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Heat and Mass Transfer

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

More or less same
Higher
Same
Very much lower

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Heat and Mass Transfer
In free convection heat transfer transition from laminar to turbulent flow is governed by the critical value of the

Prandtl number, Grashoff's number
Reynold's number, Grashoff's number
Reynold's number
Grashoff's number

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

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Heat and Mass Transfer
In convection heat transfer from hot flue gases to water tube, even though flow may be turbulent, a laminar flow region (boundary layer of film) exists close to the tube. The heat transfer through this film takes place by

Both convection and conduction
Radiation
Convection
Conduction

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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

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

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Heat and Mass Transfer
A perfect black body is one which

Reflects all heat
Is black in colour
Transmits all heat radiations
Absorbs heat radiations of all wave lengths falling on it

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