Q.Derive the expression of pressure exerted by the gas on the walls of the container.
Concept understanding — Kinetic Theory Explanation
Kinetic Theory Explanation
Imagine you're sitting in a quiet room. The air around you feels still, but it isn't. Every second, billions of tiny particles — molecules of nitrogen and oxygen — are zipping past you at hundreds of metres per second. You don't feel them because they're too small, and they're moving in every direction at once. But if you put your hand near a hot stove, you suddenly feel heat. Why?
The answer is the kinetic theory of matter. It's a way of explaining what we observe at the human scale (temperature, pressure, heat) by thinking about what's happening at the molecular scale.
The core idea
The kinetic theory says three simple things:
- All matter is made of tiny particles (atoms or molecules) that are in constant, random motion.
- The particles collide with each other and with the walls of their container — these collisions are perfectly elastic (no energy is lost).
- The average kinetic energy of these particles is directly proportional to the temperature of the substance.
That's it. Everything else — pressure, diffusion, the way a gas expands when heated — follows from these three statements.
Building intuition
Think of a single gas molecule bouncing around inside a box. It hits a wall, bounces off, and keeps going. Each time it hits the wall, it exerts a tiny force. Now multiply that by billions of molecules hitting every square centimetre of wall every second. That constant, collective force is what we measure as pressure.
Now heat the box. The molecules move faster — their average kinetic energy increases. They hit the walls harder and more often. Pressure goes up. If the walls can move (like a piston), the gas expands until the pressure inside equals the pressure outside.
This is why a bicycle tyre feels hot after you pump it: you're doing work on the air, compressing it, which increases the average kinetic energy of the molecules — and that's exactly what temperature is.
Temperature is not the total kinetic energy of all molecules — it's the average kinetic energy per molecule. A large cold object can have more total energy than a small hot one, but its molecules move slower on average.
The precise statement
For an ideal gas (a gas where intermolecular forces are negligible and collisions are perfectly elastic), the kinetic theory gives us a direct mathematical link:
Average kinetic energy per molecule=23kBT
where kB is Boltzmann's constant (1.38×10−23J/K) and T is the absolute temperature in Kelvin.
This means that at the same temperature, all gas molecules — regardless of their mass — have the same average kinetic energy. A light hydrogen molecule moves faster than a heavy oxygen molecule at the same temperature, but their average kinetic energies are equal.
From this, we can derive the ideal gas law:
PV=31Nmv2=NkBT
where P is pressure, V is volume, N is the number of molecules, m is the mass of one molecule, and v2 is the mean square speed.
PV=nRT
This is the familiar ideal gas law. The kinetic theory shows it's not just an empirical rule — it follows directly from the motion of molecules.
What the theory explains
The kinetic theory isn't just abstract. It explains everyday phenomena:
- Evaporation cools you: The fastest molecules escape from a liquid surface, leaving behind slower ones. The average kinetic energy drops — so the temperature drops.
- Diffusion: Molecules spread out because they're constantly moving and colliding, gradually mixing with neighbouring molecules.
- Brownian motion: Pollen grains jitter under a microscope because they're being bombarded unevenly by invisible water molecules.
- Why gases are compressible but liquids aren't: In a gas, molecules are far apart with lots of empty space. In a liquid, they're already touching.
A common mistake is to think that all molecules in a gas move at the same speed. They don't — there's a distribution of speeds (the Maxwell-Boltzmann distribution). Some are slow, some are very fast, but most are near the average. Temperature changes the shape of this distribution, not just the average.
The limits
The kinetic theory as described works perfectly for ideal gases. Real gases deviate at high pressures (molecules get close enough for forces to matter) and low temperatures (molecules slow down enough for attractions to become significant). But even then, the theory gives us a starting point — we add corrections (like van der Waals equation) to account for real behaviour.
For solids and liquids, the same basic idea applies — particles vibrate about fixed positions (solids) or slide past each other (liquids) — but the mathematics becomes more complex because the particles are never far apart.
