Chapter 8: Q 8.20 (page 345)
Use a computer to plot as a function of kT/, as predicted by mean field theory, for a two-dimensional Ising model (with a square lattice).
Short Answer
Therefore,
Chapter 8: Q 8.20 (page 345)
Use a computer to plot as a function of kT/, as predicted by mean field theory, for a two-dimensional Ising model (with a square lattice).
Therefore,
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Get started for freeFor each of the diagrams shown in equation 8.20, write down the corresponding formula in terms of functions, and explain why the symmetry factor gives the correct overall coefficient.
By changing variables as in the text, express the diagram in equation in terms of the same integral as in the equation. Do the same for the last two diagrams in the first line of the equation. Which diagrams cannot be written in terms of this basic integral?
In this problem you will use the mean field approximation to analyse the behaviour of the Ising model near the critical point.
(a) Prove that, when
(b) Use the result of part (a) to find an expression for the magnetisation of the Ising model, in the mean field approximation, when T is very close to the critical temperature. You should find (not to be confused with 1/kT) is a critical exponent, analogous to the f defined for a fluid in Problem 5.55. Onsager's exact solution shows that in two dimensions, while experiments and more sophisticated approximations show that in three dimensions. The mean field approximation, however, predicts a larger value.
(c) The magnetic susceptibility is defined as . The behaviour of this quantity near the critical point is conventionally written as , where y is another critical exponent. Find the value of in the mean field approximation, and show that it does not depend on whether T is slightly above or slightly below Te. (The exact value of y in two dimensions turns out to be 7/4, while in three dimensions .)
Problem 8.8. Show that the virial coefficient depends on the diagrams in equation 8.23 that have dots. Write the third virial coefficient, in terms of an integral of functions. Why it would be difficult to carry out this integral?
For a two-dimensional Ising model on a square lattice, each dipole (except on the edges) has four "neighbors"-above, below, left, and right. (Diagonal neighbors are normally not included.) What is the total energy (in terms of ) for the particular state of the square lattice shown in Figure 8.4?
Figure 8.4. One particular state of an Ising model on a square lattice (Problem 8.15).
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