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Heat and Mass Transfer

Heat and Mass Transfer
The total emissivity power is .defined as the total amount of radiation emitted by a black body per unit

Time
Area
Thickness
Temperature

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Heat and Mass Transfer
Thermal diffusivity is a

Dimensionless parameter
Function of temperature
Physical property of a substance
All of these

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Heat and Mass Transfer
The heat transfer by conduction through a thick sphere is given by

Q = 8πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 6πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 4πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 2πkr1 r2 (T1 - T2)/ (r2 - r1)

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Heat and Mass Transfer
The most commonly used method for the design of duct size is the

Static regains method
Dual or double method
Equal friction method
Velocity reduction method

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

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

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Heat and Mass Transfer
The energy distribution of an ideal reflector at higher temperatures is largely in the range of

Wavelength has nothing to do with it
Longer wavelength
Shorter wavelength
Remain same at all wavelengths

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