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Maxwell–Boltzmann distribution

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Distribution of molecular speeds.

Key relationf(v) ∝ v²e^{−mv²/2kT}

The fraction of molecules with speed v is f(v) ∝ v²e^{−mv²/2kT}: few slow, few very fast, with a peak and a long tail. Higher T broadens and shifts the peak.

Worked example

The tail explains evaporation and chemical reaction rates.

Common mistake

It describes speeds of a large sample in equilibrium.

In more detail

The Maxwell-Boltzmann distribution gives the fraction of molecules with each speed in a gas at a given temperature. Molecules have a range of speeds, not a single value.

Real-world uses

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Frequently asked questions

Why does the distribution have a tail?

A few molecules move much faster than average because of random collisions.

How does temperature change it?

Higher temperature widens the distribution and shifts it to higher speeds.

Are all molecules moving at the same speed?

No. They have a wide range of speeds, and the distribution describes how many have each speed at a given temperature.

Related topics in Kinetic Theory & Statistical Physics

Degrees of freedom · Equipartition theorem · Specific heats of gases · Most probable speed · Average, rms and most probable speeds · Law of atmospheres

← All Kinetic Theory & Statistical Physics topics