More
Less
Same
More or less; depending on the system
C. Same
Temperature
Pressure
Composition
All (A), (B) and (C)
Helmholtz
Gibbs
Both a & b
Neither 'a' nor 'b'
Not a function of its pressure
Not a function of its nature
Not a function of its temperature
Unity, if it follows PV = nRT
At constant pressure, solubility of a gas in a liquid diminishes with rise in temperature
Normally, the gases which are easily liquefied are more soluble in common solvents
The gases which are capable of forming ions in aqueous solution are much more soluble in water than in other solvents
At constant pressure, solubility of a gas in a liquid increases with rise in temperature
Ideal
Real
Isotonic
None of these
Infinity
Minus infinity
Zero
None of these
Shifting the equilibrium towards right
Shifting the equilibrium towards left
No change in equilibrium condition
None of these
R loge 4
R log10 4
Cv log10 4
Cv loge 4
Low T, low P
High T, high P
Low T, high P
High T, low P
Low pressure and high temperature
Low pressure and low temperature
High pressure and low temperature
High pressure and high temperature
Simultaneous pressure & temperature change
Heating
Cooling
Both (B) and (C)
The energy change of a system undergoing any reversible process is zero
It is not possible to transfer heat from a lower temperature to a higher temperature
The total energy of system and surrounding remains the same
None of the above
Adiabatic expansion
Joule-Thomson effect
Both (A) and (B)
Neither (A) nor (B)
Prediction of the extent of a chemical reaction
Calculating absolute entropies of substances at different temperature
Evaluating entropy changes of chemical reaction
Both (B) and (C)
Equation of state
Gibbs Duhem equation
Ideal gas equation
None of these
First law
Zeroth law
Third law
Second law
RT d ln P
RT d ln f
R d ln f
None of these
Virial co-efficients are universal constants
Virial co-efficients 'B' represents three body interactions
Virial co-efficients are function of temperature only
For some gases, Virial equations and ideal gas equations are the same
Pressure
Solubility
Temperature
None of these
dE = Tds - PdV
dQ = CvdT + PdV
dQ = CpdT + Vdp
Tds = dE - PdV
Free expansion of a gas
Compression of air in a compressor
Expansion of steam in a turbine
All (A), (B) & (C)
Is the most efficient of all refrigeration cycles
Has very low efficiency
Requires relatively large quantities of air to achieve a significant amount of refrigeration
Both (B) and (C)
(∂P/∂V)T
(∂V/∂T)P
(∂P/∂V)V
All (A), (B) & (C)
Momentum
Mass
Energy
None of these
Vapor pressure
Partial pressure
Chemical potential
None of these
Representing actual behaviour of real gases
Representing actual behaviour of ideal gases
The study of chemical equilibria involving gases at atmospheric pressure
None of these
-19.4
-30.2
55.2
-55.2
Temperature vs. enthalpy
Temperature vs. enthalpy
Entropy vs. enthalpy
Temperature vs. internal energy
T
T and P
T, P and Z
T and Z
T1/(T1-T2)
T2/(T1-T2)
T1/T2
T2/R1