Chemistry·Core Principles

van der Waals Equation — Core Principles

NEET UG
Version 1Updated 22 Mar 2026

Core Principles

The van der Waals equation is a modified ideal gas law that accounts for the non-ideal behavior of real gases. It introduces two key corrections: a pressure correction and a volume correction. The pressure correction, an2V2a\frac{n^2}{V^2}, is added to the observed pressure 'P' and accounts for the attractive intermolecular forces between gas molecules.

A larger 'a' value indicates stronger attractions. The volume correction, nbnb, is subtracted from the container volume 'V' and accounts for the finite volume occupied by the gas molecules themselves (excluded volume).

A larger 'b' value indicates larger molecular size. The equation is (P+an2V2)(Vnb)=nRT(P + a\frac{n^2}{V^2})(V - nb) = nRT. This equation helps explain phenomena like gas liquefaction and deviations from ideal gas behavior, especially at high pressures and low temperatures where real gas properties become significant.

Understanding 'a' and 'b' is crucial for predicting gas behavior.

Important Differences

vs Ideal Gas Equation

AspectThis TopicIdeal Gas Equation
Molecular VolumeNegligible (point masses)Finite and non-negligible (corrected by 'b' term)
Intermolecular ForcesAbsent (no attraction/repulsion)Present (attractive forces corrected by 'a' term)
Equation$PV = nRT$$(P + a rac{n^2}{V^2})(V - nb) = nRT$
ApplicabilityHigh T, Low P (approximates real gases)Better for real gases, especially at low T, high P
Compressibility Factor (Z)$Z = 1$ always$Z eq 1$ (can be $>1$ or $<1$)
The ideal gas equation, $PV=nRT$, is a simplified model assuming point-like molecules with no interactions. In contrast, the van der Waals equation is a more realistic model for real gases, incorporating corrections for the finite volume of gas molecules (via constant 'b') and the attractive intermolecular forces between them (via constant 'a'). This makes the van der Waals equation more accurate in describing gas behavior, particularly under conditions of high pressure and low temperature where real gases significantly deviate from ideal behavior.
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