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Heat and Mass Transfer

Heat and Mass Transfer
The automobile radiator is a heat exchanger of

Parallel flow type
Cross flow type
Regenerator type
Counter flow type

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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

Three
Two
One
Four

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Heat and Mass Transfer
The value of the wavelength for maximum emissive power is given by

Stefan's law
Planck's law
Fourier's law
Wien’s law

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Heat and Mass Transfer
Depending on the radiating properties, a body will be white when(Where a = absorptivity, p = reflectivity, x = transmissivity)

P = 0, x = 0 and a = 1
X = 0, a + p = 1
P = 0, x = 1 and a = 0
P=1, T = 0 and a = 0

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Heat and Mass Transfer
Depending on the radiating properties, a body will be black when (Where a = absorptivity, p = reflectivity, X = transmissivity.)

X = 0, a + p = 0
P = 0, x = 1 and a = 0
P = 0, x = 0 and a = 1
P= 1, T = 0 and a = 0

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Heat and Mass Transfer
According to Stefan Boltzmann law, the total radiation from a black body per second per unit area is directly proportional to the

Absolute temperature
Cube of the absolute temperature
Square of the absolute temperature
Fourth power of the absolute temperature

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