2.73
28.3
273
283
B. 28.3
Is the most efficient of all refrigeration cycles
Has very low efficiency
Requires relatively large quantities of air to achieve a significant amount of refrigeration
Both (B) and (C)
Process must be isobaric
Temperature must decrease
Process must be adiabatic
Both (B) and (C)
∞
0
Maximum
Minimum
Any
A perfect
An easily liquefiable
A real
Less than
More than
Same as
Not related to
Molecular size
Temperature
Volume
Pressure
Zeroth
First
Second
Third
A real gas on expansion in vacuum gets heated up
An ideal gas on expansion in vacuum gets cooled
An ideal gas on expansion in vacuum gets heated up
A real gas on expansion in vacuum cools down whereas ideal gas remains unaffected
0
273
25
None of these
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
Non-flow reversible
Adiabatic
Both (A) and (B)
Neither (A) nor (B)
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
Value of absolute entropy
Energy transfer
Direction of energy transfer
None of these
Adiabatic
Isothermal
Isometric
None of these
The values of (∂P/∂V)T and (∂2P/∂V2)T are zero for a real gas at its critical point
Heat transferred is equal to the change in the enthalpy of the system, for a constant pressure, non-flow, mechanically reversible process
Thermal efficiency of a Carnot engine depends upon the properties of the working fluid besides the source & sink temperatures
During a reversible adiabatic process, the entropy of a substance remains constant
Direction of energy transfer
Reversible processes only
Irreversible processes only
None of these
Ethyl chloride or methyl chloride
Freon-12
Propane
NH3 or CO2
Melting of ice
Condensation of alcohol vapor
Sudden bursting of a cycle tube
Evaporation of water
An open system of constant composition
A closed system of constant composition
An open system with changes in composition
A closed system with changes in composition
A homogeneous solution (say of phenol water) is formed
Mutual solubility of the two liquids shows a decreasing trend
Two liquids are completely separated into two layers
None of these
μ = (∂P/∂T)H
μ = (∂T/∂P)H
μ = (∂E/∂T)H
μ = (∂E/∂P)H
Chemical potential
Activity
Fugacity
Activity co-efficient
Low T, low P
High T, high P
Low T, high P
High T, low P
Pressure
Volume
Temperature
All (A), (B) & (C)
Violates second law of thermodynamics
Involves transfer of heat from low temperature to high temperature
Both (A) and (B)
Neither (A) nor (B)
Cv.dT
Cp.dT
∫ Cp.dT
∫ Cv.dT
∞
-ve
0
+ve
More than
Less than
Equal to
Not related to
Henry's law
Law of mass action
Hess's law
None of these