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. 2012 Jul;183(7):1481–1490. doi: 10.1016/j.cpc.2012.02.008

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© 2012 Elsevier B.V.

Open Access under CC BY-NC-ND 3.0 license

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Fig. 2 — cAIC-Differences $Δ_{p}$ for the polynomial models over all crystal structures of MH1. (A) MH1 α-helix of G-ALPHA1: 2nd vector component $f_{2}$ . (B) MH1 α-helix of G-ALPHA2: 2nd vector component $f_{2}$ . (C) MH1 α-helix of G-ALPHA1: 3rd vector component $f_{3}$ . (D) MH1 α-helix of G-ALPHA2: 3rd vector component $f_{3}$ .