Kinetic Theory | Fluid Mechanics |
N: Liouville equation for N particles |
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N ‒ 1: Liouville equation for N ‒ 1 particles |
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N ‒ 2: Liouville equation for N ‒ 2 particles |
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3: Liouville equation for N = 3 particles |
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2:D2(f2) = J2(f3) | ⇒ |
with tertiary molecular chaos (Tsugé equation) | with (Kármán-Howarth equation) |
1:D(f) = J(f2) where D denotes differential operator, and J is the collision integral operator. | ⇒ (Reynolds averaged Navier-Stokes equation) |