Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
C. Zero at absolute zero temperature for a perfect crystalline substance
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)
The distribution law
Followed from Margules equation
A corollary of Henry's law
None of these
SO2
NH3
CCl2F2
C2H4Cl2
In which there is a temperature drop
Which is exemplified by a non-steady flow expansion
Which can be performed in a pipe with a constriction
In which there is an increase in temperature
Expansion valve
Condenser
Refrigerator
Compressor
Adiabatic
Isometric
Isentropic
Isothermal
Molal concentration difference
Molar free energy
Partial molar free energy
Molar free energy change
Moisture free ice
Solid helium
Solid carbon dioxide
None of these
Like internal energy and enthalpy, the absolute value of standard entropy for elementary substances is zero
Melting of ice involves increase in enthalpy and a decrease in randomness
The internal energy of an ideal gas depends only on its pressure
Maximum work is done under reversible conditions
Pressure
Volume
Temperature
All (A), (B) & (C)
The amount of work needed is path dependent
Work alone cannot bring out such a change of state
The amount of work needed is independent of path
More information is needed to conclude anything about the path dependence or otherwise of the work needed
λb/Tb
Tb/λb
√(λb/Tb)
√(Tb/λb)
Both the processes are adiabatic
Both the processes are isothermal
Process A is isothermal while B is adiabatic
Process A is adiabatic while B is isothermal
Temperature
Pressure
Volume
Entropy
1
2
3
4
Molar concentration
Quantity (i.e. number of moles)
Both (A) and (B)
Neither (A) nor (B)
Straight line
Sine curve
Parabola
Hyperbola
349
651
667
1000
Calorific value
Heat of reaction
Heat of combustion
Heat of formation
0
∞
50
100
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
Cp/Cv
Cp/(CP-R)
1 + (R/CV)
All (A), (B) and (C)
Mass
Energy
Momentum
None of these
Air cycle
Carnot cycle
Ordinary vapour compression cycle
Vapour compression with a reversible expansion engine
Extensive property
Intensive property
Force which drives the chemical system to equilibrium
Both (B) and (C)
Cv.dT
Cp.dT
∫ Cp.dT
∫ Cv.dT
Solution
Formation
Dilution
Combustion
Enthalpy
Internal energy
Either (A) or (B)
Neither (A) nor (B)
∞
0
< 0
> 0
Unity
Zero
That of the heat of reaction
Infinity