First law of thermodynamics
Newton's law of cooling
Newton's law of heating
Stefan's law
B. Newton's law of cooling
J/m² sec
J/m °K sec
W/m °K
Option (B) and (C) above
More than those for liquids
Less than those for liquids
More than those for solids
Dependent on the viscosity
From one particle of the body to another without the actual motion of the particles
From one particle of the body to another by the actual motion of the heated particles
From a hot body to a cold body, in a straight line, without affecting the intervening medium
None of the above
Thermometer
Thermistor
Thermocouple
None of these
W/m²K
W/m²
W/mK
W/m
Conduction
Convection
Radiation
None of these
The heat transfer in liquid and gases takes place according to convection.
The amount of heat flow through a body is dependent upon the material of the body.
The thermal conductivity of solid metals increases with rise in temperature
Logarithmic mean temperature difference is not equal to the arithmetic mean temperature difference.
Direct mixing of hot and cold fluids
A complete separation between hot and cold fluids
Flow of hot and cold fluids alternately over a surface
Generation of heat again and again
First law of thermodynamics
Newton's law of cooling
Newton's law of heating
Stefan's law
Radiant heat is proportional to fourth power of absolute temperature
Emissive power depends on temperature
Emissive power and absorptivity are constant for all bodies
Ratio of emissive power to absorptive power for all bodies is same and is equal to the emissive power of a perfectly black body.
m²/hr
m²/hr °C
kcal/m² hr
kcal/m. hr °C
RN = hl/k
RN = μ cp/k
RN = ρ V l /μ
RN = V²/t.cp
Cold water inlet and outlet
Hot medium inlet and outlet
Hot medium outlet and cold water inlet
Hot medium outlet and cold water outlet
Increase
Decrease
Remain unaffected
May increase/decrease depending on temperature and thickness of insulation
Wien's law
Stefan's law
Kirchhoff's law
Planck's law
Q = [2πlk (T₁ - T₂)]/2.3 log (r₂/r₁)
Q = 2.3 log (r₂/r₁)/[2πlk (T₁ - T₂)]
Q = [2π (T₁ - T₂)]/2.3 lk log (r₂/r₁)
Q = = 2πlk/2.3 (T₁ - T₂) log (r₂/r₁)
Shorter wavelength
Longer wavelength
Remain same at all wavelengths
Wavelength has nothing to do with it
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kirchhoff's law
Temperature
Thickness
Area
Time
Is black in colour
Reflects all heat
Transmits all heat radiations
Absorbs heat radiations of all wave lengths falling on it
Black bodies
Polished bodies
All coloured bodies
All of the above
Minimum energy
Maximum energy
Both (A) and (B)
None of these
Conduction
Convection
Radiation
Conduction and convection
Directly proportional to the thermal conductivity
Inversely proportional to density of substance
Inversely proportional to specific heat
All of the above
Glass
Water
Plastic
Air
Q = 2πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 4πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 6πkr1 r2 (T1 - T2)/ (r2 - r1)
Q = 8πkr1 r2 (T1 - T2)/ (r2 - r1)
Thermal conductivity
Thermal diffusivity
Density
Dynamic viscosity
Improve heat transfer
Provide support for tubes
Prevent stagnation of shell side fluid
All of these
Domestic refrigerators
Water coolers
Room air conditioners
All of these
Below which a gas does not obey gas laws
Above which a gas may explode
Below which a gas is always liquefied
Above which a gas will never liquefied