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Boltzmann Collision Integral


The Boltzmann collision integral, also called the Boltzmann collision operator, gives the change caused by binary elastic collisions in a nonnegative function f(v) that describes particle density over velocity space. For particles of equal mass, one common form is

 Q(f,f)(v)=int_(R^3)int_(S^2)B(v-v_*,omega)[f(v^')f(v_*^')-f(v)f(v_*)]domegad^3v_*.

Here omega lies on the unit sphere, and the pairs of velocities (v,v_*) and (v^',v_*^') are related by v^'=1/2(v+v_*)+1/2|v-v_*|omega and v_*^'=1/2(v+v_*)-1/2|v-v_*|omega. The nonnegative function B weights collisions according to their relative velocity and scattering direction. The first product in the integrand accounts for particles entering velocity v, while the second product accounts for particles leaving it.


See also

Function, Integral, Integrand, Unit Sphere, Velocity

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References

Cercignani, C.; Illner, R.; and Pulvirenti, M. The Mathematical Theory of Dilute Gases. New York: Springer-Verlag, 1994. https://doi.org/10.1007/978-1-4419-8524-8.

Cite this as:

Weisstein, Eric W. "Boltzmann Collision Integral." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/BoltzmannCollisionIntegral.html

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