T = [RT/(V- b)] - [a/√T. V(V + b)]
PV/RT = 1 + (B/V) + (C/V2) + ……
n1u2 + μ2μ1 = 0
None of these
B. PV/RT = 1 + (B/V) + (C/V2) + ……
Reversible and isothermal
Irreversible and constant enthalpy
Reversible and constant entropy
Reversible and constant enthalpy
First law
Zeroth law
Third law
Second law
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Pressure
Composition
Temperature
All (A), (B) and (C)
Lowest
Highest
Average
None of these
Decrease in temperature
Increase in temperature
No change in temperature
Change in temperature which is a function of composition
(T2 - T1)/T2
(T2 - T1)/T1
(T1 - T2)/T2
(T1 - T2)/T1
5 & 3
3.987 & 1.987
1.987 & 0.66
0.66 & 1.987
0.25
0.5
0.75
1
The distribution law
Followed from Margules equation
A corollary of Henry's law
None of these
0
1
2
3
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the substance
Air cycle
Carnot cycle
Ordinary vapour compression cycle
Vapour compression with a reversible expansion engine
6738.9
6753.5
7058.3
9000
Less
More
Same
Dependent on climatic conditions
0°C
273°C
100°C
-273°C
Volume
Density
Temperature
Pressure
Any
A perfect
An easily liquefiable
A real
Helmholtz
Gibbs
Both a & b
Neither 'a' nor 'b'
Ideal
Real
Isotonic
None of these
2HI H2 + I2
N2O4 2NO2
2SO2 + O2 2SO3
None of these
dE = CpdT
dE = CvdT
dQ = dE + pdV
dW = pdV
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
T
T and P
T, P and Z
T and Z
0
1
y = 1.44
1.66
A closed system does not permit exchange of mass with its surroundings but may permit exchange of energy.
An open system permits exchange of both mass and energy with its surroundings
The term microstate is used to characterise an individual, whereas macro-state is used to designate a group of micro-states with common characteristics
None of the above
(∂P/∂V)T
(∂V/∂T)P
(∂P/∂V)V
All (A), (B) & (C)
Equal to its density
The reciprocal of its density
Proportional to pressure
None of these
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
Negative
Zero
Infinity
None of these