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Heat and Mass Transfer

Heat and Mass Transfer
The ratio of surface convection resistance to the internal conduction resistance is known as

Biot number
Grashoff number
Stanton number
Prandtl number

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Heat and Mass Transfer
When α is absorptivity, ρ is reflectivity and τ is transmissivity, then for a diathermanous body,

α = 0, ρ = 1 and τ = 0
α = 0, ρ = 0 and τ = 1
α = 1, ρ = 0 and τ = 0
α + ρ = 1 and τ = 0

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Heat and Mass Transfer
Depending on the radiating properties, a body will be black when (Where a = absorptivity, p = reflectivity, X = transmissivity.)

P = 0, x = 0 and a = 1
P= 1, T = 0 and a = 0
X = 0, a + p = 0
P = 0, x = 1 and a = 0

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Heat and Mass Transfer
Depending on the radiating properties, a body will be opaque when

X = 0, a + p = 1
P = 0, x = 0 and a = 1
P=1, x = 0 and a = 0
P = 0, x = 1 and a = 0

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Heat and Mass Transfer
Moisture would find its way into insulation by vapour pressure unless it is prevented by

Less thermal conductivity insulator
High vapour pressure
A vapour seal
High thickness of insulation

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

Planck's law
Wien’s law
Stefan's law
Fourier's law

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MORE MCQ ON Heat and Mass Transfer

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