3. The velocity profile for laminar flow between two plates, as in Fig.3, is 2umaxy(h-y) h² v=w=0 W If the wall temperature is Tw at both walls, use the incompressible flow energy equation to solve for the temperature distribution T (y) between the walls for steady flow. Energy equation: y=h y=0 U= AY pcp dT dt u(y) = kV²T +9 Tw T(y) X

Elements Of Electromagnetics
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Author:Sadiku, Matthew N. O.
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3. The velocity profile for laminar flow between two plates, as in Fig.3, is
2umaxy(h - y)
h2
v=W=0
W
If the wall temperature is Tw at both walls, use the incompressible flow energy equation to
solve for the temperature distribution T (y) between the walls for steady flow.
Energy equation:
y=h
y=0
U =
AY
pcp
dT
dt
u(y)
: kV²T +4
Tw
W
T(y)
Fig.3. Fluid flow between two walls
X
Transcribed Image Text:3. The velocity profile for laminar flow between two plates, as in Fig.3, is 2umaxy(h - y) h2 v=W=0 W If the wall temperature is Tw at both walls, use the incompressible flow energy equation to solve for the temperature distribution T (y) between the walls for steady flow. Energy equation: y=h y=0 U = AY pcp dT dt u(y) : kV²T +4 Tw W T(y) Fig.3. Fluid flow between two walls X
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