Zero
One
Two
Three
B. One
Reversible and isothermal
Isothermal and irreversible
Reversible and adiabatic
Adiabatic and irreversible
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance
μ = (∂P/∂T)H
μ = (∂T/∂P)H
μ = (∂E/∂T)H
μ = (∂E/∂P)H
1.987 cal/gm mole °K
1.987 BTU/lb. mole °R
Both (A) and (B)
Neither (A) nor (B)
Reverse Carnot cycle
Ordinary vapour-compression cycle
Vapour-compression process with a reversible expansion engine
Air refrigeration cycle
Enthalpy
Pressure
Entropy
None of these
SO2
NH3
CCl2F2
C2H4Cl2
RT d ln P
RT d ln f
R d ln f
None of these
0
1
2
3
Gibbs-Duhem equation
Gibbs-Helmholtz equation
Third law of thermodynamics
Joule-Thomson effect
Hour
Day
Minute
Second
Property of the system
Path function
Point function
State description of a system
Specific heat
Latent heat of vaporisation
Viscosity
Specific vapor volume
Chemical potential
Fugacity
Both (A) and (B)
Neither (A) nor (B)
Does not depend upon temperature
Is independent of pressure only
Is independent of volume only
Is independent of both pressure and volume
Accomplishes only space heating in winter
Accomplishes only space cooling in summer
Accomplishes both (A) and (B)
Works on Carnot cycle
Cold reservoir approaches zero
Hot reservoir approaches infinity
Either (A) or (B)
Neither (A) nor (B)
The net change in entropy in any reversible cycle is always zero
The entropy of the system as a whole in an irreversible process increases
The entropy of the universe tends to a maximum
The entropy of a substance does not remain constant during a reversible adiabatic change
Low temperature
High pressure
Both (A) and (B)
Neither (A) nor (B)
Calorific value
Heat of reaction
Heat of combustion
Heat of formation
Adiabatic process
Endothermic reaction
Exothermic reaction
Process involving a chemical reaction
Pressure vs. enthalpy
Pressure vs. volume
Enthalpy vs. entropy
Temperature vs. entropy
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
Sublimation
Vaporisation
Melting
Either (A), (B) or (C)
0
∞
+ve
-ve
Fugacity
Partial pressure
Activity co-efficient
All (A), (B), and (C)
n = y = 1.4
n = 0
n = 1
n = 1.66
Volume, mass and number of moles
Free energy, entropy and enthalpy
Both (A) and (B)
None of these
72
92
142
192
Freon
Liquid sulphur dioxide
Methyl chloride
Ammonia