Low pressure & high temperature
High pressure & low temperature
Low pressure & low temperature
None of these
A. Low pressure & high temperature
Lewis-Randall
Margules
Van Laar
Both (B) & (C)
A = H - TS
A = E - TS
A = H + TS
None of these
Logarithmic
Arithmetic
Geometric
Harmonic
Increases
Decreases
Remains unchanged
Data insufficient, can't be predicted
Zero
Negative
Very large compared to that for endothermic reaction
Not possible to predict
Entropy and enthalpy are path functions
In a closed system, the energy can be exchanged with the surrounding, while matter cannot be exchanged
All the natural processes are reversible in nature
Work is a state function
0
1
2
3
2
0
3
1
Concentration
Mass
Temperature
Entropy
Volume
Density
Temperature
Pressure
The energy change of a system undergoing any reversible process is zero
It is not possible to transfer heat from a lower temperature to a higher temperature
The total energy of system and surrounding remains the same
None of the above
Reversible isothermal
Irreversible isothermal
Reversible adiabatic
None of these
Enthalpy
Entropy
Pressure
None of these
Does not depend upon temperature
Is independent of pressure only
Is independent of volume only
Is independent of both pressure and volume
Triple point
Boiling point
Below triple point
Always
More
Less
Same
Unpredictable; depends on the particular reaction
∞
0
Maximum
Minimum
Volume
Pressure
Temperature
All (A), (B) and (C)
Simultaneous pressure & temperature change
Heating
Cooling
Both (B) and (C)
Non-flow reversible
Adiabatic
Both (A) and (B)
Neither (A) nor (B)
Fugacity
Activity co-efficient
Free energy
All (A), (B) & (C)
Adiabatic process
Endothermic reaction
Exothermic reaction
Process involving a chemical reaction
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
Rate of heat transmission
Initial state only
End states only
None of these
Ideal
Real
Isotonic
None of these
1
< 1
> 1
>> 1
Same as Carnot cycle
Same as reverse Carnot cycle
Dependent on the refrigerant's properties
The least efficient of all refrigeration processes
ds = 0
ds < 0
ds > 0
ds = Constant
Increases
Decreases
Remain constant
Increases linearly
Molar concentration
Quantity (i.e. number of moles)
Both (A) and (B)
Neither (A) nor (B)