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. 2012 Nov 21;103(10):2167–2176. doi: 10.1016/j.bpj.2012.10.013

Table 1.

Change in the integral of quasielastic neutron dynamic susceptibility χ″(q,ν) and dynamic structure factor S(q,ω)

Region Residues Number of H values χ″(q,ν) Relative increase (%) S(q,ω) Relative increase (%)
B/C loop 78–105 161 8.8 ± 0.6 13.5 ± 1.1
F/G loop 186–193 43 6.1 ± 1.6 9.4 ± 2.3
β5 sheet 385–400 88 6.7 ± 0.4 7.5 ± 0.8
β4 sheet 305–313 59 5.0 ± 1.0 6.1 ± 1.4
I-helix kink 243–254 78 4.6 ± 0.3 5.4 ± 0.3
Total of the above 429 6.8 ± 0.7 9.4 ± 1.1
Remainder protein 2121 0.5 ± 0.03 0.9 ± 0.04
Entire protein 1–414 2550 3.3 ± 0.1 2.6 ± 0.1

These are for various regions in substrate-free CYP101, relative to the camphor-bound form over energy range 2–200 μeV (i.e., 0.5–50 GHz) calculated from MD simulations.