July 8-11, 2009, FRIAS, Freiburg (Germany)&lt;br /&gt;
*[http://www.cecam.org/workshop-286.html Structural Transitions in Solids: Theory, Simulations, Experiments and Visualization Techniques] July 8, 2009 to July 11, 2009 CECAM-USI, Lugano (Switzerland)&lt;br /&gt;
*[http://fomms.org FOMMS 2009, Fourth International Conference Foundations of Molecular Modeling and Simulation] Semiahmoo Resort, Blaine, WA (USA)  12-16 July 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-308.html Computer Simulation Approaches to Study Self-Assembly: From Patchy Nano-Colloids to Virus Capsids]  July 13, 2009 to July 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.md-net.org.uk/events/bath_jul_2009.htm EPSRC Network Mathematical Challenges of Molecular Dynamics] 13-15 July (2009) Bath, United Kingdom.&lt;br /&gt;
*[http://www.cecam.org/workshop-279.html New Trends in Simulating Colloids: from Models to Applications] July 15, 2009 to July 18, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD144/index.asp Faraday Discussion 144: Multiscale Modelling of Soft Matter] University of Groningen (The Netherlands) 20 - 22 July 2009&lt;br /&gt;
*[http://www2.yukawa.kyoto-u.ac.jp/~ykis2009/Welcome.html Frontiers in Nonequilibrium Physics: Fundamental Theory, Glassy &amp;amp; Granular Materials, and Computational Physics] July 21 - August 21, 2009  Kyoto (Japan)&lt;br /&gt;
*[http://www.cecam.org/workshop-293.html Fundamental Aspects of Deterministic Thermostats] July 27, 2009 to July 29, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program IV]  2nd-9th August 2009 Towler Institute, Tuscany, (Italy)&lt;br /&gt;
*[http://www.warwick.ac.uk/go/quantsim09  EPSRC Symposium Workshop on Quantum Simulations] 24th-28th August 2009 University of Warwick (United Kingdom)&lt;br /&gt;
*[http://itf.fys.kuleuven.be/~fpspXII/ Fundamental Problems in Statistical Physics XII] August 31 - September 11, 2009 Leuven (Belgium)&lt;br /&gt;
*[http://denali.phys.uniroma1.it/~idmrcs6/ 6th International Discussion Meeting on Relaxations in Complex Systems] August 31- September 5, 2009, Roma (Italy)&lt;br /&gt;
*[http://www.dft09.org/ International Conference on the Applications of Density Functional Theory in Chemistry and Physics] August 31st to September 4th 2009  Lyon (France)&lt;br /&gt;
*[http://www.dfrl.ucl.ac.uk/CCP5/ccp5.htm CCP5 Annual Meeting 2009 Structure Prediction]  7th to  9th, September 2009 London (United Kingdom)&lt;br /&gt;
*[http://fises.dfa.uhu.es/fises09/ XVI Congreso de Física Estadística] Huelva, 10-12  September  2009, Spain&lt;br /&gt;
*[http://th-www.if.uj.edu.pl/zfs/smoluchowski/ 22nd Marian Smoluchowski Symposium On Statistical Physics] 12-17 September 2009 Zakopane (Poland)&lt;br /&gt;
*[http://www.isis.rl.ac.uk/largescale/loq/SAS2009/SAS2009.htm SAS-2009] XIV International Conference on Small-Angle Scattering, Sunday 13 - Friday 18 September, 2009, Oxford (UK)&lt;br /&gt;
*[http://www.esc.sandia.gov/dsmc09/dsmc09.html Direct Simulation Monte Carlo workshop] September 13-16, 2009 Santa Fe, New Mexico, USA,&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/PHYSASPECTS_09/index.html Physical Aspects of Polymer Science] 14-16 September 2009 Bristol (United Kingdom)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
__NOTOC__&lt;br /&gt;
[[category: Miscellaneous]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Conferences</id>
		<title>Conferences</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Conferences"/>
				<updated>2009-09-22T07:43:33Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Conf. added&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The following is a chronological list of conferences, seminars, or meetings related to thermodynamics, statistical mechanics, soft condensed matter, many-body problems, complex fluids etc. &lt;br /&gt;
===2009===&lt;br /&gt;
====September====&lt;br /&gt;
*[http://www.thermodynamics2009.org/ Thermodynamics 2009] September 23-25  Imperial College London , U.K. (2009)&lt;br /&gt;
====October====&lt;br /&gt;
*[http://paginas.fe.up.pt/~equifase/ EQUIFASE 2009] VIII Iberoamerican Conference on Phase Equilibria and Fluid Properties for Process Design, Praia da Rocha, Portugal 17-21 October 2009&lt;br /&gt;
*[http://cint.lanl.gov/workshop2009/ Multiple Length Scales in Polymers and Complex Fluids] October 18- 21, 2009 Bishop's Lodge, Santa Fe (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-290.html Classical Density Functional Theory Methods in Soft and Hard Matter] October 21, 2009 to October 23, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://seneca.fis.ucm.es/parr/ktlog2_09 kTlog2 '09: Computing Matters Workshop] 22-24 October, 2009, Toledo (Spain)&lt;br /&gt;
====November====&lt;br /&gt;
*[http://www.dfi.uchile.cl/~granular09/Welcome.html Southern Workshop on Granular Materials 2009 - SWGM09] November 30 to December 4 2009, Viña del Mar (Chile)&lt;br /&gt;
*[http://www.lorentzcenter.nl/lc/web/2009/357/info.php3?wsid=357 Subdivide and Tile: Triangulating spaces for understanding the world] Nov 16 to 20 Nov 20 2009, Leiden (Netherlands)&lt;br /&gt;
&lt;br /&gt;
====December====&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 102nd Statistical Mechanics Conference]  Rutgers University, December 13-15, 2009 (USA)&lt;br /&gt;
*[http://www.cmmp.org.uk/ Condensed Matter and Materials Physics (CMMP)] 15-17 December 2009 Warwick University (United Kingdom)&lt;br /&gt;
&lt;br /&gt;
===2010===&lt;br /&gt;
====May====&lt;br /&gt;
*[http://www.ppeppd2010.cn/ Properties and Phase Equilibria for Product and Process Design] May 16-21, 2010 Suzhou, Jiangsu (China)&lt;br /&gt;
====June====&lt;br /&gt;
*[http://liblice.icpf.cas.cz/2010/2010.php Eighth  Liblice Conference on the Statistical Mechanics of Liquids] June 13-18, 2010 Brno (Czech Republic)&lt;br /&gt;
&lt;br /&gt;
====July====&lt;br /&gt;
*[http://ismc2010.ugr.es International Soft Matter Conference 2010] 5th-8th July 2010, Granada, Spain&lt;br /&gt;
*[http://www.statphys.org.au StatPhys 24: XXIV International Conference on Statistical Physics of the International Union for Pure and Applied Physics (IUPAP)] 19-23 July, (2010). Cairns (Australia)&lt;br /&gt;
&lt;br /&gt;
==Previous conferences==&lt;br /&gt;
=====2007=====&lt;br /&gt;
*[http://www.simbioma.cecam.org/ Simulation of Hard Bodies] April 16 to April 19 2007 in Lyon.&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 97th Statistical Mechanics Conference] May 6-8, 2007 Rutgers University&lt;br /&gt;
*[http://www.ucm.es/info/molecsim/luis/workshop.htm Workshop on Theory and Computer Simulations of Inhomogenoeus Fluids] May 16-18, 2007, Universidad Complutense, Madrid.&lt;br /&gt;
*[http://www-thphys.physics.ox.ac.uk/users/JuliaYeomans/OxfordWorkshop/home.php Mesoscale Modelling for Complex Fluids and Flows] June 25--27, 2007 University of Oxford, UK.&lt;br /&gt;
*[http://www.ecns2007.org 4th European Conference on Neutron Scattering] Lund, Sweden 25-29 June 2007&lt;br /&gt;
*[http://www.realitygrid.org/CompSci07 Computational Science 2007] 25-26 June 2007  The Royal Society, London&lt;br /&gt;
*[https://www.cecam.fr/index.php?content=activities/workshop New directions in liquid state theory] CECAM workshop, 2 - 4 July, 2007 at ENS, Lyon, France.&lt;br /&gt;
*[http://www.cecam.fr/index.php?content=activities/workshop&amp;amp;action=details&amp;amp;wid=157 Fluid phase behaviour and critical phenomena from liquid state theories and simulations] 5-7 July  2007 CECAM workshop, Lyon, France.&lt;br /&gt;
*[http://www.statphys23.org/ STATPHYS 23] Genova, Italy, from July 9 to 13, 2007.&lt;br /&gt;
*[http://www.iupac2007.org/ 41st IUPAC World Chemistry Conference] Turin, Italy, August 5-11th&lt;br /&gt;
*[http://www.srcf.ucam.org/~jae1001/ccp5_2007 CCP5 Annual Conference] 29th-31st August 2007 New Hall, Cambridge, UK&lt;br /&gt;
*[http://ccp2007.ulb.ac.be CCP 2007] Brussels  5-8 September  2007&lt;br /&gt;
*[http://www.castep.org CASTEP Workshop] 17th - 21st September 2007 University of York, UK&lt;br /&gt;
*[http://thermo2007.ifp.fr Thermodynamics 2007] 26-28 September 2007, IFP - Rueil-Malmaison (France)&lt;br /&gt;
*[http://www.iccmse.org/  International Conference of Computational Methods in Sciences and Engineering 2007] Corfu, Greece, 25-30 September 2007&lt;br /&gt;
*[http://www.chem.unisa.it/polnan/index.html Polymers in Nanotechnology] 27-28th September 2007, Salerno, Italy.&lt;br /&gt;
*[http://www.fz-juelich.de/iff/ismc2007/  International Soft Matter Conference 2007] 1 - 4 October 2007, Eurogress, Aachen (Germany)&lt;br /&gt;
*[http://www.escet.urjc.es/~fisica/encuentro_complejos/index.html II Meeting on Modelling of Complex Systems]  Universidad Rey Juan Carlos, Mostoles (Madrid), October 25-26 2007&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/SCD/event_22663.html Structuring Colloidal Dispersions by External Fields] 21 November 2007, Institute of Physics, London, United Kingdom&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 98th Statistical Mechanics Conference] December 16-18, 2007, Rutgers University, New Jersey, USA.&lt;br /&gt;
=====2008=====&lt;br /&gt;
*[http://www.iop.org/activity/groups/subject/lcf/Events/file_25833.pdf Recent Advances in the Understanding of Confined Fluids: from Superfluids to Oil Reservoirs] 9-11 January, Cosener's House, Abingdon UK&lt;br /&gt;
*[http://academic.sun.ac.za/summerschool/2008.html  Workshop on Soft Condensed Matter and Physics of Biological Systems - Perspectives and topics for South Africa]  23 Jan 2008 - 1 Feb 2008 National Institute for Theoretical Physics at Stellenbosch Institute of Advanced Study, Stellenbosch, Western Cape, South Africa&lt;br /&gt;
*[http://bifi.unizar.es/events/bifi2008/main.htm Bifi 2008 Large Scale Simulations of Complex Systems, Condensed Matter and Fusion Plasma] 6–8 February 2008, Zaragoza, Spain&lt;br /&gt;
