The expansion of a gas in vacuum is an irreversible process
An isometric process is a constant pressure process
Entropy change for a reversible adiabatic process is zero
Free energy change for a spontaneous process is negative
B. An isometric process is a constant pressure process
Pressure to critical pressure
Critical pressure to pressure
Pressure to pseudocritical pressure
Pseudocritical pressure to pressure
Phase rule variables are intensive properties
Heat and work are both state function
The work done by expansion of a gas in vacuum is zero
CP and CV are state function
30554
10373
4988.4
4364.9
Number of intermediate chemical reactions involved
Pressure and temperature
State of combination and aggregation in the beginning and at the end of the reaction
None of these
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance
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
Less than
Same as
More than
Half
Decrease in temperature
Increase in temperature
No change in temperature
Change in temperature which is a function of composition
Low pressure and high temperature
Low pressure and low temperature
High pressure and low temperature
High pressure and high temperature
The values of (∂P/∂V)T and (∂2P/∂V2)T are zero for a real gas at its critical point
Heat transferred is equal to the change in the enthalpy of the system, for a constant pressure, non-flow, mechanically reversible process
Thermal efficiency of a Carnot engine depends upon the properties of the working fluid besides the source & sink temperatures
During a reversible adiabatic process, the entropy of a substance remains constant
12 P1V1
6 P1 V1
3 P1V1
P1 V1
Low pressure & high temperature
High pressure & low temperature
Low pressure & low temperature
None of these
Heating takes place
Cooling takes place
Pressure is constant
Temperature is constant
Zero
Positive
Negative
None of these
Temperature only
Temperature and pressure only
Temperature, pressure and liquid composition xi only
Temperature, pressure, liquid composition xi and vapour composition yi
Zero
Unity
Infinity
None of these
T
√T
T2
1/√T
-2 RT ln 0.5
-RT ln 0.5
0.5 RT
2 RT
Increase the partial pressure of H2
Increase the partial pressure of I2
Increase the total pressure and hence shift the equilibrium towards the right
Not affect the equilibrium conditions
Pressure vs. enthalpy
Pressure vs. volume
Enthalpy vs. entropy
Temperature vs. entropy
Decreases
Increases
Remain same
Decreases linearly
F = A + PV
F = E + A
F = A - TS
F = A + TS
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
its internal energy (U) decreases and its entropy (S) increases
U and S both decreases
U decreases but S is constant
U is constant but S decreases
300 × (32/7)
300 × (33/5)
300 × (333/7)
300 × (35/7)
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Triple point
Boiling point
Below triple point
Always
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
Le-Chatelier principle
Kopp's rule
Law of corresponding state
Arrhenius hypothesis
Temperature
Pressure
Volume
None of these