Increases
Decreases
Remain constant
May increase or decrease depending on temperature
A. Increases
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.
Equal to
Directly proportional to
Inversely proportional to
None of these
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
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)
Energy transferred by convection to that by conduction
Kinematic viscosity to thermal diffusivity
Inertia force to viscous force
None of the above
Its temperature
Nature of the body
Kind and extent of its surface
All of the above
The total radiation from a black body per second per unit area is directly proportional to the fourth power of the absolute temperature
The wave length corresponding to the maximum energy is proportional to the absolute temperature
The ratio of the emissive power and absorptive power of all bodies is the same and is equal to the emissive power of a perfectly black body
None of the above
Aluminium
Steel
Brass
Copper
0.002
0.02
0.01
0.1
Stanton number
Nusselt number
Biot number
Peclet number
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
20°C
40°C
60°C
66.7°C
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
Conduction
Convection
Radiation
Conduction and convection
Increases
Decreases
Remain constant
May increase or decrease depending on temperature
More than those for liquids
Less than those for liquids
More than those for solids
Dependent on the viscosity
Stanton number
Biot number
Peclet number
Grashoff number
Universal gas constant
Kinematic viscosity
Thermal conductivity
Planck's constant
Conduction
Convection
Radiation
Conduction and convection
S.H/(S.H + L.H)
(S.H + L.H) /S.H
(L.H - S.H)/S.H
S.H/(L.H - S.H)
Moisture
Density
Temperature
All of the above
Grashoff number and Reynold number
Grashoff number and Prandtl number
Prandtl number and Reynold number
Grashoff number, Prandtl number and Reynold number
Pb = pa - pv
Pb = pa + pv
Pb = pa × pv
Pb = pa/pv
Thermal resistance
Thermal coefficient
Temperature gradient
Thermal conductivity
RN = hl/k
RN = μ cp/k
RN = ρ V l /μ
RN = V²/t.cp
Same
Higher
More or less same
Very much lower
0.45
0.55
0.40
0.75
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.
Zeroth law of thermodynamics
First law of thermodynamic
Second law of the thermodynamics
Kirchoff's law
0.1
0.3
0.7
1.7