*[http://events.dechema.de/Tagungen/MolMod+Workshop.html International Workshop Molecular Modeling and Simulation in Applied Material Science] March 10-11,  DECHEMA-Haus, Frankfurt am Main, Germany&lt;br /&gt;
*[http://www.aps.org/meetings/march/index.cfm APS March Meeting] March 10-14, 2008. New Orleans, Louisiana, USA&lt;br /&gt;
*[http://users.physik.tu-muenchen.de/metz/jerusalem.html Modelling anomalous diffusion and relaxation]  23–28 March 2008, Jerusalem, Israel&lt;br /&gt;
*[http://www.newton.cam.ac.uk/programmes/CSM/csmw02.html Markov-Chain Monte Carlo Methods] 25 March to 28 March 2008 Isaac Newton Institute for Mathematical Sciences, Cambridge, UK &lt;br /&gt;
*[http://www.usal.es/~fises/ XV Congreso de Física Estadística (Fises' 08)] 27-29 March 2008, Salamanca, Spain&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/CMMP08/event_26545.html Condensed Matter and Materials Physics (CMMP)]  26-28 March 2008 Royal Holloway, University of London, UK&lt;br /&gt;
*[http://www.icmab.es/softmatter2008/index.html SoftMatter 2008] &amp;quot;Workshop on Electrostatic Effects in Soft Matter: Bringing Experiments, Theory and Simulation Together&amp;quot; 10 – 11 April ICMAB-CSIC, Barcelona, Spain.&lt;br /&gt;
*[http://www.icmab.es/11emscf/index.html 11th European Meeting on Supercritical Fluids] &amp;quot;New Perspectives in Supercritical Fluids: Nanoscience, Materials and Processing&amp;quot; 4-7 May 2008, ICMAB-CSIC, Barcelona, Spain&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 99th Statistical Mechanics Conference] May 11-13, 2008 Rutgers University,  USA&lt;br /&gt;
*[http://www.fondation-pgg.org/events/degennesdays/ DeGennesDays] 15-17 May 2008 Collège de France, Paris.&lt;br /&gt;
*[http://www.ill.fr/Events/rktsymposium/  Surfaces and Interfaces in Soft Matter and Biology SISMB 2008] &amp;quot;The impact and future of neutron reflectivity - A Symposium in Honor of Robert K. Thomas&amp;quot; 21-23 May 2008, Institut Laue-Langevin (Grenoble, France).&lt;br /&gt;
*[http://www.plmmp.univ.kiev.ua/ Physics of Liquid Matter: Modern Problems] May 23-26, 2008, Kyiv National Taras Shevchenko University, Ukraine&lt;br /&gt;
*[http://www.ffn.ub.es/sitges/ XXI Sitges Conference] XXI Sitges Conference on Statistical Mechanics. Statistical Mechanics of Molecular Biophysics  2nd-6th June 2008, Sitges, Spain&lt;br /&gt;
*[http://www1.ci.uc.pt/gcpi/poly2008 Polyelectrolytes 2008]  16th-19th June 2008, Coimbra, Portugal&lt;br /&gt;
*[http://www-spht.cea.fr/Meetings/BegRohu2008/index.html The Beg Rohu Summer School: Manifolds in random media, random matrices and extreme value statistics] 16th - 28th June 2008, French National Sailing School, Quiberon peninsula, France.&lt;br /&gt;
*[http://www.chm.bris.ac.uk/cms/ Computational Molecular Science 2008] 22nd – 25th June 2008, Cirencester, UK.&lt;br /&gt;
*[http://www.liquids2008.se/ 7th Liquid Matter Conference] 27 June - 1 July 2008  Lund, Sweden&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School 2008] University of Sheffield, England July 6 - July 15 2008.&lt;br /&gt;
*Potentials Workshop: Recent developments in interatomic potentials 7-8 July 2008  Oxford, UK&lt;br /&gt;
*[http://www.lcc-toulouse.fr/molmat2008/ MOLMAT2008 International Symposium on Molecular Materials based on Chemistry, Solid State Physics, Theory and Nanotechnology]   July 8-11th  2008 Toulouse, France&lt;br /&gt;
*[http://www2.polito.it/eventi/sigmaphi2008/ SigmaPhi2008] 14th -18th July 2008 Kolympari, Crete, Greece&lt;br /&gt;
*[http://www.cecam.org/workshop-188.html Dissipative Particle Dynamics: Addressing deficiencies and establishing new frontiers] July, 16th-18th 2008  CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/event_22243.html Molecular Dynamics for Non-Adiabatic Processes] 21 July 2008 to 22 July 2008 Institute of Physics, London&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcitaa_08/announcement.html Quantum Monte Carlo in the Apuan Alps IV] 26th July - Sat 2nd August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.cecam.org/workshop-215.html New directions in the theory and modelling of liquid crystals] July, 28th 2008 to July, 30th 2008, CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcatcp_08/announcement.html Quantum Monte Carlo and the CASINO program III] 3rd August - Sun 10th August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.icct2008.org/ 20th International Conference on Chemical Thermodynamics] August 3-8, 2008, Warsaw, Poland.&lt;br /&gt;
*[http://perso.ens-lyon.fr/thierry.dauxois/LORIS/LesHouchesSummerSchool2008.html Long-Range Interacting Systems] Summer School in Les Houches (France), 4-29 August 2008&lt;br /&gt;
*[http://ctbp.ucsd.edu/summer_school08/apply2008.html Coarse-Grained Physical Modeling of Biological Systems: Advanced Theory and Methods] August 11-15, 2008 University of California San Diego&lt;br /&gt;
*[http://www.chem.ucl.ac.uk/astrosurf/SIPML.html Surface and Interface Processes at the Molecular Level]  17 - 23 August 2008, Lucca, Italy&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD141/index.asp  Faraday Discussion 141: Water - From Interfaces to the Bulk] 27 - 29 August 2008 Heriot-Watt University, Edinburgh, United Kingdom&lt;br /&gt;
*[http://ectp18.conforganizer.net   18th European Conference on Thermophysical Properties]  31 Aug-4 Sep 2008 Pau, France&lt;br /&gt;
*[http://iber2008.df.fct.unl.pt/  9th Iberian Joint Meeting on Atomic and Molecular Physics - IBER 2008]  7-9th September,  Capuchos, Portugal&lt;br /&gt;
*[http://www.cmmp.ucl.ac.uk/~dmd/ccp5.htm  CCP5 Annual Meeting: Surfaces and Interfaces] 8-10th September, London, UK&lt;br /&gt;
*[http://ergodic.ugr.es/cp/ 10th  Granada  Seminar on Computational and Statistical Physics: Modeling and Simulation of New Materials] September 15-19, 2008 Granada, Spain&lt;br /&gt;
*[http://www.cecam.org/workshop-222.html Standardisation and databasing of ab-initio and classical simulations] September, 18th 2008 to September, 19th 2008  CECAM-ETHZ, Zurich, Switzerland&lt;br /&gt;
*[http://www.iccmse.org/ International Conference of Computational Methods in Sciences and Engineering 2008 (ICCMSE 2008)]  25-30 September, Crete, Greece&lt;br /&gt;
*[http://www.mmm2008.org/bin/view.pl/Main/WebHome Multscale Materials Modeling] 27–31 October 2008, Tallahassee, Florida USA&lt;br /&gt;
*[http://www.aiche.org/Conferences/AnnualMeeting/index.aspx 2008 AIChE Annual Meeting] November 16-21 2008 Philadelphia, Pennsylvania USA&lt;br /&gt;
*[http://www.ihp.jussieu.fr/ceb/Trimestres/T08-4/C3/index.html Statistical mechanics] Paris (France) 8-12 December 2008&lt;br /&gt;
*[http://complex.ffn.ub.es/bcnetworkshop BCNet Workshop] Trends and perspectives in complex networks. Barcelona (Spain) 10-12 December 2008&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 100th Statistical Mechanics Conference]  Rutgers University, (USA) 13-18 December 2008&lt;br /&gt;
=====2009=====&lt;br /&gt;
*[http://www.ccpb.ac.uk/events/conference/2009/ Biomolecular Simulation 2009] 6-8 January, Yorkshire Museum and Gardens, York, United Kingdom 2009&lt;br /&gt;
*[http://www.fisica.unam.mx/externos/wintermeeting/ XXXVIII edition of the Winter Meeting on Statistical Physics] Taxco, Guerrero (Mexico) 6th - 9th January, 2009.&lt;br /&gt;
*[http://www.ucl.ac.uk/msl/events/2009/workshop09.htm 2009 MSL Workshop: Accessing large length and time scales with accurate quantum methods]  12th - 13th January 2009 University College London (United Kingdom)&lt;br /&gt;
*[http://euler.us.es/%7Eopap/stochgame/index-en.html Stochastic Models in Physics, Biology, and Social Sciences] Carmona (Sevilla), Spain February 12-14 (2009)&lt;br /&gt;
*[http://hera.physik.uni-konstanz.de/igk/news/workshops/homepage/index.html Frontiers of Soft Condensed Matter 2009]  Les Houches () 15-20 February  2009&lt;br /&gt;
*[http://www.mpipks-dresden.mpg.de/~mbsffe09/ Many-body systems far from equilibrium: Fluctuations, slow dynamics and long-range interactions] Max Planck Institute for the Physics of Complex Systems Dresden, Germany February 16 - 27 (2009)&lt;br /&gt;
*[http://www.formulation.org.uk/Conference_flyers_Sept2007_on/Flyer-sims.pdf Workshop on advances in modelling for formulations]  25th of March 2009 at GSK Waybridge (United Kingdom)&lt;br /&gt;
*[http://www.physik.uni-leipzig.de/~janke/meco34/ 34th Conference of the Middle European Cooperation in Statistical Physics] 30 March - 01 April 2009 Universität Leipzig (Germany)&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws2/ Workshop II: The Boltzmann Equation: DiPerna-Lions Plus 20 Years] April 15-17 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-313.html Computational Studies of Defects in Nanoscale Carbon Materials]  May 11, 2009 to May 13, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.cecam.org/workshop-320.html Modeling of Carbon and Inorganic Nanotubes and Nanostructures]  May 13, 2009 to May 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ima.umn.edu/2008-2009/W5.18-22.09/ Molecular Simulations: Algorithms, Analysis, and Applications] Institute for Mathematics and its Applications, University of Minnesota (USA), May 18-22, 2009&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws4/ Workshop IV: Asymptotic Methods for Dissipative Particle Systems] May 18-22 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-310.html Computer Simulation in Food Science: CFD meets Soft Matter]  May 25, 2009 to May 27, 2009 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://complenet09.diit.unict.it  CompleNet 2009] International Workshop on Complex Networks. Catania (Italy),  May 26-28, 2009&lt;br /&gt;
*[http://go.warwick.ac.uk/maths/research/events/2008_2009/symposium/wks5/ EPSRC Symposium Workshop on Molecular Dynamics] Monday 1 – Friday 5 June (2009) Warwick (United Kingdom)&lt;br /&gt;
