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Heat and Mass Transfer

Heat and Mass Transfer
Stefan Boltzmann law is applicable for heat transfer by

Convection
Conduction
Radiation
Conduction and radiation combined

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Heat and Mass Transfer
Thermal conductivity of glass wool varies from sample to sample because of variation in

Density
Porosity
Composition
All of these

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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

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

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Heat and Mass Transfer
Metals are good conductors of heat because

Their atoms collide frequently
They contain free electrons
They have high density
Their atoms are relatively far apart

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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
One
Three
Four

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Heat and Mass Transfer
Absorptivity of a body will be equal to its emissivity

At critical temperature
At one particular temperature
When system is under thermal equilibrium
At all temperatures

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