# Van der Waals equation of state: further expansion

When studying the equation of state for an ideal gas, it's possible to deviate from it and introduce corrections both to the pressure and to the volume. In doing so, we can obtain the Van der Waals equation of state: $$\left(P+\dfrac{a}{v^2}\right)(v-b)=T$$ where $$k_B$$ has been set equal to 1 and $$v=V/N$$ is the specific volume.

Both the parameters $$a$$ and $$b$$ have some physical meaning: namely, $$a$$ is a measure of the attractive forces among the molecules of the system whereas $$b$$ measures the "effective space" occupied by the molecules. I also know it's possible to obtain the same equation of state from a mean-field theory of condensation, and again it's possible to interpret physically the parameters $$a$$ and $$b$$ introducing for example the excluded volume and characterizing in an adequate way the Lennard-Jones potential.

Nevertheless, if we want to proceed further and carrying on the virial expansion up to third or fourth order we would obtain more and more corrections to the Van der Waals equation.

What will be the physical meaning of this? In other words, when and why are these further corrections needed and what do they represent? In what theory do they appear and are they connected to physical properties of the system?

• Could you elaborate a bit more about the process to derive the Van der Waals equation (e.g. which is the Hamiltonian)? Otherwise, could you provide some references? I think that this would make your question more accessible to a wider audience that is not used to these concepts.
– Javi
Commented Oct 21, 2022 at 10:21
• If you are moving from an ideal gas law into real gas equation, at first, you'll need to decide which real gas law would be most suitable to you,- of which are many. Commented Oct 21, 2022 at 11:52
• @AgniusVasiliauskas Of course, I was focusing on the Van der Waals model since from an instructional point of view it is the most used and known. Commented Oct 21, 2022 at 14:34