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Real gases do not always follow the ideal gas law because gas particles have volume and attract each other. This cheat sheet helps students compare ideal and real gases, understand when deviations become important, and use the Van der Waals equation correctly. It is especially useful for high-pressure, low-temperature, and intermolecular force problems in chemistry.

The ideal gas law PV=nRTPV = nRT assumes particles have no volume and no attractions, but real gases need corrections. The Van der Waals equation (P+an2V2)(Vnb)=nRT\left(P + a\frac{n^2}{V^2}\right)(V - nb) = nRT adjusts pressure for attractions and volume for particle size. The constants aa and bb depend on the gas and help predict how strongly a gas deviates from ideal behavior.

Key Facts

  • The ideal gas law is PV=nRTPV = nRT, where PP is pressure, VV is volume, nn is moles, RR is the gas constant, and TT is temperature in kelvin.
  • Real gases behave most ideally at high temperature and low pressure because particles are far apart and moving fast.
  • The Van der Waals equation is (P+an2V2)(Vnb)=nRT\left(P + a\frac{n^2}{V^2}\right)(V - nb) = nRT.
  • The pressure correction an2V2a\frac{n^2}{V^2} accounts for attractive forces that make the measured pressure lower than ideal.
  • The volume correction nbnb accounts for the actual volume occupied by gas particles, so the free space is VnbV - nb.
  • A larger aa value means stronger intermolecular attractions and greater pressure deviation from ideal behavior.
  • A larger bb value means larger particle volume and greater excluded-volume deviation from ideal behavior.
  • The compressibility factor is Z=PVnRTZ = \frac{PV}{nRT}, with Z=1Z = 1 for an ideal gas, Z<1Z < 1 when attractions dominate, and Z>1Z > 1 when particle volume dominates.

Vocabulary

Real gas
A gas that deviates from ideal behavior because its particles have volume and experience intermolecular forces.
Ideal gas
A theoretical gas whose particles have no volume, no attractions, and obey PV=nRTPV = nRT exactly.
Van der Waals equation
An equation of state, (P+an2V2)(Vnb)=nRT\left(P + a\frac{n^2}{V^2}\right)(V - nb) = nRT, that corrects the ideal gas law for real gas behavior.
Pressure correction
The term an2V2a\frac{n^2}{V^2} added to pressure to account for attractions between gas particles.
Volume correction
The term nbnb subtracted from volume to account for the space occupied by gas particles themselves.
Compressibility factor
The ratio Z=PVnRTZ = \frac{PV}{nRT} that shows how much a gas deviates from ideal behavior.

Common Mistakes to Avoid

  • Using Celsius instead of kelvin, which is wrong because gas law equations require absolute temperature, so use T(K)=T(C)+273.15T(K) = T(^\circ C) + 273.15.
  • Forgetting to square nn in the pressure correction, which is wrong because the attraction correction is an2V2a\frac{n^2}{V^2}, not anV2a\frac{n}{V^2}.
  • Subtracting nbnb from pressure instead of volume, which is wrong because nbnb corrects the available volume and must appear as VnbV - nb.
  • Assuming all gases have the same aa and bb values, which is wrong because these constants depend on particle size and intermolecular forces.
  • Treating Z<1Z < 1 as particle-volume dominance, which is wrong because Z<1Z < 1 usually means attractions lower the pressure below the ideal value.

Practice Questions

  1. 1 Calculate the ideal pressure of 2.00 mol2.00\ \text{mol} of gas in a 10.0 L10.0\ \text{L} container at 300 K300\ \text{K} using R=0.0821 LatmmolKR = 0.0821\ \frac{\text{L}\cdot\text{atm}}{\text{mol}\cdot\text{K}}.
  2. 2 For 1.00 mol1.00\ \text{mol} of a gas with a=1.39 L2atmmol2a = 1.39\ \frac{\text{L}^2\cdot\text{atm}}{\text{mol}^2} in a 2.00 L2.00\ \text{L} container, calculate the pressure correction an2V2a\frac{n^2}{V^2}.
  3. 3 For 3.00 mol3.00\ \text{mol} of a gas with b=0.0391 Lmolb = 0.0391\ \frac{\text{L}}{\text{mol}} in a 5.00 L5.00\ \text{L} container, calculate the corrected volume VnbV - nb.
  4. 4 Explain why a gas at high pressure and low temperature is more likely to deviate from PV=nRTPV = nRT than the same gas at low pressure and high temperature.