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Heat and Mass Transfer

Heat and Mass Transfer
According to Wien's law, the wavelength corresponding to maximum energy is proportion to

T
Absolute temperature (T)
I²
F

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

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

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Heat and Mass Transfer
The value of Prandtl number for air is about

0.1
0.3
1.7
0.7

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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
One
Four
Two

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Heat and Mass Transfer
An electric cable of aluminium conductor (k = 240 W/mK) is to be insulated with rubber (k = 0.15 W/mK). The cable is to be located in air (h = 6 W/m²). The critical thickness of insulation will be

25 mm
800 mm
40 mm
160 mm

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Heat and Mass Transfer
The heat transfer from a hot body to a cold body is directly proportional to the surface area and difference of temperatures between the two bodies. This statement is called

First law of thermodynamics
Newton's law of cooling
Stefan's law
Newton's law of heating

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