SAME FLUID 4. SAME FLUID FLOW PATTERN SELECT THE CORRECT ANSWER USI...

3. Same fluid

4. Same fluid flow pattern

Select the correct answer using the code given below:

(a) 1 only

(b) 1 and 2

(c) 3 and 4

(d) 4 only

IES-28. The average Nusselt number in laminar natural convection from a

vertical wall at 180°C with still air at 20°C is found to be 48. If the wall

temperature becomes 30°C, all other parameters remaining same, the

average Nusselt number will be:

[IES-2002]

(a) 8

(b) 16

(c) 24

(d) 32

IES-29. For fully-developed turbulent flow in a pipe with heating, the Nusselt

number N

u

, varies with Reynolds number R

e

and Prandtl number P

r

as

[IES-2003]

(a)

R P

e

0.5

r

1

3

(b)

R P

e

0.8

r

0.2

(c)

R P

e

0.8

r

0.4

(d)

R P

e

0.8

r

0.3

IES-30. For laminar flow over a flat plate, the local heat transfer coefficient 'h

x

'

varies as x

-1/2

, where x is the distance from the leading edge (x = 0) of

the plate. The ratio of the average coefficient 'h

a

' between the leading

Page 46 of 97

edge and some location 'A' at x = x on the plate to the local heat transfer

coefficient 'h

x

' at A is:

[IES-1999]

(a) 1

(b) 2

(c) 4

(d) 8

IES-31. When there is a flow of fluid over a flat plate of length 'L', the average

heat transfer coefficient is given by (Nu

x

= Local Nusselt number; other

symbols have the usual meaning)

[IES-1997]

L

k

Nu dx

1

L

(b)

dx

d

( )

h

x

(c)

(a)

x

h dx

x

L

L

(d)

0

IES-32. In the case of turbulent flow through a horizontal isothermal cylinder

of diameter 'D', free convection heat transfer coefficient from the

cylinder will:

[IES-1997]

(a) Be independent of diameter

(b) Vary as D

3/4

(c)

Vary

as

D

1/4

(d) Vary as D

1/2

IES-33. Match List-I (Dimensionless quantity) with List-II (Application) and

select the correct answer using the codes given below the lists:

List-I

List-II

[IES-1993]

A. Stanton number

1. Natural convection for ideal gases

B. Grashof number

2. Mass transfer

C. Peclet number

3. Forced convection

D.

Schmidt number

4.

Forced convection for small

Prandtl number

Codes: A

B

C

D

A

B

C

D

(a)

2

4

3

1

(b)

3

1

4

2

(c)

3

4

1

2

(d)

2

1

3

4

IES-34. Assertion (A): All analyses of heat transfer in turbulent flow must

eventually rely on experimental data.

[IES-2000]

Reason (R): The eddy properties vary across the boundary layer and no

adequate theory is available to predict their behaviour.

(a) Both A and R are individually true and R is the correct explanation of A

(b) Both A and R are individually true but R is not the correct explanation of A

(c) A is true but R is false

(d) A is false but R is true

Page 47 of 97

IES-35.

Match the velocity profiles labelled A, B, C and D with the following

situations: [IES-1998]