Molecular size
Temperature
Volume
Pressure
B. Temperature
Melting point of ice
Melting point of wax
Boiling point of liquids
None of these
Reversible isothermal
Irreversible isothermal
Reversible adiabatic
None of these
Like internal energy and enthalpy, the absolute value of standard entropy for elementary substances is zero
Melting of ice involves increase in enthalpy and a decrease in randomness
The internal energy of an ideal gas depends only on its pressure
Maximum work is done under reversible conditions
TR/(T2 - TR) × (T1 - T2)/T1
TR/(T2 - TR) × T1/(T1 - T2)
TR/(T1 - TR) × (T1 - T2)/T1
None of these
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
72
92
142
192
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
(∂T/∂V)S = - (∂P/∂S)V
(∂S/∂P)T = - (∂V/∂T)P
(∂V/∂S)P = (∂T/∂P)S
(∂S/∂V)T = (∂P/∂T)V
0°C and 760 mm Hg
15°C and 760 mm Hg
20°C and 760 mm Hg
0°C and 1 kgf/cm2
Zero
50%
Almost 100%
unpredictable
Molal concentration difference
Molar free energy
Partial molar free energy
Molar free energy change
Lewis-Randall rule
Statement of Van't Hoff Equation
Le-Chatelier's principle
None of these
Fugacity
Partial pressure
Activity co-efficient
All (A), (B), and (C)
Enthalpy remains constant
Entropy remains constant
Temperature remains constant
None of these
State functions
Path functions
Intensive properties
Extensive properties
Compressibility
Work done under adiabatic condition
Work done under isothermal condition
Co-efficient of thermal expansion
Increases, for an exothermic reaction
Decreases, for an exothermic reaction
Increases, for an endothermic reaction
None of these
Ideal compression of air
Free expansion of an ideal gas
Adiabatic expansion of steam in a turbine
Adiabatic compression of a perfect gas
Reaction mechanism
Calculation of rates
Energy transformation from one form to another
None of these
Solid-vapor
Solid-liquid
Liquid-vapor
All (A), (B) and (C)
Kelvin's
Antoines
Kirchoffs
None of these
Not liquify (barring exceptions)
Immediately liquify
Never liquify however high the pressure may be
None of these
Chemical potential
Surface tension
Heat capacity
None of these
Molecular size
Volume
Pressure
Temperature
Entropy
Gibbs free energy
Internal energy
All (A), (B) & (C)
Pressure and temperature
Reduced pressure and reduced temperature
Critical pressure and critical temperature
None of these
Below
At
Above
Either 'b' or 'c'
μi = (∂F/∂ni)T, P, ni
μi = (∂A/∂ni)T, P, ni
μi = (∂F/∂ni)T, P
μi = (∂A/∂ni)T, P
A heating effect
No change in temperature
A cooling effect
Either (A) or (C)
Endothermic
Exothermic
Isothermal
Adiabatic