*[http://www.cecam.org/workshop-272.html Theoretical Modeling of Transport in Nanostructures]  June 2, 2009 to June 5, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland) &lt;br /&gt;
*[http://www.mpip-mainz.mpg.de/mmsd/ Mainz Materials Simulation Days] 3-5 June 2009 Max Planck Institute for Polymer Research (Germany)&lt;br /&gt;
*[http://www.soms.ethz.ch/workshop2009 Coping with Crises in Complex Socio-Economic Systems] ETH Zurich (Switzerland), June 8-13, 2009&lt;br /&gt;
*[[MOSSNOHO Workshop 2009]] 16 of June 2009, Universidad Complutense de Madrid (Spain)&lt;br /&gt;
*[http://cftc.cii.fc.ul.pt/Workshops/flowNjam/index.html Flow(ers) and jam(mers): from liquid crystals to grains] Lisbon (Portugal) 17-19 June 2009&lt;br /&gt;
*[http://ipht.cea.fr/Meetings/BegRohu2009/ Beg Rohu Summer School: Quantum Physics Out of Equilibrium] Ecole Nationale de Voile (France) 15-27 June 2009&lt;br /&gt;
*[http://symp17.boulder.nist.gov  Seventeenth Symposium on Thermophysical Properties] Boulder, Colorado (USA), June 21-26, 2009&lt;br /&gt;
*[http://www.fhi-berlin.mpg.de/th/Meetings/DFT-workshop-Berlin2009/ Hands-on Tutorial on Ab Initio Molecular Simulations: Toward a First-Principles Understanding of Materials Properties and Functions] Berlin (Germany) June 22-July 1 2009&lt;br /&gt;
*[https://www.irphe.univ-mrs.fr/~fe09 Fluid and Elasticity] Carry-le-Rouet, near Marseilles (France) June 23-26, 2009&lt;br /&gt;
*[http://www.icmp.lviv.ua/statphys2009/ Statistical Physics: Modern Trends and Applications] June 23-25, 2009 Lviv, (Ukraine)&lt;br /&gt;
*[http://www.fuw.edu.pl/~wssph/ 3rd Warsaw School of Statistical Physics] Kazimierz Dolny (Poland), 27 June - 4 July, 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-298.html Modeling and Simulation of Water at Interfaces from Ambient to Supercooled Conditions] June 29, 2009 to July 1, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School] University of Sheffield  (England) July 5 - July 14 2009 &lt;br /&gt;
*[http://math.arizona.edu/~goriely/leshouches/home.html  New trends in the Physics and Mechanics of Biological Systems&amp;quot;]  Les Houches (France), 6-31 July 2009&lt;br /&gt;
*[http://research.yale.edu/boulder/Boulder-2009/index.html Nonequilibrium Statistical Mechanics: Fundamental Problems and Applications] July 6-24  2009 Boulder (USA)&lt;br /&gt;
*[http://www.xrqtc.cat/index.php/ca/homew New trends in Computational Chemistry for Industry Applications] July 6-7 Barcelona (Spain)&lt;br /&gt;
*[http://www.frias.uni-freiburg.de/BFF Computational Methods for Soft Matter and Biological Systems] July 8-11, 2009, FRIAS, Freiburg (Germany)&lt;br /&gt;
*[http://www.cecam.org/workshop-286.html Structural Transitions in Solids: Theory, Simulations, Experiments and Visualization Techniques] July 8, 2009 to July 11, 2009 CECAM-USI, Lugano (Switzerland)&lt;br /&gt;
*[http://fomms.org FOMMS 2009, Fourth International Conference Foundations of Molecular Modeling and Simulation] Semiahmoo Resort, Blaine, WA (USA)  12-16 July 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-308.html Computer Simulation Approaches to Study Self-Assembly: From Patchy Nano-Colloids to Virus Capsids]  July 13, 2009 to July 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.md-net.org.uk/events/bath_jul_2009.htm EPSRC Network Mathematical Challenges of Molecular Dynamics] 13-15 July (2009) Bath, United Kingdom.&lt;br /&gt;
*[http://www.cecam.org/workshop-279.html New Trends in Simulating Colloids: from Models to Applications] July 15, 2009 to July 18, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD144/index.asp Faraday Discussion 144: Multiscale Modelling of Soft Matter] University of Groningen (The Netherlands) 20 - 22 July 2009&lt;br /&gt;
*[http://www2.yukawa.kyoto-u.ac.jp/~ykis2009/Welcome.html Frontiers in Nonequilibrium Physics: Fundamental Theory, Glassy &amp;amp; Granular Materials, and Computational Physics] July 21 - August 21, 2009  Kyoto (Japan)&lt;br /&gt;
*[http://www.cecam.org/workshop-293.html Fundamental Aspects of Deterministic Thermostats] July 27, 2009 to July 29, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program IV]  2nd-9th August 2009 Towler Institute, Tuscany, (Italy)&lt;br /&gt;
*[http://www.warwick.ac.uk/go/quantsim09  EPSRC Symposium Workshop on Quantum Simulations] 24th-28th August 2009 University of Warwick (United Kingdom)&lt;br /&gt;
*[http://itf.fys.kuleuven.be/~fpspXII/ Fundamental Problems in Statistical Physics XII] August 31 - September 11, 2009 Leuven (Belgium)&lt;br /&gt;
*[http://denali.phys.uniroma1.it/~idmrcs6/ 6th International Discussion Meeting on Relaxations in Complex Systems] August 31- September 5, 2009, Roma (Italy)&lt;br /&gt;
*[http://www.dft09.org/ International Conference on the Applications of Density Functional Theory in Chemistry and Physics] August 31st to September 4th 2009  Lyon (France)&lt;br /&gt;
*[http://www.dfrl.ucl.ac.uk/CCP5/ccp5.htm CCP5 Annual Meeting 2009 Structure Prediction]  7th to  9th, September 2009 London (United Kingdom)&lt;br /&gt;
*[http://fises.dfa.uhu.es/fises09/ XVI Congreso de Física Estadística] Huelva, 10-12  September  2009, Spain&lt;br /&gt;
*[http://th-www.if.uj.edu.pl/zfs/smoluchowski/ 22nd Marian Smoluchowski Symposium On Statistical Physics] 12-17 September 2009 Zakopane (Poland)&lt;br /&gt;
*[http://www.isis.rl.ac.uk/largescale/loq/SAS2009/SAS2009.htm SAS-2009] XIV International Conference on Small-Angle Scattering, Sunday 13 - Friday 18 September, 2009, Oxford (UK)&lt;br /&gt;
*[http://www.esc.sandia.gov/dsmc09/dsmc09.html Direct Simulation Monte Carlo workshop] September 13-16, 2009 Santa Fe, New Mexico, USA,&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/PHYSASPECTS_09/index.html Physical Aspects of Polymer Science] 14-16 September 2009 Bristol (United Kingdom)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
__NOTOC__&lt;br /&gt;
[[category: Miscellaneous]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Conferences</id>
		<title>Conferences</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Conferences"/>
				<updated>2009-07-07T09:02:40Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: new October conference&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The following is a chronological list of conferences, seminars, or meetings related to thermodynamics, statistical mechanics, soft condensed matter, many-body problems, complex fluids etc. &lt;br /&gt;
===2009===&lt;br /&gt;
====July====&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School] University of Sheffield  (England) July 5 - July 14 2009 &lt;br /&gt;
*[http://math.arizona.edu/~goriely/leshouches/home.html  New trends in the Physics and Mechanics of Biological Systems&amp;quot;]  Les Houches (France), 6-31 July 2009&lt;br /&gt;
*[http://research.yale.edu/boulder/Boulder-2009/index.html Nonequilibrium Statistical Mechanics: Fundamental Problems and Applications] July 6-24  2009 Boulder (USA)&lt;br /&gt;
*[http://www.xrqtc.cat/index.php/ca/homew New trends in Computational Chemistry for Industry Applications] July 6-7 Barcelona (Spain)&lt;br /&gt;
*[http://www.frias.uni-freiburg.de/BFF Computational Methods for Soft Matter and Biological Systems] July 8-11, 2009, FRIAS, Freiburg (Germany)&lt;br /&gt;
*[http://www.cecam.org/workshop-286.html Structural Transitions in Solids: Theory, Simulations, Experiments and Visualization Techniques] July 8, 2009 to July 11, 2009 CECAM-USI, Lugano (Switzerland)&lt;br /&gt;
*[http://fomms.org FOMMS 2009, Fourth International Conference Foundations of Molecular Modeling and Simulation] Semiahmoo Resort, Blaine, WA (USA)  12-16 July 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-308.html Computer Simulation Approaches to Study Self-Assembly: From Patchy Nano-Colloids to Virus Capsids]  July 13, 2009 to July 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.md-net.org.uk/events/bath_jul_2009.htm EPSRC Network Mathematical Challenges of Molecular Dynamics] 13-15 July (2009) Bath, United Kingdom.&lt;br /&gt;
*[http://www.cecam.org/workshop-279.html New Trends in Simulating Colloids: from Models to Applications] July 15, 2009 to July 18, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD144/index.asp Faraday Discussion 144: Multiscale Modelling of Soft Matter] University of Groningen (The Netherlands) 20 - 22 July 2009&lt;br /&gt;
*[http://www2.yukawa.kyoto-u.ac.jp/~ykis2009/Welcome.html Frontiers in Nonequilibrium Physics: Fundamental Theory, Glassy &amp;amp; Granular Materials, and Computational Physics] July 21 - August 21, 2009  Kyoto (Japan)&lt;br /&gt;
*[http://www.cecam.org/workshop-293.html Fundamental Aspects of Deterministic Thermostats] July 27, 2009 to July 29, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
&lt;br /&gt;
====August====&lt;br /&gt;
*[http://www.vallico.net/tti/tti.html Quantum Monte Carlo and the CASINO program IV]  2nd-9th August 2009 Towler Institute, Tuscany, (Italy)&lt;br /&gt;
*[http://itf.fys.kuleuven.be/~fpspXII/ Fundamental Problems in Statistical Physics XII] August 31 - September 11, 2009 Leuven (Belgium)&lt;br /&gt;
&lt;br /&gt;
====September====&lt;br /&gt;
*[http://www.dfrl.ucl.ac.uk/CCP5/ccp5.htm CCP5 Annual Meeting 2009 Structure Prediction]  7th to  9th, September 2009 London (United Kingdom)&lt;br /&gt;
*[http://th-www.if.uj.edu.pl/zfs/smoluchowski/ 22nd Marian Smoluchowski Symposium On Statistical Physics] 12-17 September 2009 Zakopane (Poland)&lt;br /&gt;
*[http://www.isis.rl.ac.uk/largescale/loq/SAS2009/SAS2009.htm SAS-2009] XIV International Conference on Small-Angle Scattering, Sunday 13 - Friday 18 September, 2009, Oxford (UK).&lt;br /&gt;
*[http://www.esc.sandia.gov/dsmc09/dsmc09.html Direct Simulation Monte Carlo workshop] September 13-16, 2009 Santa Fe, New Mexico, USA,&lt;br /&gt;
*[http://fises.dfa.uhu.es/fises09/ XVI Congreso de Física Estadística] Huelva, 10-12  September  2009, Spain&lt;br /&gt;
