Non-flow reversible
Adiabatic
Both (A) and (B)
Neither (A) nor (B)
C. Both (A) and (B)
Temperature
Specific heat
Volume
Pressure
100
50
205
200
Becomes zero
Becomes infinity
Equals 1 kcal/kmol °K
Equals 0.24 kcal/kmol °K
Momentum
Mass
Energy
None of these
Concentration of the constituents only
Quantities of the constituents only
Temperature only
All (A), (B) and (C)
Oxygen
Nitrogen
Air
Hydrogen
Accomplishes only space heating in winter
Accomplishes only space cooling in summer
Accomplishes both (A) and (B)
Works on Carnot cycle
Does not depend upon temperature
Is independent of pressure only
Is independent of volume only
Is independent of both pressure and volume
Isothermal
Isentropic
Isobaric
Adiabatic
Increases
Decreases
Remains unchanged
Decreases linearly
Less
More
Same
Dependent on climatic conditions
Zero
Unity
Infinity
An indeterminate value
Low T, low P
High T, high P
Low T, high P
High T, low P
Representing actual behaviour of real gases
Representing actual behaviour of ideal gases
The study of chemical equilibria involving gases at atmospheric pressure
None of these
Air cycle
Carnot cycle
Ordinary vapour compression cycle
Vapour compression with a reversible expansion engine
Negative
Zero
Infinity
None of these
Ice at the base contains impurities which lowers its melting point
Due to the high pressure at the base, its melting point reduces
The iceberg remains in a warmer condition at the base
All (A), (B) and (C)
Ideal
Very high pressure
Very low temperature
All of the above
Low temperature
High pressure
Both (A) and (B)
Neither (A) nor (B)
Kp2/Kp1 = - (ΔH/R) (1/T2 - 1/T1)
Kp2/Kp1 = (ΔH/R) (1/T2 - 1/T1)
Kp2/Kp1 = ΔH (1/T2 - 1/T1)
Kp2/Kp1 = - (1/R) (1/T2 - 1/T1)
ΔF = ΔH + T [∂(ΔF)/∂T]P
ΔF = ΔH - TΔT
d(E - TS) T, V < 0
dP/dT = ΔHvap/T.ΔVvap
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance
Expansion of an ideal gas against constant pressure
Atmospheric pressure vaporisation of water at 100°C
Solution of NaCl in water at 50°C
None of these
0
1
2
3
Increase
Decrease
Remain unchanged
First fall and then rise
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)
(p + a/V2)(V - b) = nRT
PV = nRT
PV = A + B/V + C/V2 + D/V3 + ...
None of these
The expansion of a gas in vacuum is an irreversible process
An isometric process is a constant pressure process
Entropy change for a reversible adiabatic process is zero
Free energy change for a spontaneous process is negative
[∂(G/T)/∂T] = - (H/T2)
[∂(A/T)/∂T]V = - E/T2
Both (A) and (B)
Neither (A) nor (B)
Reversible and isothermal
Isothermal and irreversible
Reversible and adiabatic
Adiabatic and irreversible