1. In Class, we used a small differential volume to derive the expression for momentum thickness. Here, use a control volume approach, as shown in the figure, to derive the definition of momentum thickness, 0, for flow over a flat plate. zero shear stress, constant pressure, no through flow no slip. 0
1. In Class, we used a small differential volume to derive the expression for momentum thickness. Here, use a control volume approach, as shown in the figure, to derive the definition of momentum thickness, 0, for flow over a flat plate. zero shear stress, constant pressure, no through flow no slip. 0
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
Section: Chapter Questions
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![1. In Class, we used a small differential volume to derive the expression for momentum
thickness. Here, use a control volume approach, as shown in the figure, to derive the
definition of momentum thickness, 0, for flow over a flat plate.
zero shear stress,
constant pressure, no through flow
h> 8
no slip, ,#0](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Faaa88a78-d11f-43ae-a848-05bc2c561a23%2Fac667f70-2897-4b97-ac48-fa4fae181ffd%2Fs0ylx9l_processed.jpeg&w=3840&q=75)
Transcribed Image Text:1. In Class, we used a small differential volume to derive the expression for momentum
thickness. Here, use a control volume approach, as shown in the figure, to derive the
definition of momentum thickness, 0, for flow over a flat plate.
zero shear stress,
constant pressure, no through flow
h> 8
no slip, ,#0
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