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)
D. Both (B) and (C)
Critical
Triple
Freezing
Boiling
Reversible isothermal volume change
Heating of a substance
Cooling of a substance
Simultaneous heating and expansion of an ideal gas
5 & 3
3.987 & 1.987
1.987 & 0.66
0.66 & 1.987
Less
More
Same
More or less depending upon the extent of work done
Solid-vapor
Solid-liquid
Liquid-vapor
All (A), (B) and (C)
Decreases in all spontaneous (or irreversible) processes
Change during a spontaneous process has a negative value
Remains unchanged in reversible processes carried at constant temperature and pressure
All (A), (B) and (C)
Temperature only
Temperature and pressure only
Temperature, pressure and liquid composition xi only
Temperature, pressure, liquid composition xi and vapour composition yi
Does not depend upon temperature
Is independent of pressure only
Is independent of volume only
Is independent of both pressure and volume
Zero
Negative
Very large compared to that for endothermic reaction
Not possible to predict
Vapor pressure
Specific Gibbs free energy
Specific entropy
All (A), (B) and (C)
Always greater than one
Same at the same reduced temperature
Same at the same reduced pressure
Both (B) & (C)
Cold reservoir approaches zero
Hot reservoir approaches infinity
Either (A) or (B)
Neither (A) nor (B)
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
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
Volume
Pressure
Temperature
All (A), (B) and (C)
Decrease in velocity
Decrease in temperature
Decrease in kinetic energy
Energy spent in doing work
its internal energy (U) decreases and its entropy (S) increases
U and S both decreases
U decreases but S is constant
U is constant but S decreases
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
Isothermal
Adiabatic
Isobaric
Isochoric
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
n = y = 1.4
n = 0
n = 1
n = 1.66
Reversible isothermal
Irreversible isothermal
Reversible adiabatic
None of these
Isothermal compression
Isothermal expansion
Adiabatic expansion
Adiabatic compression
Becomes zero
Becomes infinity
Equals 1 kcal/kmol °K
Equals 0.24 kcal/kmol °K
Process must be isobaric
Temperature must decrease
Process must be adiabatic
Both (B) and (C)
Isobaric
Adiabatic
Isenthalpic
Both (B) & (C)
TVγ-1 = constant
p1-γ.TY = constant
PVγ = constant
None of these
Two temperatures only
Pressure of working fluid
Mass of the working fluid
Mass and pressure both of the working fluid
Bucket
Throttling
Separating
A combination of separating & throttling
Sub-cooled
Saturated
Non-solidifiable
None of these