In a fluid, stresses are essentially due to hydrostatic pressure p. The mechanical tension T exerted on each surface element is almost normal to it. A deviation from this law occurs with viscosity, which creates tangential stresses τ
ij
. To separate the two effects, let's take the stress tensor as :
T
ij
= – pδ
ij
+ τ
ij
( 1 )
with δ
ij
Kronecker symbol.
The viscous stresses τ
ij
lead to the dissipation of part of the mechanical energy. The evolution...
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