Is the Poisseuille flow of the previous question an
incompressible flow? Derive the principal strain rates and the
principal strain directions as a function of the radial position.
For the Poisseuille flow of the previous question, draw a thin
ring of fluid of radius at a time and a slightly
later time . Assume the ring has a square cross section
at time . Next in the cross section, using very neat
drawings show graphically that the motion of the ring cross section
consists of two uni-axial strainings plus a solid-body rotation.
If the surface temperature of a river is given by
and the surface water flows with a speed
, then
what is assuming that the water particles stay at the same
temperature? (Hint:
if the water particles
stay at the same temperature.)
A boat is cornering through this river such that its position is
given by , . What is the rate of change
of the water temperature experienced by the boat
in terms of the functions and ?
Write the velocity derivative tensor for ideal stagnation point
flow. (With the velocity field as discussed in class.) From this
tensor, decide whether or not ideal stagnation point flow is an
incompressible flow. Find the strain rate tensor. Diagonalize it.
What are the principal strain rates? What are the principal strain
axes (i.e. the directions of
,
, and )?
Neatly sketch the deformation of an initially square particle
(aligned with the principal strain axes), during a small time
interval. Also sketch the deformation of an initially circular
particle.