Directly proportional to the thermal conductivity
Inversely proportional to density of substance
Inversely proportional to specific heat
All of the above
D. All of the above
Their atoms collide frequently
Their atoms are relatively far apart
They contain free electrons
They have high density
Universal gas constant
Kinematic viscosity
Thermal conductivity
Planck's constant
A grey body is one which absorbs all radiations incident on it.
At thermal equilibrium, the emissivity and absorptivity are same.
The energy absorbed by a body to the total energy falling on it, is called emissivity.
A perfect body is one which is black in colour.
At all temperatures
At one particular temperature
When system is under thermal equilibrium
At critical temperature
Nature of body
Temperature of body
Type of surface of body
All of the above
Shorter wavelength
Longer wavelength
Remain same at all wavelengths
Wavelength has nothing to do with it
RN = hl/k
RN = μ cp/k
RN = ρ V l /μ
RN = V²/t.cp
Thermal coefficient
Thermal resistance
Thermal conductivity
None of these
Stanton number
Biot number
Peclet number
Grashoff number
Face area
Time
Thickness
Temperature difference
More than those for liquids
Less than those for liquids
More than those for solids
Dependent on the viscosity
S.H/(S.H + L.H)
(S.H + L.H) /S.H
(L.H - S.H)/S.H
S.H/(L.H - S.H)
Reynold's number
Grashoff's number
Reynold's number, Grashoff's number
Prandtl number, Grashoff's number
k₁ k₂
(k₁ + k₂)
(k₁ + k₂)/ k₁ k₂
2 k₁ k₂/ (k₁ + k₂)
k/h₀
2k/h₀
h₀/k
h₀/2k
6
9
27
81
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
Conduction
Convection
Radiation
Conduction and convection
Conduction
Convection
Radiation
Conduction and radiation combined
Higher
Lower
Same
Depends on the area of heat exchanger
Wien's law
Planck's law
Stefan's law
Fourier's law
Increases
Decreases
Remain constant
May increase or decrease depending on temperature
Fourier equation
Stefan-Boltzmann equation
Newton Reichmann equation
Joseph-Stefan equation
I.C. engine
Air preheaters
Heating of building in winter
None of the above
Conduction
Convection
Radiation
Conduction and convection
Increases
Decreases
Remain constant
May increase or decrease depending on temperature
Equivalent thickness of film
Thermal conductivity Equivalent thickness of film Specific heat × Viscosity
Thermal conductivity Molecular diffusivity of momentum Thermal diffusivity
Film coefficient × Inside diameter Thermal conductivity
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.
0.45
0.55
0.40
0.75
Solids
Liquids
Gases
None of these