You can estimate the size of any diagram by realizing that fr is of order 1 out to a distance of about the diameter of a molecule, andf0 beyond that. Hence, a three-dimensional integral of a product of f's will generally give a result that is of the order of the volume of a molecule. Estimate the sizes of all the diagrams shown explicitly in equation8.20 and explain why it was necessary to rewrite the series in exponential form.

Short Answer

Expert verified

The sizes of all the diagrams shown explicitly in the equation 8.20are 1NvV

2N3v2V2

3N4v3V3

4N3v2V2

5N4v3V36N5v3V37N6v2V28N4v3V3

and the explanation to rewrite the series in exponential form is explained below.

Step by step solution

01

Given Information 

We need to find the necessary to rewrite the series in exponential form.

02

Simplify

In this problem we need to write size of the diagrams in equation , the diagrams are shown in the following figure, for simplicity I will indicate each equation by its number in the figure. The integral for these diagrams are:

1=12NN1V2d3r1d3r2f122=12NN1N2V3d3r1d3r2d3r3f12f233=18NN1N2N3V4d3r1d3r2d3r3d3r4f12f344=16NN1N2V3d3r1d3r2d3r3f12f23f315=16NN1N2N3V4d3r1d3r2d3r3d3r4f14f24f346=14NN1N2N3N4V5d3r1d3r2d3r3d3r4d3r5f12f34f457=18NN1N2N3N4NV6×d3r1d3r2d3r3d3r4d3r5d3r6f12f34f568=16NN1N2N3V4d3r1d3r2d3r3d3r4f13f12f24

03

Calculation

according to the above equation, we can write (realizing that fris in order of 1out of the distance about the diameter of the molecule and f0beyond that):

1NvV

what I have done here is just approximate NN-1, and since we have only one factor of we have one factor of fwhere is the sized volume of the molecule and the integration over the renaming factor of rgives the volume so the volume in the denominator reduced by one order. For the second diagram we get:

2N3v2V2

and so on, we can write:

3N4v3V3

For the fourth diagram, we need to change the coordinates of the diagram as follow:

ra=r1rrb=r1r3

so we can write:

4=16N3V2d3rad3rbfrafrbfrarb4N3v2V2

Following the same method above, we can write the size for the rest of the diagram as:

5N4v3V36N5v3V37N6v2V28N4v3V3

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Most popular questions from this chapter

Modify the ising program to compute the average energy of the system over all iterations. To do this, first add code to the initialise subroutine compute the initial energy of the lattice; then, whenever a dipole is flipped, change the energy variable by the appropriate amount. When computing the average energy, be sure to average over all iterations, not just those iterations in which a dipole is actually flipped (why?). Run the program for a 5 x 5 lattice for T values from 4 down to l in reasonably small intervals, then plot the average energy as a function of T. Also plot the heat capacity. Use at least 1000 iterations per dipole for each run, preferably more. If your computer is fast enough, repeat for a 10x 10 lattice and for a 20 x 20 lattice. Discuss the results. (Hint: Rather than starting over at each temperature with a random initial state, you can save time by starting with the final state generated at the previous, nearby temperature. For the larger lattices you may wish to save time by considering only a smaller temperature interval, perhaps from 3 down to 1.5.)

Implement the ising program on your favourite computer, using your favourite programming language. Run it for various lattice sizes and temperatures and observe the results. In particular:

(a) Run the program with a 20 x 20 lattice at T = 10, 5, 4, 3, and 2.5, for at least 100 iterations per dipole per run. At each temperature make a rough estimate of the size of the largest clusters.

(b) Repeat part (a) for a 40 x 40 lattice. Are the cluster sizes any different? Explain. (c) Run the program with a 20 x 20 lattice at T = 2, 1.5, and 1. Estimate the average magnetisation (as a percentage of total saturation) at each of these temperatures. Disregard runs in which the system gets stuck in a metastable state with two domains.

(d) Run the program with a 10x 10 lattice at T = 2.5. Watch it run for 100,000 iterations or so. Describe and explain the behaviour.

(e) Use successively larger lattices to estimate the typical cluster size at temperatures from 2.5 down to 2.27 (the critical temperature). The closer you are to the critical temperature, the larger a lattice you'll need and the longer the program will have to run. Quit when you realise that there are better ways to spend your time. Is it plausible that the cluster size goes to infinity as the temperature approaches the critical temperature?

Consider an Ising model in the presence of an external magnetic field B, which gives each dipole an additional energy of -μBB if it points up and +μBB if it points down (whereμB is the dipole's magnetic moment). Analyse this system using the mean field approximation to find the analogue of equation 8.50. Study the solutions of the equation graphically, and discuss the magnetisation of this system as a function of both the external field strength and the temperature. Sketch the region in the T-B plane for which the equation has three solutions.

Show that, if you don't make too many approximations, the exponential series in equation 8.22 includes the three-dot diagram in equation 8.18. There will be some leftover terms; show that these vanish in the thermodynamic limit.

Show that the Lennard-Jones potential reaches its minimum value at r=r0, and that its value at this minimum is -u0. At what value of rdoes the potential equal zero?

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