Van der Waals Is Just A Correction Term That Makes Gases Behave Better
When you first learn gas laws in intro chemistry, you treat everything like an ideal gas. PV equals nRT, done, move on. Real gases don't give a damn about that equation when pressure gets high or temperature drops. Molecules have volume. They attract each other. The ideal gas law pretends none of that matters, which is fine if you're doing rough calculations at room conditions and low pressure, but it falls apart fast once you step outside that comfortable zone. Van der Waals is the equation that fixes this by adding two correction terms, one for molecular volume and one for intermolecular attraction, and it's been around since 1873 so there is nothing mysterious about it. The equation looks like this, and I am going to write it out plainly since you will need it: (P plus a times n squared over V squared) times (V minus n times b) equals nRT. The a constant accounts for attraction between molecules. Higher a means stronger attraction, which shows up as lower pressure than you would expect from an ideal gas. The b constant accounts for the fact that molecules take up space. You can't compress a gas infinitely because the molecules themselves are physical objects with finite size. These constants are experimentally determined for each gas, not theoretical guesses. I ran into a real problem with this last year while modeling supercritical CO2 flow through a narrow capillary at around 320 kelvin and 80 bar. The ideal gas law was predicting a volumetric flow rate that was roughly 18 percent higher than what our pressure transducers were actually reading. The CO2 was dense enough that the excluded volume term b mattered, and the attractive forces were significant enough that a mattered too. Plugging in the Van der Waals constants for CO2, which are approximately 3.592 liter-squared-bar per mole squared for a and 0.04267 liter per mole for b, brought the predicted density within about 2 percent of the measured value. Not perfect, but a lot better than being wrong by a sixth of your reading.
The constants for common gases are straightforward to look up. Nitrogen has an a value of 1.370 and b of 0.0387. Oxygen is 1.364 and 0.0318. Water vapor is different because hydrogen bonding makes a much larger at 5.464, which is why water deviates so aggressively from ideal behavior. Helium is nearly ideal because its a is only 0.0346 and b is 0.0238, which is why you will rarely see anyone bother with Van der Waals corrections for helium unless they are being extremely precise.
The Practical Problems Nobody Warns You About
Van der Waals is better than the ideal gas law but it is still just a cubic equation with approximations built in. It struggles near the critical point where the distinction between liquid and gas blurs out. It does not handle mixtures without mixing rules, and the standard quadratic mixing rules for a and b are themselves approximate. For engineering work with natural gas mixtures, you would typically use something like the Redlich-Kwong or Peng-Robinson equation instead, which were designed specifically to handle hydrocarbon systems more accurately across wider temperature and pressure ranges. I found this out the hard way when someone on my team tried using Van der Waals for a methane-ethane mixture at 250 kelvin and 60 bar and got phase behavior predictions that were clearly wrong. The mixture was entering the two-phase region but the equation was treating it as single phase. Switching to Peng-Robinson fixed it immediately, and the calculations only took a minute longer since we were already using a spreadsheet-based solver. The lesson here is that Van der Waals is fine for pure substances at moderate conditions, but it is not a general-purpose tool and you should know where its limits are before you trust it. Another thing that catches people off guard is the algebra. Solving for volume given pressure and temperature requires finding the real root of a cubic equation. There is no simple rearrangement that isolates V. You either use the cubic formula, which is tedious by hand, or you iterate numerically. Most people just plug it into a solver. Similarly, solving for pressure is trivial since it just rearranges directly. Solving for temperature is also straightforward. The asymmetry here is worth noting because it affects how you set up your calculations depending on which variable is unknown.
Get the Full Details

For a quick reference, the Van der Waals constants table is easy to find online and I would recommend keeping one bookmarked rather than memorizing values. The equation itself is simple enough to remember, but the constants are not intuitive and looking them up takes seconds. If you are doing this by hand for an exam or field calculation, you will waste more time searching than you save by not having them written down. The Van der Waals concept also extends beyond the equation itself into Van der Waals forces, which are the actual intermolecular interactions the a term models. These include London dispersion forces, dipole-dipole interactions, and dipole-induced dipole effects. Understanding which force dominates for a given substance helps you predict whether a will be large or small without needing to look it up. Nonpolar molecules with large electron clouds have strong dispersion forces and therefore higher a values, which is why iodine has a a of 6.49 while neon sits at 0.211. The trend is consistent and useful if you need a quick estimate.
When To Actually Use This Versus Something Else
Use Van der Waals when you need a reasonable correction to ideal gas behavior for a pure substance and you do not have access to more sophisticated software or tables. It is acceptable for academic work, rough engineering estimates, and situations where being within 5 to 10 percent is sufficient. Do not use it when you are working near the critical point, handling mixtures with components that have very different polarities, or doing precision work where even 2 percent error matters. In those cases, move to Peng-Robinson, Soave-Redlich-Kwong, or look up data from the NIST Chemistry WebBook, which has experimental values for thousands of substances. I have seen people attach a lot of confidence to Van der Waals results because the equation looks clean and the math is familiar. It is not the most accurate equation of state by any measure, but it is transparent about what it is doing, which is more than you can say for many black-box solvers you will encounter in industry software. Sometimes knowing that your result is approximate and understanding why it is approximate is more valuable than getting a slightly more accurate number from a model you do not fully understand. There is also a pedagogical value to working through Van der Waals by hand at least once. It forces you to confront the assumptions behind the ideal gas law and see exactly where those assumptions break down. That understanding carries over to every other equation of state you will encounter later, whether it is Virial, Redlich-Kwong, or something more modern. You will recognize the patterns faster because you have already seen the simplest version of the problem laid bare.
So what is Van der Waals really. It is a practical correction to ideal gas behavior that accounts for molecular size and attraction through two empirically determined constants. It works well enough for pure substances away from critical conditions, it fails in ways you can usually predict in advance, and it gives you a foundation for understanding more complex equations without overwhelming you with additional parameters. That is about all there is to it.
