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Heat and Mass Transfer

Heat and Mass Transfer
Stefan Boltzmann law is applicable for heat transfer by

Conduction and radiation combined
Radiation
Conduction
Convection

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Heat and Mass Transfer
A cube at high temperature is immersed in a constant temperature bath. It loses heat from its top, bottom and side surfaces with heat transfer coefficients of h₁, h₂ and h₃ respectively. The average heat transfer coefficient for the cube is

h₁ + h₂ + h₃
1/h₁ + 1/h₂ + 1/h₃
None of these
(h₁.h₂.h₃)1/3

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Heat and Mass Transfer
According to Newton's law of cooling, the heat transfer from a hot body to a cold body is

Both (A) and (B)
Directly proportional to the surface area
Directly proportional to the difference of temperatures between the two bodies
Either (A) or (B)

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Heat and Mass Transfer
The ratio of the thickness of thermal boundary layer to the thickness of hydrodynamic boundary layer is equal to (Prandtl number) n, where n is equal to

-1
=-2/3
1
=-1/3

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Heat and Mass Transfer
A composite slab has two layers of different materials with thermal conductivities k₁ and k₂. If each layer has the same thickness, then the equivalent thermal conductivity of the slab will be

(k₁ + k₂)/ k₁ k₂
(k₁ + k₂)
2 k₁ k₂/ (k₁ + k₂)
k₁ k₂

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Heat and Mass Transfer
The transfer of heat by molecular collision is smallest in

Solids
Gases
Liquids
None of these

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