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Heat Transfer

Heat Transfer
The heat flux in the nucleate boiling regimes is proportional to (where, ΔT = excess temperature)

(ΔT)⁴
(ΔT)²
(ΔT)³
√(ΔT)

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Heat Transfer
Steady state one dimensional heat flow by conduction as given by Fourier's low does not assume that

Boundary surfaces are isothermal
Material is anisotropic
Constant temperature gradient exists
There is no internal heat generation

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Heat Transfer
In a shell and tube heat exchanger, square pitch compared to triangular pitch

Can pack more surface area into a shell of given diameter
None of these
Gives a higher shell side pressure drop
Gives a lower shell side pressure drop

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Heat Transfer
The average heat transfer co-efficient for laminar film condensation on vertical surface is inversely proportional to (where, ΔT = Temperature drop across condensate film )

None of the listed here
ΔT
(ΔT)1/4
(ΔT)2

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Heat Transfer
The local surface conductance for laminar film condensation on vertical surface is (where, t = film thickness)

∝ t
∝ 1/t
Independent of 't'
∝ √t

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Heat Transfer
A sphere of radius 'R₁' is enclosed in a sphere of radius 'R₂'. The view (or shape) factor for radiative heat transfer of the outer sphere with respect to the inner sphere is

R₂/(R₁+R₂)
(R₁/R₂)2
1

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