[∂(G/T)/∂T] = - (H/T2)
[∂(A/T)/∂T]V = - E/T2
Both (A) and (B)
Neither (A) nor (B)
C. Both (A) and (B)
CV
Entropy change
Gibbs free energy
None of these
Henry's law
Law of mass action
Hess's law
None of these
High thermal conductivity
Low freezing point
Large latent heat of vaporisation
High viscosity
Volume
Pressure
Temperature
All a, b & c
0
∞
+ ve
- ve
Van Laar equation
Margules equation
Wilson's equation
All (A), (B) and (C)
Less than
Equal to
More than
Either (B) or (C); depends on the type of alloy
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
0.5
3.5
4.5
8.5
100,000 kW
160,000 kW
200,000 kW
320,000 kW
Zeroth
First
Second
Third
Zeroth
First
Second
Third
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)
Decreases
Increases
Remains constant
Decreases logarithmically
Zero
Positive
Negative
None of these
In which there is a temperature drop
Which is exemplified by a non-steady flow expansion
Which can be performed in a pipe with a constriction
In which there is an increase in temperature
Less
More
Same
More or less depending upon the extent of work done
Lewis-Randall rule
Statement of Van't Hoff Equation
Le-Chatelier's principle
None of these
Increases
Decreases
Remains unchanged
Data insufficient, can't be predicted
Isothermal
Isobaric
Polytropic
Adiabatic
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
Melting of ice
Condensation of alcohol vapor
Sudden bursting of a cycle tube
Evaporation of water
Single phase fluid of varying composition
Single phase fluid of constant composition
Open as well as closed systems
Both (B) and (C)
P + F - C = 2
C = P - F + 2
F = C - P - 2
P = F - C - 2
(∂T/∂V)S = - (∂P/∂S)V
(∂S/∂P)T = - (∂V/∂T)P
(∂V/∂S)P = (∂T/∂P)S
(∂S/∂V)T = (∂P/∂T)V
The concentration of each component should be same in the two phases
The temperature of each phase should be same
The pressure should be same in the two phases
The chemical potential of each component should be same in the two phases
The energy change of a system undergoing any reversible process is zero
It is not possible to transfer heat from a lower temperature to a higher temperature
The total energy of system and surrounding remains the same
None of the above
Snow melts into water
A gas expands spontaneously from high pressure to low pressure
Water is converted into ice
Both (B) & (C)
Entropy
Internal energy
Enthalpy
Gibbs free energy
300 × (32/7)
300 × (33/5)
300 × (333/7)
300 × (35/7)