Volume
Enthalpy
Both (A) & (B)
Neither (A) nor (B)
C. Both (A) & (B)
Doubling the absolute temperature as well as pressure of the gas
Reducing pressure to one fourth at constant temperature
Reducing temperature to one fourth at constant pressure
Reducing the temperature to half and doubling the pressure
Increased COP
Same COP
Decreased COP
Increased or decreased COP; depending upon the type of refrigerant
Zeroth
First
Second
Third
Becomes zero
Becomes infinity
Equals 1 kcal/kmol °K
Equals 0.24 kcal/kmol °K
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
Volume
Pressure
Temperature
All a, b & c
Less
More
Same
More or less depending upon the extent of work done
Minimum temperature attainable
Temperature of the heat reservoir to which a Carnot engine rejects all the heat that is taken in
Temperature of the heat reservoir to which a Carnot engine rejects no heat
None of these
100,000 kW
160,000 kW
200,000 kW
320,000 kW
Free energy
Entropy
Refractive index
None of these
Maxwell's equation
Thermodynamic equation of state
Equation of state
Redlich-Kwong equation of state
Matter
Energy
Neither matter nor energy
Both matter and energy
RT ln K
-RT ln K
-R ln K
T ln K
Pressure vs. enthalpy
Pressure vs. volume
Enthalpy vs. entropy
Temperature vs. entropy
Adiabatic
Isothermal
Isometric
None of these
H = E - PV
H = F - TS
H - E = PV
None of these
Kelvin's
Antoines
Kirchoffs
None of these
Work required to refrigeration obtained
Refrigeration obtained to the work required
Lower to higher temperature
Higher to lower temperature
Zero
Negative
Very large compared to that for endothermic reaction
Not possible to predict
Increase
Decrease
Remain unaltered
Increase or decrease; depends on the particular reaction
Cp < Cv
Cp = Cv
Cp > Cv
C ≥ Cv
(dF)T, p <0
(dF)T, p = 0
(dF)T, p > 0
(dA)T, v >0
Molten sodium
Molten lead
Mercury
Molten potassium
Volume of the liquid phase is negligible compared to that of vapour phase
Vapour phase behaves as an ideal gas
Heat of vaporisation is independent of temperature
All (A), (B) & (C)
0°C
273°C
100°C
-273°C
Carnot
Air
Absorption
vapour-ejection
Entropy
Temperature
Enthalpy
Pressure
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)
580
640
1160
Data insufficient; can't be computed
μ° + RT ln f
μ°+ R ln f
μ° + T ln f
μ° + R/T ln f