Reflected
Refracted
Transmitted
Absorbed
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.
Is black in colour
Reflects all heat
Transmits all heat radiations
Absorbs heat radiations of all wave lengths falling on it
Cold body to hot body
Hot body to cold body
Smaller body to larger body
Larger body to smaller body
Conduction
Convection
Radiation
Scattering
Watt/cm² °K
Watt/cm4 °K
Watt²/cm °K⁴
Watt/cm² °K⁴
P = 0, x = 0 and a = 1
P= 1, T = 0 and a = 0
P = 0, x = 1 and a = 0
X = 0, a + p = 0 Where a = absorptivity, p = reflectivity, X = transmissivity.
Its temperature
Nature of the body
Kind and extent of its surface
All of the above
0.1
0.23
0.42
0.51
Energy transferred by convection to that by conduction
Kinematic viscosity to thermal diffusivity
Inertia force to viscous force
None of the above
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kirchhoff's law
Stanton number
Biot number
Peclet number
Grashoff number
Absolute temperature (T)
I²
F
T
Increase
Decrease
Remain unaffected
May increase/decrease depending on temperature and thickness of insulation
Blast furnace
Heating of building
Cooling of parts in furnace
Heat received by a person from fireplace
6
9
27
81
k/h₀
2k/h₀
h₀/k
h₀/2k
Black body
Grey body
Opaque body
White body
Absolute temperature
Square of temperature
Fourth power of absolute temperature
Fourth power of temperature
High thickness of insulation
High vapour pressure
Less thermal conductivity insulator
A vapour seal
Grashoff number
Nusselt number
Weber number
Prandtl number
It is impossible to transfer heat from low temperature source to t high temperature source
Heat transfer by radiation requires no medium
All bodies above absolute zero emit radiation
Heat transfer in most of the cases takes place by combination of conduction, convection and radiation
The time taken to attain the final temperature to be measured
The time taken to attain 50% of the value of initial temperature difference
The time taken to attain 63.2% of the value of initial temperature difference
Determined by the time taken to reach 100°C from 0°C
P = 0, x = 0 and a = 1
P=1, T = 0 and a = 0
P = 0, x = 1 and a = 0
X = 0, a + p = 1 Where a = absorptivity, p = reflectivity, x = transmissivity
Thermal conductivity to the equivalent thickness of the film of fluid
Temperature drop through the films of fluids to the thickness of film of fluids
Thickness of film of fluid to the thermal conductivity
Thickness of film of fluid to the temperature drop through the films of fluids
I.C. engine
Air preheaters
Heating of building in winter
None of the above
Electric heater
Steam condenser
Boiler
Refrigerator condenser coils
k₁ k₂
(k₁ + k₂)
(k₁ + k₂)/ k₁ k₂
2 k₁ k₂/ (k₁ + k₂)
Shorter wavelength
Longer wavelength
Remain same at all wavelengths
Wavelength has nothing to do with it
The better insulation must be put inside
The better insulation must be put outside
One could place either insulation on either side
One should take into account the steam temperature before deciding as to which insulation is put where