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orestis.malaspin
lattice-boltzmann
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2366fd59
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2366fd59
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1 year ago
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orestis.malaspin
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added banner and started hermite expansion
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lattice-boltzmann.com/content/2-hermite-expansion.md
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lattice-boltzmann.com/content/2-hermite-expansion.md
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lattice-boltzmann.com/content/2-hermite-expansion.md
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title = "Polynomial expansion of the BGK equation"
description = "A possible polynomial expansion of the BGK equation"
date = 2024-03-14
weight = 2
slug = "hermite"
draft = true
[taxonomies]
tags = ["LBM", "Hermite", "Expansion"]
[extra]
math = true
math_auto_render = true
toc = true
+++
## Macroscopic quantities
In the
[
preceding chapter
](
../dimensionless
)
we introduced the density distribution function $f$ and its
non-dimensional counterpart $f^
\a
st$. From now on, we will assume that all quantities are without dimensions
and omit the $^
\a
st$. Apart from making the dimensional analysis of the Navier--Stokes and the Boltzmann equation
we never discussed the actual link between the quantities present in each equation. It will be the aim of this
section. Actually macroscopic quantities are related to moments of $f$ as
$$
\b
egin{align}
\r
ho(
\b
m{x}, t)&=
\i
nt_{-
\i
nfty}^
\i
nfty f(
\b
m{x},
\b
m{
\x
i}, t)
\m
athrm{d}
\b
m{
\x
i},
\\\\
\r
ho(
\b
m{x}, t)
\b
m{u}(
\b
m{x}, t)&=
\i
nt_{-
\i
nfty}^
\i
nfty f(
\b
m{x},
\b
m{
\x
i}, t)
\b
m{
\x
i}
\m
athrm{d}
\b
m{
\x
i},
\e
nd{align}
$$
where the density, $
\r
ho$, and the momentum $
\r
ho
\b
m{u}$ are the zeroth and first order moment of $f$.
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