Gibbs-Duhem
Maxwell's
Clapeyron
None of these
C. Clapeyron
Kelvin's
Antoines
Kirchoffs
None of these
Heat absorbed
Work done
Both (A) & (B)
Neither (A) nor (B)
Saturated vapour
Solid
Gas
Liquid
Low temperature
High pressure
Both (A) and (B)
Neither (A) nor (B)
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Below
At
Above
Either 'b' or 'c'
Mole fraction
Activity
Pressure
Activity co-efficient
Freezing
Triple
Boiling
Boyle
0
273
25
None of these
Entropy
Temperature
Enthalpy
Pressure
Amount of energy transferred
Direction of energy transfer
Irreversible processes only
Non-cyclic processes only
With pressure changes at constant temperature
Under reversible isothermal volume change
During heating of an ideal gas
During cooling of an ideal gas
Only enthalpy change (ΔH) is negative
Only internal energy change (ΔE) is negative
Both ΔH and ΔE are negative
Enthalpy change is zero
Not a function of its pressure
Not a function of its nature
Not a function of its temperature
Unity, if it follows PV = nRT
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)
(atm)Δx, when Δx is negative
(atm)Δx, when Δx is positive
Dimensionless, when Δx = 0
(atm)Δx2, when Δx > 0
Enthalpy remains constant
Entropy remains constant
Temperature remains constant
None of these
0
1
∞
None of these
Volume, mass and number of moles
Free energy, entropy and enthalpy
Both (A) and (B)
None of these
Gibbs-Duhem
Gibbs-Helmholtz
Maxwell's
None of these
< 0
> 0
= 0
None of these
Zero
One
Infinity
Negative
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
50 kcal/hr
200 BTU/hr
200 BTU/minute
200 BTU/day
More than
Less than
Equal to
Not related to
ΔF = ΔH + T [∂(ΔF)/∂T]P
ΔF = ΔH - TΔT
d(E - TS) T, V < 0
dP/dT = ΔHvap/T.ΔVvap
300 × (32/7)
300 × (33/5)
300 × (333/7)
300 × (35/7)
Low T, low P
High T, high P
Low T, high P
High T, low P
Zeroth
First
Second
Third
Increase the partial pressure of I2
Decrease the partial pressure of HI
Diminish the degree of dissociation of HI
None of these