The Maxwell-Boltzmann Distribution: Difference between revisions
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===A Mathematical Model=== | ===A Mathematical Model=== | ||
The Maxwell–Boltzmann distribution is the function | |||
:<math> f(v) = \sqrt{\left(\frac{m}{2 \pi kT}\right)^3}\, 4\pi v^2 e^{- \frac{mv^2}{2kT}}, </math> | |||
where <math>m</math> is the particle mass and <math>kT</math> is the product of Boltzmann's constant, <math>k<math>, and thermodynamic temperature, given by <math>T<math>. | |||
===A Computational Model=== | ===A Computational Model=== | ||
Revision as of 15:09, 4 December 2015
Claimed by Sai Srinivas
The Main Idea
State, in your own words, the main idea for this topic
A Mathematical Model
The Maxwell–Boltzmann distribution is the function
- [math]\displaystyle{ f(v) = \sqrt{\left(\frac{m}{2 \pi kT}\right)^3}\, 4\pi v^2 e^{- \frac{mv^2}{2kT}}, }[/math]
where [math]\displaystyle{ m }[/math] is the particle mass and [math]\displaystyle{ kT }[/math] is the product of Boltzmann's constant, <math>k<math>, and thermodynamic temperature, given by <math>T<math>.
A Computational Model
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