High temperature
Low pressure
Low temperature only
Both low temperature and high pressure
D. Both low temperature and high pressure
Gibbs-Duhem
Maxwell's
Clapeyron
None of these
Cv.dT
Cp.dT
∫ Cp.dT
∫ Cv.dT
States that n1dμ1 + n2dμ2 + ....njdμj = 0, for a system of definite composition at constant temperature and pressure
Applies only to binary systems
Finds no application in gas-liquid equilibria involved in distillation
None of these
F = E - TS
F = H - TS
F = H + TS
F = E + TS
∞
+ve
0
-ve
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
Infinity
Minus infinity
Zero
None of these
Below
At
Above
Either 'b' or 'c'
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
Specific volume
Work
Pressure
Temperature
Calorific value
Heat of reaction
Heat of combustion
Heat of formation
Surface tension of a substance vanishes at critical point, as there is no distinction between liquid and vapour phases at its critical point
Entropy of a system decreases with the evolution of heat
Change of internal energy is negative for exothermic reactions
The eccentric factor for all materials is always more than one
Ideal
Real
Isotonic
None of these
Solids
Liquids
Gases
All (A), (B) & (C)
Always exists
May exist
Never exists
Is difficult to predict
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)
Snow melts into water
A gas expands spontaneously from high pressure to low pressure
Water is converted into ice
Both (B) & (C)
With pressure changes at constant temperature
Under reversible isothermal volume change
During heating of an ideal gas
During cooling of an ideal gas
R loge 4
R log10 4
Cv log10 4
Cv loge 4
Expansion in an engine
Following a constant pressure cycle
Throttling
None of these
The net change in entropy in any reversible cycle is always zero
The entropy of the system as a whole in an irreversible process increases
The entropy of the universe tends to a maximum
The entropy of a substance does not remain constant during a reversible adiabatic change
0
1
2
3
Violates second law of thermodynamics
Involves transfer of heat from low temperature to high temperature
Both (A) and (B)
Neither (A) nor (B)
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
CO2
H2
O2
N2
Work done under adiabatic condition
Co-efficient of thermal expansion
Compressibility
None of these
Volume
Density
Temperature
Pressure
Heat capacity
Molal heat capacity
Pressure
Concentration
Less than
Same as
More than
Half
Adiabatic process
Endothermic reaction
Exothermic reaction
Process involving a chemical reaction