Kinetic Theory of Gases — NEET Physics Notes
The kinetic theory of gases explains the behaviour of gases in terms of motion of molecules. This topic connects macroscopic gas laws (PV = nRT) with the microscopic molecular picture — a key conceptual chapter in NEET Physics.
Quick Revision
- Assumptions: Gas consists of large number of molecules, negligible volume, no intermolecular forces, elastic collisions, average KE ∝ temperature
- Pressure: P = (⅓) ρ v̄² = (⅓) (Nm/v) v̄²
- RMS Velocity: v_rms = √(3P/ρ) = √(3kT/m) = √(3RT/M)
- Average KE: (½) mv̄² = (3/2) kT per molecule
- Degrees of Freedom: f = 2 for monoatomic, 5 for diatomic, 6 for polyatomic
- Equipartition Theorem: Energy equally distributed among degrees of freedom — each degree gets (½) kT
- Gas Law: PV = nRT (universal gas constant R = 8.314 J/mol·K)
Standard Study
Kinetic Theory Assumptions
- Large number of molecules moving in random directions
- Volume of molecules is negligible compared to gas volume
- No intermolecular forces (except during collisions)
- Collisions between molecules are perfectly elastic
- Time spent in collisions is negligible compared to time between collisions
- Gas is in thermal equilibrium — uniform temperature throughout
Pressure Derivation
- Pressure P = (⅓) ρ v̄² (derived from momentum transfer during collisions)
- Alternatively: P = (Nm v̄²) / (3V)
- Combining with ideal gas equation: v_rms = √(3P/ρ)
Gas Velocities
RMS Velocity:
- v_rms = √(3kT/m) = √(3P/ρ)
- Depends only on temperature and molecular mass
- Lighter gases have higher RMS speed at same temperature
Most Probable Speed:
- v_mp = √(2kT/m) = √(2P/ρ)
- Speed at which maximum molecules are found
Average Speed:
- v_av = √(8kT/πm) = √(8RT/πM)
- Arithmetic mean of molecular speeds
Relation: v_mp : v_av : v_rms = √2 : √(8/π) : √3 ≈ 1 : 1.13 : 1.22
Maxwell-Boltzmann Distribution
- Number of molecules with speed between v and v+dv
- Curve is skewed — most probable speed is at the peak
- As temperature increases, curve shifts right and flattens
- RMS speed always greater than most probable speed
Degrees of Freedom and Specific Heat
Monatomic Gas (He, Ne — 3 degrees of freedom):
- C_v = (3/2)R
- C_p = C_v + R = (5/2)R
- γ = C_p/C_v = 5/3 ≈ 1.67
Diatomic Gas (O₂, N₂ — 5 degrees of freedom at room temp):
- C_v = (5/2)R
- C_p = C_v + R = (7/2)R
- γ = C_p/C_v = 7/5 = 1.4
Polyatomic Gas (6+ degrees of freedom):
- C_v = f × (R/2)
- γ depends on f
Ideal Gas Equation
- PV = nRT = NkT
- P = pressure, V = volume, n = moles, N = molecules
- R = 8.314 J/mol·K, k = R/NA = 1.38 × 10⁻²³ J/K
Deep Study
Real Gases and Van der Waals Equation
- Real gases deviate from ideal behaviour at high pressure and low temperature
- Van der Waals equation: (P + a(n/V)²)(V − nb) = nRT
- a = accounts for intermolecular attraction
- b = excluded volume (molecular volume)
Mean Free Path
- Average distance travelled by a molecule between successive collisions
- λ = 1/(√2 × π × d² × n/V)
- d = molecular diameter, n/V = number density
- inversely proportional to pressure — lower pressure means longer mean free path
Diffusion and Effusion
- Graham’s Law: Rate of diffusion ∝ 1/√M
- Ratio of diffusion rates: r₁/r₂ = √(M₂/M₁)
- Effusion: Gas escaping through a small hole — same dependence on molecular weight
Behavior at Different Scales
- At very low pressures (high vacuum), mean free path is very large
- Gas molecules move in straight lines between collisions
- Collision frequency decreases with decreasing pressure
Exam Tips
- rms speed formula: √(3kT/m) — depends on temperature and molecular mass
- Average KE of gas molecule = (3/2) kT — depends only on temperature, not on gas type
- Degrees of freedom determine specific heats — monatomic = 3 DOF, diatomic = 5 DOF
- γ = C_p/C_v is greater for monoatomic than diatomic (5/3 > 7/5)
- At same temperature, lighter molecules move faster (v_rms ∝ 1/√M)
- Mean free path inversely proportional to pressure — important in vacuum applications
- Ideal gas equation PV = nRT is universal — works for all gases
Common Pitfalls
- Confusing rms, average, and most probable speeds — remember their ratio
- Forgetting that at higher temperature, gas molecules move faster
- Not knowing which degrees of freedom contribute at room temperature vs high temperature
- Confusing specific heat at constant volume vs constant pressure (Cp = Cv + R)
- Applying kinetic theory assumptions to real gases without accounting for deviations
- Confusing mean free path with distance between molecules
Suggested Study Order
- Kinetic theory assumptions and molecular picture
- Derivation of pressure formula from kinetic theory
- RMS, average, and most probable speeds
- Maxwell-Boltzmann distribution (conceptual)
- Degrees of freedom and equipartition theorem
- Specific heats and γ relation
- Real gases and van der Waals equation
- Mean free path, diffusion, and effusion