Vapour pressure is relatively low and the temperature does not vary over wide limits
Vapour obeys the ideal gas law and the latent heat of vaporisation is constant
Volume in the liquid state is negligible compared with that in the vapour state
All (A), (B) and (C)
D. All (A), (B) and (C)
Increases
Decreases
Remains unchanged
Decreases linearly
TVγ-1 = constant
p1-γ.TY = constant
PVγ = constant
None of these
Violates second law of thermodynamics
Involves transfer of heat from low temperature to high temperature
Both (A) and (B)
Neither (A) nor (B)
dE = CpdT
dE = CvdT
dQ = dE + pdV
dW = pdV
Vapor pressure
Partial pressure
Chemical potential
None of these
Unity
Activity
Both (A) & (B)
Neither (A) nor (B)
Isothermal
Adiabatic
Isobaric
Isochoric
Pressure
Volume
Mass
None of these
Mole fraction
Fugacity at the same temperature and pressure
Partial pressure
None of these
Boyle
Inversion
Critical
Reduced
Molar concentration
Temperature
Internal energy
None of these
Pressure remains constant
Pressure is increased
Temperature remains constant
None of these
The statement as per Gibbs-Helmholtz
Called Lewis-Randall rule
Henry's law
None of these
Less than
More than
Equal to or higher than
Less than or equal to
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Minimum temperature attainable
Temperature of the heat reservoir to which a Carnot engine rejects all the heat that is taken in
Temperature of the heat reservoir to which a Carnot engine rejects no heat
None of these
Increase the partial pressure of H2
Increase the partial pressure of I2
Increase the total pressure and hence shift the equilibrium towards the right
Not affect the equilibrium conditions
< 0
> 0
= 0
None of these
Increases with rise in pressure
Decreases with rise in pressure
Is independent of pressure
Is a path function
0
< 0
< 1
> 1
-94 kcal
+94 kcal
> 94 kcal
< -94 kcal
1.572
1.9398
3.389
4.238
Pressure
Composition
Temperature
All (A), (B) and (C)
Critical
Triple
Freezing
Boiling
Non-flow reversible
Adiabatic
Both (A) and (B)
Neither (A) nor (B)
Virial co-efficients are universal constants
Virial co-efficients 'B' represents three body interactions
Virial co-efficients are function of temperature only
For some gases, Virial equations and ideal gas equations are the same
3
1
2
0
Infinity
Unity
Constant
Negative
Vapour pressure is relatively low and the temperature does not vary over wide limits
Vapour obeys the ideal gas law and the latent heat of vaporisation is constant
Volume in the liquid state is negligible compared with that in the vapour state
All (A), (B) and (C)
Endothermic
Exothermic
Isothermal
Adiabatic