a) Why doesn’t the surface roughness affect the pressure drop in a laminar pipe flow?  b) For bluff bodies, the drag coefficient decreases abruptly when the flow becomes turbulent. Why?  c) Consider a spinning ball (in the clockwise direction) moving with a velocity U. Explain how the lift force is formed on the ball and show its direction.  U w d) For flow over streamlined bodies, drag force usually increases when the flow becomes turbulent.Why?

Elements Of Electromagnetics
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Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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Explain briefly in your own words (parts a-d)
a) Why doesn’t the surface roughness affect the pressure drop in a laminar pipe flow? 
b) For bluff bodies, the drag coefficient decreases abruptly when the flow becomes turbulent. Why? 
c) Consider a spinning ball (in the clockwise direction) moving with a velocity U. Explain how the lift force is formed on the ball and show its direction. 
U
w
d) For flow over streamlined bodies, drag force usually increases when the flow becomes turbulent.Why? 
e) Consider a pipe with a radius R and length L (extending from (1) to (2)). Inside the pipe there is a solid cylinder with a radius k×R (k  1). The planes (1) and (2), separated by a distance L have pressures P1 and P2 respectively, with P1 > P2. At t = 0, the inner solid cylinder suddenly begins to be pulled at a constant speed U in the negative z direction. The
fluid is an incompressible Newtonian liquid with dynamic viscosity μ and density ρ. In order
to find the solution for the velocity field in the annular region between the pipe wall and the solid cylinder starting from t = 0, we must simplify the z-component of the Navier-Stokes equations which is given below the figure

 

Simply the z-component of the Navier-Stokes equation based on the description of the flow.
For each term you are dropping out, write down the corresponding reason

Explain briefly in your own words (parts a-d)
a) Why doesn't the surface roughness affect the pressure drop in a laminar pipe flow?
b) For bluff bodies, the drag coefficient decreases abruptly when the flow becomes
turbulent. Why?
c) Consider a spinning ball (in the clockwise direction) moving with a velocity U. Explain how the
lift force is formed on the ball and show its direction.
d) For flow over streamlined bodies, drag force usually increases when the flow becomes turbulent.
Why?
e) Consider a pipe with a radius R and length L (extending from (1) to (2)). Inside the pipe
there is a solid eylinder with a radius k*R (k < 1). The planes (1) and (2), separated by a
distance L have pressures P, and P: respectively, with P, > P:. At t = 0, the inner solid
cylinder suddenly begins to be pulled at a constant speed U in the negative z direction. The
fluid is an incompressible Newtonian liquid with dynamic viscosity u and density p. In order
to find the solution for the velocity field in the annular region between the pipe wall and the
solid cylinder starting from t= 0, we must simplify the z-component of the Navier-Stokes
equations which is given below the figure.
nner oyinder speed U
Radus
Perspective View
Radus
End View
Direction of gravity
1 'n, o'n,
P8.
Simply the z-component of the Navier-Stokes equation based on the description of the flow.
For each term you are dropping out, write down the corresponding reason
Transcribed Image Text:Explain briefly in your own words (parts a-d) a) Why doesn't the surface roughness affect the pressure drop in a laminar pipe flow? b) For bluff bodies, the drag coefficient decreases abruptly when the flow becomes turbulent. Why? c) Consider a spinning ball (in the clockwise direction) moving with a velocity U. Explain how the lift force is formed on the ball and show its direction. d) For flow over streamlined bodies, drag force usually increases when the flow becomes turbulent. Why? e) Consider a pipe with a radius R and length L (extending from (1) to (2)). Inside the pipe there is a solid eylinder with a radius k*R (k < 1). The planes (1) and (2), separated by a distance L have pressures P, and P: respectively, with P, > P:. At t = 0, the inner solid cylinder suddenly begins to be pulled at a constant speed U in the negative z direction. The fluid is an incompressible Newtonian liquid with dynamic viscosity u and density p. In order to find the solution for the velocity field in the annular region between the pipe wall and the solid cylinder starting from t= 0, we must simplify the z-component of the Navier-Stokes equations which is given below the figure. nner oyinder speed U Radus Perspective View Radus End View Direction of gravity 1 'n, o'n, P8. Simply the z-component of the Navier-Stokes equation based on the description of the flow. For each term you are dropping out, write down the corresponding reason
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