Boynton and Bramley equation of state

The Boynton and Bramley equation of state is given by

$\left(p+{\frac {a}{V^{2}}}\right)(V-b)={\frac {RT}{\left(1+{\frac {\psi ^{2}}{T^{2}}}\right)}}$

where $\psi$ is a characteristic temperature. and where:

• $p$ is the pressure,
• $V$ is the volume,
• $T$ is the absolute temperature,
• $R$ is the molar gas constant; $R=N_{A}k_{B}$, with $N_{A}$ being the Avogadro constant and $k_{B}$ being the Boltzmann constant.
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For this equation at the critical point one has

${\frac {RT_{c}}{p_{c}V_{c}}}={\frac {8}{3}}\left(1+{\frac {\psi ^{2}}{T_{c}^{2}}}\right)$