The takeaway
The kinetic theory is a bridge between the microscopic world we can't see and the macroscopic world we experience. It tells us that heat is motion, pressure is collisions, and temperature is average energy. Once you internalise that, a huge chunk of physics and chemistry becomes intuitive.
Many students find this page while searching "Kinetic Theory Explanation formula physics" or "Kinetic Theory Explanation important questions and answers"; the concept sits firmly within the Class 11 Physics NCERT/CBSE syllabus. It's also a frequent building block for numericals in JEE Main, NEET and state engineering/medical entrance exams, so treating it as a one-time memorisation task rather than an understood idea tends to backfire later.
Tracking the momentum an elastically-colliding molecule transfers to a wall, and counting how many molecules hit it per unit time, gives P=31nmv2.
P=31VNmv2, derived in full below.
Step 1. Consider N molecules of mass m in a cubical container of side l. A molecule with velocity components (vx,vy,vz) strikes the right-hand wall; since the collision is elastic, it rebounds with −vx while vy,vz stay unchanged.
Step 2. The molecule's momentum change is −2mvx, so by conservation of momentum the wall gains momentum 2mvx per collision.
Step 3. In time Δt, only molecules within a slab of volume AvxΔt next to the wall, moving toward it, can strike it; with random motion, half of these are moving the right way, giving 2nAvxΔt collisions in time Δt (n = number density).
Step 4. Total momentum transferred: Δp=2nAvxΔt×2mvx=Anmvx2Δt.
Step 5. Force: F=Δp/Δt=nmAvx2; pressure: P=F/A=nmvx2.
Step 6. Averaging over all molecules and using isotropy (vx2=31v2, since v2=vx2+vy2+vz2=3vx2) gives the final result P=31nmv2=31VNmv2.
Step 7. Although a cubical container was used purely for calculational convenience, the wall area cancels out of the final formula, so the result holds for a container of any shape.
P=31VNmv2.
Derive the momentum transferred per collision, count collisions per unit time on a wall, and average over all molecules using isotropy.
- Forgetting the factor of 1/2 in the collision count (only half the molecules in the slab move toward the wall).
- Skipping the isotropy step that replaces v_x-squared with (1/3) of the mean square speed.
- CBSE 2026Set ANNUAL1 markMCQQ.The potential energy of an ideal gas is(a) (3/2)kB T(b) (2/3)kB T(c) zero(d) 3kB T
›Reveal solutionSolution
Ideal-gas molecules have no mutual forces, so their potential energy is zero. Answer (C).
The ideal-gas model assumes point molecules with no forces between them except during instantaneous elastic collisions. With no intermolecular forces, there is no potential energy of interaction; all the internal energy of an ideal gas is kinetic. Hence the potential energy is taken as zero.
✓Final answer(C) zero.
- CBSE 2023Set ANNUAL1 markQ.State the law of equipartition of energy for a gas system.
›Reveal solutionSolution
Each degree of freedom of a gas molecule contributes an average energy of (1/2) kB T, in thermal equilibrium.
A gas molecule can store energy in different independent 'ways' of moving — translational motion along the x, y, z axes, rotation about different axes, and vibration of bonds. Each such independent way a molecule can possess energy is called a degree of freedom.
The law of equipartition of energy states that for a system in thermal equilibrium at absolute temperature T, the total internal energy is distributed EQUALLY among all its degrees of freedom, and each degree of freedom (each quadratic term in the energy expression, e.g. (1/2)mv_x^2) contributes on average an energy of (1/2) kB T per molecule, where kB is Boltzmann's constant.
For example, a monatomic gas molecule has 3 translational degrees of freedom (motion along x, y, z), so its average energy is 3 x (1/2) kB T = (3/2) kB T. A diatomic gas molecule (like N2 or O2) additionally has 2 rotational degrees of freedom (about the two axes perpendicular to the bond axis), giving 5 x (1/2) kB T = (5/2) kB T at moderate temperatures (vibrational modes become significant only at higher temperatures).
✓Final answerThe law of equipartition of energy: in thermal equilibrium, the total energy of a gas system is shared equally among all its degrees of freedom, each contributing an average (1/2) kB T of energy per molecule.
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