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Heat and Mass Transfer

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

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

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Heat and Mass Transfer
Thermal conductivity of wood depends on

Temperature
All of these
Density
Moisture

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

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Heat and Mass Transfer
The heat transfer by conduction through a thick sphere is given by

Q = 4πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 2πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 6πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 8πkr1 r2 (T1 - T2)/ (r2 - r1)

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Heat and Mass Transfer
Two long parallel surfaces each of emissivity 0.7 are maintained at different temperatures and accordingly have radiation heat exchange between them. It is desired to reduce 75% of the radiant heat transfer by inserting thin parallel shields of emissivity 1 on both sides. The number of shields should be

Four
Two
One
Three

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Heat and Mass Transfer
Temperature of steam at around 540°C can be measured by

Thermometer
Thermocouple
Thermistor
None of these

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