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Heat and Mass Transfer

Heat and Mass Transfer
The unit of Stefan Boltzmann constant is

watt/cm4 °K
watt/cm3 °K
watt/cm2 °K⁴
watt2/cm °K⁴

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Heat and Mass Transfer
Fourier's law of heat conduction is valid for

Regular surfaces having non-uniform temperature gradients
One dimensional cases only
Two dimensional cases only
Three dimensional cases only

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Heat and Mass Transfer
The amount of heat flow through a body by conduction is

Dependent upon the material of the body
Directly proportional to the temperature difference on the two faces of the body
All of these
Directly proportional to the surface area of the body

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Heat and Mass Transfer
Total emissivity of polished silver compared to black body is

Higher
Same
Very much lower
More or less same

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Heat and Mass Transfer
LMTD in case of counter flow heat exchanger as compared to parallel flow heat exchanger is

Depends on the area of heat exchanger
Same
Higher
Lower

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Heat and Mass Transfer
40% of incident radiant energy on the surface of a thermally transparent body is reflected back. If the transmissivity of the body be 0.15, then the emissivity of surface is

0.55
0.4
0.75
0.45

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