k/h₀
2k/h₀
h₀/k
h₀/2k
B. 2k/h₀
Grashoff number and Reynold number
Grashoff number and Prandtl number
Prandtl number and Reynold number
Grashoff number, Prandtl number and Reynold number
High thickness of insulation
High vapour pressure
Less thermal conductivity insulator
A vapour seal
Absorptive power
Emissive power
Absorptivity
Emissivity
Temperature
Wave length
Physical nature
All of the above
Electric heater
Steam condenser
Boiler
Refrigerator condenser coils
Watt/mK
Watt/m²K²
Watt/m²K4
Watt/mK²
Increases
Decreases
Remain constant
May increase or decrease depending on temperature
Their atoms collide frequently
Their atoms are relatively far apart
They contain free electrons
They have high density
One dimensional cases only
Two dimensional cases only
Three dimensional cases only
Regular surfaces having non-uniform temperature gradients
Varies with temperature
Varies with the wave length of incident ray
Varies with both
Does not vary with temperature and wave length of the incident ray
From one particle of the body to another without the actual motion of the particles
From one particle of the body to another by the actual motion of the heated particles
From a hot body to a cold body, in a straight line, without affecting the intervening medium
None of the above
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
Grashoff number
Nusselt number
Weber number
Prandtl number
At all temperatures
At one particular temperature
When system is under thermal equilibrium
At critical temperature
Better insulation should be put over pipe and better one over it
Inferior insulation should be put over pipe and better one over it
Both may be put in any order
Whether to put inferior OIL over pipe or the better one would depend on steam temperature
Thermal conductivity
Thermal diffusivity
Density
Dynamic viscosity
k/h₀
2k/h₀
h₀/k
h₀/2k
Improve heat transfer
Provide support for tubes
Prevent stagnation of shell side fluid
All of these
A.Cmin/U
U/A.Cmin
A.U.Cmin
A.U/Cmin
Thermal resistance
Thermal coefficient
Temperature gradient
Thermal conductivity
0.45
0.55
0.40
0.75
kcal/m²
kcal/hr °C
kcal/m² hr °C
kcal/m hr °C
h₁ + h₂ + h₃
(h₁.h₂.h₃)1/3
1/h₁ + 1/h₂ + 1/h₃
None of these
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
Absorptive power
Emissive power
Emissivity
None of these
Thermometer
Thermistor
Thermocouple
None of these
Radiant heat is proportional to fourth power of absolute temperature
Emissive power depends on temperature
Emissive power and absorptivity are constant for all bodies
Ratio of emissive power to absorptive power for all bodies is same and is equal to the emissive power of a perfectly black body.
Emissivity
Transmissivity
Reflectivity
Intensity of radiation
k. A. (dT/dx)
k. A. (dx/dT)
k. (dT/dx)
k. (dx/dT)
Watt/cm² °K
Watt/cm4 °K
Watt²/cm °K⁴
Watt/cm² °K⁴