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. 2013 Dec 20;15(1):75–99. doi: 10.3390/ijms15010075

Figure 9.

Figure 9.

(a) The change of the interhelical angle (Δθ) between the α1 and α2 helices for the apo-Atox1 model (light blue) and the binary models (cyan); and (b) The time-dependence of the interhelical angles along with the respective integrated distributions for the apo-Atox1 (light blue), CisPt + Atox1 (green), TransPt + Atox1 (magenta) and OxaliPt + Atox1 (cyan) models.