1. Chapter at a Glance
The kinetic theory of gases explains the behaviour of a gas — its pressure, temperature and heat capacity — from the motion of its tiny molecules. It shows that pressure comes from molecules hitting the walls and that temperature measures their average kinetic energy. NEET usually asks one question: on rms speed, the law of equipartition, degrees of freedom or mean free path.
- rms speed and how it depends on T and molar mass.
- Average kinetic energy per molecule, (3/2)kT.
- Degrees of freedom and γ for mono-, di- and polyatomic gases.
- Ideal gas equation in its different forms.
- Mean free path and its dependence on pressure and size.
2. Ideal Gas and Its Assumptions
- Ideal gas equation: PV = nRT = NkBT, where R = 8.314 J mol⁻¹ K⁻¹, kB = 1.38 × 10⁻²³ J K⁻¹ and NA = 6.02 × 10²³ mol⁻¹.
- It combines Boyle's law (PV constant at fixed T), Charles' law (V ∝ T at fixed P) and Avogadro's law (equal volumes of gases at the same T and P contain equal numbers of molecules).
- Kinetic theory assumptions: molecules are tiny compared with the space between them; they move randomly and collide elastically; there are no forces between them except during collisions; collisions take negligible time.
- Real gases behave ideally at low pressure and high temperature.
- Dalton's law: total pressure of a gas mixture = sum of partial pressures.
3. Pressure and Temperature
- Average translational kinetic energy of a molecule = (3/2)kBT — the same for all gases at the same temperature.
- Total translational KE of one mole = (3/2)RT.
- rms speed vrms = √(3RT/M) = √(3kBT/m) = √(3P/ρ). It depends on T and M, not on pressure (at fixed T).
- Other speeds: most probable √(2RT/M) and average √(8RT/πM). Order: vmp < vavg < vrms, in the ratio √2 : √(8/π) : √3.
4. Degrees of Freedom and Equipartition
The law of equipartition of energy states that, in equilibrium, each degree of freedom (each independent way a molecule can store energy) has an average energy of ½kBT.
| Gas type | Degrees of freedom f | Cv | Cp | γ = 1 + 2/f |
|---|---|---|---|---|
| Monoatomic (He, Ne, Ar) | 3 (translational) | 3R/2 | 5R/2 | 1.67 |
| Diatomic, rigid (O₂, N₂, H₂) | 5 (3 trans + 2 rot) | 5R/2 | 7R/2 | 1.40 |
| Diatomic, with vibration | 7 | 7R/2 | 9R/2 | 1.29 |
| Polyatomic, rigid non-linear (CH₄) | 6 | 3R | 4R | 1.33 |
Internal energy of n moles U = (f/2)nRT. For a mixture: Cv,mix = (n₁Cv1 + n₂Cv2)/(n₁ + n₂).
5. Mean Free Path
It is the average distance a molecule travels between two collisions (n = molecules per unit volume, d = molecular diameter). It is larger at low pressure and for smaller molecules. At room conditions it is about 10⁻⁷ m, a few hundred times the molecular size.
6. Formula Master Table
| Quantity | Formula |
|---|---|
| Ideal gas | PV = nRT = NkBT |
| Kinetic pressure | P = ⅓ρvrms² |
| KE per molecule | (3/2)kBT |
| rms speed | √(3RT/M) |
| Energy per degree of freedom | ½kBT |
| Internal energy | U = (f/2)nRT |
| γ from f | γ = 1 + 2/f |
| Mean free path | λ = kBT/(√2πd²P) |
7. Master Summary Table
| Concept | Key point | NEET Note |
|---|---|---|
| Pressure | From molecular collisions | P = ⅓ρv² |
| Temperature | Measures average KE | Same KE for all gases at same T |
| rms speed | ∝ √(T/M) | Independent of P at fixed T |
| Equipartition | ½kT per degree of freedom | Diatomic f = 5 |
| Specific heats | Cp − Cv = R | γ = 1 + 2/f |
| Mean free path | ∝ T/(d²P) | Halving P doubles λ |
8. Mind Map
- PV = nRT
- Assumptions
- Gas laws
- P = ⅓ρv²
- KE = (3/2)kT
- vrms, vavg, vmp
- Speed distribution
- Degrees of freedom
- Equipartition
- Mean free path
9. Tips and Tricks
- To make vrms n times, make T n² times.
