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.
C. The thermal conductivity of solid metals increases with rise in temperature
0.1
0.23
0.42
0.51
25 mm
40 mm
160 mm
800 mm
Conduction
Convection
Radiation
Conduction and convection
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)
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
Absorptive power
Emissive power
Absorptivity
Emissivity
Conduction
Convection
Radiation
None of these
Wien's law
Stefan's law
Kirchhoff's law
Planck's law
Higher
Lower
Same
Depends upon the shape of body
Change vapour into liquid
Change liquid into vapour
Increase the temperature of a liquid or vapour
Convert water into steam and superheat it
Conduction
Convection
Radiation
Conduction and convection
0.002
0.02
0.01
0.1
Conduction
Convection
Radiation
Conduction and convection
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
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)
Convection
Radiation
Forced convection
Free convection
20°C
40°C
60°C
66.7°C
W/m²K
W/m²
W/mK
W/m
Directly proportional to the surface area of the body
Directly proportional to the temperature difference on the two faces of the body
Dependent upon the material of the body
All of the above
Black bodies
Polished bodies
All coloured bodies
All of the above
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
k/h₀
2k/h₀
h₀/k
h₀/2k
Kirchhoff's law
Stefan's law
Wines law
Planck's law
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
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
Black body
Grey body
Opaque body
White body
Density
Coefficient of viscosity
Gravitational force
All of these
Black radiation
Full radiation
Total radiation
All of these
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.
Steam
Solid ice
Melting ice
Water