
The motion of point P' relative to neighboring point P is
given by
.
![]()
Take the velocity derivatives tensor A apart into symmetric and antisymmetric parts:
![]()
The symmetric part is called the strain-rate tensor. By rotating the coordinate system, to x',y',z', it becomes diagonal:

The trace of the tensor is the rate of (volume) expansion of the fluid.
The asymmetric part corresponds to solid body motion:

Vorticity is important: when there are no viscous effects, no vorticity will be generated.
The line integral of the velocity along a closed contour is called the
circulation
of that contour:
![]()
Exercise:
What can you say aboutif
?
Questions: 4.2, 5, 7, 8, 9.