Increases
Decreases
Remains unchanged
Data insufficient, can't be predicted
C. Remains unchanged
Van Laar
Margules
Gibbs-Duhem
Gibbs-Duhem-Margules
Free expansion of a gas
Compression of air in a compressor
Expansion of steam in a turbine
All (A), (B) & (C)
Same in both the phases
Zero in both the phases
More in vapour phase
More in liquid phase
Zeroth
First
Second
Third
μi = (∂F/∂ni)T, P, ni
μi = (∂A/∂ni)T, P, ni
μi = (∂F/∂ni)T, P
μi = (∂A/∂ni)T, P
6738.9
6753.5
7058.3
9000
Zero
Positive
Negative
Indeterminate
Isothermal
Adiabatic
Isobaric
Isochoric
4 J
∞
0
8 J
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
Tds = dE + dW
dE - dW = Tds
dW - dE = Tds
Tds - dW + dE >0
Activity
Fugacity
Activity co-efficient
Fugacity co-efficient
Isobaric
Adiabatic
Isenthalpic
Both (B) & (C)
Straight line
Sine curve
Parabola
Hyperbola
Becomes zero
Becomes infinity
Equals 1 kcal/kmol °K
Equals 0.24 kcal/kmol °K
By throttling
By expansion in an engine
At constant pressure
None of these
Shifting the equilibrium towards right
Shifting the equilibrium towards left
No change in equilibrium condition
None of these
35 K
174 K
274 K
154 K
A real gas on expansion in vacuum gets heated up
An ideal gas on expansion in vacuum gets cooled
An ideal gas on expansion in vacuum gets heated up
A real gas on expansion in vacuum cools down whereas ideal gas remains unaffected
Heat capacity
Molal heat capacity
Pressure
Concentration
Hess's
Kirchoff's
Lavoisier and Laplace
None of these
RT d ln P
R d ln P
R d ln f
None of these
CV
Entropy change
Gibbs free energy
None of these
Expansion of an ideal gas against constant pressure
Atmospheric pressure vaporisation of water at 100°C
Solution of NaCl in water at 50°C
None of these
Increases
Decreases
Remain constant
Increases linearly
Isothermal
Irreversible
Adiabatic
Reversible
0
1
2
3
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
Is the most efficient of all refrigeration cycles
Has very low efficiency
Requires relatively large quantities of air to achieve a significant amount of refrigeration
Both (B) and (C)
0.25
0.5
0.75
1