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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.

SpeedExpression
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 typeTranslationalRotationalTotal f (low T)
Monatomic303
Diatomic325
Triatomic (non-linear)336

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:

$$C_V = \frac{f}{2}R, \quad C_P = C_V + R = \left(\frac{f}{2}+1\right)R, \quad \gamma = \frac{C_P}{C_V} = 1 + \frac{2}{f}$$

GasC_VC_Pγ
Monatomic (f=3)(3/2)R(5/2)R1.67
Diatomic (f=5)(5/2)R(7/2)R1.40
Triatomic (f=6)3R4R1.33

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

Are these Kinetic Theory notes free?

Yes — the Kinetic Theory notes for Physics (Class 11) on Siksha Sarovar are completely free to read, with no account required.

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.