⚛️ Physics — Class XI

Kinetic Theory

How molecules in perpetual motion give rise to pressure, temperature, and the behaviour of gases

📖 Chapter 12 ⏱ ~50 min read 🏷️ Molecular Physics

Table of Contents

  1. Introduction
  2. Molecular Nature of Matter
  3. Behaviour of Gases
  4. Kinetic Theory of an Ideal Gas
  5. Law of Equipartition of Energy
  6. Specific Heat Capacity
  7. Mean Free Path

12.1 Introduction

Kinetic theory explains the behaviour of gases based on the idea that gas consists of rapidly moving atoms or molecules. This is possible as the inter-atomic forces, which are short range and important for solids and liquids, can be neglected for gases.

💡 Feynman's Atomic Hypothesis

"All things are made of atoms — little particles that move around in perpetual motion, attracting each other when they are a little distance apart, but repelling upon being squeezed into one another." — Richard Feynman

12.2 Molecular Nature of Matter

The discovery that matter is made up of atoms is one of the most significant in all of science. Dalton's atomic theory explained the laws of definite and multiple proportions. Avogadro's hypothesis states that equal volumes of all gases at equal temperature and pressure have equal number of molecules.

N = nNₐ = (m/M)Nₐ
N = number of molecules, n = moles, Nₐ = 6.022 × 10²³ (Avogadro's number), M = molar mass

12.3 Behaviour of Gases

Gases obey several empirical laws that relate pressure, volume, and temperature:

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Boyle's Law

PV = constant (at constant T). Pressure inversely proportional to volume. Double the pressure → half the volume.

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Charles's Law

V/T = constant (at constant P). Volume directly proportional to absolute temperature. Heat a gas → it expands.

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Gay-Lussac's Law

P/T = constant (at constant V). Pressure directly proportional to absolute temperature.

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Avogadro's Law

V ∝ n (at constant T, P). Equal volumes of gases at same T, P contain equal number of molecules.

PV = nRT
Ideal Gas Equation. R = 8.314 J/(mol·K). n = number of moles, T = absolute temperature.

12.4 Kinetic Theory of an Ideal Gas

The kinetic theory derives the pressure of a gas from molecular collisions with the container walls. The key result connects macroscopic quantities (P, T) to microscopic properties (molecular mass and speed):

Kinetic theory of gases
Figure 12.1 — Ideal gas assumptions, pressure derivation, molecular speed distribution, and equipartition of energy
PV = (1/3)Nmv² = nkBT
N = number of molecules, m = mass of one molecule, v = rms speed

Molecular Speeds

From kinetic theory, we get three characteristic speeds:

SpeedFormulaDescription
Most probable (vₚ)√(2kBT/m)Speed at peak of distribution curve
Average (vₐᵥ)√(8kBT/πm)Mean of all molecular speeds
RMS (vᵣₘₛ)√(3kBT/m)Root mean square — relates to KE
⚠️ Temperature is Average KE

The average kinetic energy of a molecule is (1/2)mv²rms = (3/2)kBT. Temperature is a measure of the average translational kinetic energy per molecule. At the same temperature, all gases (monoatomic, diatomic) have the same average translational KE.

12.5 Law of Equipartition of Energy

The law of equipartition of energy states that in thermal equilibrium, the total energy is equally distributed among all the degrees of freedom, with each degree of freedom contributing (1/2)kBT of energy.

U = (f/2)nRT
f = degrees of freedom. Each degree contributes (1/2)kBT per molecule or (1/2)RT per mole.
Molecule TypeDegrees of Freedom (f)Total Energy (U)CᵥCₚγ = Cₚ/Cᵥ
Monoatomic (He, Ne, Ar)3 (trans only)(3/2)nRT(3/2)R(5/2)R5/3 ≈ 1.67
Diatomic (H₂, O₂, N₂)5 (3 trans + 2 rot)(5/2)nRT(5/2)R(7/2)R7/5 = 1.40
Polyatomic (CO₂, CH₄)6 (3 trans + 3 rot)3nRT3R4R4/3 ≈ 1.33

12.6 Specific Heat Capacity

Kinetic theory correctly predicts the specific heat capacities of gases. The molar specific heat at constant volume is:

Cᵥ = (f/2)R
f = degrees of freedom. Cₚ = Cᵥ + R (Mayer's relation). γ = Cₚ/Cᵥ = 1 + 2/f
💡 Why γ > 1?

Since Cₚ > Cᵥ (heat at constant pressure must also do work of expansion), γ = Cₚ/Cᵥ is always greater than 1. For monoatomic gases γ ≈ 1.67, diatomic γ ≈ 1.40, polyatomic γ ≈ 1.33. The more complex the molecule, the lower γ.

⚠️ Degrees of Freedom at High T

At very high temperatures, vibrational modes also get activated, increasing f. For diatomic molecules: f = 7 at high T (adding 2 vibrational DOF). This is why Cₚ and Cᵥ increase with temperature — kinetic theory predicts this correctly!

12.7 Mean Free Path

The mean free path (λ) is the average distance a molecule travels between successive collisions:

λ = 1 / (√2 πd²n)
d = molecular diameter, n = number density (N/V). Typical value at STP: λ ≈ 10⁻⁷ m ≈ 1000 × diameter

At STP, air molecules have a mean free path of about 70 nm, while the molecular diameter is about 0.2 nm. So a molecule travels about 350 times its own size between collisions!

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Why Air is Transparent

Molecules are far apart compared to their size. Light travels through air without hitting molecules because the mean free path for light is much larger than for gas collisions.

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Diffusion

Gas molecules spread by random collisions (mean free path determines diffusion rate). Perfume spreads through a room in minutes because molecules make millions of collisions per second.

💡 Connection to Viscosity

The viscosity of a gas is related to mean free path: η = (1/3)ρvₐᵥλ. This explains why gas viscosity increases with temperature (molecules move faster) while liquid viscosity decreases (molecules have more energy to overcome intermolecular bonds).

Ch 11 — Thermodynamics Ch 13 — Oscillations