3- Consider the flow of fluid between two large parallel isothermal plates separated by a distance L. The upper plate is moving at a constant velocity of V and maintained at temperature T, .The lower plate is stationary and a constant heat flux (q") is being applied from lower plate to fluid. By simplifying and solving the continuity, momentum and energy equations, obtain relations for temperature and velocity of fluid according to location. (Frictional heating due to viscous dissipation is negligible.) To Fluid

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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3- Consider the flow of fluid between two large parallel
isothermal plates separated by a distance L. The upper plate is
moving at a constant velocity of V and maintained at
temperature T, .The lower plate is stationary and a constant
heat flux ( q") is being applied from lower plate to fluid. By
simplifying and solving the continuity, momentum and energy
equations, obtain relations for temperature and velocity of
fluid according to location. (Frictional heating due to viscous
dissipation is negligible.)
To
L
Fluid
q"
Transcribed Image Text:3- Consider the flow of fluid between two large parallel isothermal plates separated by a distance L. The upper plate is moving at a constant velocity of V and maintained at temperature T, .The lower plate is stationary and a constant heat flux ( q") is being applied from lower plate to fluid. By simplifying and solving the continuity, momentum and energy equations, obtain relations for temperature and velocity of fluid according to location. (Frictional heating due to viscous dissipation is negligible.) To L Fluid q"
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