dP/dT = ΔH/TΔV
ln P = - (ΔH/RT) + constant
ΔF = ΔH + T [∂(ΔF)/∂T]P
None of these
B. ln P = - (ΔH/RT) + constant
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
3
2
1
0
Adiabatic process
Isothermal process
Isobaric process
All require same work
Activity
Fugacity
Activity co-efficient
Fugacity co-efficient
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
349
651
667
1000
Entropy
Gibbs free energy
Internal energy
All (A), (B) & (C)
Lewis-Randall rule
Statement of Van't Hoff Equation
Le-Chatelier's principle
None of these
Solution
Vaporisation
Formation
Sublimation
2HI H2 + I2
N2O4 2NO2
2SO2 + O2 2SO3
None of these
(atm)Δx, when Δx is negative
(atm)Δx, when Δx is positive
Dimensionless, when Δx = 0
(atm)Δx2, when Δx > 0
No heat and mass transfer
No mass transfer but heat transfer
Mass and energy transfer
None of these
Only F decreases
Only A decreases
Both F and A decreases
Both F and A increase
Both the processes are adiabatic
Both the processes are isothermal
Process A is isothermal while B is adiabatic
Process A is adiabatic while B is isothermal
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
Sublimation
Fusion
Transition
Vaporisation
x
x + 1
x + 2
x + 3
Equation of state
Gibbs Duhem equation
Ideal gas equation
None of these
Chemical potentials of a given component should be equal in all phases
Chemical potentials of all components should be same in a particular phase
Sum of the chemical potentials of any given component in all the phases should be the same
None of these
Below
At
Above
Either 'b' or 'c'
0
< 0
< 1
> 1
0
1
y = 1.44
1.66
Zero
One
Two
Three
Same
Doubled
Halved
One fourth of its original value
Increases
Decreases
Remains unchanged
Decreases linearly
Specific volume
Work
Pressure
Temperature
+ve
-ve
0
∞
Increase the partial pressure of I2
Decrease the partial pressure of HI
Diminish the degree of dissociation of HI
None of these
A closed system does not permit exchange of mass with its surroundings but may permit exchange of energy.
An open system permits exchange of both mass and energy with its surroundings
The term microstate is used to characterise an individual, whereas macro-state is used to designate a group of micro-states with common characteristics
None of the above
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