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Heat and Mass Transfer

Heat and Mass Transfer
If the temperature of a solid surface changes form 27°C to 627°C, then its emissive power changes in the ratio of

3
9
270
81

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

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

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

Planck’s law
Kirchhoff’s law
Stefan’s law
Wine’s law

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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

Four
Two
Three
One

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Heat and Mass Transfer
The concept of overall coefficient of heat transfer is used in case of heat transfer by

Convection
Conduction and convection
Radiation
Conduction

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Heat and Mass Transfer
According to Kirchoff's law, the ratio of emissive power to absorptivity for all bodies is equal to the emissive power of a

Brilliant white polished body
Black body
Red hot body
Grey body

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