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S1.5 Ideal gasesIB Chemistry SL: Revision notes

Section 1

The ideal gas model

An ideal gas is a model with these assumptions:

  • the particles are in constant random motion;
  • the particles have negligible volume compared with the container;
  • there are no intermolecular forces between particles;
  • all collisions are elastic: no kinetic energy is lost overall.

The pressure of a gas comes from particles colliding with the container walls. The average kinetic energy of the particles is proportional to the absolute temperature (kelvin).

Key termsideal gaselastic collisionpressure

Section 2

Real gases and the limits of the model

Real gases deviate from ideal behaviour, most at low temperature and high pressure.

  • At high pressure, particles are close together, so their own volume is no longer negligible and attractions between them matter.
  • At low temperature, particles move slowly, so intermolecular attractions have a bigger effect and the gas may condense.

Gases with stronger intermolecular forces (polar molecules, hydrogen bonding, many electrons) and larger molecules deviate most. Helium and hydrogen are the closest to ideal. Gases are most ideal at high temperature and low pressure.

Key termsreal gasdeviation
Exam tip

In a data question, pV/nRT below 1 means attractions dominate; above 1 means the volume of the particles dominates.

Section 3

Gas laws for a fixed mass of gas

Temperatures must be in kelvin: T/K = t/°C + 273.

  • Boyle's law (constant T): p ∝ 1/V. A plot of p against V is a curve; p against 1/V is a straight line through the origin.
  • Charles's law (constant p): V ∝ T. V against T in K is a straight line through the origin; against °C it meets the axis at −273 °C.
  • Gay-Lussac's law (constant V): p ∝ T.

The combined gas law: p₁V₁/T₁ = p₂V₂/T₂.

Key termsBoyle's lawCharles's lawcombined gas lawabsolute temperature
Common mistake

Using temperatures in °C in gas-law calculations. Always convert to kelvin first.

Section 4

The ideal gas equation

pV = nRT, where R = 8.31 J K⁻¹ mol⁻¹ (data booklet). Use SI units: p in Pa, V in m³, T in K.

Unit conversions: 1 kPa = 10³ Pa; 1 dm³ = 10⁻³ m³; 1 cm³ = 10⁻⁶ m³. (Using kPa with dm³ also works, because the two factors of 10³ cancel.)

Since n = m/M, you can find the molar mass of a volatile liquid: M = mRT/(pV).

Key termsideal gas equationgas constant
Exam tip

Write down the converted values of p, V and T before substituting; most lost marks are unit errors.

Section 5

Molar volume

At a given temperature and pressure, one mole of any ideal gas occupies the same volume, the molar volume. At 273 K and 100 kPa (STP) it is 22.7 dm³ mol⁻¹ (data booklet). So n = V ÷ 22.7 for a gas at STP (V in dm³).

The molar volume changes with conditions: it is larger at higher temperature or lower pressure. At other conditions, use pV = nRT instead.

Key termsmolar volumeSTP

Must know

  • Ideal gas: negligible particle volume, no intermolecular forces, elastic collisions.
  • Most ideal at high T and low p; deviations biggest at low T and high p.
  • Always use kelvin; p₁V₁/T₁ = p₂V₂/T₂.
  • pV = nRT in Pa, m³, K; M = mRT/pV.
  • Molar volume at STP (273 K, 100 kPa) = 22.7 dm³ mol⁻¹.

That's the notes covered.

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