Kinetic Theory — Physics Class 11 Notes (CBSE & HBSE)
Free NCERT Physics notes for Kinetic Theory (Class 11) on Siksha Sarovar, aligned to CBSE and Haryana Board (HBSE). This chapter is broken into 3 topics with clear explanations, formulas, solved examples and board-pattern practice — free to read, no sign-up required.
Board exam focus — Kinetic Theory (CBSE & HBSE)
Kinetic Theory explains the macroscopic behaviour of gases from the motion of their molecules. It develops the molecular nature of matter, the ideal gas equation, the derivation of gas pressure from molecular collisions, the kinetic interpretation of temperature and RMS speed, degrees of freedom and the law of equipartition of energy, the resulting specific heats of gases, and the concept of mean free path. CBSE and HBSE focus on the pressure derivation, RMS-speed numericals and equipartition.
Molecular Nature of Matter and the Ideal Gas
Molecular Nature of Matter
Matter is made of molecules in constant random motion. In a gas the molecules are far apart, interact only during brief collisions, and move freely in straight lines between collisions. Avogadro's number $N_A = 6.022 \times 10^{23}\ \text{mol}^{-1}$ gives the number of molecules per mole.
The Ideal Gas Equation
Combining Boyle's law ($PV = \text{const}$ at constant T), Charles' law ($V/T = \text{const}$ at constant P) and Avogadro's law gives:
$$PV = nRT$$
where $n$ is the number of moles and $R = 8.31\ \text{J mol}^{-1}\text{K}^{-1}$ is the universal gas constant. In terms of number of molecules $N$:
$$PV = N k_B T$$
where $k_B = R/N_A = 1.38 \times 10^{-23}\ \text{J/K}$ is Boltzmann's constant.
Assumptions of Kinetic Theory
- Gas molecules are point masses with negligible volume.
- No intermolecular forces except during elastic collisions.
- Collisions are perfectly elastic and of negligible duration.
- Molecular motion is random and obeys Newton's laws.
Trap: A real gas behaves ideally only at low pressure and high temperature, where molecular size and intermolecular forces become negligible.
Pressure of an Ideal Gas and Kinetic Temperature
Pressure from Molecular Motion
By considering elastic collisions of molecules with the walls of a cube, kinetic theory gives the pressure of an ideal gas:
$$P = \frac{1}{3}\frac{m N}{V}\overline{v^2} = \frac{1}{3}\rho\, \overline{v^2}$$
where $\rho$ is the density and $\overline{v^2}$ the mean-square speed. Equivalently, $PV = \tfrac{1}{3} N m \overline{v^2}$.
Kinetic Interpretation of Temperature
Comparing $PV = \tfrac{1}{3}Nm\overline{v^2}$ with $PV = Nk_B T$ gives the average translational kinetic energy per molecule:
$$\frac{1}{2}m\overline{v^2} = \frac{3}{2}k_B T$$
This is a central result: temperature is a measure of the average translational kinetic energy of molecules. It is independent of the type of gas — at the same temperature all gases have the same mean translational KE per molecule.
RMS Speed
The root-mean-square speed is:
$$v_{rms} = \sqrt{\overline{v^2}} = \sqrt{\frac{3k_B T}{m}} = \sqrt{\frac{3RT}{M}}$$
where $M$ is the molar mass. Lighter gases have higher RMS speeds at the same temperature.
| Speed | Expression |
|---|---|
| RMS speed | √(3RT/M) |
| Mean speed | √(8RT/πM) |
| Most probable speed | √(2RT/M) |
Trap: $v_{rms} > \bar{v} > v_{mp}$ always (ratio √3 : √(8/π) : √2 ≈ 1.73 : 1.60 : 1.41).
Degrees of Freedom, Equipartition and Mean Free Path
Degrees of Freedom
The degrees of freedom (f) of a molecule is the number of independent ways it can store energy.
| Gas type | Translational | Rotational | Total f (low T) |
|---|---|---|---|
| Monatomic | 3 | 0 | 3 |
| Diatomic | 3 | 2 | 5 |
| Triatomic (non-linear) | 3 | 3 | 6 |
Law of Equipartition of Energy
In thermal equilibrium, the total energy is shared equally among all active degrees of freedom, each contributing $\tfrac{1}{2}k_B T$ per molecule:
$$U = \frac{f}{2}k_B T \ \text{(per molecule)} = \frac{f}{2}RT \ \text{(per mole)}$$
Specific Heats of Gases
From $U = \tfrac{f}{2}RT$ per mole:
$$C_V = \frac{f}{2}R, \quad C_P = C_V + R = \left(\frac{f}{2}+1\right)R, \quad \gamma = \frac{C_P}{C_V} = 1 + \frac{2}{f}$$
| Gas | C_V | C_P | γ |
|---|---|---|---|
| Monatomic (f=3) | (3/2)R | (5/2)R | 1.67 |
| Diatomic (f=5) | (5/2)R | (7/2)R | 1.40 |
| Triatomic (f=6) | 3R | 4R | 1.33 |
Mean Free Path
The mean free path $\lambda$ is the average distance a molecule travels between successive collisions:
$$\lambda = \frac{1}{\sqrt{2}\,\pi d^2 n}$$
where $d$ is the molecular diameter and $n = N/V$ the number density. The mean free path increases with temperature (at constant volume) and decreases with pressure/density.
Trap: λ is inversely proportional to number density, hence inversely proportional to pressure at constant temperature.
Frequently asked questions
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Do these notes follow CBSE and HBSE?
Yes. The Kinetic Theory notes are NCERT-aligned and include guidance for both CBSE and Haryana Board (HBSE), with important questions and MCQs for revision.
What does the Kinetic Theory chapter cover?
Concept explanations, key formulas and definitions, fully solved examples and board-pattern practice questions for Kinetic Theory.