9-3 Lennard-Jones potential: Difference between revisions
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Let us consider the space divided in two regions: | Let us consider the space divided in two regions: | ||
* <math> x < 0 </math>: this region is occupied by a ''diffuse'' solid with density <math> \rho_s </math> composed of Lennard-Jones atoms | * <math> x < 0 </math>: this region is occupied by a ''diffuse'' solid with density <math> \rho_s </math> composed of 12-6 [[Lennard-Jones model|Lennard-Jones]] atoms | ||
with paremeters <math> \sigma_s </math> and <math> \epsilon_a </math> | with paremeters <math> \sigma_s </math> and <math> \epsilon_a </math> | ||
Revision as of 12:55, 23 March 2007
[EN CONSTRUCCION]
Functional form
The 9-3 Lennard-Jones potential is related to the standard Lennard-Jones potential.
It takes the form:
The minimum value of is obtained at , with
- ,
Applications
It is commonly used to model the interaction between the particles of a fluid with a flat structureless solid wall.
Interaction between a solid and a fluid molecule
Let us consider the space divided in two regions:
- : this region is occupied by a diffuse solid with density composed of 12-6 Lennard-Jones atoms
with paremeters and
Our aim is to compute the total interaction between this solid and a molecule located at a position .
[TO BE CONTINUED]