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Heat and Mass Transfer

Heat and Mass Transfer
The concept of overall coefficient of heat transfer is used in case of heat transfer by

Radiation
Conduction and convection
Conduction
Convection

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

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

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

Black body
White body
Grey body
Opaque body

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Heat and Mass Transfer
Thermal diffusivity of a substance is

Inversely proportional to density of substance
Directly proportional to the thermal conductivity
All of these
Inversely proportional to specific heat

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Heat and Mass Transfer
Two plates spaced 150 mm apart are maintained at 1000°C and 70°C. The heat transfer will take place mainly by

Forced convection
Free convection
Convection
Radiation

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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

One
Four
Three
Two

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