Increases
Decreases
Remains unchanged
Decreases linearly
A. Increases
Enthalpy
Volume
Both 'a' & 'b'
Neither 'a' nor 'b'
Increases with increase in pressure
Decreases with increase in temperature
Is independent of temperature
None of these
A closed system does not permit exchange of mass with its surroundings but may permit exchange of energy.
An open system permits exchange of both mass and energy with its surroundings
The term microstate is used to characterise an individual, whereas macro-state is used to designate a group of micro-states with common characteristics
None of the above
At constant pressure
By throttling
By expansion in an engine
None of these
Same in both the phases
Zero in both the phases
More in vapour phase
More in liquid phase
Volume of the liquid phase is negligible compared to that of vapour phase
Vapour phase behaves as an ideal gas
Heat of vaporisation is independent of temperature
All (A), (B) & (C)
T
T and P
T, P and Z
T and Z
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)
1
2
3
4
Henry's law
Law of mass action
Hess's law
None of these
Rate of change of vapour pressure with temperature
Effect of an inert gas on vapour pressure
Calculation of ΔF for spontaneous phase change
Temperature dependence of heat of phase transition
System (of partially miscible liquid pairs), in which the mutual solubility increases with rise in temperature, are said to possess an upper consolute temperature
Systems, in which the mutual solubility increases with decrease in temperature, are said to possess lower consolute temperature
Nicotine-water system shows both an upper as well as a lower consolute temperature, implying that they are partially miscible between these two limiting temperatures
None of these
Decreases
Increases
Remains constant
Decreases logarithmically
Not changed
Decreasing
Increasing
Data sufficient, can't be predicted
Volume
Enthalpy
Both (A) & (B)
Neither (A) nor (B)
Increases
Decreases
Remains unchanged
Data insufficient, can't be predicted
Increase the partial pressure of I2
Decrease the partial pressure of HI
Diminish the degree of dissociation of HI
None of these
ΔF = ΔH + T [∂(ΔF)/∂T]P
ΔF = ΔH - TΔT
d(E - TS) T, V < 0
dP/dT = ΔHvap/T.ΔVvap
Less than
Same as
More than
Half
2
0
1
3
Specific volume
Work
Pressure
Temperature
1
2
3
0
T2/(T1 - T2)
T1/(T1 - T2)
(T1 - T2)/T1
(T1 - T2)/T2
+ve
-ve
0
Either of the above three; depends on the nature of refrigerant
Ideal compression of air
Free expansion of an ideal gas
Adiabatic expansion of steam in a turbine
Adiabatic compression of a perfect gas
Enthalpy
Internal energy
Either (A) or (B)
Neither (A) nor (B)
Pressure must be kept below 5.2 atm
Temperature must be kept above - 57°C
Pressure must be kept below 5.2 atm. and temperature must be kept above 57°C
Pressure and temperature must be kept below 5.2 atm. and - 57°C respectively
Freon
Liquid sulphur dioxide
Methyl chloride
Ammonia
Compressibility
Work done under adiabatic condition
Work done under isothermal condition
Co-efficient of thermal expansion
Freezing
Triple
Boiling
Boyle