Melting point of ice
Melting point of wax
Boiling point of liquids
None of these
A. Melting point of ice
Free expansion of a gas
Compression of air in a compressor
Expansion of steam in a turbine
All (A), (B) & (C)
Single phase fluid of varying composition
Single phase fluid of constant composition
Open as well as closed systems
Both (B) and (C)
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
R loge 4
R log10 4
Cv log10 4
Cv loge 4
PV
2PV
PV/2
0
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the gas
Isolated
Open
Insulated
Closed
Minimum
Zero
Maximum
Indeterminate
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance
Zero
One
Infinity
Negative
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
Decreases in all spontaneous (or irreversible) processes
Change during a spontaneous process has a negative value
Remains unchanged in reversible processes carried at constant temperature and pressure
All (A), (B) and (C)
The concentration of each component should be same in the two phases
The temperature of each phase should be same
The pressure should be same in the two phases
The chemical potential of each component should be same in the two phases
Enthalpy
Entropy
Pressure
None of these
Entropy
Gibbs energy
Internal energy
Enthalpy
Joule-Thomson co-efficient
Specific heat at constant pressure (Cp)
co-efficient of thermal expansion
Specific heat at constant volume (CV)
+ve
0
-ve
∞
Increase
Decrease
Remain unchanged
First fall and then rise
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
Chemical potential
Surface tension
Heat capacity
None of these
Surface tension
Free energy
Specific heat
Refractive index
Same
Doubled
Halved
One fourth of its original value
Le-Chatelier principle
Kopp's rule
Law of corresponding state
Arrhenius hypothesis
4 J
∞
0
8 J
Heat pump
Heat engine
Carnot engine
None of these
Adiabatic
Isothermal
Isometric
None of these
A closed system does not permit exchange of mass with its surroundings but may permit exchange of energy.
An open system permits exchange of both mass and energy with its surroundings
The term microstate is used to characterise an individual, whereas macro-state is used to designate a group of micro-states with common characteristics
None of the above
Zeroth
First
Second
Third
It is exothermic
It is isenthalpic
It takes place isothermally
It takes place at constant volume
T1/(T1-T2)
T2/(T1-T2)
T1/T2
T2/R1