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!<br />

!<br />

!<br />

eigenvector. The resulting reordering of rows and columns of the contact matrix is such<br />

that residues tend to be grouped with those they are in contact with, regardless of their<br />

place in the protein sequence. The matrix then consists of only two submatrices, and the<br />

numerical problem is only that of finding the optimal boundary between them. The<br />

optimal choice of boundary is that which maximizes the period of oscillation of an<br />

equivalent two-mass-spring system per supplementary Equation 9:<br />

" = µ<br />

#10<br />

I12 $12 s [9]<br />

Where the reduced mass is used:<br />

µ = N1N2 . [10]<br />

N1 + N2 Here<br />

!<br />

N 1 and<br />

N 2 are the number of residues in the first and second submatrices, and<br />

the sum of the interface contacts.<br />

After reordering there is only a single boundary, and thus only N evaluations of τ are<br />

needed, whereas without this reordering some power of N evaluations would be needed.<br />

199<br />

!<br />

I 12 is

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