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
C. Virial co-efficients are function of temperature only
Equilibrium
Adiabatic
Steady
Unsteady
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
Isothermal
Isobaric
Polytropic
Adiabatic
Entropy
Temperature
Internal energy
Enthalpy
Low pressure & high temperature
High pressure & low temperature
Low pressure & low temperature
None of these
Pressure
Composition
Temperature
All (A), (B) and (C)
Entropy
Temperature
Enthalpy
Pressure
Entropy
Gibbs energy
Internal energy
Enthalpy
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
(dF)T, p <0
(dF)T, p = 0
(dF)T, p > 0
(dA)T, v >0
-273
0
-78
5
+ve
-ve
0
Either of the above three; depends on the nature of refrigerant
Cp/Cv
Cp/(CP-R)
1 + (R/CV)
All (A), (B) and (C)
Not liquify (barring exceptions)
Immediately liquify
Never liquify however high the pressure may be
None of these
2
0
1
3
Low pressure and high temperature
Low pressure and low temperature
Low temperature and high pressure
High temperature and high pressure
The melting point of wax
The boiling point of a liquid
Both (A) and (B)
Neither (A) nor (B)
0
< 0
> 0
A function of pressure
Reversible and isothermal
Irreversible and constant enthalpy
Reversible and constant entropy
Reversible and constant enthalpy
Cold reservoir approaches zero
Hot reservoir approaches infinity
Either (A) or (B)
Neither (A) nor (B)
5 & 3
3.987 & 1.987
1.987 & 0.66
0.66 & 1.987
Expansion of a real gas
Reversible isothermal volume change
Heating of an ideal gas
Cooling of a real gas
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
Pressure remains constant
Pressure is increased
Temperature remains constant
None of these
Snow melts into water
A gas expands spontaneously from high pressure to low pressure
Water is converted into ice
Both (B) & (C)
Ice at the base contains impurities which lowers its melting point
Due to the high pressure at the base, its melting point reduces
The iceberg remains in a warmer condition at the base
All (A), (B) and (C)
H = E - PV
H = F - TS
H - E = PV
None of these
Mole fraction
Activity
Pressure
Activity co-efficient
Temperature
Pressure
Composition
All (A), (B) and (C)
n = y = 1.4
n = 0
n = 1
n = 1.66