Only F decreases
Only A decreases
Both F and A decreases
Both F and A increase
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
Hess's
Kirchoff's
Lavoisier and Laplace
None of these
1.572
1.9398
3.389
4.238
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)
Third law of thermodynamics
Second law of thermodynamics
Nernst heat theorem
Maxwell's relations
Water
Air
Evaporative
Gas
dE = Tds - PdV
dQ = CvdT + PdV
dQ = CpdT + Vdp
Tds = dE - PdV
Increases with increase in pressure
Decreases with increase in temperature
Is independent of temperature
None of these
Vapor compression cycle using expansion valve
Air refrigeration cycle
Vapor compression cycle using expansion engine
Carnot refrigeration cycle
J/s
J.S
J/kmol
kmol/J
A = H - TS
A = E - TS
A = H + TS
None of these
Non-uniformly
Adiabatically
Isobarically
Isothermally
[∂(G/T)/∂T] = - (H/T2)
[∂(A/T)/∂T]V = - E/T2
Both (A) and (B)
Neither (A) nor (B)
Superheated vapour
Partially condensed vapour with quality of 0.9
Saturated vapour
Partially condensed vapour with quality of 0.1
+ve
-ve
0
Either of the above three; depends on the nature of refrigerant
1
< 1
> 1
>> 1
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
Isobaric
Isothermal
Isentropic
Isometric
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)
(dF)T, p <0
(dF)T, p = 0
(dF)T, p > 0
(dA)T, v >0
Latent heat of vaporisation
Chemical potential
Molal boiling point
Heat capacity
Expansion in an engine
Following a constant pressure cycle
Throttling
None of these
Solids
Liquids
Gases
All (A), (B) & (C)
Chemical potential
Fugacity
Both (A) and (B)
Neither (A) nor (B)
Heat capacity
Molal heat capacity
Pressure
Concentration
Not liquify (barring exceptions)
Immediately liquify
Never liquify however high the pressure may be
None of these
Bucket
Throttling
Separating
A combination of separating & throttling
Molar concentration
Quantity (i.e. number of moles)
Both (A) and (B)
Neither (A) nor (B)
Air cycle
Carnot cycle
Ordinary vapor compression cycle
Vapor compression with a reversible expansion engine