*[http://www.thermodynamics2009.org/ Thermodynamics 2009] September 23-25  Imperial College London , U.K. (2009)&lt;br /&gt;
&lt;br /&gt;
====October====&lt;br /&gt;
*[http://paginas.fe.up.pt/~equifase/ EQUIFASE 2009] VIII Iberoamerican Conference on Phase Equilibria and Fluid Properties for Process Design, Praia da Rocha, Portugal 17-21 October 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-290.html Classical Density Functional Theory Methods in Soft and Hard Matter] October 21, 2009 to October 23, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://seneca.fis.ucm.es/parr/ktlog2_09 kTlog2 '09: Computing Matters Workshop] 22-24 October, 2009, Toledo (Spain)&lt;br /&gt;
&lt;br /&gt;
===2010===&lt;br /&gt;
====May====&lt;br /&gt;
*[http://www.ppeppd2010.cn/ Properties and Phase Equilibria for Product and Process Design] May 16-21, 2010 Suzhou, Jiangsu (China)&lt;br /&gt;
====June====&lt;br /&gt;
*[http://liblice.icpf.cas.cz/2010/2010.php Eighth  Liblice Conference on the Statistical Mechanics of Liquids] June 13-18, 2010 Brno (Czech Republic)&lt;br /&gt;
&lt;br /&gt;
====July====&lt;br /&gt;
*[http://www.statphys.org.au StatPhys 24: XXIV International Conference on Statistical Physics of the International Union for Pure and Applied Physics (IUPAP)] 19-23 July, (2010). Cairns (Australia)&lt;br /&gt;
&lt;br /&gt;
==Previous conferences==&lt;br /&gt;
=====2007=====&lt;br /&gt;
*[http://www.simbioma.cecam.org/ Simulation of Hard Bodies] April 16 to April 19 2007 in Lyon.&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 97th Statistical Mechanics Conference] May 6-8, 2007 Rutgers University&lt;br /&gt;
*[http://www.ucm.es/info/molecsim/luis/workshop.htm Workshop on Theory and Computer Simulations of Inhomogenoeus Fluids] May 16-18, 2007, Universidad Complutense, Madrid.&lt;br /&gt;
*[http://www-thphys.physics.ox.ac.uk/users/JuliaYeomans/OxfordWorkshop/home.php Mesoscale Modelling for Complex Fluids and Flows] June 25--27, 2007 University of Oxford, UK.&lt;br /&gt;
*[http://www.ecns2007.org 4th European Conference on Neutron Scattering] Lund, Sweden 25-29 June 2007&lt;br /&gt;
*[http://www.realitygrid.org/CompSci07 Computational Science 2007] 25-26 June 2007  The Royal Society, London&lt;br /&gt;
*[https://www.cecam.fr/index.php?content=activities/workshop New directions in liquid state theory] CECAM workshop, 2 - 4 July, 2007 at ENS, Lyon, France.&lt;br /&gt;
*[http://www.cecam.fr/index.php?content=activities/workshop&amp;amp;action=details&amp;amp;wid=157 Fluid phase behaviour and critical phenomena from liquid state theories and simulations] 5-7 July  2007 CECAM workshop, Lyon, France.&lt;br /&gt;
*[http://www.statphys23.org/ STATPHYS 23] Genova, Italy, from July 9 to 13, 2007.&lt;br /&gt;
*[http://www.iupac2007.org/ 41st IUPAC World Chemistry Conference] Turin, Italy, August 5-11th&lt;br /&gt;
*[http://www.srcf.ucam.org/~jae1001/ccp5_2007 CCP5 Annual Conference] 29th-31st August 2007 New Hall, Cambridge, UK&lt;br /&gt;
*[http://ccp2007.ulb.ac.be CCP 2007] Brussels  5-8 September  2007&lt;br /&gt;
*[http://www.castep.org CASTEP Workshop] 17th - 21st September 2007 University of York, UK&lt;br /&gt;
*[http://thermo2007.ifp.fr Thermodynamics 2007] 26-28 September 2007, IFP - Rueil-Malmaison (France)&lt;br /&gt;
*[http://www.iccmse.org/  International Conference of Computational Methods in Sciences and Engineering 2007] Corfu, Greece, 25-30 September 2007&lt;br /&gt;
*[http://www.chem.unisa.it/polnan/index.html Polymers in Nanotechnology] 27-28th September 2007, Salerno, Italy.&lt;br /&gt;
*[http://www.fz-juelich.de/iff/ismc2007/  International Soft Matter Conference 2007] 1 - 4 October 2007, Eurogress, Aachen (Germany)&lt;br /&gt;
*[http://www.escet.urjc.es/~fisica/encuentro_complejos/index.html II Meeting on Modelling of Complex Systems]  Universidad Rey Juan Carlos, Mostoles (Madrid), October 25-26 2007&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/SCD/event_22663.html Structuring Colloidal Dispersions by External Fields] 21 November 2007, Institute of Physics, London, United Kingdom&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 98th Statistical Mechanics Conference] December 16-18, 2007, Rutgers University, New Jersey, USA.&lt;br /&gt;
=====2008=====&lt;br /&gt;
*[http://www.iop.org/activity/groups/subject/lcf/Events/file_25833.pdf Recent Advances in the Understanding of Confined Fluids: from Superfluids to Oil Reservoirs] 9-11 January, Cosener's House, Abingdon UK&lt;br /&gt;
*[http://academic.sun.ac.za/summerschool/2008.html  Workshop on Soft Condensed Matter and Physics of Biological Systems - Perspectives and topics for South Africa]  23 Jan 2008 - 1 Feb 2008 National Institute for Theoretical Physics at Stellenbosch Institute of Advanced Study, Stellenbosch, Western Cape, South Africa&lt;br /&gt;
*[http://bifi.unizar.es/events/bifi2008/main.htm Bifi 2008 Large Scale Simulations of Complex Systems, Condensed Matter and Fusion Plasma] 6–8 February 2008, Zaragoza, Spain&lt;br /&gt;
*[http://events.dechema.de/Tagungen/MolMod+Workshop.html International Workshop Molecular Modeling and Simulation in Applied Material Science] March 10-11,  DECHEMA-Haus, Frankfurt am Main, Germany&lt;br /&gt;
*[http://www.aps.org/meetings/march/index.cfm APS March Meeting] March 10-14, 2008. New Orleans, Louisiana, USA&lt;br /&gt;
*[http://users.physik.tu-muenchen.de/metz/jerusalem.html Modelling anomalous diffusion and relaxation]  23–28 March 2008, Jerusalem, Israel&lt;br /&gt;
*[http://www.newton.cam.ac.uk/programmes/CSM/csmw02.html Markov-Chain Monte Carlo Methods] 25 March to 28 March 2008 Isaac Newton Institute for Mathematical Sciences, Cambridge, UK &lt;br /&gt;
*[http://www.usal.es/~fises/ XV Congreso de Física Estadística (Fises' 08)] 27-29 March 2008, Salamanca, Spain&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/CMMP08/event_26545.html Condensed Matter and Materials Physics (CMMP)]  26-28 March 2008 Royal Holloway, University of London, UK&lt;br /&gt;
*[http://www.icmab.es/softmatter2008/index.html SoftMatter 2008] &amp;quot;Workshop on Electrostatic Effects in Soft Matter: Bringing Experiments, Theory and Simulation Together&amp;quot; 10 – 11 April ICMAB-CSIC, Barcelona, Spain.&lt;br /&gt;
*[http://www.icmab.es/11emscf/index.html 11th European Meeting on Supercritical Fluids] &amp;quot;New Perspectives in Supercritical Fluids: Nanoscience, Materials and Processing&amp;quot; 4-7 May 2008, ICMAB-CSIC, Barcelona, Spain&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/index.html 99th Statistical Mechanics Conference] May 11-13, 2008 Rutgers University,  USA&lt;br /&gt;
*[http://www.fondation-pgg.org/events/degennesdays/ DeGennesDays] 15-17 May 2008 Collège de France, Paris.&lt;br /&gt;
*[http://www.ill.fr/Events/rktsymposium/  Surfaces and Interfaces in Soft Matter and Biology SISMB 2008] &amp;quot;The impact and future of neutron reflectivity - A Symposium in Honor of Robert K. Thomas&amp;quot; 21-23 May 2008, Institut Laue-Langevin (Grenoble, France).&lt;br /&gt;
*[http://www.plmmp.univ.kiev.ua/ Physics of Liquid Matter: Modern Problems] May 23-26, 2008, Kyiv National Taras Shevchenko University, Ukraine&lt;br /&gt;
*[http://www.ffn.ub.es/sitges/ XXI Sitges Conference] XXI Sitges Conference on Statistical Mechanics. Statistical Mechanics of Molecular Biophysics  2nd-6th June 2008, Sitges, Spain&lt;br /&gt;
*[http://www1.ci.uc.pt/gcpi/poly2008 Polyelectrolytes 2008]  16th-19th June 2008, Coimbra, Portugal&lt;br /&gt;
*[http://www-spht.cea.fr/Meetings/BegRohu2008/index.html The Beg Rohu Summer School: Manifolds in random media, random matrices and extreme value statistics] 16th - 28th June 2008, French National Sailing School, Quiberon peninsula, France.&lt;br /&gt;
*[http://www.chm.bris.ac.uk/cms/ Computational Molecular Science 2008] 22nd – 25th June 2008, Cirencester, UK.&lt;br /&gt;
*[http://www.liquids2008.se/ 7th Liquid Matter Conference] 27 June - 1 July 2008  Lund, Sweden&lt;br /&gt;
*[http://www.ccp5.ac.uk/SSCCP5/main.html CCP5 Methods in Molecular Simulation Summer School 2008] University of Sheffield, England July 6 - July 15 2008.&lt;br /&gt;
*Potentials Workshop: Recent developments in interatomic potentials 7-8 July 2008  Oxford, UK&lt;br /&gt;
*[http://www.lcc-toulouse.fr/molmat2008/ MOLMAT2008 International Symposium on Molecular Materials based on Chemistry, Solid State Physics, Theory and Nanotechnology]   July 8-11th  2008 Toulouse, France&lt;br /&gt;
*[http://www2.polito.it/eventi/sigmaphi2008/ SigmaPhi2008] 14th -18th July 2008 Kolympari, Crete, Greece&lt;br /&gt;
*[http://www.cecam.org/workshop-188.html Dissipative Particle Dynamics: Addressing deficiencies and establishing new frontiers] July, 16th-18th 2008  CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.iop.org/Conferences/Forthcoming_Institute_Conferences/event_22243.html Molecular Dynamics for Non-Adiabatic Processes] 21 July 2008 to 22 July 2008 Institute of Physics, London&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcitaa_08/announcement.html Quantum Monte Carlo in the Apuan Alps IV] 26th July - Sat 2nd August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.cecam.org/workshop-215.html New directions in the theory and modelling of liquid crystals] July, 28th 2008 to July, 30th 2008, CECAM-EPFL, Lausanne, Switzerland&lt;br /&gt;
*[http://www.vallico.net/tti/master.html?http://www.vallico.net/tti/qmcatcp_08/announcement.html Quantum Monte Carlo and the CASINO program III] 3rd August - Sun 10th August The Towler Institute, Vallico Sotto, Tuscany, Italy&lt;br /&gt;
*[http://www.icct2008.org/ 20th International Conference on Chemical Thermodynamics] August 3-8, 2008, Warsaw, Poland.&lt;br /&gt;
*[http://perso.ens-lyon.fr/thierry.dauxois/LORIS/LesHouchesSummerSchool2008.html Long-Range Interacting Systems] Summer School in Les Houches (France), 4-29 August 2008&lt;br /&gt;
