(∂P/∂V)T
(∂V/∂T)P
(∂P/∂V)V
All (A), (B) & (C)
A. (∂P/∂V)T
H = E - PV
H = F - TS
H - E = PV
None of these
He
N2
O2
H2
Entropy
Temperature
Internal energy
Enthalpy
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
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
The available energy in an isolated system for all irreversible (real) processes decreases
The efficiency of a Carnot engine increases, if the sink temperature is decreased
The reversible work for compression in non-flow process under isothermal condition is the change in Helmholtz free energy
All (A), (B) and (C)
Pressure and temperature
Reduced pressure and reduced temperature
Critical pressure and critical temperature
None of these
Compression ratio of an Otto engine is comparatively higher than a diesel engine
Efficiency of an Otto engine is higher than that of a diesel engine for the same compression ratio
Otto engine efficiency decreases with the rise in compression ratio, due to decrease in work produced per quantity of heat
Diesel engine normally operates at lower compression ratio than an Otto engine for an equal output of work
0
1
2
3
Isothermal
Adiabatic
Isobaric
Isometric
1
2
3
4
dE = CpdT
dE = CvdT
dQ = dE + pdV
dW = pdV
Isochoric
Isobaric
Adiabatic
Isothermal
Less
More
Same
Dependent on climatic conditions
Zero
One
Infinity
Negative
Polar
Non-polar
Both (A) & (B)
Neither (A) nor (B)
Enthalpies of all elements in their standard states are assumed to be zero
Combustion reactions are never endothermic in nature
Heat of reaction at constant volume is equal to the change in internal energy
Clausius-Clapeyron equation is not applicable to melting process
Van Laar
Margules
Gibbs-Duhem
Gibbs-Duhem-Margules
High thermal conductivity
Low freezing point
Large latent heat of vaporisation
High viscosity
Chemical potential
Activity
Fugacity
Activity co-efficient
Entropy
Gibbs energy
Internal energy
Enthalpy
Zero
Positive
Negative
Indeterminate
(∂E/∂ni)S, v, nj
(∂G/∂ni)T, P, nj = (∂A/∂ni) T, v, nj
(∂H/∂ni)S, P, nj
All (A), (B) and (C)
Solubility increases as temperature increases
Solubility increases as temperature decreases
Solubility is independent of temperature
Solubility increases or decreases with temperature depending on the Gibbs free energy change of solution
Evaporation
Liquid extraction
Drying
Distillation
Specific volume
Work
Pressure
Temperature
With pressure changes at constant temperature
Under reversible isothermal volume change
During heating of an ideal gas
During cooling of an ideal gas
< 0
> 0
= 0
None of these
Chemical potentials of a given component should be equal in all phases
Chemical potentials of all components should be same in a particular phase
Sum of the chemical potentials of any given component in all the phases should be the same
None of these
Zero
Unity
Infinity
Negative