The stress components consist of pressure and friction terms. We
write
(4.49)
where T
U
denotes the viscous components. Later, we shall include
additional dissipative terms due to turbulence in
τ
0
·.
The momentum
equations are now
(4.50)
with
If the τ
0
· terms are neglected, the fluid is said to be frictionless or
inviscid.
For this case,
(4.51)
and the stress transformation relations reduce to
(4.52)
According to (4.52), an inviscid fluid cannot resist a tangential
boundary surface force, i.e. one can apply only a norma ...
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