Sub-cooled
Saturated
Non-solidifiable
None of these
A. Sub-cooled
Violates second law of thermodynamics
Involves transfer of heat from low temperature to high temperature
Both (A) and (B)
Neither (A) nor (B)
Equation of state
Gibbs Duhem equation
Ideal gas equation
None of these
Solids
Liquids
Gases
All (A), (B) & (C)
Saturated vapour
Solid
Gas
Liquid
Melting of ice
Condensation of alcohol vapor
Sudden bursting of a cycle tube
Evaporation of water
dE = CpdT
dE = CvdT
dQ = dE + pdV
dW = pdV
Gibbs-Duhem equation
Gibbs-Helmholtz equation
Third law of thermodynamics
Joule-Thomson effect
In an isothermal system, irreversible work is more than reversible work
Under reversible conditions, the adiabatic work is less than isothermal work
Heat, work, enthalpy and entropy are all 'state functions'
Matter and energy cannot be exchanged with the surroundings in a closed system
Stirling
Brayton
Rankine
Both (B) and (C)
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
Fugacity
Activity co-efficient
Free energy
All (A), (B) & (C)
Reaction mechanism
Calculation of rates
Energy transformation from one form to another
None of these
The distribution law
Followed from Margules equation
A corollary of Henry's law
None of these
+ve
-ve
0
∞
(T2 - T1)/T2
(T2 - T1)/T1
(T1 - T2)/T2
(T1 - T2)/T1
Critical temperature
Melting point
Freezing point
Both (B) and (C)
ΔF = ΔH + T [∂(ΔF)/∂T]P
ΔF = ΔH - TΔT
d(E - TS) T, V < 0
dP/dT = ΔHvap/T.ΔVvap
Ideal
Real
Isotonic
None of these
Isothermal
Isobaric
Polytropic
Adiabatic
Isothermal
Isentropic
Isobaric
Adiabatic
Rate of heat transmission
Initial state only
End states only
None of these
At low temperature and high pressure
At standard state
Both (A) and (B)
In ideal state
Cp/Cv
Cp/(CP-R)
1 + (R/CV)
All (A), (B) and (C)
Adiabatic
Isothermal
Isometric
None of these
2
0
3
1
T
√T
T2
1/√T
Solution
Vaporisation
Formation
Sublimation
High thermal conductivity
Low freezing point
Large latent heat of vaporisation
High viscosity
Decrease in temperature
Increase in temperature
No change in temperature
Change in temperature which is a function of composition
1
< 1
> 1
Either (B) or (C), depends on the nature of the gas