The radial velocity component in an incompressible, two- dimensional flow field (v, = 0) is 5- %3D v, = 2r + 31² sin 0 Determine the corresponding tangential velocity component, vg, required to satisfy conservation of mass.

Elements Of Electromagnetics
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• Y:EA
09B/s
* etisalat
sheet 2.pdf
->
The radial velocity component in an incompressible, two-
dimensional flow field (v, = 0) is
5-
v, = 2r + 31² sin 0
Determine the corresponding tangential velocity component, vg,
required to satisfy conservation of mass.
If the velocity field is given by V = axri – ayj, and a is a con-
stant, find the circulation around the closed curve shown in Fig. 2 .
6-
(1, 2)
(2, 2)
(1, 1)
(2, 1)
Fig. 2
Damietta University
Faculty of Engineering
Mechanical Engineering Department
Fluid Mechanics II
7-
For a steady, two-dimensional, incompressible flow, the ve-
locity is given by V = (ax – cy)i + (-ay + cx)j, where a and c
are constants. Show that this flow can be considered inviscid.
Determine the shearing stress for an incompressible Newtonian
31
8-
Transcribed Image Text:• Y:EA 09B/s * etisalat sheet 2.pdf -> The radial velocity component in an incompressible, two- dimensional flow field (v, = 0) is 5- v, = 2r + 31² sin 0 Determine the corresponding tangential velocity component, vg, required to satisfy conservation of mass. If the velocity field is given by V = axri – ayj, and a is a con- stant, find the circulation around the closed curve shown in Fig. 2 . 6- (1, 2) (2, 2) (1, 1) (2, 1) Fig. 2 Damietta University Faculty of Engineering Mechanical Engineering Department Fluid Mechanics II 7- For a steady, two-dimensional, incompressible flow, the ve- locity is given by V = (ax – cy)i + (-ay + cx)j, where a and c are constants. Show that this flow can be considered inviscid. Determine the shearing stress for an incompressible Newtonian 31 8-
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