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
(T2 - T1)/T2
(T2 - T1)/T1
(T1 - T2)/T2
(T1 - T2)/T1
(dF)T, p <0
(dF)T, p = 0
(dF)T, p > 0
(dA)T, v >0
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
Not a function of its pressure
Not a function of its nature
Not a function of its temperature
Unity, if it follows PV = nRT
Decreases in all spontaneous (or irreversible) processes
Change during a spontaneous process has a negative value
Remains unchanged in reversible processes carried at constant temperature and pressure
All (A), (B) and (C)
Entropy
Temperature
Enthalpy
Pressure
Extensive property
Intensive property
Force which drives the chemical system to equilibrium
Both (B) and (C)
Saturated vapour
Solid
Gas
Liquid
P1ACBP2P1
ACBB1A1A
ACBDA
ADBB1A1A
Always greater than one
Same at the same reduced temperature
Same at the same reduced pressure
Both (B) & (C)
Same as Carnot cycle
Same as reverse Carnot cycle
Dependent on the refrigerant's properties
The least efficient of all refrigeration processes
Steam to ethylene ratio
Temperature
Pressure
None of these
Volume
Density
Temperature
Pressure
Only ΔE = 0
Only ΔH =0
ΔE = ΔH = 0
dQ = dE
Pressure
Composition
Temperature
All (A), (B) and (C)
Volume, mass and number of moles
Free energy, entropy and enthalpy
Both (A) and (B)
None of these
Temperature only
Temperature and pressure only
Temperature, pressure and liquid composition xi only
Temperature, pressure, liquid composition xi and vapour composition yi
Isothermal
Isentropic
Isobaric
Adiabatic
Two different gases behave similarly, if their reduced properties (i.e. P, V and T) are same
The surface of separation (i. e. the meniscus) between liquid and vapour phase disappears at the critical temperature
No gas can be liquefied above the critical temperature, howsoever high the pressure may be.
The molar heat of energy of gas at constant volume should be nearly constant (about 3 calories)
Gibbs-Duhem
Maxwell's
Clapeyron
None of these
Pressure
Solubility
Temperature
None of these
First law
Zeroth law
Third law
Second law
12 P1V1
6 P1 V1
3 P1V1
P1 V1
Rate of heat transmission
Initial state only
End states only
None of these
High temperature
Low pressure
Low temperature only
Both low temperature and high pressure
T
√T
T2
1/√T
Rectangle
Rhombus
Trapezoid
Circle
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
Zero
Unity
Infinity
Negative