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Heat and Mass Transfer

Heat and Mass Transfer
The unit of Stefan Boltzmann constant is

watt/cm2 °K⁴
watt2/cm °K⁴
watt/cm4 °K
watt/cm3 °K

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Heat and Mass Transfer
The rate of heat flow through a body is Q = [kA (T₁ - T₂)]/x. The term x/kA is known as

Thermal coefficient
Thermal conductivity
None of these
Thermal resistance

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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

Convection
Both convection and conduction
Radiation
Conduction

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Heat and Mass Transfer
Pick up the wrong case. Heat flowing from one side to other depends directly on

Temperature difference
Face area
Time
Thickness

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Heat and Mass Transfer
Unit of thermal conductivity in M.K.S. units is

K cal/hr m² °C
K cal m/hr m² °C
K calm/hr °C
K cal/kg m² °C

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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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