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Heat and Mass Transfer

Heat and Mass Transfer
When absorptivity (α) = 1, reflectivity (ρ) = 0 and transmissivity (τ) = 0, then the body is said to be a

Grey body
White body
Black body
Opaque body

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Heat and Mass Transfer
Sensible heat factor is given by (where S.H. = Sensible heat, and L.H. = Latent heat)

S.H/(L.H - S.H)
S.H/(S.H + L.H)
(S.H + L.H) /S.H
(L.H - S.H)/S.H

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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
Longer wavelength
Shorter wavelength
Wavelength has nothing to do with it

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

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Heat and Mass Transfer
According to Stefan's law, the total radiation from a black body per second per unit area is proportional to

T
T2
Absolute temperature
T5

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

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

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