Same as Carnot cycle
Same as reverse Carnot cycle
Dependent on the refrigerant's properties
The least efficient of all refrigeration processes
B. Same as reverse Carnot cycle
0
1
2
3
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
State functions
Path functions
Intensive properties
Extensive properties
Adiabatic
Isothermal
Isometric
None of these
d ln p/dt = Hvap/RT2
d ln p/dt = RT2/Hvap
dp/dt = RT2/Hvap
dp/dt = Hvap/RT2
Saturated vapour
Solid
Gas
Liquid
Freon-12
Ethylene
Ammonia
Carbon dioxide
< 0
> 0
= 0
None of these
Isothermally
Isobarically
Adiabatically
None of these
Any
A perfect
An easily liquefiable
A real
Air cycle
Carnot cycle
Ordinary vapor compression cycle
Vapor compression with a reversible expansion engine
Simultaneous pressure & temperature change
Heating
Cooling
Both (B) and (C)
0
∞
+ve
-ve
Cp of monatomic gases such as metallic vapor is about 5 kcal/kg.atom
The heat capacity of solid inorganic substance is exactly equal to the heat capacity of the substance in the molten state
There is an increase in entropy, when a spontaneous change occurs in an isolated system
At absolute zero temperature, the heat capacity for many pure crystalline substances is zero
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Adiabatic process
Endothermic reaction
Exothermic reaction
Process involving a chemical reaction
Tds = dE - dW = 0
dE - dW - Tds = 0
Tds - dE + dW < 0
Tds - dT + dW < 0
ΔF = ΔH + T [∂(ΔF)/∂T]P
ΔF = ΔH - TΔT
d(E - TS) T, V < 0
dP/dT = ΔHvap/T.ΔVvap
Increases with increase in pressure
Decreases with increase in temperature
Is independent of temperature
None of these
Less than
More than
Equal to or higher than
Less than or equal to
Increases
Decreases
Remains unchanged
First decreases and then increases
Rate of change of vapour pressure with temperature
Effect of an inert gas on vapour pressure
Calculation of ΔF for spontaneous phase change
Temperature dependence of heat of phase transition
+ve
0
-ve
∞
0
1
2
3
Gibbs-Duhem equation
Gibbs-Helmholtz equation
Third law of thermodynamics
Joule-Thomson effect
Reverse Carnot cycle
Ordinary vapour-compression cycle
Vapour-compression process with a reversible expansion engine
Air refrigeration cycle
0
1
2
3
Equal to its density
The reciprocal of its density
Proportional to pressure
None of these
Enthalpies of all elements in their standard states are assumed to be zero
Combustion reactions are never endothermic in nature
Heat of reaction at constant volume is equal to the change in internal energy
Clausius-Clapeyron equation is not applicable to melting process
Less pronounced
More pronounced
Equal
Data insufficient, can't be predicted