Approximate the two body correlation function as
Eqn 1
Where Sk(r) is as shown in figure 1
Figure 1 SK(r)
The two-body correlation function is defined to be
Eqn 2
Form
Eqn 3
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Minimize this by setting the partials with respect to cm equal to zero.
Eqn 4
The array of k,m S values becomes
Eqn 5
Thus the equation for the coefficients becomes
Eqn 6
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Any coordinate can be 1 and any other can be 2 so that this is
Note that this merely amounts to counting the number of distances in the ranges rm to rm+1 and dividing by the appropriate volume factor.
The
Markov chain method is to put N particles in the volume V. Move particle j a small amount.
Evaluate the change in . If
. Note that this will
not happen in the beginning if all particles start on lattice sites. If with probability
Use the Markov chain – see ..\..\integration\MonteCarlo\Expectation value of H.htm for details -with a periodically repeated box containing ~64 atoms. Combine this with the OZ equations ..\..\Fourier\OZeqn.doc .htm to find the two body correlation function for a Lennard Jones Liquid. Do this at both a high T ~ 10000 and for a low T ~ 100. Send me plots of the various g(r) ‘s. Periodic distances are discussed in ..\..\integration\MonteCarlo\Periodic Distance.htm.