Calculate real gas pressure accounting for molecular volume and intermolecular attraction. Understand the deviation from the Ideal Gas Law.
Last Updated: 5/6/2026
Container volume in liters
Absolute temperature (0°C = 273.15 K)
Amount of gas (molar quantity)
Presets: N₂: a=1.36, b=0.0386 | O₂: a=1.36, b=0.0318 | CO₂: a=3.658, b=0.04267 | H₂O: a=5.537, b=0.03049
The Ideal Gas Law (PV = nRT) is a cornerstone of chemistry and physics, providing elegant simplicity by assuming gas molecules occupy negligible volume and exert no forces on each other. This approximation works remarkably well at high temperatures and low pressures, where molecules are far apart and intermolecular interactions are minimal. However, at lower temperatures or higher pressures—conditions common in industrial processes, cryogenics, and compressed gas cylinders—real gas behavior deviates significantly from ideality. Molecules experience attractive forces (van der Waals forces: London dispersion, dipole-dipole, hydrogen bonding) and occupy finite volumes, leading to pressures that differ from the Ideal Gas Law predictions by 1−50% or more.
The Van der Waals equation, derived by Johannes van der Waals in 1873, corrects these effects through two empirical constants: a and b. The constant a accounts for intermolecular attractive forces, reducing the pressure exerted on container walls (since molecules are partly "stuck" together). The constant b represents the excluded volume—the space unavailable to the gas because molecules themselves occupy finite volume. Different gases have distinct a and b values reflecting their molecular size and intermolecular forces. For instance, CO₂ has a larger a than N₂, indicating stronger intermolecular attractions. This calculator allows exploration of how these corrections modify gas pressure in real-world conditions.
Input the volume of the container (in liters), absolute temperature (in Kelvin), and number of moles of gas. For example, 0.5 L at 273 K (0°C) with 1 mole simulates a cooled, compressed gas.
Choose presets for your gas (N₂, O₂, CO₂, H₂O) or enter custom a (attraction parameter) and b (excluded volume). Higher a values indicate stronger intermolecular forces; higher b indicates larger molecular size.
The calculator displays both the ideal gas pressure (from PV = nRT) and the real gas pressure (from Van der Waals). The percentage deviation shows how much reality diverges from the ideal model—large deviations occur under extreme conditions.
If real pressure is above ideal, the b effect (molecular volume) dominates. If below, the a effect (attractive forces) dominates. Most real gases at high pressure show pressure above ideal due to finite molecular size.
Scenario: A lab technician pressurizes 1 mole of CO₂ gas in a 0.5 L rigid cylinder at 0°C (273.15 K). Compare the ideal gas pressure with the real gas pressure predicted by Van der Waals, using CO₂ constants: a = 3.658 L²·atm/mol², b = 0.04267 L/mol.
At high pressures, low temperatures, or with gases having strong intermolecular forces (like CO₂ or H₂O vapor), the Ideal Gas Law becomes inaccurate. Van der Waals corrections are essential in cryogenics, compressed gas systems, and near phase transitions. Check the deviation percentage; if > 5%, Van der Waals is recommended.
The "a" parameter quantifies intermolecular attractive forces (van der Waals forces). Larger "a" means stronger attraction (e.g., CO₂ has a ≈ 3.66 vs. N₂ ≈ 1.36). These attractions reduce pressure because molecules are partly held back, not hitting walls as forcefully.
The "b" parameter is the excluded volume per mole—the space occupied by molecules themselves. Larger "b" indicates bigger molecules. For most gases, b is 1–10% of the container volume. This effect increases pressure because fewer free-moving molecules fit in the available space.
It depends on the regime. At room temperature and modest compression, CO₂'s strong attractions (large a) dominate, pulling pressure down. At very high pressures, the excluded volume (b) effect becomes dominant, pushing pressure up. N₂ has weaker attractions, so the b-effect dominates earlier.
Van der Waals provides qualitative insight but is not precise enough for accurate phase diagrams. However, it correctly predicts that cooling and compression favor condensation. For quantitative work, use NIST data or more sophisticated equations of state (Virial, Peng-Robinson).
Z = PV / (nRT). For ideal gas, Z = 1. For real gases, Z < 1 often means attractions dominate (pressure reduced); Z > 1 means excluded volume dominates (pressure increased). Van der Waals predictions modify Z from the ideal value, showing how far reality deviates.
In the classical Van der Waals model, "a" and "b" are treated as constants independent of temperature. In reality, they exhibit weak temperature dependence, especially near phase transitions. For most practical engineering calculations, constant values are acceptable.
Consult published thermodynamic databases (NIST, Dortmund Data Bank) or literature. Constants are sometimes estimated from critical temperature and pressure: a ≈ 27R²T_c² / (64P_c) and b ≈ RT_c / (8P_c). Many chemistry textbooks also provide tables.
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