9-3 Lennard-Jones potential: Difference between revisions

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== Functional form ==
The '''9-3 Lennard-Jones potential''' is related to the [[Lennard-Jones model| Lennard-Jones potential]].
The 9-3 Lennard-Jones potential is related to the [[Lennard-Jones model|standard Lennard-Jones potential]].
It has the following form:
 
It takes the form:


: <math>
: <math>
\Phi(r) = \frac{ 3 \sqrt{3}}{ 2} \epsilon \left[ \left( \frac{\sigma}{r} \right)^9 -  
\Phi_{12}(r) = \frac{ 3 \sqrt{3}}{ 2} \epsilon \left[ \left( \frac{\sigma}{r} \right)^9 -  
\left( \frac{ \sigma }{r} \right)^3 \right].
\left( \frac{ \sigma }{r} \right)^3 \right].
</math>
</math>


where <math>\Phi(r)</math> is the [[intermolecular pair potential]].
where <math>\Phi_{12}(r)</math> is the [[intermolecular pair potential]] and <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math>.
The minimum value of <math> \Phi(r) </math> is obtained at <math> r = r_{min} </math>, with
The minimum value of <math> \Phi(r) </math> is obtained at <math> r = r_{min} </math>, with
* <math> \Phi \left( r_{min} \right) = - \epsilon </math>,
* <math> \Phi \left( r_{min} \right) = - \epsilon </math>,
* <math> \frac{ r_{min} }{\sigma} = 3^{1/6} </math>
* <math> \frac{ r_{min} }{\sigma} = 3^{1/6} </math>
== Applications ==
== Applications ==
It is commonly used to model the interaction between the particles
It is commonly used to model the interaction between the particles
of a fluid with a flat structureless solid wall.
of a fluid with a flat structureless solid wall or ''vice versa'' (Ref. 1).
 
== Interaction between a solid and a fluid molecule ==
== Interaction between a solid and a fluid molecule ==
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 12-6 [[Lennard-Jones model|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 parameters <math> \sigma_s </math> and <math> \epsilon_a </math>
with parameters <math> \sigma_s </math> and <math> \epsilon_a </math>
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- \frac{\sigma^3 }{ 2 x^3  } \right]
- \frac{\sigma^3 }{ 2 x^3  } \right]
</math>
</math>
 
==References==
 
#[http://dx.doi.org/10.1063/1.435080  Farid F. Abraham and Y. Singh "The structure of a hard-sphere fluid in contact with a soft repulsive wall", Journal of Chemical Physics '''67''' pp. 2384-2385 (1977)]
[[category:models]]
[[category:models]]

Latest revision as of 15:44, 24 July 2008

The 9-3 Lennard-Jones potential is related to the Lennard-Jones potential. It has the following form:

Φ12(r)=332ϵ[(σr)9−(σr)3].

where Φ12(r) is the intermolecular pair potential and r:=|r1−r2|. The minimum value of Φ(r) is obtained at r=rmin, with

  • Φ(rmin)=−ϵ,
  • rminσ=31/6

Applications[edit]

It is commonly used to model the interaction between the particles of a fluid with a flat structureless solid wall or vice versa (Ref. 1).

Interaction between a solid and a fluid molecule[edit]

Let us consider the space divided in two regions:

  • x<0: this region is occupied by a diffuse solid with density ρs composed of 12-6 Lennard-Jones atoms

with parameters σs and ϵa

Our aim is to compute the total interaction between this solid and a molecule located at a position xf>0. Such an interaction can be computed using cylindrical coordinates.

The interaction will be:

ΦW(x)=4ϵsfρs∫02πdϕ∫−∞−xdz∫0∞dr[σ12r(r2+z2)6−σ6r(r2+z2)3].
ΦW(x)=8πϵsfρs∫−∞−xdz[σ1210(r2+z2)5−σ64(r2+z2)2]r=∞r=0.
ΦW(x)=8πϵsfρs∫−∞−xdz[σ1210z10−σ64z4];


ΦW(x)=8πϵsfρs[−σ1290z9+σ612z3]z=−∞z=−x;
ΦW(x)=4πϵsfρsσ33[σ915x9−σ32x3]

References[edit]

  1. Farid F. Abraham and Y. Singh "The structure of a hard-sphere fluid in contact with a soft repulsive wall", Journal of Chemical Physics 67 pp. 2384-2385 (1977)