Molar volume, density, viscosity and boiling point
Refractive index and surface tension
Both (A) and (B)
None of these
C. Both (A) and (B)
RT ln K
-RT ln K
-R ln K
T ln K
(∂T/∂V)S = (∂p/∂S)V
(∂T/∂P)S = (∂V/∂S)P
(∂P/∂T)V = (∂S/∂V)T
(∂V/∂T)P = -(∂S/∂P)T
If an insoluble gas is passed through a volatile liquid placed in a perfectly insulated container, the temperature of the liquid will increase
A process is irreversible as long as Δ S for the system is greater than zero
The mechanical work done by a system is always equal to∫P.dV
The heat of formation of a compound is defined as the heat of reaction leading to the formation of the compound from its reactants
Kinematic viscosity
Work
Temperature
None of these
Low pressure & high temperature
High pressure & low temperature
Low pressure & low temperature
None of these
0.25
0.5
0.75
1
(∂P/∂V)T
(∂V/∂T)P
(∂P/∂V)V
All (A), (B) & (C)
6738.9
6753.5
7058.3
9000
Adiabatic process
Endothermic reaction
Exothermic reaction
Process involving a chemical reaction
Representing actual behaviour of real gases
Representing actual behaviour of ideal gases
The study of chemical equilibria involving gases at atmospheric pressure
None of these
Binary solutions
Ternary solutions
Azeotropic mixture only
None of these
Only ΔE = 0
Only ΔH =0
ΔE = ΔH = 0
dQ = dE
Specific heat
Latent heat of vaporisation
Viscosity
Specific vapor volume
Adiabatic
Isothermal
Isometric
None of these
T
T and P
T, P and Z
T and Z
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
Enthalpy
Volume
Both 'a' & 'b'
Neither 'a' nor 'b'
Mole fraction
Activity
Pressure
Activity co-efficient
0
∞
50
100
Contracts
Expands
Does not change in volume
Either (A), (B) or (C)
Both the processes are adiabatic
Both the processes are isothermal
Process A is isothermal while B is adiabatic
Process A is adiabatic while B is isothermal
Enthalpies of all elements in their standard states are assumed to be zero
Combustion reactions are never endothermic in nature
Heat of reaction at constant volume is equal to the change in internal energy
Clausius-Clapeyron equation is not applicable to melting process
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance
0
1
∞
None of these
Two isothermal and two isentropic
Two isobaric and two isothermal
Two isochoric and two isobaric
Two isothermals and two isochoric
The amount of work needed is path dependent
Work alone cannot bring out such a change of state
The amount of work needed is independent of path
More information is needed to conclude anything about the path dependence or otherwise of the work needed
Expansion of a real gas
Reversible isothermal volume change
Heating of an ideal gas
Cooling of a real gas
Isothermal
Adiabatic
Isentropic
Polytropic
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
Van Laar equation
Margules equation
Wilson's equation
All (A), (B) and (C)