Enthalpy
Entropy
Pressure
None of these
Maxwell's equation
Thermodynamic equation of state
Equation of state
Redlich-Kwong equation of state
At constant pressure, solubility of a gas in a liquid diminishes with rise in temperature
Normally, the gases which are easily liquefied are more soluble in common solvents
The gases which are capable of forming ions in aqueous solution are much more soluble in water than in other solvents
At constant pressure, solubility of a gas in a liquid increases with rise in temperature
Unity
Zero
That of the heat of reaction
Infinity
The expansion of a gas in vacuum is an irreversible process
An isometric process is a constant pressure process
Entropy change for a reversible adiabatic process is zero
Free energy change for a spontaneous process is negative
(R/ΔH) (1/T1 - 1/T2)
(ΔH/R) (1/T1 - 1/T2)
(ΔH/R) (1/T2 - 1/T1)
(1/R) (1/T1 - 1/T2)
Violates second law of thermodynamics
Involves transfer of heat from low temperature to high temperature
Both (A) and (B)
Neither (A) nor (B)
(∂P/∂V)T
(∂V/∂T)P
(∂P/∂V)V
All (A), (B) & (C)
0
273
25
None of these
The chemical potential of a pure substance depends upon the temperature and pressure
The chemical potential of a component in a system is directly proportional to the escaping tendency of that component
The chemical potential of ith species (μi) in an ideal gas mixture approaches zero as the pressure or mole fraction (xi) tends to be zero at constant temperature
The chemical potential of species 'i' in the mixture (μi) is mathematically represented as,μi = ∂(nG)/∂ni]T,P,nj where, n, ni and nj respectively denote the total number of moles, moles of ith species and all mole numbers except ith species. 'G' is Gibbs molar free energy
Temperature
Pressure
Volume
None of these
(p + a/V2)(V - b) = nRT
PV = nRT
PV = A + B/V + C/V2 + D/V3 + ...
None of these
Entropy
Temperature
Enthalpy
Pressure
Ideal compression of air
Free expansion of an ideal gas
Adiabatic expansion of steam in a turbine
Adiabatic compression of a perfect gas
Bertholet equation
Clausius-Clapeyron equation
Beattie-Bridgeman equation
None of these
Pressure
Volume
Temperature
All (A), (B) and (C)
Zero
+ve
-ve
Dependent on the path
Contracts
Expands
Has same volume
May contract or expand
Equilibrium
Adiabatic
Steady
Unsteady
Indeterminate
Zero
Negative
None of these
Freezing
Triple
Boiling
Boyle
Departure from ideal solution behaviour
Departure of gas phase from ideal gas law
Vapour pressure of liquid
None of these
Kelvin's
Antoines
Kirchoffs
None of these
Binary solutions
Ternary solutions
Azeotropic mixture only
None of these
Calorific value
Heat of reaction
Heat of combustion
Heat of formation
Low pressure & high temperature
High pressure & low temperature
Low pressure & low temperature
None of these
Volume
Temperature
Pressure
None of these
0
∞
+ ve
- ve
Volume
Pressure
Temperature
All (A), (B) and (C)
The energy change of a system undergoing any reversible process is zero
It is not possible to transfer heat from a lower temperature to a higher temperature
The total energy of system and surrounding remains the same
None of the above