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
D. A real gas on expansion in vacuum cools down whereas ideal gas remains unaffected
Activity co-efficient is dimensionless.
In case of an ideal gas, the fugacity is equal to its pressure.
In a mixture of ideal gases, the fugacity of a component is equal to the partial pressure of the component.
The fugacity co-efficient is zero for an ideal gas
TR/(T2 - TR) × (T1 - T2)/T1
TR/(T2 - TR) × T1/(T1 - T2)
TR/(T1 - TR) × (T1 - T2)/T1
None of these
Binary solutions
Ternary solutions
Azeotropic mixture only
None of these
Non-flow reversible
Adiabatic
Both (A) and (B)
Neither (A) nor (B)
30554
10373
4988.4
4364.9
Not changed
Decreasing
Increasing
Data sufficient, can't be predicted
5.2
6.2
0.168
Data insufficient, can't be found out
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
Simultaneous pressure & temperature change
Heating
Cooling
Both (B) and (C)
Becomes zero
Becomes infinity
Equals 1 kcal/kmol °K
Equals 0.24 kcal/kmol °K
Increase
Decrease
Remain unaltered
Increase or decrease; depends on the particular reaction
Third law of thermodynamics
Second law of thermodynamics
Nernst heat theorem
Maxwell's relations
Molar heat capacity
Internal energy
Viscosity
None of these
Gibbs-Duhem
Maxwell's
Clapeyron
None of these
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
More than
Less than
Equal to
Not related to
Disorder
Orderly behaviour
Temperature changes only
None of these
Isothermal
Adiabatic
Isobaric
Isochoric
P1ACBP2P1
ACBB1A1A
ACBDA
ADBB1A1A
0°C
273°C
100°C
-273°C
By throttling
By expansion in an engine
At constant pressure
None of these
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'
F = E - TS
F = H - TS
F = H + TS
F = E + TS
Pressure remains constant
Pressure is increased
Temperature remains constant
None of these
4 J
∞
0
8 J
Two
One
Zero
Three
2HI H2 + I2
N2O4 2NO2
2SO2 + O2 2SO3
None of these
∞
+ve
0
-ve
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
Increase
Decrease
No change
None of these