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Heat and Mass Transfer

Heat and Mass Transfer
In heat transfer, conductance equals conductivity (kcal/hr/sq.m/°C/cm) divided by

Sq. m (area)
°C (temperature)
Hr (time)
K.cal (heat)

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Heat and Mass Transfer
If the energy radiated per second per sq. cm. of the surface for wave lengths lying between λ, and λ + dλ is represented by (eλ.dλ), then eλ is called

Absorptive power
Emissive power
None of these
Emissivity

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Heat and Mass Transfer
According to Newton's law of cooling, the heat transfer from a hot body to a cold body is

Directly proportional to the difference of temperatures between the two bodies
Both (A) and (B)
Directly proportional to the surface area
Either (A) or (B)

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Heat and Mass Transfer
Thermal conductivity of air at room temperature in kcal/m hr °C is of the order of

0.1
0.002
0.01
0.02

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Heat and Mass Transfer
When heat is transferred from hot body to cold body, in a straight line, without affecting the intervening medium, it is referred as heat transfer by

Conduction
Conduction and convection
Convection
Radiation

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Heat and Mass Transfer
Thermal diffusivity is

A physical property of the material
Used as mathematical model
Function of temperature
A dimensionless parameter

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