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Heat Transfer

Heat Transfer
Radiant energy received by a body is proportional to (where, d = the distance between the object emitting radiation and that receiving it.)

d1.5
√d
d2
d

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Heat Transfer
In Fourier's law, the proportionality constant is called the

Thermal conductivity
Heat transfer co-efficient
Thermal diffusivity
Stefan-Boltzman constant

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Heat Transfer
Harmonic mean temperature difference is given by

√(ΔT₁ . ΔT₂)
2.(ΔT₁ . ΔT₂)(ΔT₁ - ΔT₂)
(ΔT₁ - ΔT₂)/(ΔT₁ . ΔT₂)
2.(ΔT₁ . ΔT₂)/(ΔT₁ + ΔT₂)

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Heat Transfer
Heat waves

Can not pass through vacuum
Both B and C
Travel in straight line
Can be reflected by a mirror

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Heat Transfer
For a given ambient air temperature with increase in the thickness of insulation of a hot cylinderical pipe, the rate of heat loss from the surface would

Decrease
Increase
First decrease and then increase
First increase and then decrease

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Heat Transfer
Nusselt number for full developed, laminar, constant property flow in a pipe at uniform heat flux is

0.72
83
4.364
18

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