Enthalpy
Entropy
Pressure
None of these
A. Enthalpy
Mole fraction
Fugacity at the same temperature and pressure
Partial pressure
None of these
Increase
Decrease
Remain unaltered
Increase or decrease; depends on the particular reaction
Chemical potentials of a given component should be equal in all phases
Chemical potentials of all components should be same in a particular phase
Sum of the chemical potentials of any given component in all the phases should be the same
None of these
High thermal conductivity
Low freezing point
Large latent heat of vaporisation
High viscosity
State functions
Path functions
Intensive properties
Extensive properties
12 P1V1
6 P1 V1
3 P1V1
P1 V1
30554
10373
4988.4
4364.9
0
1
2
3
Van Laar
Margules
Gibbs-Duhem
Gibbs-Duhem-Margules
State function
Macroscopic property
Extensive property
None of these
Low pressure and high temperature
Low pressure and low temperature
High pressure and low temperature
High pressure and high temperature
Pressure
Volume
Temperature
All (A), (B) & (C)
Binary solutions
Ternary solutions
Azeotropic mixture only
None of these
Adiabatic process
Isothermal process
Isobaric process
All require same work
Increases
Decreases
Remains unchanged
Decreases linearly
0
∞
50
100
0
∞
+ve
-ve
The conversion for a gas phase reaction increases with decrease in pressure, if there is an increase in volume accompanying the reaction
With increase in temperature, the equilibrium constant increases for an exothermic reaction
The equilibrium constant of a reaction depends upon temperature only
The conversion for a gas phase reaction increases with increase in pressure, if there is a decrease in volume accompanying the reaction
At constant pressure
By throttling
By expansion in an engine
None of these
More stable
Less stable
Not at all stable (like nascent O2)
Either more or less stable; depends on the compound
Zero
Positive
Negative
None of these
Two temperatures only
Pressure of working fluid
Mass of the working fluid
Mass and pressure both of the working fluid
∞
1
0
-ve
At low temperature and high pressure
At standard state
Both (A) and (B)
In ideal state
3
4
5
6
By throttling
By expansion in an engine
At constant pressure
None of these
The available energy in an isolated system for all irreversible (real) processes decreases
The efficiency of a Carnot engine increases, if the sink temperature is decreased
The reversible work for compression in non-flow process under isothermal condition is the change in Helmholtz free energy
All (A), (B) and (C)
Reversible and isothermal
Irreversible and constant enthalpy
Reversible and constant entropy
Reversible and constant enthalpy
d ln p/dt = Hvap/RT2
d ln p/dt = RT2/Hvap
dp/dt = RT2/Hvap
dp/dt = Hvap/RT2
Superheated vapour
Partially condensed vapour with quality of 0.9
Saturated vapour
Partially condensed vapour with quality of 0.1