Virial pressure

The virial pressure is commonly used to obtain the pressure from a general simulation. It is particularly well suited to molecular dynamics, since forces are evaluated and readily available. For pair interactions, one has:

$p={\frac {k_{B}TN}{V}}-{\frac {1}{dV}}{\overline {\sum _{i<j}{\mathbf {f} }_{ij}{\mathbf {r} }_{ij}}},$

where one can recognize an ideal term, and a second term due to the virial. The overline is an average, which would be a time average in molecular dynamics, or an ensemble average in Monte Carlo; $d$ is the dimension of the system (3 in the "real" world). ${\mathbf {f} }_{ij}$ is the force on particle $i$ exerted by particle $j$, and ${\mathbf {r} }_{ij}$ is the vector going from $i$ to $j$: ${\mathbf {r} }_{ij}={\mathbf {r} }_{j}-{\mathbf {r} }_{i}$.

This relationship is readily obtained by writing the partition function in "reduced coordinates", i.e. $x^{*}=x/L$, etc, then considering a "blow-up" of the system by changing the value of $L$. This would apply to a simple cubic system, but the same ideas can also be applied to obtain expressions for the stress tensor and the surface tension, and are also used in constant-pressure Monte Carlo.

If the interaction is central, the force is given by

${\mathbf {f} }_{ij}=-{\frac {{\mathbf {r} }_{ij}}{r_{ij}}}f(r_{ij}),$

where $f(r)$ the force corresponding to the intermolecular potential $\Phi (r)$:

$-\partial \Phi (r)/\partial r.$

For example, for the Lennard-Jones potential, $f(r)=24\epsilon (2(\sigma /r)^{12}-(\sigma /r)^{6})/r$. Hence, the expression reduces to

$p={\frac {k_{B}TN}{V}}+{\frac {1}{dV}}{\overline {\sum _{i<j}f(r_{ij})r_{ij}}}.$

Notice that most realistic potentials are attractive at long ranges, hence the first correction to the ideal pressure will be a negative contribution: the second virial coefficient. On the other hand, contributions from purely repulsive potentials, such as hard spheres, are always positive.