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)
B. Q = 4πkr1 r2 (T1 - T2)/ (r2 - r1)
Stanton number
Biot number
Peclet number
Grashoff number
Fourier equation
Stefan-Boltzmann equation
Newton Reichmann equation
Joseph-Stefan equation
In conduction, reduction in the thickness of the material and an increase in thermal conductivity.
In convection, stirring of the fluid and cleaning the heating surface.
In radiation, increasing the temperature and reducing the emissivity.
All of the above
Zeroth law of thermodynamics
First law of thermodynamic
Second law of the thermodynamics
Kirchoff's law
Change vapour into liquid
Change liquid into vapour
Increase the temperature of a liquid or vapour
Convert water into steam and superheat it
Increases
Decreases
Remain constant
May increase or decrease depending on temperature
k. A. (dT/dx)
k. A. (dx/dT)
k. (dT/dx)
k. (dx/dT)
Universal gas constant
Kinematic viscosity
Thermal conductivity
Planck's constant
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.
Conduction
Convection
Radiation
Conduction and convection
Wien's law
Planck's law
Stefan's law
Fourier's law
Higher
Lower
Same
Depends upon the shape of body
Conduction
Convection
Radiation
Conduction and convection
J/m² sec
J/m °K sec
W/m °K
Option (B) and (C) above
Conduction
Convection
Radiation
Conduction and radiation combined
Composition
Density
Porosity
All of the above
Convection
Radiation
Conduction
Both convection and conduction
Conduction
Convection
Radiation
Conduction and convection
Black bodies
Polished bodies
All coloured bodies
All of the above
Conduction
Convection
Radiation
None of these
0.002
0.02
0.01
0.1
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
First law of thermodynamics
Newton's law of cooling
Newton's law of heating
Stefan's law
Conduction
Free convection
Forced convection
Radiation
Maximum
Minimum
Zero
None of these
Conduction
Convection
Radiation
None of these
Equal to
Directly proportional to
Inversely proportional to
None of these
Stanton number
Nusselt number
Biot number
Peclet number
Domestic refrigerators
Water coolers
Room air conditioners
All of these
Directly proportional to the surface area
Directly proportional to the difference of temperatures between the two bodies
Either (A) or (B)
Both (A) and (B)