High thickness of insulation
High vapour pressure
Less thermal conductivity insulator
A vapour seal
D. A vapour seal
Thermal resistance
Thermal coefficient
Temperature gradient
Thermal conductivity
h = k/ ρS
h = ρS/k
h = S/ρk
h = kρ/S
W/m²K
W/m²
W/mK
W/m
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
Composition
Density
Porosity
All of the above
Absorptive power
Emissive power
Absorptivity
Emissivity
kcal/m²
kcal/hr °C
kcal/m² hr °C
kcal/m hr °C
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
Fourier equation
Stefan-Boltzmann equation
Newton Reichmann equation
Joseph-Stefan equation
Increases
Decreases
Remain constant
May increase or decrease depending on temperature
Higher
Lower
Same
Depends on the area of heat exchanger
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
Solids
Liquids
Gases
None of these
Moisture
Density
Temperature
All of the above
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
J/m² sec
J/m °K sec
W/m °K
Option (B) and (C) above
Shorter wavelength
Longer wavelength
Remain same at all wavelengths
Wavelength has nothing to do with it
k. A. (dT/dx)
k. A. (dx/dT)
k. (dT/dx)
k. (dx/dT)
Change vapour into liquid
Change liquid into vapour
Increase the temperature of a liquid of vapour
Convert water into steam and superheat it
Hr (time)
Sq. m (area)
°C (temperature)
K.cal (heat)
Same
Less
Greater
None of these
Conduction
Convection
Radiation
None of these
Temperature
Thickness
Area
Time
Stanton number
Nusselt number
Biot number
Peclet number
Absolute temperature
Square of the absolute temperature
Cube of the absolute temperature
Fourth power of the absolute temperature
Cold body to hot body
Hot body to cold body
Smaller body to larger body
Larger body to smaller body
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.
Convection
Radiation
Conduction
Both convection and conduction
Quantity of heat flowing in one second through one cm cube of material when opposite faces ^re maintained at a temperature difference of 1°C
Quantity of heat flowing in one second through a slab of the material of area one cm square, thickness 1 cm when its faces differ in temperature by 1°C
Heat conducted in unit time across unit area through unit thickness when a temperature difference of unity is maintained between opposite faces
All of the above
Liquids
Energy
Temperature
Entropy