- At the same T: vrms(H₂) : vrms(O₂) = √(32/2) = 4 : 1.
- Always convert M to kg mol⁻¹ (O₂: 0.032, N₂: 0.028, He: 0.004).
- For mixtures, compute Cv first, then Cp = Cv + R, then γ.
- Saying heavier molecules have more KE at the same T — KE is the same; they just move slower.
- Using °C in (3/2)kT.
- Giving a diatomic molecule 3 or 6 degrees of freedom at room temperature (it is 5).
10. Important One-liners
- Temperature of a gas is a measure of the average kinetic energy of its molecules.
- At absolute zero the kinetic energy of an ideal gas would be zero.
- rms speed does not change with pressure at constant temperature.
- Each degree of freedom contributes ½kT of energy per molecule.
- γ is largest for monoatomic gases.
- Mean free path increases when pressure decreases.
- Gases deviate from ideal behaviour at high pressure and low temperature.
11. Solved Numericals: Average to Advanced
Five average and five advanced numericals. Take R = 8.314 J mol⁻¹ K⁻¹, kB = 1.38 × 10⁻²³ J K⁻¹. Click to reveal each answer and working.
Average level
Find the rms speed of nitrogen molecules (M = 28 g mol⁻¹) at 27 °C.
Show answer & solution
Concept: vrms = √(3RT/M), T in K and M in kg mol⁻¹.
- T = 300 K; M = 0.028 kg mol⁻¹.
- vrms = √(3 × 8.314 × 300/0.028) = √(267 236).
- ≈ 517 m s⁻¹.
Answer: about 517 m s⁻¹
Find the average translational kinetic energy of a gas molecule at 127 °C.
Show answer & solution
Concept: KE = (3/2)kBT.
- T = 400 K.
- KE = 1.5 × 1.38 × 10⁻²³ × 400 = 8.28 × 10⁻²¹ J.
Answer: 8.28 × 10⁻²¹ J
At what temperature will the rms speed of oxygen molecules be half their value at 27 °C?
Show answer & solution
Concept: vrms ∝ √T.
- Half the speed needs one-fourth the temperature.
- T = 300/4 = 75 K (= −198 °C).
Answer: 75 K
A gas of density 1.2 kg m⁻³ has an rms molecular speed of 500 m s⁻¹. Find its pressure.
Show answer & solution
Concept: P = ⅓ρvrms².
- P = ⅓ × 1.2 × 250 000.
- P = 1 × 10⁵ Pa (about 1 atmosphere).
Answer: 1 × 10⁵ Pa
How many moles of gas are in a 10 L cylinder at 2 × 10⁵ Pa and 300 K?
Show answer & solution
Concept: n = PV/RT.
- V = 10 L = 0.01 m³.
- n = 2 × 10⁵ × 0.01/(8.314 × 300) = 2000/2494.
- n ≈ 0.80 mol.
Answer: about 0.80 mol
Advanced level
One mole of helium is mixed with one mole of oxygen (rigid). Find Cv, Cp and γ of the mixture.
Show answer & solution
Concept: mole-weighted average of Cv.
- Cv,mix = (1 × 1.5R + 1 × 2.5R)/2 = 2R.
- Cp,mix = 2R + R = 3R.
- γ = 3R/2R = 1.5.
Answer: 2R; 3R; 1.5
Find the internal energy of 5 g of helium at 300 K (M = 4 g mol⁻¹).
Show answer & solution
Concept: U = (f/2)nRT with f = 3 for a monoatomic gas.
- n = 5/4 = 1.25 mol.
- U = 1.5 × 1.25 × 8.314 × 300.
