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
C. 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
Critical
Boyle
Inversion
Reduced
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Ideal
Very high pressure
Very low temperature
All of the above
Vapor compression cycle using expansion valve
Air refrigeration cycle
Vapor compression cycle using expansion engine
Carnot refrigeration cycle
System (of partially miscible liquid pairs), in which the mutual solubility increases with rise in temperature, are said to possess an upper consolute temperature
Systems, in which the mutual solubility increases with decrease in temperature, are said to possess lower consolute temperature
Nicotine-water system shows both an upper as well as a lower consolute temperature, implying that they are partially miscible between these two limiting temperatures
None of these
+ve
0
-ve
∞
dQ = dE + dW
dQ = dE - dW
dE = dQ + dW
dW = dQ + dE
100,000 kW
160,000 kW
200,000 kW
320,000 kW
Two temperatures only
Pressure of working fluid
Mass of the working fluid
Mass and pressure both of the working fluid
Pressure
Solubility
Temperature
None of these
Infinity
Unity
Constant
Negative
μ° + RT ln f
μ°+ R ln f
μ° + T ln f
μ° + R/T ln f
Adiabatic
Isothermal
Isometric
None of these
Zero
One
Infinity
Negative
Is the analog of linear frictionless motion in machines
Is an idealised visualisation of behaviour of a system
Yields the maximum amount of work
Yields an amount of work less than that of a reversible process
Positive
Negative
Zero
May be positive or negative
Pressure
Volume
Temperature
All (A), (B) & (C)
Same in both the phases
Zero in both the phases
More in vapour phase
More in liquid phase
Free energy
Entropy
Refractive index
None of these
[∂(G/T)/∂T] = - (H/T2)
[∂(A/T)/∂T]V = - E/T2
Both (A) and (B)
Neither (A) nor (B)
If an insoluble gas is passed through a volatile liquid placed in a perfectly insulated container, the temperature of the liquid will increase
A process is irreversible as long as Δ S for the system is greater than zero
The mechanical work done by a system is always equal to∫P.dV
The heat of formation of a compound is defined as the heat of reaction leading to the formation of the compound from its reactants
Non-uniformly
Adiabatically
Isobarically
Isothermally
Below
At
Above
Either 'b' or 'c'
Kinematic viscosity
Work
Temperature
None of these
Conduction
Convection
Radiation
Condensation
Initial concentration of the reactant
Pressure
Temperature
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
Molar volume, density, viscosity and boiling point
Refractive index and surface tension
Both (A) and (B)
None of these
Zero
Positive
Negative
None of these
1.987 cal/gm mole °K
1.987 BTU/lb. mole °R
Both (A) and (B)
Neither (A) nor (B)