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Heat and Mass Transfer

Heat and Mass Transfer
Planck’s law holds good for

black bodies
all coloured bodies
All of these
polished bodies

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Heat and Mass Transfer
The heat transfer from a hot body to a cold body is directly proportional to the surface area and difference of temperatures between the two bodies. This statement is called

First law of thermodynamics
Newton's law of heating
Newton's law of cooling
Stefan's law

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Heat and Mass Transfer
A cube at high temperature is immersed in a constant temperature bath. It loses heat from its top, bottom and side surfaces with heat transfer coefficients of h₁, h₂ and h₃ respectively. The average heat transfer coefficient for the cube is

(h₁.h₂.h₃)1/3
None of these
1/h₁ + 1/h₂ + 1/h₃
h₁ + h₂ + h₃

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Heat and Mass Transfer
The ratio of the thickness of thermal boundary layer to the thickness of hydrodynamic boundary layer is equal to (Prandtl number) n, where n is equal to

=-2/3
-1
1
=-1/3

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Heat and Mass Transfer
A designer chooses the values of fluid flow rates and specific heats in such a manner that the heat capacities of the two fluids are equal. A hot fluid enters the counter flow heat exchanger at 100°C and leaves at 60°C. A cold fluid enters the heat exchanger at 40°C. The mean temperature difference between the two fluids is

20°C
60°C
66.7°C
40°C

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Heat and Mass Transfer
Absorptivity of a body will be equal to its emissivity

At one particular temperature
At critical temperature
When system is under thermal equilibrium
At all temperatures

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