91影视

The expression for Mayer's f function is,

$f\left(r\right)=e^{-尾u\left(r\right)}-1$

The factor,

$尾=\frac{1}{k{T}_c}$

Here,

$k=$Boltzmann constant

$T_c$= Critical temperature

Thus, the Mayer's function=

$f\left(r\right)=e^{\frac{u\left(r\right)}{kT}}-1$

$u\left(r\right)$= potential energy due to interaction of any pair of molecules.

Considering the gaseous molecules are "hard hemispheres". If the separation between them $r$is more than the intermolecular separation $r_0$then potential energy is,

$u\left(r\right)=0$

$\text{If}r<r_0\text{, then the potential energy is,}$

$u\left(r\right)=鈭�$

$B\left(T\right)=-2蟺{鈭�}_0^{鈭�}{r}^{2}f\left(r\right)dr$

$=-2蟺\left[{鈭�}_0^{r_0}{r}^{2}f\left(r\right)dr\right]$

$=-2蟺\left[{鈭�}_0^{r_0}{r}^2\left(e^{-\frac{m\left(r\right)}{kT}}\right)\right]$

$=-2蟺\left[{鈭�}_0^{蟺}{r}^2\left(e^{-0}\right)\right]$

$=-2蟺{鈭�}_0^{r_0}{r}^{2}dr$

$=2蟺\left(\frac{r_0^3}{3}\right)$

From the equation we can say that the second virial coefficient is independent of temperature.

The second order virial expansion term,

$P=\left(\frac{NB\left(T\right)}{V}\right)$

Substituting the $B\left(T\right)=2蟺\left(\frac{r_0^3}{3}\right)$in the equation,

$P=\left(\frac{N}{V}\right)2蟺\left(\frac{r_0^3}{3}\right)$

$=\left(2蟺r_0^3\right)\frac{N}{3}$

Thus, the second order virial expansion is,

$P=\left(2蟺r_0^3\right)\frac{N}{3}$