Shorter wavelength
Longer wavelength
Remain same at all wavelengths
Wavelength has nothing to do with it
A. Shorter wavelength
Face area
Time
Thickness
Temperature difference
h = k/ ρS
h = ρS/k
h = S/ρk
h = kρ/S
Conduction
Convection
Radiation
Conduction and convection
In heat exchanger design as a safety factor
In case of Newtonian fluids
When a liquid exchanges heat with a gas
None of the above
More than those for liquids
Less than those for liquids
More than those for solids
Dependent on the viscosity
P = 0, x = 0 and a = 1
P=1, x = 0, and a = 0
P = 0, T= 1, and a = 0
X = 0, a + p = 1
Density
Coefficient of viscosity
Gravitational force
All of these
I.C. engine
Air preheaters
Heating of building in winter
None of the above
Varies with temperature
Varies with wavelength of the incident ray
Is equal to its emissivity
Does not vary with temperature and. wavelength of the incident ray
Cold water inlet and outlet
Hot medium inlet and outlet
Hot medium outlet and cold water inlet
Hot medium outlet and cold water outlet
Grashoff number and Reynold number
Grashoff number and Prandtl number
Prandtl number and Reynold number
Grashoff number, Prandtl number and Reynold number
Less than those for gases
Less than those for liquids
More than those for liquids and gases
More or less same as for liquids and gases
P = 0, x = 0 and a = 1
P=1, x = 0 and a = 0
P = 0, x = 1 and a = 0
X = 0, a + p = 1 Where a = absorptivity, p = reflectivity, X = transmissivity.
Its temperature
Nature of the body
Kind and extent of its surface
All of the above
Grashoff number
Biot number
Stanton number
Prandtl number
A.Cmin/U
U/A.Cmin
A.U.Cmin
A.U/Cmin
Convection
Radiation
Forced convection
Free convection
Remain same
Decreases
Increases
May increase or decrease depending upon temperature
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.
20°C
40°C
60°C
66.7°C
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
α = 1, ρ = 0 and τ = 0
α = 0, ρ = 1 and τ = 0
α = 0, ρ = 0 and τ = 1
α + ρ = 1 and τ = 0
At all temperatures
At one particular temperature
When system is under thermal equilibrium
At critical temperature
Emissivity
Transmissivity
Reflectivity
Intensity of radiation
Radiators in automobile
Condensers and boilers in steam plants
Condensers and evaporators in refrigeration and air conditioning units
All of the above
Kirchhoff's law
Stefan's law
Wines law
Planck's law
Conduction
Convection
Radiation
Conduction and convection
Conduction
Convection
Radiation
Conduction and radiation combined
Wien's law
Planck's law
Stefan's law
Fourier's law