Addition of inert gas favours the forward reaction, when Δx is positive
Pressure has no effect on equilibrium, when Δn = 0
Addition of inert gas has no effect on the equilibrium constant at constant volume for any value of Δx (+ ve, - ve) or zero)
All 'a', 'b' & 'c'
D. All 'a', 'b' & 'c'
Less pronounced
More pronounced
Equal
Data insufficient, can't be predicted
If an insoluble gas is passed through a volatile liquid placed in a perfectly insulated container, the temperature of the liquid will increase
A process is irreversible as long as Δ S for the system is greater than zero
The mechanical work done by a system is always equal to∫P.dV
The heat of formation of a compound is defined as the heat of reaction leading to the formation of the compound from its reactants
Adiabatic expansion
Joule-Thomson effect
Both (A) and (B)
Neither (A) nor (B)
Closed
Open
Isolated
Non-thermodynamic
(∂T/∂V)S = - (∂P/∂S)V
(∂S/∂P)T = - (∂V/∂T)P
(∂V/∂S)P = (∂T/∂P)S
(∂S/∂V)T = (∂P/∂T)V
Straight line
Sine curve
Parabola
Hyperbola
Slower than Y
Faster than Y
Three times slower than Y
Three times faster than Y
Shift the equilibrium towards right
Give higher yield of NH3
Both (B) and (C)
Neither (A) nor (B)
Lewis-Randall rule
Statement of Van't Hoff Equation
Le-Chatelier's principle
None of these
Extensive property
Intensive property
Force which drives the chemical system to equilibrium
Both (B) and (C)
Expansion in an engine
Following a constant pressure cycle
Throttling
None of these
Decrease on addition of Cl2
Increase on addition of an inert gas at constant pressure
Decrease on increasing the pressure of the system
None of these
Increases
Decreases
Remain constant
Increases linearly
Adiabatic
Isometric
Isentropic
Isothermal
Rectangle
Rhombus
Trapezoid
Circle
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
Property of the system
Path function
Point function
State description of a system
Latent heat of vaporisation
Chemical potential
Molal boiling point
Heat capacity
Decreases
Increases
Remain same
May increase or decrease; depends on the nature of the gas
Superheated vapour
Partially condensed vapour with quality of 0.9
Saturated vapour
Partially condensed vapour with quality of 0.1
0
1
2
3
Sub-cooled
Saturated
Non-solidifiable
None of these
Calorific value
Heat of reaction
Heat of combustion
Heat of formation
Isothermal
Adiabatic
Both (A) & (B)
Neither (A) nor (B)
CV
Enthalpy change
Free energy change
None of these
1.987 cal/gm mole °K
1.987 BTU/lb. mole °R
Both (A) and (B)
Neither (A) nor (B)
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
At constant pressure
By throttling
By expansion in an engine
None of these
Zero
Positive
Negative
Indeterminate
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