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Heat and Mass Transfer

Heat and Mass Transfer
An ordinary passenger aircraft requires a cooling system of capacity.

8 TR
4 TR
10 TR
2 TR

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Heat and Mass Transfer
A designer chooses the values of fluid flow rates and specific heats in such a manner that the heat capacities of the two fluids are equal. A hot fluid enters the counter flow heat exchanger at 100°C and leaves at 60°C. A cold fluid enters the heat exchanger at 40°C. The mean temperature difference between the two fluids is

40°C
20°C
66.7°C
60°C

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Heat and Mass Transfer
Absorptivity of a body will be equal to its emissivity

At all temperatures
At critical temperature
At one particular temperature
When system is under thermal equilibrium

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Heat and Mass Transfer
Joule sec is the unit of

Kinematic viscosity
Thermal conductivity
Planck's constant
Universal gas constant

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Heat and Mass Transfer
In a heat exchanger with one fluid evaporating or condensing, the surface area required is least in

Counter flow
Cross flow
Parallel flow
All of these

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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

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

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