*[http://ctbp.ucsd.edu/summer_school08/apply2008.html Coarse-Grained Physical Modeling of Biological Systems: Advanced Theory and Methods] August 11-15, 2008 University of California San Diego&lt;br /&gt;
*[http://www.chem.ucl.ac.uk/astrosurf/SIPML.html Surface and Interface Processes at the Molecular Level]  17 - 23 August 2008, Lucca, Italy&lt;br /&gt;
*[http://www.rsc.org/ConferencesAndEvents/RSCConferences/FD141/index.asp  Faraday Discussion 141: Water - From Interfaces to the Bulk] 27 - 29 August 2008 Heriot-Watt University, Edinburgh, United Kingdom&lt;br /&gt;
*[http://ectp18.conforganizer.net   18th European Conference on Thermophysical Properties]  31 Aug-4 Sep 2008 Pau, France&lt;br /&gt;
*[http://iber2008.df.fct.unl.pt/  9th Iberian Joint Meeting on Atomic and Molecular Physics - IBER 2008]  7-9th September,  Capuchos, Portugal&lt;br /&gt;
*[http://www.cmmp.ucl.ac.uk/~dmd/ccp5.htm  CCP5 Annual Meeting: Surfaces and Interfaces] 8-10th September, London, UK&lt;br /&gt;
*[http://ergodic.ugr.es/cp/ 10th  Granada  Seminar on Computational and Statistical Physics: Modeling and Simulation of New Materials] September 15-19, 2008 Granada, Spain&lt;br /&gt;
*[http://www.cecam.org/workshop-222.html Standardisation and databasing of ab-initio and classical simulations] September, 18th 2008 to September, 19th 2008  CECAM-ETHZ, Zurich, Switzerland&lt;br /&gt;
*[http://www.iccmse.org/ International Conference of Computational Methods in Sciences and Engineering 2008 (ICCMSE 2008)]  25-30 September, Crete, Greece&lt;br /&gt;
*[http://www.mmm2008.org/bin/view.pl/Main/WebHome Multscale Materials Modeling] 27–31 October 2008, Tallahassee, Florida USA&lt;br /&gt;
*[http://www.aiche.org/Conferences/AnnualMeeting/index.aspx 2008 AIChE Annual Meeting] November 16-21 2008 Philadelphia, Pennsylvania USA&lt;br /&gt;
*[http://www.ihp.jussieu.fr/ceb/Trimestres/T08-4/C3/index.html Statistical mechanics] Paris (France) 8-12 December 2008&lt;br /&gt;
*[http://complex.ffn.ub.es/bcnetworkshop BCNet Workshop] Trends and perspectives in complex networks. Barcelona (Spain) 10-12 December 2008&lt;br /&gt;
*[http://www.math.rutgers.edu/events/smm/ 100th Statistical Mechanics Conference]  Rutgers University, (USA) 13-18 December 2008&lt;br /&gt;
=====2009=====&lt;br /&gt;
*[http://www.ccpb.ac.uk/events/conference/2009/ Biomolecular Simulation 2009] 6-8 January, Yorkshire Museum and Gardens, York, United Kingdom 2009&lt;br /&gt;
*[http://www.fisica.unam.mx/externos/wintermeeting/ XXXVIII edition of the Winter Meeting on Statistical Physics] Taxco, Guerrero (Mexico) 6th - 9th January, 2009.&lt;br /&gt;
*[http://www.ucl.ac.uk/msl/events/2009/workshop09.htm 2009 MSL Workshop: Accessing large length and time scales with accurate quantum methods]  12th - 13th January 2009 University College London (United Kingdom)&lt;br /&gt;
*[http://euler.us.es/%7Eopap/stochgame/index-en.html Stochastic Models in Physics, Biology, and Social Sciences] Carmona (Sevilla), Spain February 12-14 (2009)&lt;br /&gt;
*[http://hera.physik.uni-konstanz.de/igk/news/workshops/homepage/index.html Frontiers of Soft Condensed Matter 2009]  Les Houches () 15-20 February  2009&lt;br /&gt;
*[http://www.mpipks-dresden.mpg.de/~mbsffe09/ Many-body systems far from equilibrium: Fluctuations, slow dynamics and long-range interactions] Max Planck Institute for the Physics of Complex Systems Dresden, Germany February 16 - 27 (2009)&lt;br /&gt;
*[http://www.formulation.org.uk/Conference_flyers_Sept2007_on/Flyer-sims.pdf Workshop on advances in modelling for formulations]  25th of March 2009 at GSK Waybridge (United Kingdom)&lt;br /&gt;
*[http://www.physik.uni-leipzig.de/~janke/meco34/ 34th Conference of the Middle European Cooperation in Statistical Physics] 30 March - 01 April 2009 Universität Leipzig (Germany)&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws2/ Workshop II: The Boltzmann Equation: DiPerna-Lions Plus 20 Years] April 15-17 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-313.html Computational Studies of Defects in Nanoscale Carbon Materials]  May 11, 2009 to May 13, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.cecam.org/workshop-320.html Modeling of Carbon and Inorganic Nanotubes and Nanostructures]  May 13, 2009 to May 15, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
*[http://www.ima.umn.edu/2008-2009/W5.18-22.09/ Molecular Simulations: Algorithms, Analysis, and Applications] Institute for Mathematics and its Applications, University of Minnesota (USA), May 18-22, 2009&lt;br /&gt;
*[http://www.ipam.ucla.edu/programs/ktws4/ Workshop IV: Asymptotic Methods for Dissipative Particle Systems] May 18-22 (2009) Los Angeles (USA)&lt;br /&gt;
*[http://www.cecam.org/workshop-310.html Computer Simulation in Food Science: CFD meets Soft Matter]  May 25, 2009 to May 27, 2009 CECAM-HQ-EPFL, Lausanne, (Switzerland) &lt;br /&gt;
*[http://complenet09.diit.unict.it  CompleNet 2009] International Workshop on Complex Networks. Catania (Italy),  May 26-28, 2009&lt;br /&gt;
*[http://go.warwick.ac.uk/maths/research/events/2008_2009/symposium/wks5/ EPSRC Symposium Workshop on Molecular Dynamics] Monday 1 – Friday 5 June (2009) Warwick (United Kingdom)&lt;br /&gt;
*[http://www.cecam.org/workshop-272.html Theoretical Modeling of Transport in Nanostructures]  June 2, 2009 to June 5, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland) &lt;br /&gt;
*[http://www.mpip-mainz.mpg.de/mmsd/ Mainz Materials Simulation Days] 3-5 June 2009 Max Planck Institute for Polymer Research (Germany)&lt;br /&gt;
*[http://www.soms.ethz.ch/workshop2009 Coping with Crises in Complex Socio-Economic Systems] ETH Zurich (Switzerland), June 8-13, 2009&lt;br /&gt;
*[[MOSSNOHO Workshop 2009]] 16 of June 2009, Universidad Complutense de Madrid (Spain)&lt;br /&gt;
*[http://cftc.cii.fc.ul.pt/Workshops/flowNjam/index.html Flow(ers) and jam(mers): from liquid crystals to grains] Lisbon (Portugal) 17-19 June 2009&lt;br /&gt;
*[http://ipht.cea.fr/Meetings/BegRohu2009/ Beg Rohu Summer School: Quantum Physics Out of Equilibrium] Ecole Nationale de Voile (France) 15-27 June 2009&lt;br /&gt;
*[http://symp17.boulder.nist.gov  Seventeenth Symposium on Thermophysical Properties] Boulder, Colorado (USA), June 21-26, 2009&lt;br /&gt;
*[http://www.fhi-berlin.mpg.de/th/Meetings/DFT-workshop-Berlin2009/ Hands-on Tutorial on Ab Initio Molecular Simulations: Toward a First-Principles Understanding of Materials Properties and Functions] Berlin (Germany) June 22-July 1 2009&lt;br /&gt;
*[https://www.irphe.univ-mrs.fr/~fe09 Fluid and Elasticity] Carry-le-Rouet, near Marseilles (France) June 23-26, 2009&lt;br /&gt;
*[http://www.icmp.lviv.ua/statphys2009/ Statistical Physics: Modern Trends and Applications] June 23-25, 2009 Lviv, (Ukraine)&lt;br /&gt;
*[http://www.fuw.edu.pl/~wssph/ 3rd Warsaw School of Statistical Physics] Kazimierz Dolny (Poland), 27 June - 4 July, 2009&lt;br /&gt;
*[http://www.cecam.org/workshop-298.html Modeling and Simulation of Water at Interfaces from Ambient to Supercooled Conditions] June 29, 2009 to July 1, 2009 CECAM-HQ-EPFL, Lausanne (Switzerland)&lt;br /&gt;
&lt;br /&gt;
__NOTOC__&lt;br /&gt;
[[category: Miscellaneous]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/MOSSNOHO_Workshop_2009</id>
		<title>MOSSNOHO Workshop 2009</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/MOSSNOHO_Workshop_2009"/>
				<updated>2009-06-12T11:14:45Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Enlace a Capillary_waves&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:log_mossnoho1.gif|300px|frameless|right]]&lt;br /&gt;
La reunión del  Programa de Investigación [http://www.icmm.csic.es/mossnoho/ MOSSNOHO/MODELICO] 2009 se celebrará el día 16 de junio en la [http://www.ucm.es/info/ccquim/ Facultad de Ciencias Químicas] de la  [http://www.ucm.es/ Universidad Complutense de Madrid].&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Aquí esta el programa '''preliminar'''. Las charlas son de 20 minutos más 10 minutos para preguntas.&lt;br /&gt;
==Horario de las charlas==&lt;br /&gt;
{| style=&amp;quot;width:90%; height:85px&amp;quot; border=&amp;quot;3&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
|Horario || Ponente || Titulo de  la charla || Institución || Departamento/Grupo de investigación&lt;br /&gt;
|-&lt;br /&gt;
| 10:00-10:30 || [http://cab.inta.es/03_01_01_curriculum.php?lab_id=&amp;amp;laboratorio=&amp;amp;per_id=30&amp;amp;idioma=ESP Susanna  C. Manrubia] || ''Evolución y adaptación de poblaciones moleculares y virales de RNA'' || [http://cab.inta.es/ Centro de Astrobiología] || Grupo de Sistemas Evolutivos&lt;br /&gt;
|- &lt;br /&gt;
| 10:30-11:00 || José Maria Guil || ''Microcalorimetria de adsorción'' ||  [http://www.iqfr.csic.es/ CSIC Instituto de Química-Física &amp;quot;Rocasolano&amp;quot;]  || [http://www.iqfr.csic.es/electroquimica/Departamento.htm  Química-Física de Interfases y Electroquímica]&lt;br /&gt;
|-[http://cacharro.quim.ucm.es/&lt;br /&gt;
| 11:00-11:30 || [http://www.icmm.csic.es/Teoria/basjav.htm José Antonio Verges] || ''Estadísticas cuánticas del transporte electrónico a través de sistemas desordenados'' || [http://www.icmm.csic.es/ CSIC Instituto de Ciencia de Materiales de Madrid] || [http://www.icmm.csic.es/Teoria/ Condensed Matter Theory]&lt;br /&gt;
|-&lt;br /&gt;
| 11:30-12:00 || '''Café''' || || || &lt;br /&gt;
|-&lt;br /&gt;
| 12:00-12:30 || [http://cacharro.quim.ucm.es/ José Luis F. Abascal] ||''Propiedades anómalas del agua: región líquida y subenfriada'' || [http://www.ucm.es/ Universidad Complutense de Madrid] || [http://www.ucm.es/info/quifi/ Departamento de Química Física I]&lt;br /&gt;
|-&lt;br /&gt;
