The statement as per Gibbs-Helmholtz
Called Lewis-Randall rule
Henry's law
None of these
B. Called Lewis-Randall rule
Temperature
Pressure
Composition
All (A), (B) and (C)
Increases
Decreases
Remains unchanged
Decreases linearly
Increases
Decreases
Remains unchanged
Data insufficient, can't be predicted
Does not depend upon temperature
Is independent of pressure only
Is independent of volume only
Is independent of both pressure and volume
More than
Less than
Equal to
Not related to
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
100
50
205
200
A gas may have more than one inversion temperatures
The inversion temperature is different for different gases
The inversion temperature is same for all gases
The inversion temperature is the temperature at which Joule-Thomson co-efficient is infinity
(∂T/∂V)S = - (∂P/∂S)V
(∂S/∂P)T = - (∂V/∂T)P
(∂V/∂S)P = (∂T/∂P)S
(∂S/∂V)T = (∂P/∂T)V
(dF)T, p <0
(dF)T, p = 0
(dF)T, p > 0
(dA)T, v >0
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
Melting of ice
Condensation of alcohol vapor
Sudden bursting of a cycle tube
Evaporation of water
R loge 4
R log10 4
Cv log10 4
Cv loge 4
Le-Chatelier principle
Kopp's rule
Law of corresponding state
Arrhenius hypothesis
Adiabatic expansion
Joule-Thomson effect
Both (A) and (B)
Neither (A) nor (B)
(∂E/∂T)V
(∂E/∂V)T
(∂E/∂P)V
(∂V/∂T)P
< 0
> 0
= 0
None of these
Pressure and temperature
Reduced pressure and reduced temperature
Critical pressure and critical temperature
None of these
Shifting the equilibrium towards right
Shifting the equilibrium towards left
No change in equilibrium condition
None of these
0
+ve
-ve
∞
(∂T/∂V)S = (∂p/∂S)V
(∂T/∂P)S = (∂V/∂S)P
(∂P/∂T)V = (∂S/∂V)T
(∂V/∂T)P = -(∂S/∂P)T
Not have a sub-atmospheric vapour pressure at the temperature in the refrigerator coils
Not have unduly high vapour pressure at the condenser temperature
Both (A) and (B)
Have low specific heat
Binary solutions
Ternary solutions
Azeotropic mixture only
None of these
Path
Point
State
None of these
Is the analog of linear frictionless motion in machines
Is an idealised visualisation of behaviour of a system
Yields the maximum amount of work
Yields an amount of work less than that of a reversible process
States that n1dμ1 + n2dμ2 + ....njdμj = 0, for a system of definite composition at constant temperature and pressure
Applies only to binary systems
Finds no application in gas-liquid equilibria involved in distillation
None of these
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
-94 kcal
+94 kcal
> 94 kcal
< -94 kcal
448
224
22.4
Data insufficient; can't be computed
√(2KT/m)
√(3KT/m)
√(6KT/m)
3KT/m