Physics:Bhatnagar–Gross–Krook operator
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Short description: Collision operator used in a computational fluid dynamics technique
The Bhatnagar–Gross–Krook operator (abbreviated BGK operator) term refers to a collision operator used in the Boltzmann equation and in the lattice Boltzmann method, a computational fluid dynamics technique. It is given by the following formula:
- [math]\displaystyle{ \Omega_i=-\tau^{-1}(n_i-n_i^{EQ}) }[/math]
where [math]\displaystyle{ n_i^{EQ} }[/math] is a local equilibrium value for the population of particles in the direction of link [math]\displaystyle{ \mathbf{e}_i }[/math] The term [math]\displaystyle{ \tau }[/math] is a relaxation time, and related to the viscosity.
The operator is named after Prabhu L. Bhatnagar, Eugene P. Gross, and Max Krook, the three scientists who introduced it in a paper in Physical Review in 1954.[1]
References
- ↑ P.L. Bhatnagar; E.P. Gross; M. Krook (1954). "A Model for Collision Processes in Gases. I. Small Amplitude Processes in Charged and Neutral One-Component Systems". Physical Review 94 (3): 511–525. doi:10.1103/PhysRev.94.511. Bibcode: 1954PhRv...94..511B.
- S. Succi (2001). The Lattice Boltzmann Equation for Fluid Dynamics and Beyond. Oxford University Press. ISBN 978-0-19-850398-9.
Original source: https://en.wikipedia.org/wiki/Bhatnagar–Gross–Krook operator.
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