| 12:30-13:00 || [http://www.dmae.upm.es/bartolo.html Bartolo Luque] || ''Visibilidad: una nueva herramienta de análisis de series temporales'' || [http://www2.upm.es/institucional Universidad Politécnica de Madrid] || [http://www.dmae.upm.es/ Departamento Matemática Aplicada y Estadística]&lt;br /&gt;
|-&lt;br /&gt;
| 13:00-13:30 || Alfonso Paez || ''Polímeros vivos de FtsZ en el proceso de división celular'' ||   [http://www.uam.es/ Universidad Autónoma de Madrid] || [http://www.uam.es/departamentos/ciencias/fisicateoricamateria/propia/fluidos.html Investigación en física estadística de líquidos complejos y biofísica]&lt;br /&gt;
|-&lt;br /&gt;
| 13:30-14:30 || '''Comida''' || || ||&lt;br /&gt;
|-&lt;br /&gt;
| 14:30-15:00 || [http://www.qft.iqfr.csic.es/personal/alberto/ Alberto Gallardo] || ''Modelado y simulación de adsorción en arcillas con pilares'' || [http://www.iqfr.csic.es/ CSIC Instituto de Química-Física &amp;quot;Rocasolano&amp;quot; ]  || [http://www.qft.iqfr.csic.es/ Grupo de Química Física Teórica]&lt;br /&gt;
|-  &lt;br /&gt;
| 15:00-15:30 || [http://oboe.quim.ucm.es/jfg.html Juan Freire] || ''Investigación de la compatibilidad de mezclas de polímeros y del comportamiento molecular de dendrímeros por simulación numérica''  || [http://www.uned.es/ Universidad Nacional de Educación a Distancia (UNED)] || [http://www.uned.es/dpto-fisicoquimica/index.htm Departamento de Ciencias y Técnicas Fisicoquímicas]&lt;br /&gt;
|- &lt;br /&gt;
| 15:30-16:00 || [http://emoles.quim.ucm.es/carlos.html Carlos Vega] || ''La importancia de los efectos cuánticos en el agua'' ||  [http://www.ucm.es/ Universidad Complutense de Madrid] || [http://emoles.quim.ucm.es/ Termodinámica Estadística de Fluidos Moleculares]&lt;br /&gt;
|-&lt;br /&gt;
| 16:00-16:30 || '''Café''' || || || &lt;br /&gt;
|-&lt;br /&gt;
| 16:30-17:00 || [http://www.uam.es/personal_pdi/ciencias/rdelgado/ Rafael Delagado Buscalioni]  || ''Estructura e hidrodinámica de [[Capillary_waves| ondas capilares]] nanoscópicas'' ||  [http://www.uam.es/ Universidad Autónoma de Madrid] || [http://www.uam.es/departamentos/ciencias/fisicateoricamateria/propia/ Departamento de Física Teórica de la Materia Condensada]&lt;br /&gt;
|-&lt;br /&gt;
| 17:00-17:30 || [http://www.uc3m.es/portal/page/portal/dpto_matematicas/profesorado/Jos%E9%20%C1ngel%20Capit%E1n José A. Capitán] || ''Cuasiecosistemas y la catástrofe de extinción'' || [http://www.uc3m.es/portal/page/portal/inicio Universidad Carlos III de Madrid] || [http://gisc.uc3m.es Grupo Interdisciplinar de Sistemas Complejos]&lt;br /&gt;
|-&lt;br /&gt;
| 17:30-18:00 || [http://www.iem.csic.es/fmacro/fismacr_doc/fismacr_bio/tiberio.htm Tiberio Ezquerra] || ''Estructura y Dinámica de la Materia Condesada Blanda y Polimérica: Actividad del grupo SOFMAT'' || [http://www.iem.csic.es/ CSIC  Instituto de Estructura de la Materia] || [http://www.iem.cfmac.csic.es/fmacro/softmatpol/ Soft and Polymeric Condensed Matter Group]&lt;br /&gt;
|-&lt;br /&gt;
| 18:00-18:30 || [http://www.complex.etsit.urjc.es/jmbuldu/ Javier Martín Buldú] || ''Competición de dominios de sincronización en redes complejas y detección dinámica de interfaces'' || [http://www.urjc.es/ Universidad Rey Juan Carlos]  || [http://www.complex.etsit.urjc.es/ Complex Systems Group]&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
==Como llegar==&lt;br /&gt;
La [http://www.ucm.es/info/ccquim/ Facultad de Ciencias Químicas]  se encuentra situada en el Campus de Moncloa de la UCM. [http://www.ucm.es/info/ccquim/pags.php?p=5 Mapa].&lt;br /&gt;
El workshop tendrá lugar en el salón de actos situado en el sotano del la biblioteca:&lt;br /&gt;
[[Image:UCM_salon_biblio.png|400px|frameless|center]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Image:logo_sumaeducmadrid-org.jpg|300px|frameless|center]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/First_law_of_thermodynamics</id>
		<title>First law of thermodynamics</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/First_law_of_thermodynamics"/>
				<updated>2009-06-08T09:09:26Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Q, W both &amp;quot;upon&amp;quot; the system&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The '''first law of thermodynamics''' is a statement of the conservation of energy for thermal processes:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left.dU\right.=\delta Q+ \delta W&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Where ''U'' is the [[internal energy]] of the system, i.e.&lt;br /&gt;
ignoring the external energy of the system, for example&lt;br /&gt;
motion of the center of mass of the system, or the presence &lt;br /&gt;
of an external field. ''Q'' is the net [[heat]] entering the&lt;br /&gt;
system and ''W'' is the [[work]] done upon the system.&lt;br /&gt;
&lt;br /&gt;
For reversible changes&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left.dW\right.=-p~dV  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and for irreversible changes&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left.dW\right. &amp;gt; -p~dV &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;p&amp;lt;/math&amp;gt; is the [[pressure]] and &amp;lt;math&amp;gt;V&amp;lt;/math&amp;gt; is the volume.&lt;br /&gt;
&lt;br /&gt;
For an adiabatic system (i.e. a system in which no heat enters or leaves)&lt;br /&gt;
then if two bodies of different [[temperature |temperatures]] are placed in contact&lt;br /&gt;
and then separated then the sum of the heat within the system is unchanged (see&lt;br /&gt;
[[adiabatic process]].&lt;br /&gt;
This is conservation of energy. The first law of thermodynamics does not&lt;br /&gt;
provide information on the direction of the heat transfer (if any).&lt;br /&gt;
In other words, the common experience that the hotter object gives&lt;br /&gt;
heat to the colder object, the direction of heat flow from hot to cold,&lt;br /&gt;
is left to the [[second law of thermodynamics]].&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1098/rstl.1850.0004 James Prescott Joule &amp;quot;On the Mechanical Equivalent of Heat&amp;quot;, Philosophical Transactions of the Royal Society of London '''140''' pp. 61-82 (1850)]&lt;br /&gt;
[[Category: Classical thermodynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Work</id>
		<title>Work</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Work"/>
				<updated>2009-06-08T09:07:19Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: W=-pdV on compression or expansion, but always ''upon'' (I am 98% sure)&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The mechanical '''work''', ''W'', performed ''upon'' a gas is given by&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;W = - \int_\alpha^\beta p ~dV&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\alpha&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\beta&amp;lt;/math&amp;gt; are points in state space, ''p'' is the [[pressure]]&lt;br /&gt;
and ''V'' is the volume. The mechanical work done ''by'' the gas has the opposite sign (a common&lt;br /&gt;
source of mistakes).&lt;br /&gt;
&lt;br /&gt;
For reversible changes,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left.dW\right.=-p~dV  &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and for irreversible changes&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left.dW\right. &amp;gt; -p~dV &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[category: classical thermodynamics]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Argon</id>
		<title>Argon</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Argon"/>
				<updated>2009-05-22T10:46:50Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Fixed wrong T_t&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:Lennard-Jones.png|thumb| The Lennard-Jones model for argon.]]&lt;br /&gt;
'''Argon''' (Ar) has a mass of 39.948 [[atomic mass units | umas]]. Sadus and Prausnitz have shown that three-body repulsion makes a significant contribution to [[Idealised models#Three-body potentials|three-body interactions]] in the liquid phase&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.471172 Richard J. Sadus and J. M. Prausnitz &amp;quot;Three-body interactions in fluids from molecular simulation: Vapor–liquid phase coexistence of argon&amp;quot;, Journal of Chemical Physics '''104''' pp. 4784-4787 (1996)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
(for use of the [[Axilrod-Teller interaction]] see &lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevA.45.3659 Phil Attard &amp;quot;Pair-hypernetted-chain closure for three-body potentials: Results for argon with the Axilrod-Teller triple-dipole potential&amp;quot;, Physical Review A '''45''' pp. 3659-3669 (1992)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevE.55.2707     J. A. Anta, E. Lomba and M. Lombardero &amp;quot;Influence of three-body forces on the gas-liquid coexistence of simple fluids: The phase equilibrium of argon&amp;quot;, Physical Review E '''55''' pp. 2707-2712 (1997)]&amp;lt;/ref&amp;gt;). &lt;br /&gt;
However, the generic [[Lennard-Jones model]] has been frequently used due to its simplicity; some parameters are quoted in the next section. A specific interatomic potential for Ar has been proposed by Aziz &lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.466051  Ronald A. Aziz &amp;quot;A highly accurate interatomic potential for argon&amp;quot;, Journal of Chemical Physics '''99''' p. 4518 (1993)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property  &amp;lt;ref&amp;gt;[http://www.webelements.com/argon/physics.html Argon physical properties en webelements]  &amp;lt;/ref&amp;gt; || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 83.8058 K  || 69 kPa&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || 150.87 K || 4.898 MPa&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 83.80 K ||&lt;br /&gt;
|-&lt;br /&gt;
| Boiling point ||87.30 K ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Lennard-Jones parameters==&lt;br /&gt;
