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The string will have a nodal point in the middle which remains stationary. A drum head<br />

(effectively two dimensional) similarly will have nodal lines, depending on which mode<br />

is excited. A three dimensional object such as a tuning fork or a protein will have a<br />

surface which describes the locus of points that remain stationary when the object<br />

vibrates at one of its normal frequencies. The displacements of points on opposite sides<br />

of this nodal surface have opposite sign.[74] If the structure in question is composed of<br />

two rigid regions connected by a flexible region, then points within each rigid region will<br />

move in a correlated fashion, and points in different regions will tend to be anticorrelated<br />

to conserve center of mass motion. The velocities change sign at the nodal surface, and<br />

therefore the latter might be expected to coincide with the flexible region or hinge[47, 61,<br />

64, 76]. This leads to the following two ideas:<br />

The HAG set consists of proteins with two domains separated by a single (possibly multi-<br />

stranded) flexible region. This single hinge should correspond to a single nodal surface.<br />

The lowest order mode has the smallest number of nodes and (assuming the equipartition<br />

theorem applies) the largest displacements and therefore the coincidence of nodal surface<br />

with hinge should be strongest for this mode.<br />

There may be multiple degrees of freedom about the hinge, and therefore to some degree<br />

the second, third, and higher modes might also coincide with the hinge.<br />

To test these ideas, we extracted the mobility score,<br />

!<br />

166<br />

M ik for each residue i in the<br />

mode, for k = 1 to 7. This quantity is the square fluctuation of residue i in mode k,<br />

!<br />

normalized such that the most mobile residue has mobility Mik =1 for mode k. We then<br />

!<br />

k th

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