Monty Hall
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I'm reading http://www.ndsu.edu/fileadmin/physics.ndsu.edu/Wagner/LBbook.pdf (pg 12, 3.2.2) about the lattice Boltzmann method. I'm speaking of his specfic form of the Maxwell-Boltzmann and his claim that the integral of equilibrium distribution is equal to n
\int f^0 = n
f^0(v)=\frac{n}{(2\pi\theta)^{3/2}}e^{-(v-u)^2/2\theta}
But when I use gaussian integrals I don't get n but rather \frac{n}{2\pi\theta}. What am I missing?
\int f^0 = n
f^0(v)=\frac{n}{(2\pi\theta)^{3/2}}e^{-(v-u)^2/2\theta}
But when I use gaussian integrals I don't get n but rather \frac{n}{2\pi\theta}. What am I missing?