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Upon binding ATP, M rotates approximately 45° with respect to S. The large scale of<br />

this change and the existence of structural domains makes BC a good test case for our<br />

method.<br />

We used the BC subunit of Aquifex aeolicus PC[103] as the starting or apo structure.<br />

The ligand-free BC subunit of E. coli ACC has been crystallized (PDB ID: 1DV1), but<br />

many residues are disordered and so the structure of the M domain is not entirely<br />

clear.[104] No ATP-bound structure of A. aeolicus BC is available, and so we used ATP-<br />

bound BC from E. coli ACC[104] as our holo structure. The sequence differences<br />

between the starting and holo structures had an impact on the results as we will discuss.<br />

FlexOracle[90] predicts a hinge at residues 86-89 and 182-185, which can be used to<br />

choose the location of L.<br />

The significant sequence and structural differences between the starting and holo<br />

structures, which come from different organisms, made comparison on the basis of<br />

sRMSD difficult. As we did for GlnBP, in figure 5.4.a we color the conformers by<br />

sRMSD. The lowest-sRMSD conformer is indicated by the larg sphere. However that<br />

conformer was only partially closed, and visibly different from the holo structure, shown<br />

in inset 5.4.c. The structure that minimizes the fitness function (inset 5.4.d) bears clear<br />

similarities to the holo in relative domain orientation. The starting structure (inset 5.4.b)<br />

shows the extent of the Domain 3 motion involved.<br />

258

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