μ = (∂P/∂T)H
μ = (∂T/∂P)H
μ = (∂E/∂T)H
μ = (∂E/∂P)H
B. μ = (∂T/∂P)H
Oxygen
Nitrogen
Air
Hydrogen
Low temperature
High pressure
Both (A) and (B)
Neither (A) nor (B)
1
< 1
> 1
>> 1
Pressure
Solubility
Temperature
None of these
Solids
Liquids
Gases
All (A), (B) & (C)
State functions
Path functions
Intensive properties
Extensive properties
0
< 0
> 0
A function of pressure
Zero
Negative
Very large compared to that for endothermic reaction
Not possible to predict
Below
At
Above
Either 'b' or 'c'
States that n1dμ1 + n2dμ2 + ....njdμj = 0, for a system of definite composition at constant temperature and pressure
Applies only to binary systems
Finds no application in gas-liquid equilibria involved in distillation
None of these
A heating effect
No change in temperature
A cooling effect
Either (A) or (C)
T
√T
T2
1/√T
Moisture free ice
Solid helium
Solid carbon dioxide
None of these
0.25
0.5
0.75
1
Supersaturated
Superheated
Both (A) and (B)
Neither (A) nor (B)
Increased COP
Same COP
Decreased COP
Increased or decreased COP; depending upon the type of refrigerant
Pressure
Volume
Mass
None of these
At constant pressure, solubility of a gas in a liquid diminishes with rise in temperature
Normally, the gases which are easily liquefied are more soluble in common solvents
The gases which are capable of forming ions in aqueous solution are much more soluble in water than in other solvents
At constant pressure, solubility of a gas in a liquid increases with rise in temperature
Sublimation
Fusion
Transition
Vaporisation
Temperature vs. enthalpy
Temperature vs. enthalpy
Entropy vs. enthalpy
Temperature vs. internal energy
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
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
0
1
2
3
RT d ln P
R d ln P
R d ln f
None of these
270
327
300
540
Tds = dE + dW
dE - dW = Tds
dW - dE = Tds
Tds - dW + dE >0
Bucket
Throttling
Separating
A combination of separating & throttling
Water
Air
Evaporative
Gas
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
Reversible and isothermal
Isothermal and irreversible
Reversible and adiabatic
Adiabatic and irreversible