Question Details

Consider steady, viscous, fully developed flow of a fluid through a circular pipe of internal diameter D. We know that the velocity profile forms a paraboloid about the pipe centre line, given by :  V = C ( r 2 D 2 4 ) m/s, where C is a constant. The rate of kinetic energy (in J/s) at the control surface A-B, as shown in the figure, is proportional to Dn. The value of n is ________.

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Correct Answer :

Correct answer is : 8

K . E = o R 1 2 ( ρ v 2 π r . d r ) v 2 = o R 1 2 ρ v 3 2 π r . d r

K . E = o R 1 2 ρ 2 π r . [ C ( r 2 D 2 4 ) ] 3 d r

v = C ( r 2 D 2 4 ) = C ( r 2 R 2 ) = C ( R 2 r 2 )

K . E = o R ρ π r [ C ( R 2 r 2 ) ] 3 d r

K . E = o R ρ π C 3 R 6 [ ( 1 r 2 R 2 ) ] 3 r d r

Now,

∵ (a - b)3 = a3 – b3 – 3ab (a - b)

K . E = ρ π C 3 R 6 o R ( 1 r 2 R 2 ) 3 r d r

K . E = ρ C 3 π R 6 0 R [ 1 r 6 R 6 3 r 2 R 2 ( 1 r 2 R 2 ) ] r d r

K . E = ρ C 3 π R 6 0 R [ r r 7 R 6 3 r 3 R 2 ( 1 r 2 R 2 ) ] d r

K . E = ρ C 3 π R 6 [ r 2 2 r 8 8 R 6 3 R 2 r 4 4 + 3 R 4 r 6 6 ] 0 R

K . E = ρ C 3 π R 6 [ R 2 2 R 2 8 3 4 R 2 + 1 2 R 2 0 ]

K . E = ρ C 3 π R 6 [ 4 R 2 R 2 6 R 2 + 4 R 2 8 ] = ρ C 3 π R 6 R 2 8 = ρ C 3 π 8 R 8

K . E = ρ C 3 π 8 D 8 256

Solution :

The correct answer is 8.

Problem Analysis:
We are given a steady, viscous, fully developed flow of a fluid through a circular pipe of internal diameter D (and radius R = D/2). The velocity profile in terms of radial coordinate r is parabolic and given by:

V = - C ( r 2 - D 2 4 )

where C is a constant. We need to find the power index n such that the rate of kinetic energy (kinetic energy flux) crossing the control surface A-B shown in the figure is proportional to Dn.

Step 1: Express velocity V in terms of radius R
Since the pipe radius is R = D 2 , we can write:

R 2 = D 2 4

Substituting this into the velocity profile:

V = - C ( r 2 - R 2 ) = C ( R 2 - r 2 )

Step 2: Formulate the rate of kinetic energy (kinetic energy flux)
Consider an elemental circular ring of radius r and thickness dr on the cross-section A-B. The area of this elemental ring is:

d A = 2 π r d r

The mass flow rate through this ring is:

d m ˙ = ρ V d A = ρ V ( 2 π r d r )

The rate of kinetic energy (K.E.) associated with this mass flow is:

d ( K . E . ) = 1 2 d m ˙ V 2 = 1 2 ( ρ V 2 π r d r ) V 2 = ρ π V 3 r d r

Step 3: Integrate over the entire pipe cross-section
Integrating from r = 0 to r = R:

K . E . = 0 R ρ π V 3 r d r

Substituting the expression for V:

K . E . = 0 R ρ π [ C ( R 2 - r 2 ) ] 3 r d r


K . E . = �� π C 3 0 R ( R 2 - r 2 ) 3 r d r

Step 4: Solve the integral
Using u-substitution, let:

u = R 2 - r 2

Then:

d u = - 2 r d r r d r = - d u 2

Changing the limits of integration:
When r = 0, u = R2.
When r = R, u = 0.
Substituting these into the integral:

K . E . = ρ π C 3 R 2 0 u 3 ( - d u 2 )

Using the minus sign to flip the integration limits:

K . E . = 1 2 ρ π C 3 0 R 2 u 3 d u


K . E . = 1 2 ρ π C 3 [ u 4 4 ] 0 R 2 = 1 2 ρ π C 3 ( R 8 4 ) = ρ π C 3 8 R 8

Step 5: Determine proportionality in terms of D
Substituting R = D 2 :

K . E . = ρ π C 3 8 ( D 2 ) 8 = ρ π C 3 2048 D 8

This clearly shows that:

K . E . D 8

Comparing this to the given relation Dn, we find:

n = 8

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  • GATE
  • intermediate
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  • mechanical engineering

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