- U ≈ 4677 J.
Answer: about 4.68 kJ
The absolute temperature of a gas is doubled and it is replaced by a gas of half the molar mass. By what factor does the rms speed change?
Show answer & solution
Concept: vrms ∝ √(T/M).
- T/M becomes (2T)/(M/2) = 4(T/M).
- vrms becomes √4 = 2 times.
Answer: doubles
The pressure of a gas is halved and its absolute temperature is doubled. By what factor does its mean free path change?
Show answer & solution
Concept: λ = kBT/(√2πd²P) ∝ T/P.
- T/P becomes (2T)/(P/2) = 4(T/P).
- λ becomes 4 times.
Answer: 4 times
Find vmp, vavg and vrms for helium (M = 4 g mol⁻¹) at 400 K.
Show answer & solution
Concept: RT/M = 8.314 × 400/0.004 ≈ 8.31 × 10⁵ m² s⁻².
- vmp = √(2 × 8.31 × 10⁵) ≈ 1290 m s⁻¹.
- vavg = √(8 × 8.31 × 10⁵/π) ≈ 1455 m s⁻¹.
- vrms = √(3 × 8.31 × 10⁵) ≈ 1579 m s⁻¹.
- Order vmp < vavg < vrms ✓.
Answer: about 1290, 1455 and 1579 m s⁻¹
12. NEET-pattern Questions with Detailed Answers
These questions are original and modelled on concepts repeatedly asked in NEET UG.
The average kinetic energy of a gas molecule is directly proportional to:
- √T
- T
- T²
- 1/T
Show solution
KE = (3/2)kBT ∝ T (absolute temperature). The rms speed is ∝ √T.
Answer: (B)
The number of degrees of freedom of a rigid diatomic molecule is:
- 3
- 5
- 6
- 7
Show solution
Three translational plus two rotational = 5 (rotation about the bond axis does not count).
Answer: (B)
At the same temperature, the ratio of rms speeds of hydrogen and oxygen molecules is:
- 1 : 4
- 4 : 1
- 1 : 16
- 16 : 1
Show solution
v ∝ 1/√M: √(32/2) = 4, so 4 : 1.
Answer: (B)
The internal energy of one mole of a monoatomic ideal gas at temperature T is:
- RT/2
- RT
- 3RT/2
- 5RT/2
Show solution
U = (f/2)RT with f = 3 ⇒ 3RT/2. 5RT/2 would be for a rigid diatomic gas.
Answer: (C)
If the pressure of a gas is increased at constant temperature, the rms speed of its molecules:
- Increases
- Decreases
- Remains unchanged
- Becomes zero
Show solution
vrms = √(3RT/M) depends only on T and M; raising P at fixed T just raises the density.
Answer: (C)
For a gas whose molecules have f degrees of freedom, γ equals:
- 1 + f/2
- 1 + 2/f
- 2/f
- f/(f + 2)
Show solution
Cv = fR/2, Cp = (f/2 + 1)R ⇒ γ = (f + 2)/f = 1 + 2/f.
Answer: (B)
The rms speed of a gas at 27 °C is v. Its rms speed at 927 °C is:
- v√2
- 2v
- 4v
- v/2
Show solution
T changes from 300 K to 1200 K (4 times), so vrms becomes √4 = 2 times. Using °C (27 → 927) would wrongly suggest a much larger change.
Answer: (B)
The mean free path of gas molecules depends on the molecular diameter d as:
- d
- 1/d
- 1/d²
- d²
Show solution
λ = 1/(√2πd²n): larger molecules present a bigger target (∝ d²) and collide more often.
Answer: (C)
13. Quick Revision Summary
- PV = nRT = NkBT; P = ⅓ρvrms².
- KE per molecule (3/2)kBT — same for all gases at the same T.
- vrms = √(3RT/M); vmp < vavg < vrms.
- ½kBT per degree of freedom; f = 3, 5, 6; γ = 1 + 2/f.
- λ = kBT/(√2πd²P).