ABSTRACT
For compressible viscous fluid motion equations:
ρ ρ
ρ ρ
du dt
F p x
p y
p z
dv dt
F p x
p y
p
= + ∂ ∂
+ ∂ ∂
+ ∂ ∂
= + ∂ ∂
+ ∂ ∂
+ ∂ zy
z dw dt
F p x
p y
p z
∂ +
∂ ∂
+ ∂ ∂
+ ∂ ∂
⎧
⎨
⎪⎪⎪
⎩
⎪⎪⎪ρ ρ=
F F Fbx by bz, , are on the unit mass of fluid mass force component in three directions; pyx is flow of the body stress tensor components [1].
