Maxwell–Boltzmann distribution

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Script error: No such module "infobox3cols". The Maxwell–Boltzmann distribution is a probability distribution used for describing the speeds of particles in a gas that is in thermal equilibrium. It is named after James Clerk Maxwell and Ludwig Boltzmann. The distribution is applicable to the classical ideal gas, where the particles do not interact with each other except for very brief collisions in which they exchange energy and momentum.

Derivation[edit | edit source]

The Maxwell–Boltzmann distribution can be derived from the principles of statistical mechanics. It describes the distribution of speeds among the molecules of a gas in thermal equilibrium. The probability density function for the speed \( v \) of a particle is given by: \[ f(v) = \left( \frac{m}{2 \pi k_B T} \right)^{3/2} 4 \pi v^2 \exp \left( - \frac{mv^2}{2k_B T} \right) \] where:

Properties[edit | edit source]

The Maxwell–Boltzmann distribution has several important properties:

  • The distribution is skewed to the right, meaning that there are more particles with speeds lower than the most probable speed.
  • The mean speed, median speed, and most probable speed are different.
  • The distribution becomes broader and shifts to higher speeds as the temperature increases.

Applications[edit | edit source]

The Maxwell–Boltzmann distribution is fundamental in the field of kinetic theory of gases. It is used to predict the behavior of gases in various conditions, including:

Related Distributions[edit | edit source]

The Maxwell–Boltzmann distribution is related to other statistical distributions:

See Also[edit | edit source]

References[edit | edit source]

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