Path
Point
State
None of these
A. Path
Heat pump
Heat engine
Carnot engine
None of these
Constant volume
Polytropic
Adiabatic
Constant pressure
Vapor pressure
Partial pressure
Chemical potential
None of these
Pressure vs. enthalpy
Pressure vs. volume
Enthalpy vs. entropy
Temperature vs. entropy
Accomplishes only space heating in winter
Accomplishes only space cooling in summer
Accomplishes both (A) and (B)
Works on Carnot cycle
Cp/Cv
Cp/(CP-R)
1 + (R/CV)
All (A), (B) and (C)
5.2
6.2
0.168
Data insufficient, can't be found out
Cp < Cv
Cp = Cv
Cp > Cv
C ≥ Cv
The distribution law
Followed from Margules equation
A corollary of Henry's law
None of these
High thermal conductivity
Low freezing point
Large latent heat of vaporisation
High viscosity
Water
Air
Evaporative
Gas
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
First law
Zeroth law
Third law
Second law
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
Becomes zero
Becomes infinity
Equals 1 kcal/kmol °K
Equals 0.24 kcal/kmol °K
Use of only one graph for all gases
Covering of wide range
Easier plotting
More accurate plotting
[∂(G/T)/∂T] = - (H/T2)
[∂(A/T)/∂T]V = - E/T2
Both (A) and (B)
Neither (A) nor (B)
Isochoric
Isobaric
Adiabatic
Isothermal
Activity
Fugacity
Activity co-efficient
Fugacity co-efficient
Increase
Decrease
No change
None of these
Pressure
Composition
Temperature
All (A), (B) and (C)
0
1
2
3
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
RT d ln P
RT d ln f
R d ln f
None of these
2
0
3
1
Initial concentration of the reactant
Pressure
Temperature
None of these
Steam to ethylene ratio
Temperature
Pressure
None of these
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
Molar volume, density, viscosity and boiling point
Refractive index and surface tension
Both (A) and (B)
None of these
Slower than Y
Faster than Y
Three times slower than Y
Three times faster than Y