By throttling
By expansion in an engine
At constant pressure
None of these
A. By throttling
Decreases
Increases
Remain same
May increase or decrease; depends on the nature of the gas
He
N2
O2
H2
Δ H = 0 and ΔS = 0
Δ H ≠ 0 and ΔS = 0
Δ H ≠ 0 and ΔS ≠ 0
Δ H = 0 and ΔS ≠ 0
Reversible isothermal volume change
Heating of a substance
Cooling of a substance
Simultaneous heating and expansion of an ideal gas
In standard state
At high pressure
At low temperature
In ideal state
Does not depend upon temperature
Is independent of pressure only
Is independent of volume only
Is independent of both pressure and volume
Freezing
Triple
Boiling
Boyle
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)
The chemical potential of a pure substance depends upon the temperature and pressure
The chemical potential of a component in a system is directly proportional to the escaping tendency of that component
The chemical potential of ith species (μi) in an ideal gas mixture approaches zero as the pressure or mole fraction (xi) tends to be zero at constant temperature
The chemical potential of species 'i' in the mixture (μi) is mathematically represented as,μi = ∂(nG)/∂ni]T,P,nj where, n, ni and nj respectively denote the total number of moles, moles of ith species and all mole numbers except ith species. 'G' is Gibbs molar free energy
x
x + 1
x + 2
x + 3
Increase the partial pressure of I2
Decrease the partial pressure of HI
Diminish the degree of dissociation of HI
None of these
RT ln K
-RT ln K
-R ln K
T ln K
Accomplishes only space heating in winter
Accomplishes only space cooling in summer
Accomplishes both (A) and (B)
Works on Carnot cycle
Process must be isobaric
Temperature must decrease
Process must be adiabatic
Both (B) and (C)
Cp < Cv
Cp = Cv
Cp > Cv
C ≥ Cv
Entropy
Temperature
Enthalpy
Pressure
0
1
< 1
> 1
The surface tension vanishes
Liquid and vapour have the same density
There is no distinction between liquid and vapour phases
All (A), (B) and (C)
0
1
2
3
Solid-vapor
Solid-liquid
Liquid-vapor
All (A), (B) and (C)
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
Matter
Energy
Neither matter nor energy
Both matter and energy
d ln p/dt = Hvap/RT2
d ln p/dt = RT2/Hvap
dp/dt = RT2/Hvap
dp/dt = Hvap/RT2
Gibbs-Duhem
Van Laar
Gibbs-Helmholtz
Margules
0
1
y = 1.44
1.66
Unity
Activity
Both (A) & (B)
Neither (A) nor (B)
Is increasing
Is decreasing
Remain constant
Data insufficient, can't be predicted
Increase
Decrease
Not alter
None of these
Increase the partial pressure of H2
Increase the partial pressure of I2
Increase the total pressure and hence shift the equilibrium towards the right
Not affect the equilibrium conditions
Pressure
Temperature
Volume
Molar concentration