Depression in Freezing point and Elevation in Boiling point

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Depression in Freezing Point: Depression in freezing point means freezing point of solution is always less than that of its pure solvent due to lowering of vapour pressure of solution. Depression in freezing point have the formula as given below, ∆T f = i × K f × m                                       eq.. (1) K f = cryoscopic constant This equation tells us that depression of freezing point depends only on   molality of solutions, so it is a colligative property. m= 1000W 2 /W 1 ×M 2                           putting the value of molality in we get          ∆T f   = i × K f × 1000W 2 /W 1 ×M 2        ...

Fugacity and Activity in thermodynamics

 

Fugacity and Activity in Thermodynamics

Fugacity and Chemical Potential

How to determine fugacity of a gas?

Fugacity and Activity:

G.N. Lewis in 1901 introduced the concept of fugacity to explain the actual behavior of real gases in chemical equilibrium at high pressures. It is mainly employed in connection with gases mixture but the introductory treatment is restricted to pure gases.

Fugacity indicates the escaping tendency of a component or a substance. High gas pressure indicates the tendency of gas molecules to escape outside the container. Similarly high fugacity indicates a greater tendency of a component or a substance to escape, dissolve or intermix.

Fugacity may be explained as a substitute for pressure to explain the behavior of real gases and the activity may be defined as the substitute for the concentration to explain the behavior of a non- ideal or real solution. Mathematically, fugacity (f) is defined as

                          LimP→0 f/P = 1

i.e. as the pressure approaches zero fugacity approaches pressure. This means that fugacity is the measure of the pressure of the real gases.

We know that Gibb’s free energy is equal to

                          dG = VdP - SdT

Now, at constant temperature dT= 0,

Hence above equation becomes dG = VdP                                            eq…… (1)

For one mole of an ideal gas equation of state becomes PV = RT

Therefore,         V = [RT/P]                                                                      eq……(2)

Hence Gibb’s free energy eq becomes, dG = [RT/P]dP = RT d (lnP)

Above equation is for ideal gas, if the gas is not ideal then pressure is replaced by fugacity

Hence,              dG = RT d(lnf)                                                                 eq……(3)

Chemical Potential and Fugacity :

In a mixture of real gases, the chemical potential of constituent i  is given by

                          μ = μi0 + RTlnfi

Where fi is the fugacity of the constituent i in the mixture. Similarly in non- ideal solutions the chemical potential of any component i is given by

                           μ = μi0 + RTlnai

where ai is the activity of the component i in the solution.

Activity:

It has been observed that thermodynamic variables (H, S, G etc.) of a substance in pure state are different from those in a state of solution .i.e., when a substance goes into solution the state of aggregation or dispersion changes and H, S and G also change. This means apart from pressure and temperature these variables also change with change of composition. The concept of activity gives an index to measure these changes when a pure substance goes into state of solution.

Fugacity and activity coefficient:

To get fugacity the pressure has to be corrected by multiplying with suitable factor.

           f = γ × P                                                                 eq……(4)

γ is called activity coefficient of the gas, γ = f/P

Hence activity coefficient of a gas can be defined as,” the ratio of fugacity of a gas to the pressure of the gas in the same state.”

For ideal gases γ is always equal to 1. For real gases γ is always less than 1.

Similarly in non-ideal solutions the concentration has to be corrected to give activity as follows

                    a= γ × C                                                     eq…….(5)

 γ represents the activity coefficient of that component of a solution whose concentration is C.

                      γ = a/C

For ideal solutions γ = 1 so a=C

Determination of fugacity of a gas:

To determine the fugacity of a gas at any pressure where it deviates from ideal behavior the following procedure is used.

We know dG = VdP from eq….(1), and dG = RT d(lnf) from eq….(3)

So,                VdP = RT dln f                                         eq……(6)

                     [ Δlnf/δP]T = V/RT

For an ideal gas the volume of 1 mole RT/P. For a real gas this volume is represented by a and is given by

                          a = RT/P- V

                          V = RT/P- a

By putting the value of V in eq ….(6) we get

                          RT (dP/P) – adP =RT dlnf

Dividing both side sby RT we get

                           dlnf = dP/P – a(dP/RT) or dlnf = dlnP - a(dP/RT)

                           dlnf – dlnP = -a(dP/RT)

                           dln(f/P) = -a (1/RT )dP

If this result is integrated between low virtually zero, pressure and given pressure P at constant temperature then

                          dlnf = -1/RT 0P adP

Graphical method for determination of fugacity



 

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