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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 rate of heat flow through a body is Q = [kA (T₁ - T₂)]/x. The term x/kA is known as

Thermal conductivity
Thermal resistance
None of these
Thermal coefficient

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Heat and Mass Transfer
Two long parallel surfaces each of emissivity 0.7 are maintained at different temperatures and accordingly have radiation heat exchange between them. It is desired to reduce 75% of the radiant heat transfer by inserting thin parallel shields of emissivity 1 on both sides. The number of shields should be

Two
Three
One
Four

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Heat and Mass Transfer
Cork is a good insulator because it has

Low density
Free electrons
Porous body
Atoms colliding frequency

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

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

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Heat and Mass Transfer
The insulation ability of an insulator with the presence of moisture would

Decrease
Remain unaffected
May increase/decrease depending on temperature and thickness of insulation
Increase

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