The [[Lennard-Jones model |Lennard-Jones]] parameters for liquid argon are listed in the following table:&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Authors || &amp;lt;math&amp;gt;\epsilon/k_B&amp;lt;/math&amp;gt; (K) || &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt;  (nm)|| Reference&lt;br /&gt;
|- &lt;br /&gt;
| Rowley, Nicholson and Parsonage || 119.8   || 0.3405  || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0021-9991(75)90042-X   L. A. Rowley, D. Nicholson and N. G. Parsonage &amp;quot;Monte Carlo grand canonical ensemble calculation in a gas-liquid transition region for 12-6 Argon&amp;quot;, Journal of Computational Physics  '''17''' pp. 401-414 (1975)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|- &lt;br /&gt;
|Barker, Fisher and Watts  ||142.095   ||  0.33605  || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1080/00268977100101821 J. A. Barker,  R. A. Fisher and R. O. Watts &amp;quot;Liquid argon: Monte carlo and molecular dynamics calculations&amp;quot;, Molecular Physics '''21''' pp. 657-673 (1971)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|- &lt;br /&gt;
| White   || 125.7   ||  0.3345    || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.479848 John A. White &amp;quot;Lennard-Jones as a model for argon and test of extended renormalization group calculations&amp;quot;, Journal of Chemical Physics '''111''' pp. 9352-9356 (1999)]&amp;lt;/ref&amp;gt; parameter set #4&lt;br /&gt;
|}&lt;br /&gt;
==Radial distribution function==&lt;br /&gt;
[[Radial distribution function]]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevA.7.2130 J. L. Yarnell, M. J. Katz, R. G. Wenzel and S. H. Koenig &amp;quot;Structure Factor and Radial Distribution Function for Liquid Argon at 85°K&amp;quot;, Physical Review A '''7''' pp. 2130-2144 (1973)]&lt;br /&gt;
==Quantum simulations==&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268978900100811 J. R. Melrose and K. Singer &amp;quot;An investigation of supercooled Lennard-Jones argon by quantum mechanical and classical Monte Carlo simulation&amp;quot;, Molecular Physics '''66''' 1203-1214 (1989)]&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
'''Related material'''&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268976400100611 H. C. Longuet-Higgins and  B. Widom &amp;quot;A rigid sphere model for the melting of argon&amp;quot;, Molecular Physics '''8''' pp. 549-556 (1964)]&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268976800100721 D. Henderson and J. A. Barker &amp;quot;On the solidification of argon&amp;quot;, Molecular Physics '''14''' pp. 587-589 (1968)]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevA.5.2238  F. Lado &amp;quot;Numerical Calculation of the Density Autocorrelation Function for Liquid Argon&amp;quot;, Physical Review A '''5''' pp. 2238-2244 (1972)]&lt;br /&gt;
&lt;br /&gt;
[[category: models]]&lt;br /&gt;
{{Numeric}}&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Physical_properties_of_water</id>
		<title>Physical properties of water</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Physical_properties_of_water"/>
				<updated>2009-05-22T10:43:24Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Some water properties&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{stub-general}}&lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property &amp;lt;ref&amp;gt;[http://en.wikipedia.org/wiki/Water_(data_page) Water data on wikipedia]  &amp;lt;/ref&amp;gt;  || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 273.16 K || 0.6117 kPa&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || 647 K || 22.1 MPa&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 273.15 K  || &lt;br /&gt;
|-&lt;br /&gt;
| Boiling point || 373.124 K ||&lt;br /&gt;
|}&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[category: water]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Argon</id>
		<title>Argon</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Argon"/>
				<updated>2009-05-22T10:38:43Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added link to webelements&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:Lennard-Jones.png|thumb| The Lennard-Jones model for argon.]]&lt;br /&gt;
'''Argon''' (Ar) has a mass of 39.948 [[atomic mass units | umas]]. Sadus and Prausnitz have shown that three-body repulsion makes a significant contribution to [[Idealised models#Three-body potentials|three-body interactions]] in the liquid phase&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.471172 Richard J. Sadus and J. M. Prausnitz &amp;quot;Three-body interactions in fluids from molecular simulation: Vapor–liquid phase coexistence of argon&amp;quot;, Journal of Chemical Physics '''104''' pp. 4784-4787 (1996)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
(for use of the [[Axilrod-Teller interaction]] see &lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevA.45.3659 Phil Attard &amp;quot;Pair-hypernetted-chain closure for three-body potentials: Results for argon with the Axilrod-Teller triple-dipole potential&amp;quot;, Physical Review A '''45''' pp. 3659-3669 (1992)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevE.55.2707     J. A. Anta, E. Lomba and M. Lombardero &amp;quot;Influence of three-body forces on the gas-liquid coexistence of simple fluids: The phase equilibrium of argon&amp;quot;, Physical Review E '''55''' pp. 2707-2712 (1997)]&amp;lt;/ref&amp;gt;). &lt;br /&gt;
However, the generic [[Lennard-Jones model]] has been frequently used due to its simplicity; some parameters are quoted in the next section. A specific interatomic potential for Ar has been proposed by Aziz &lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.466051  Ronald A. Aziz &amp;quot;A highly accurate interatomic potential for argon&amp;quot;, Journal of Chemical Physics '''99''' p. 4518 (1993)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property  &amp;lt;ref&amp;gt;[http://www.webelements.com/argon/physics.html Argon physical properties en webelements]  &amp;lt;/ref&amp;gt; || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 83.8058 K  || 69 kPa&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || 50.87 K || 4.898 MPa&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 83.80 K ||&lt;br /&gt;
|-&lt;br /&gt;
| Boiling point ||87.30 K ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Lennard-Jones parameters==&lt;br /&gt;
The [[Lennard-Jones model |Lennard-Jones]] parameters for liquid argon are listed in the following table:&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Authors || &amp;lt;math&amp;gt;\epsilon/k_B&amp;lt;/math&amp;gt; (K) || &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt;  (nm)|| Reference&lt;br /&gt;
|- &lt;br /&gt;
| Rowley, Nicholson and Parsonage || 119.8   || 0.3405  || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0021-9991(75)90042-X   L. A. Rowley, D. Nicholson and N. G. Parsonage &amp;quot;Monte Carlo grand canonical ensemble calculation in a gas-liquid transition region for 12-6 Argon&amp;quot;, Journal of Computational Physics  '''17''' pp. 401-414 (1975)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|- &lt;br /&gt;
|Barker, Fisher and Watts  ||142.095   ||  0.33605  || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1080/00268977100101821 J. A. Barker,  R. A. Fisher and R. O. Watts &amp;quot;Liquid argon: Monte carlo and molecular dynamics calculations&amp;quot;, Molecular Physics '''21''' pp. 657-673 (1971)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|- &lt;br /&gt;
| White   || 125.7   ||  0.3345    || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.479848 John A. White &amp;quot;Lennard-Jones as a model for argon and test of extended renormalization group calculations&amp;quot;, Journal of Chemical Physics '''111''' pp. 9352-9356 (1999)]&amp;lt;/ref&amp;gt; parameter set #4&lt;br /&gt;
|}&lt;br /&gt;
==Radial distribution function==&lt;br /&gt;
[[Radial distribution function]]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevA.7.2130 J. L. Yarnell, M. J. Katz, R. G. Wenzel and S. H. Koenig &amp;quot;Structure Factor and Radial Distribution Function for Liquid Argon at 85°K&amp;quot;, Physical Review A '''7''' pp. 2130-2144 (1973)]&lt;br /&gt;
==Quantum simulations==&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268978900100811 J. R. Melrose and K. Singer &amp;quot;An investigation of supercooled Lennard-Jones argon by quantum mechanical and classical Monte Carlo simulation&amp;quot;, Molecular Physics '''66''' 1203-1214 (1989)]&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
'''Related material'''&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268976400100611 H. C. Longuet-Higgins and  B. Widom &amp;quot;A rigid sphere model for the melting of argon&amp;quot;, Molecular Physics '''8''' pp. 549-556 (1964)]&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268976800100721 D. Henderson and J. A. Barker &amp;quot;On the solidification of argon&amp;quot;, Molecular Physics '''14''' pp. 587-589 (1968)]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevA.5.2238  F. Lado &amp;quot;Numerical Calculation of the Density Autocorrelation Function for Liquid Argon&amp;quot;, Physical Review A '''5''' pp. 2238-2244 (1972)]&lt;br /&gt;
&lt;br /&gt;
[[category: models]]&lt;br /&gt;
{{Numeric}}&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Potassium</id>
		<title>Potassium</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Potassium"/>
