Order parameters: Difference between revisions
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:<math> S_2 = \langle \frac{ | An '''order parameter''' is some observable physical quantity that is able to distinguish between | ||
two distinct phases. The choice of order parameter is not necessarily unique. | |||
==Solid-liquid transition== | |||
Possible choices: | |||
*Fourier transform of the density | |||
*Shear modulus | |||
==Isotropic-nematic transition== | |||
The '''uniaxial order parameter''' is zero for an isotropic fluid and one for a perfectly aligned system. First one calculates a director vector <ref>[http://dx.doi.org/10.1080/00268978400101951 R. Eppenga and D. Frenkel "Monte Carlo study of the isotropic and nematic phases of infinitely thin hard platelets", Molecular Physics '''52''' pp. 1303-1334 (1984)]</ref> | |||
:<math>Q_{\alpha \beta} | |||
= \frac{1}{N} | |||
\sum_{j=1}^{N} \left( \frac{3}{2} | |||
\hat e_{j \alpha} \hat e_{j \beta} | |||
-\frac{1}{2} \delta_{\alpha\beta}\right),~~~~~\alpha, \beta = x, y, z,</math> | |||
where <math>Q</math> is a second rank tensor, <math>\hat e_{j}</math> is a unit | |||
vector along the molecular long | |||
axis, | |||
and <math>\delta_{\alpha\beta}</math> is the [[Kronecker delta]]. | |||
Diagonalisation of this tensor | |||
gives three eigenvalues <math>\lambda_+</math>, <math>\lambda_0</math> and <math>\lambda_-</math>, | |||
and <math>n</math> is the eigenvector associated | |||
with the largest eigenvalue (<math>\lambda_+</math>). | |||
From this director vector the nematic order | |||
parameter is calculated from <ref>[http://dx.doi.org/10.1002/mats.1992.040010402 Anna A. Mercurieva, Tatyana M. Birshtein "Liquid-crystalline ordering in two-dimensional systems with discrete symmetry", Die Makromolekulare Chemie, Theory and Simulations '''1''' pp. 205-214 (1992)]</ref> | |||
:<math>S_2 =\frac{d \langle \cos^2 \theta \rangle -1}{d-1}</math> | |||
where ''d'' is the dimensionality of the system. | |||
i.e. in three dimensions <ref>[http://dx.doi.org/10.1016/0167-7322(95)00918-3 Mark R. Wilson "Determination of order parameters in realistic atom-based models of liquid crystal systems", Journal of Molecular Liquids '''68''' pp. 23-31 (1996)]</ref> | |||
:<math>S_2 = \lambda _{+}= \langle P_2( n \cdot e)\rangle = \langle P_2(\cos\theta )\rangle =\langle \frac{3}{2} \cos^{2} \theta - \frac{1}{2} \rangle | |||
</math> | |||
where <math>S_2</math> is known as the uniaxial order parameter. | |||
Here <math>P_2</math> is the second order | |||
[[Legendre polynomials | Legendre polynomial]], | |||
<math>\theta</math> is the angle between a molecular axes and | |||
the director <math>n</math>, and the angle brackets | |||
indicate an ensemble average. | |||
==Tetrahedral order parameter== | |||
<ref>[http://dx.doi.org/10.1080/002689798169195 P. -L. Chau and A. J. Hardwick "A new order parameter for tetrahedral configurations", Molecular Physics '''93''' pp. 511-518 (1998)]</ref> | |||
==See also== | |||
*[[Landau theory of second-order phase transitions]] | |||
==References== | |||
<references/> | |||
;Related reading | |||
*[http://dx.doi.org/10.1103/PhysRevA.10.1881 Joseph P. Straley "Ordered phases of a liquid of biaxial particles", Physical Review A '''10''' pp. 1881 - 1887 (1974)] | |||
*[http://dx.doi.org/10.1063/1.479982 Denis Merlet, James W. Emsley, Philippe Lesot and Jacques Courtieu "The relationship between molecular symmetry and second-rank orientational order parameters for molecules in chiral liquid crystalline solvents", Journal of Chemical Physics '''111''' pp. 6890-6896 (1999)] | |||
*[http://dx.doi.org/10.1063/1.3548889 Erik E. Santiso and Bernhardt L. Trout "A general set of order parameters for molecular crystals", Journal of Chemical Physics '''134''' 064109 (2011)] | |||
[[category: liquid crystals]] |
Latest revision as of 11:47, 15 February 2011
An order parameter is some observable physical quantity that is able to distinguish between two distinct phases. The choice of order parameter is not necessarily unique.
Solid-liquid transition[edit]
Possible choices:
- Fourier transform of the density
- Shear modulus
Isotropic-nematic transition[edit]
The uniaxial order parameter is zero for an isotropic fluid and one for a perfectly aligned system. First one calculates a director vector [1]
where is a second rank tensor, is a unit vector along the molecular long axis, and is the Kronecker delta. Diagonalisation of this tensor gives three eigenvalues , and , and is the eigenvector associated with the largest eigenvalue (). From this director vector the nematic order parameter is calculated from [2]
where d is the dimensionality of the system.
i.e. in three dimensions [3]
where is known as the uniaxial order parameter. Here is the second order Legendre polynomial, is the angle between a molecular axes and the director , and the angle brackets indicate an ensemble average.
Tetrahedral order parameter[edit]
See also[edit]
References[edit]
- ↑ R. Eppenga and D. Frenkel "Monte Carlo study of the isotropic and nematic phases of infinitely thin hard platelets", Molecular Physics 52 pp. 1303-1334 (1984)
- ↑ Anna A. Mercurieva, Tatyana M. Birshtein "Liquid-crystalline ordering in two-dimensional systems with discrete symmetry", Die Makromolekulare Chemie, Theory and Simulations 1 pp. 205-214 (1992)
- ↑ Mark R. Wilson "Determination of order parameters in realistic atom-based models of liquid crystal systems", Journal of Molecular Liquids 68 pp. 23-31 (1996)
- ↑ P. -L. Chau and A. J. Hardwick "A new order parameter for tetrahedral configurations", Molecular Physics 93 pp. 511-518 (1998)
- Related reading
- Joseph P. Straley "Ordered phases of a liquid of biaxial particles", Physical Review A 10 pp. 1881 - 1887 (1974)
- Denis Merlet, James W. Emsley, Philippe Lesot and Jacques Courtieu "The relationship between molecular symmetry and second-rank orientational order parameters for molecules in chiral liquid crystalline solvents", Journal of Chemical Physics 111 pp. 6890-6896 (1999)
- Erik E. Santiso and Bernhardt L. Trout "A general set of order parameters for molecular crystals", Journal of Chemical Physics 134 064109 (2011)