Problem 8.8. Show that the nthvirial coefficient depends on the diagrams in equation 8.23 that have ndots. Write the third virial coefficient, C(T), in terms of an integral of f-functions. Why it would be difficult to carry out this integral?

Short Answer

Expert verified

The third virial coefficient isC(T)=13!f(r)dr2.

Step by step solution

01

Given Information

Virial coefficient =nth

Dots denoted by =n

02

Explanation

Let's begin with the definition of the nthVirial Coefficient.

Vn(T)=1n!d3rf(r)n

If we consider diagrams in 8.23, we have

We need to have another d3rifor each dot and a fijfor each link when translating diagrams into integrals.

In this case, the symmetry factor, Nvalue, and Vvalue are not relevant since they are in front of the integral.

In this example, we can see how every dot gives us one d3rintegral:

Find the value of:

localid="1651136353483" =12N(N1)(N2)V3d3r1d3r2d3r3f12f23

=12N(N1)(N2)V3d3r1d3r2f12d3rf(r)=12N(N1)(N2)V3d3r1d3rf(r)d3rf(r)

03

Explanation

Similarly to the second example, the third virial coefficient CTinvolves one more f-link, and so can be calculated by:

=12N(N1)(N2)V3d3r1d3r2d3r3f12f23f13

=12N(N1)(N2)V3d3r1d3r2d3r3f12f23f13=12N(N1)(N2)V3d3r1d3r2f12f13f(r)dr,r=r2r3=12N(N1)(N2)V3d3r1f13frdrf(r)dr,r=r2r1=12N(N1)(N2)V3d3r1f13C(T)3!

Therefore, C(T)is obtained by looking at 8.32 (partial by Vprovides a +sign, and2+3is a factor out of the equation):

We get:

C(T)=13!f(r)dr2

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Most popular questions from this chapter

In this section I've formulated the cluster expansion for a gas with a fixed number of particles, using the "canonical" formalism of Chapter 6. A somewhat cleaner approach, however, is to use the "grand canonical" formalism introduced in Section 7.1, in which we allow the system to exchange particles with a much larger reservoir.

(a) Write down a formula for the grand partition function (Z) of a weakly interacting gas in thermal and diffusive equilibrium with a reservoir at fixed T andµ. Express Z as a sum over all possible particle numbers N, with each term involving the ordinary partition function Z(N).

(b) Use equations 8.6 and 8.20 to express Z(N) as a sum of diagrams, then carry out the sum over N, diagram by diagram. Express the result as a sum of similar diagrams, but with a new rule 1 that associates the expression (>./vQ) J d3ri with each dot, where >. = e13µ,. Now, with the awkward factors of N(N - 1) · · · taken care of, you should find that the sum of all diagrams organizes itself into exponential form, resulting in the formula

Note that the exponent contains all connected diagrams, including those that can be disconnected by removal of a single line.

(c) Using the properties of the grand partition function (see Problem 7.7), find diagrammatic expressions for the average number of particles and the pressure of this gas.

(d) Keeping only the first diagram in each sum, express N(µ) and P(µ) in terms of an integral of the Mayer /-function. Eliminate µ to obtain the same result for the pressure (and the second virial coefficient) as derived in the text.

(e) Repeat part (d) keeping the three-dot diagrams as well, to obtain an expression for the third virial coefficient in terms of an integral of /-functions. You should find that the A-shaped diagram cancels, leaving only the triangle diagram to contribute to C(T).

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Use the cluster expansion to write the total energy of a monatomic nonideal gas in terms of a sum of diagrams. Keeping only the first diagram, show that the energy is approximatelyU32NkT+N2V·2π0r2u(r)e-βu(r)drUse a computer to evaluate this integral numerically, as a function of T, for the Lennard-Jones potential. Plot the temperature-dependent part of the correction term, and explain the shape of the graph physically. Discuss the correction to the heat capacity at constant volume, and compute this correction numerically for argon at room temperature and atmospheric pressure.

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