				<updated>2009-05-22T10:37:45Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Added link to webelements&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Potassium''' (K) is a [[liquid metal]] with a mass of 39.0983 [[atomic mass units | umas]]. &lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property &amp;lt;ref&amp;gt;[http://www.webelements.com/potassium/physics.html Potassium physical properties en webelements]  &amp;lt;/ref&amp;gt;  || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 336.53 K  || ??&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || 2223 K || ??&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 336.53 K  ||&lt;br /&gt;
|-&lt;br /&gt;
| Boiling point || 1032 K ||&lt;br /&gt;
|}&lt;br /&gt;
[[category: models]]&lt;br /&gt;
{{Numeric}}&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Potassium</id>
		<title>Potassium</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Potassium"/>
				<updated>2009-05-22T10:33:56Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: T_t fixed&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Potassium''' (K) is a [[liquid metal]] with a mass of 39.0983 [[atomic mass units | umas]]. &lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 336.53 K  || ??&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || 2223 K || ??&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 336.53 K  ||&lt;br /&gt;
|-&lt;br /&gt;
| Boiling point || 1032 K ||&lt;br /&gt;
|}&lt;br /&gt;
[[category: models]]&lt;br /&gt;
{{Numeric}}&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Potassium</id>
		<title>Potassium</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Potassium"/>
				<updated>2009-05-22T10:32:44Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: T_c added&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Potassium''' (K) is a [[liquid metal]] with a mass of 39.0983 [[atomic mass units | umas]]. &lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 336.35 K  || ??&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || 2223 K || ??&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 336.53 K  ||&lt;br /&gt;
|-&lt;br /&gt;
| Boiling point || 1032 K ||&lt;br /&gt;
|}&lt;br /&gt;
[[category: models]]&lt;br /&gt;
{{Numeric}}&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Potassium</id>
		<title>Potassium</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Potassium"/>
				<updated>2009-05-22T10:31:10Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: New potassium entry, with some physical properties (as done with Ar)&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Potassium''' (K) is a [[liquid metal]] with a mass of 39.0983 [[atomic mass units | umas]]. &lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 336.35 K  || ??&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || ?? || ??&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 336.53 K  ||&lt;br /&gt;
|-&lt;br /&gt;
| Boiling point || 1032 K ||&lt;br /&gt;
|}&lt;br /&gt;
[[category: models]]&lt;br /&gt;
{{Numeric}}&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Argon</id>
		<title>Argon</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Argon"/>
				<updated>2009-05-22T10:23:43Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:Lennard-Jones.png|thumb| The Lennard-Jones model for argon.]]&lt;br /&gt;
'''Argon''' (Ar) has a mass of 39.948 [[atomic mass units | umas]]. Sadus and Prausnitz have shown that three-body repulsion makes a significant contribution to [[Idealised models#Three-body potentials|three-body interactions]] in the liquid phase&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.471172 Richard J. Sadus and J. M. Prausnitz &amp;quot;Three-body interactions in fluids from molecular simulation: Vapor–liquid phase coexistence of argon&amp;quot;, Journal of Chemical Physics '''104''' pp. 4784-4787 (1996)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
(for use of the [[Axilrod-Teller interaction]] see &lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevA.45.3659 Phil Attard &amp;quot;Pair-hypernetted-chain closure for three-body potentials: Results for argon with the Axilrod-Teller triple-dipole potential&amp;quot;, Physical Review A '''45''' pp. 3659-3669 (1992)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevE.55.2707     J. A. Anta, E. Lomba and M. Lombardero &amp;quot;Influence of three-body forces on the gas-liquid coexistence of simple fluids: The phase equilibrium of argon&amp;quot;, Physical Review E '''55''' pp. 2707-2712 (1997)]&amp;lt;/ref&amp;gt;). &lt;br /&gt;
However, the generic [[Lennard-Jones model]] has been frequently used due to its simplicity; some parameters are quoted in the next section. A specific interatomic potential for Ar has been proposed by Aziz &lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.466051  Ronald A. Aziz &amp;quot;A highly accurate interatomic potential for argon&amp;quot;, Journal of Chemical Physics '''99''' p. 4518 (1993)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Thermophysical properties  ==&lt;br /&gt;
&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Property || Temperature || Pressure&lt;br /&gt;
|-&lt;br /&gt;
| Triple point || 83.8058 K  || 69 kPa&lt;br /&gt;
|-&lt;br /&gt;
| Critical point || 50.87 K || 4.898 MPa&lt;br /&gt;
|-&lt;br /&gt;
| Melting point || 83.80 K ||&lt;br /&gt;
|-&lt;br /&gt;
| Boiling point ||87.30 K ||&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Lennard-Jones parameters==&lt;br /&gt;
The [[Lennard-Jones model |Lennard-Jones]] parameters for liquid argon are listed in the following table:&lt;br /&gt;
{| border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| Authors || &amp;lt;math&amp;gt;\epsilon/k_B&amp;lt;/math&amp;gt; (K) || &amp;lt;math&amp;gt;\sigma&amp;lt;/math&amp;gt;  (nm)|| Reference&lt;br /&gt;
|- &lt;br /&gt;
| Rowley, Nicholson and Parsonage || 119.8   || 0.3405  || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1016/0021-9991(75)90042-X   L. A. Rowley, D. Nicholson and N. G. Parsonage &amp;quot;Monte Carlo grand canonical ensemble calculation in a gas-liquid transition region for 12-6 Argon&amp;quot;, Journal of Computational Physics  '''17''' pp. 401-414 (1975)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|- &lt;br /&gt;
|Barker, Fisher and Watts  ||142.095   ||  0.33605  || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1080/00268977100101821 J. A. Barker,  R. A. Fisher and R. O. Watts &amp;quot;Liquid argon: Monte carlo and molecular dynamics calculations&amp;quot;, Molecular Physics '''21''' pp. 657-673 (1971)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
|- &lt;br /&gt;
| White   || 125.7   ||  0.3345    || &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.479848 John A. White &amp;quot;Lennard-Jones as a model for argon and test of extended renormalization group calculations&amp;quot;, Journal of Chemical Physics '''111''' pp. 9352-9356 (1999)]&amp;lt;/ref&amp;gt; parameter set #4&lt;br /&gt;
|}&lt;br /&gt;
==Radial distribution function==&lt;br /&gt;
[[Radial distribution function]]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevA.7.2130 J. L. Yarnell, M. J. Katz, R. G. Wenzel and S. H. Koenig &amp;quot;Structure Factor and Radial Distribution Function for Liquid Argon at 85°K&amp;quot;, Physical Review A '''7''' pp. 2130-2144 (1973)]&lt;br /&gt;
==Quantum simulations==&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268978900100811 J. R. Melrose and K. Singer &amp;quot;An investigation of supercooled Lennard-Jones argon by quantum mechanical and classical Monte Carlo simulation&amp;quot;, Molecular Physics '''66''' 1203-1214 (1989)]&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
'''Related material'''&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268976400100611 H. C. Longuet-Higgins and  B. Widom &amp;quot;A rigid sphere model for the melting of argon&amp;quot;, Molecular Physics '''8''' pp. 549-556 (1964)]&lt;br /&gt;
*[http://dx.doi.org/10.1080/00268976800100721 D. Henderson and J. A. Barker &amp;quot;On the solidification of argon&amp;quot;, Molecular Physics '''14''' pp. 587-589 (1968)]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevA.5.2238  F. Lado &amp;quot;Numerical Calculation of the Density Autocorrelation Function for Liquid Argon&amp;quot;, Physical Review A '''5''' pp. 2238-2244 (1972)]&lt;br /&gt;
&lt;br /&gt;
[[category: models]]&lt;br /&gt;
{{Numeric}}&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

	<entry>
		<id>http://ww.sklogwiki.org/SklogWiki/index.php/Voronoi_particles</id>
		<title>Voronoi particles</title>
		<link rel="alternate" type="text/html" href="http://ww.sklogwiki.org/SklogWiki/index.php/Voronoi_particles"/>
				<updated>2009-05-19T16:30:02Z</updated>
		
		<summary type="html">&lt;p&gt;Dduque: Change from P.E.'s group to M.S. et al&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Stub-general}}&lt;br /&gt;
In a series of articles Mar Serrano et al. have proposed a fluid particle model based on the [[ Voronoi cells | Voronoi tessellation ]]. This &amp;quot;fluid particle model&amp;quot; is similar to [[Smooth Particle methods | SPH]], but the choice of volume for a particle is given naturally by the volume of its Voronoi cell.&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1103/PhysRevE.64.046115 Mar Serrano and Pep Español &amp;quot;Thermodynamically consistent mesoscopic fluid particle model&amp;quot;, Physical Review E '''64''' p. 046115 (2001)]&lt;br /&gt;
#[http://dx.doi.org/10.1088/0305-4470/35/7/310  Mar Serrano, Gianni De Fabritiis2, Pep Español, Eirik G Flekkøy, and Peter V Coveney &amp;quot;Mesoscopic dynamics of Voronoi fluid particles&amp;quot;,  Journal of Physics A '''35''' pp. 1605-1625  (2001)]&lt;br /&gt;
#[http://dx.doi.org/10.1007/s10955-005-8414-y Mar Serrano, Pep Español, and Ignacio Zúñiga &amp;quot;Voronoi Fluid Particle Model for Euler Equations&amp;quot;, Journal of Statistical Physics '''121''' pp.  133-147 (2005)]&lt;br /&gt;
[[Category: Computer simulation techniques]]&lt;/div&gt;</summary>
		<author><name>Dduque</name></author>	</entry>

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