Two
One
Zero
Three
B. One
Isobaric
Isothermal
Isentropic
Isometric
Increase
Decrease
No change
None of these
0
∞
+ve
-ve
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
Oxygen
Nitrogen
Air
Hydrogen
2.73
28.3
273
283
Matter
Energy
Neither matter nor energy
Both matter and energy
Pressure
Composition
Temperature
All (A), (B) and (C)
More in vapour phase
More in liquid phase
Same in both the phases
Replaced by chemical potential which is more in vapour phase
Saturated vapour
Solid
Gas
Liquid
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
Lewis-Randall rule
Statement of Van't Hoff Equation
Le-Chatelier's principle
None of these
F = E - TS
F = H - TS
F = H + TS
F = E + TS
dP/dT = ΔH/TΔV
ln P = - (ΔH/RT) + constant
ΔF = ΔH + T [∂(ΔF)/∂T]P
None of these
Pressure
Composition
Temperature
All (A), (B) and (C)
0
1
2
3
Work done under adiabatic condition
Co-efficient of thermal expansion
Compressibility
None of these
Adiabatic expansion
Joule-Thomson effect
Both (A) and (B)
Neither (A) nor (B)
Does not need the addition of external work for its functioning
Transfers heat from high temperature to low temperature
Accomplishes the reverse effect of the heat engine
None of these
Stirling
Brayton
Rankine
None of these
Carnot
Air
Absorption
vapour-ejection
Adiabatic process
Endothermic reaction
Exothermic reaction
Process involving a chemical reaction
RT d ln P
RT d ln f
R d ln f
None of these
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
Isobaric
Adiabatic
Isenthalpic
Both (B) & (C)
Entropy
Gibbs free energy
Internal energy
All (A), (B) & (C)
Two different gases behave similarly, if their reduced properties (i.e. P, V and T) are same
The surface of separation (i. e. the meniscus) between liquid and vapour phase disappears at the critical temperature
No gas can be liquefied above the critical temperature, howsoever high the pressure may be.
The molar heat of energy of gas at constant volume should be nearly constant (about 3 calories)
Compressibility
Work done under adiabatic condition
Work done under isothermal condition
Co-efficient of thermal expansion
Single phase fluid of varying composition
Single phase fluid of constant composition
Open as well as closed systems
Both (B) and (C)
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance