ds = 0
ds <0
ds > 0
ds = Constant
C. ds > 0
Less than
Same as
More than
Half
Zero
One
Infinity
Negative
Eutectic
Triple
Plait
Critical
μ° + RT ln f
μ°+ R ln f
μ° + T ln f
μ° + R/T ln f
μi = (∂F/∂ni)T, P, ni
μi = (∂A/∂ni)T, P, ni
μi = (∂F/∂ni)T, P
μi = (∂A/∂ni)T, P
Fugacity
Activity co-efficient
Free energy
All (A), (B) & (C)
A . x22
Ax1
Ax2
Ax12
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
TR/(T2 - TR) × (T1 - T2)/T1
TR/(T2 - TR) × T1/(T1 - T2)
TR/(T1 - TR) × (T1 - T2)/T1
None of these
Boyle
Inversion
Critical
Reduced
Molal concentration difference
Molar free energy
Partial molar free energy
Molar free energy change
Entropy
Gibbs free energy
Internal energy
All (A), (B) & (C)
Decrease in temperature
Increase in temperature
No change in temperature
Change in temperature which is a function of composition
The statement as per Gibbs-Helmholtz
Called Lewis-Randall rule
Henry's law
None of these
Temperature
Pressure
Volume
Entropy
Third law of thermodynamics
Second law of thermodynamics
Nernst heat theorem
Maxwell's relations
Latent heat of vaporisation
Chemical potential
Molal boiling point
Heat capacity
Only ΔE = 0
Only ΔH =0
ΔE = ΔH = 0
dQ = dE
(T2 - T1)/T2
(T2 - T1)/T1
(T1 - T2)/T2
(T1 - T2)/T1
Internal energy
Enthalpy
Entropy
All (A), (B) & (C)
Fugacity
Activity co-efficient
Free energy
None of these
Reaction mechanism
Calculation of rates
Energy transformation from one form to another
None of these
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
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
Solids
Liquids
Gases
All (A), (B) & (C)
Increases
Decreases
Remains unchanged
Data insufficient, can't be predicted
Directly proportional to pressure
Inversely proportional to pressure
Unity at all pressures
None of these
Reversible isothermal
Irreversible isothermal
Reversible adiabatic
None of these
Equal to its density
The reciprocal of its density
Proportional to pressure
None of these
Increases
Decreases
Remain same
Decreases linearly