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Heat and Mass Transfer

Heat and Mass Transfer
Thermal conductivity of glass wool varies from sample to sample because of variation in

Porosity
All of these
Density
Composition

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

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Heat and Mass Transfer
Heat transfer takes place as per

Zeroth law of thermodynamics
Kirchoff's law
Second law of the thermodynamics
First law of thermodynamic

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Heat and Mass Transfer
The rate of energy transferred by convection to that by conduction is called

Nusselt number
Stanton number
Biot number
Peclet number

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Heat and Mass Transfer
The expression Q = ρ AT4 is called

Fourier equation
Newton Reichmann equation
Stefan-Boltzmann equation
Joseph-Stefan equation

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Heat and Mass Transfer
Heat flows from one body to other when they have

Different specific heat
Different heat contents
Different temperatures
Different atomic structure

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