Isobaric
Isothermal
Isentropic
Isometric
A. Isobaric
n = y = 1.4
n = 0
n = 1
n = 1.66
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
Free energy
Entropy
Refractive index
None of these
Not changed
Decreasing
Increasing
Data sufficient, can't be predicted
The concentration of each component should be same in the two phases
The temperature of each phase should be same
The pressure should be same in the two phases
The chemical potential of each component should be same in the two phases
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
Matter
Energy
Neither matter nor energy
Both matter and energy
Moisture free ice
Solid helium
Solid carbon dioxide
None of these
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Helmholtz
Gibbs
Both a & b
Neither 'a' nor 'b'
Freezing
Triple
Boiling
Boyle
Chemical potential
Fugacity
Both (A) and (B)
Neither (A) nor (B)
Specific volume
Work
Pressure
Temperature
Reverse Carnot cycle
Ordinary vapour-compression cycle
Vapour-compression process with a reversible expansion engine
Air refrigeration cycle
Less
More
Same
More or less depending upon the extent of work done
Increase
Decrease
No change
None of these
Heat capacity
Molal heat capacity
Pressure
Concentration
5.2
6.2
0.168
Data insufficient, can't be found out
Heating takes place
Cooling takes place
Pressure is constant
Temperature is constant
T
T and P
T, P and Z
T and Z
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance
Path
Point
State
None of these
Non-flow reversible
Adiabatic
Both (A) and (B)
Neither (A) nor (B)
Same
Doubled
Halved
One fourth of its original value
Temperature
Pressure
Volume
Entropy
Two different gases behave similarly, if their reduced properties (i.e. P, V and T) are same
The surface of separation (i. e. the meniscus) between liquid and vapour phase disappears at the critical temperature
No gas can be liquefied above the critical temperature, howsoever high the pressure may be.
The molar heat of energy of gas at constant volume should be nearly constant (about 3 calories)
Stirling
Brayton
Rankine
None of these
0
273
25
None of these
Temperature
Pressure
Volume
None of these
Carnot
Air
Absorption
vapour-ejection