Density
Coefficient of viscosity
Gravitational force
All of these
D. All of these
Electric heater
Steam condenser
Boiler
Refrigerator condenser coils
Conduction
Convection
Radiation
Conduction and convection
Thermometer
Thermistor
Thermocouple
None of these
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)
Kirchhoff's law
Stefan's law
Wines law
Planck's law
Parallel flow
Counter flow
Cross flow
All of these
Shorter wavelength
Longer wavelength
Remain same at all wavelengths
Wavelength has nothing to do with it
Conduction
Convection
Radiation
None of these
First law of thermodynamics
Newton's law of cooling
Newton's law of heating
Stefan's law
At all temperatures
At one particular temperature
When system is under thermal equilibrium
At critical temperature
Grashoff number and Reynold number
Grashoff number and Prandtl number
Prandtl number and Reynold number
Grashoff number, Prandtl number and Reynold number
Grashoff number
Biot number
Stanton number
Prandtl number
J/m² sec
J/m °K sec
W/m °K
Option (B) and (C) above
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
Different heat contents
Different specific heat
Different atomic structure
Different temperatures
Minimum energy
Maximum energy
Both (A) and (B)
None of these
Increase
Decrease
Remain unaffected
May increase/decrease depending on temperature and thickness of insulation
Added insulation will increase heat loss
Added insulation will decrease heat loss
Convective heat loss will be less than conductive heat loss
Heat flux will decrease
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
Directly proportional to the thermal conductivity
Inversely proportional to density of substance
Inversely proportional to specific heat
All of the above
Change vapour into liquid
Change liquid into vapour
Increase the temperature of a liquid or vapour
Convert water into steam and superheat it
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
Iron
Lead
Concrete
Wood
Stanton number
Nusselt number
Biot number
Peclet number
tm = (Δt1 - Δt2)/ loge (Δt1/Δt2)
tm = loge (Δt1/Δt2)/ (Δt1 - Δt2)
tm = tm = (Δt1 - Δt2) loge (Δt1/Δt2)
tm = loge (Δt1 - Δt2)/ Δt1/Δt2
Thermal resistance
Thermal coefficient
Temperature gradient
Thermal conductivity
0.1
0.3
0.7
1.7
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
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
Increases
Decreases
Remain constant
May increase or decrease depending on temperature