Violates second law of thermodynamics
Involves transfer of heat from low temperature to high temperature
Both (A) and (B)
Neither (A) nor (B)
B. Involves transfer of heat from low temperature to high temperature
Lewis-Randall
Margules
Van Laar
Both (B) & (C)
3
1
2
0
Increase the partial pressure of I2
Decrease the partial pressure of HI
Diminish the degree of dissociation of HI
None of these
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
Positive
Negative
Zero
May be positive or negative
100,000 kW
160,000 kW
200,000 kW
320,000 kW
Increases with rise in pressure
Decreases with rise in pressure
Is independent of pressure
Is a path function
(∂P/∂V)T
(∂V/∂T)P
(∂P/∂V)V
All (A), (B) & (C)
Moisture free ice
Solid helium
Solid carbon dioxide
None of these
State functions
Path functions
Intensive properties
Extensive properties
Van Laar equation
Margules equation
Wilson's equation
All (A), (B) and (C)
Gibbs-Duhem equation
Gibbs-Helmholtz equation
Third law of thermodynamics
Joule-Thomson effect
Freezing
Triple
Boiling
Boyle
Cold reservoir approaches zero
Hot reservoir approaches infinity
Either (A) or (B)
Neither (A) nor (B)
P + F - C = 2
C = P - F + 2
F = C - P - 2
P = F - C - 2
Path
Point
State
None of these
Pressure remains constant
Pressure is increased
Temperature remains constant
None of these
Activity co-efficient is dimensionless.
In case of an ideal gas, the fugacity is equal to its pressure.
In a mixture of ideal gases, the fugacity of a component is equal to the partial pressure of the component.
The fugacity co-efficient is zero for an ideal gas
Becomes zero
Becomes infinity
Equals 1 kcal/kmol °K
Equals 0.24 kcal/kmol °K
Low temperature
High pressure
Both (A) and (B)
Neither (A) nor (B)
Heat capacity of a crystalline solid is zero at absolute zero temperature
Heat transfer from low temperature to high temperature source is not possible without external work
Gases having same reduced properties behaves similarly
None of these
Compression ratio of an Otto engine is comparatively higher than a diesel engine
Efficiency of an Otto engine is higher than that of a diesel engine for the same compression ratio
Otto engine efficiency decreases with the rise in compression ratio, due to decrease in work produced per quantity of heat
Diesel engine normally operates at lower compression ratio than an Otto engine for an equal output of work
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
Like internal energy and enthalpy, the absolute value of standard entropy for elementary substances is zero
Melting of ice involves increase in enthalpy and a decrease in randomness
The internal energy of an ideal gas depends only on its pressure
Maximum work is done under reversible conditions
None of these
Low temperature and high pressure
Low temperature and low pressure
High temperature and high pressure
High temperature and low pressure
Polar
Non-polar
Both (A) & (B)
Neither (A) nor (B)
Pressure vs. enthalpy
Pressure vs. volume
Enthalpy vs. entropy
Temperature vs. entropy
Zero
Unity
Infinity
An indeterminate value
Pressure
Solubility
Temperature
None of these