Ideal gases
The mole and the Avogadro constant, the ideal gas equation pV = nRT = NkT, the kinetic theory assumptions, deriving pV = ⅓Nm⟨c²⟩, and linking the mean kinetic energy of a molecule to temperature.
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In 30 seconds
- The mole: 1 mol contains N_A = 6.02 × 10²³ particles.
- An ideal gas obeys pV = nRT (n moles) = NkT (N molecules), with T in kelvin. R = 8.31 J K⁻¹ mol⁻¹; k = R/N_A = 1.38 × 10⁻²³ J K⁻¹.
- Kinetic theory: molecules bouncing off the walls change momentum, giving pressure: pV = ⅓Nm⟨c²⟩.
- Temperature measures the mean kinetic energy of the molecules: ½m⟨c²⟩ = (3/2)kT.
By the end you can
- Understand amount of substance in moles and the Avogadro constant.
- Recall and use pV = nRT and pV = NkT.
- State the basic assumptions of the kinetic theory of gases.
- Derive and use pV = ⅓Nm⟨c²⟩, and link mean kinetic energy to temperature.
1The ideal gas equation
pV = nRT
Ideal gas — a gas that obeys pV ∝ T at all pressures, volumes and temperatures (T in kelvin).
Find the number of moles of gas in 0.024 m³ at 1.0 × 10⁵ Pa and 290 K.
- n = pV/RT = 1.0 × 10⁵ × 0.024/(8.31 × 290) C1
- n = 1.0 mol A1
A sealed rigid container of gas is heated from 300 K to 375 K. By what factor does the pressure change?
- constant V: p/T is constant C1
- p₂ = p₁ × 375/300 = 1.25 p₁ A1
2Kinetic theory
Assumptions
| Assumption | Why it matters |
|---|---|
| A large number of molecules in random motion | pressure is the same in all directions, and statistics work |
| Molecules have negligible volume compared with the container | V is the volume available for motion |
| No intermolecular forces except during collisions | no potential energy: internal energy is all kinetic |
| Collisions are elastic | no kinetic energy is lost |
| The time of a collision is negligible compared with the time between collisions | collisions are instantaneous |
Deriving pV = ⅓Nm⟨c²⟩
- One molecule in a cube of side L: it hits a wall with velocity u, changing momentum by 2mu. Time between hits on that wall: 2L/u. Average force = 2mu ÷ (2L/u) = mu²/L.
- N molecules: total force = Nm⟨u²⟩/L, so pressure = Nm⟨u²⟩/L³ = Nm⟨u²⟩/V.
- Three dimensions: ⟨c²⟩ = ⟨u²⟩ + ⟨v²⟩ + ⟨w²⟩ = 3⟨u²⟩ (random motion), so pV = ⅓Nm⟨c²⟩.
Find the mean kinetic energy of a molecule at 300 K, and the r.m.s. speed of nitrogen molecules (mass 28 u).
- E = (3/2)kT = 1.5 × 1.38 × 10⁻²³ × 300 = 6.2 × 10⁻²¹ J C1 A1
- crms = √(3kT/m) = √(3 × 1.38 × 10⁻²³ × 300/(28 × 1.66 × 10⁻²⁷)) = 517 m s⁻¹ A1
Test yourself — cover the answers first
Quick check
- State the Avogadro constant.
- What happens to the mean KE of molecules if T (in K) doubles?
- Name one assumption of kinetic theory.
- Find the r.m.s. speed of speeds 2, 4, 6 m s⁻¹.
- How many molecules are in 2 mol?
Exam-style
- A gas at 1.2 × 10⁵ Pa occupies 3.0 × 10⁻³ m³ at 27 °C. Find the number of molecules.
- By what factor does c_rms change if T rises from 300 K to 1200 K?
- Show that p = ⅓ρ⟨c²⟩.
Show answers
- 6.02 × 10²³ mol⁻¹
- it doubles
- e.g. collisions are elastic
- √(56/3) = 4.32 m s⁻¹
- 1.2 × 10²⁴
- N = pV/kT = 360/(1.38 × 10⁻²³ × 300) = 8.7 × 10²²
- c_rms ∝ √T, so it doubles
- pV = ⅓Nm⟨c²⟩ and ρ = Nm/V, so p = ⅓ρ⟨c²⟩
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