Below
At
Above
Either 'b' or 'c'
A. Below
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
By throttling
By expansion in an engine
At constant pressure
None of these
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
2HI H2 + I2
N2O4 2NO2
2SO2 + O2 2SO3
None of these
Equal to its density
The reciprocal of its density
Proportional to pressure
None of these
Bomb
Separating
Bucket
Throttling
√(2KT/m)
√(3KT/m)
√(6KT/m)
3KT/m
F = E - TS
F = H - TS
F = H + TS
F = E + TS
Kelvin's
Antoines
Kirchoffs
None of these
Always greater than one
Same at the same reduced temperature
Same at the same reduced pressure
Both (B) & (C)
Vapor pressure
Partial pressure
Chemical potential
None of these
Kp2/Kp1 = - (ΔH/R) (1/T2 - 1/T1)
Kp2/Kp1 = (ΔH/R) (1/T2 - 1/T1)
Kp2/Kp1 = ΔH (1/T2 - 1/T1)
Kp2/Kp1 = - (1/R) (1/T2 - 1/T1)
0
+ve
-ve
∞
P + F - C = 2
C = P - F + 2
F = C - P - 2
P = F - C - 2
Same as Carnot cycle
Same as reverse Carnot cycle
Dependent on the refrigerant's properties
The least efficient of all refrigeration processes
Negative
Zero
Infinity
None of these
Simultaneous pressure & temperature change
Heating
Cooling
Both (B) and (C)
Free energy
Entropy
Refractive index
None of these
Heating occurs
Cooling occurs
Pressure is constant
Temperature is constant
Zero
Unity
Infinity
Negative
Increases, for an exothermic reaction
Decreases, for an exothermic reaction
Increases, for an endothermic reaction
None of these
Increase
Decrease
Remain unchanged
First fall and then rise
Two different gases behave similarly, if their reduced properties (i.e. P, V and T) are same
The surface of separation (i. e. the meniscus) between liquid and vapour phase disappears at the critical temperature
No gas can be liquefied above the critical temperature, howsoever high the pressure may be.
The molar heat of energy of gas at constant volume should be nearly constant (about 3 calories)
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
Gibbs-Duhem
Maxwell's
Clapeyron
None of these
Zeroth
First
Second
Third
Work done under adiabatic condition
Co-efficient of thermal expansion
Compressibility
None of these
Henry's law
Law of mass action
Hess's law
None of these
0
1
2
3
Decrease in temperature
Increase in temperature
No change in temperature
Change in temperature which is a function of composition