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Heat and Mass Transfer

Heat and Mass Transfer
Heat transfer by radiation mainly depends upon

Its temperature
All of these
Kind and extent of its surface
Nature of the body

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Heat and Mass Transfer
The critical temperature is the temperature

Above which a gas may explode
Below which a gas does not obey gas laws
Below which a gas is always liquefied
Above which a gas will never liquefied

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Heat and Mass Transfer
Reynolds number (RN) is given by (where h = Film coefficient, l = Linear dimension, V = Velocity of fluid, k = Thermal conductivity, t = Temperature, ρ = Density of fluid, cp = Specific heat at constant pressure, and μ = Coefficient of absolute viscosity)

RN = ρ V l /μ
RN = hl/k
RN = V²/t.cp
RN = μ cp/k

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

Absolute temperature
T
T5
T2

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Heat and Mass Transfer
The thermal diffusivities for solids are generally

Less than those for gases
More than those for liquids and gases
More or less same as for liquids and gases
Less than those for liquids

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Heat and Mass Transfer
Thermal conductivity of air at room temperature in kcal/m hr °C is of the order of

0.1
0.01
0.02
0.002

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MORE MCQ ON Heat and Mass Transfer

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