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Heat and Mass Transfer

Heat and Mass Transfer
The total emissivity power is .defined as the total amount of radiation emitted by a black body per unit

Thickness
Time
Area
Temperature

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Heat and Mass Transfer
The energy distribution of an ideal reflector at higher temperatures is largely in the range of

Remain same at all wavelengths
Wavelength has nothing to do with it
Shorter wavelength
Longer wavelength

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Heat and Mass Transfer
Two balls of same material and finish have their diameters in the ratio of 2: 1 and both are heated to same temperature and allowed to cool by radiation. Rate of cooling by big ball as compared to smaller one will be in the ratio of

0.043055555555556
0.16736111111111
0.042361111111111
0.084027777777778

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Heat and Mass Transfer
The ratio of the emissive power and absorptive power of all bodies is the same and is equal to the emissive power of a perfectly black body. This statement is known as

Wien's law
Kirchhoff's law
Stefan's law
Planck's law

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Heat and Mass Transfer
Thermal conductivity of air at room temperature in kcal/m hr °C is of the order of

0.1
0.02
0.002
0.01

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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

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

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MORE MCQ ON Heat and Mass Transfer

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