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. Author manuscript; available in PMC: 2016 Nov 25.
Published in final edited form as: J Phys Chem B. 2015 Nov 12;119(47):14892–14904. doi: 10.1021/acs.jpcb.5b09299

Figure 4.

Figure 4

A) Motional model for the fluctuations of the phenylalanine side chains. The motions around the χ2 dihedral angle consist of large-angle ring-flips and small-angle fluctuations, parameterized by angle α. The diagram displays sites' connectivities according to the strong collision model, illustrated for one of the Cδ-D bonds. The motion around the χ1 dihedral angle is modeled via the restricted diffusion of the Cβ – Cγ axis along an arc and is approximated by small nearest neighbor jumps. B) Potential corresponding to the model of motions around the χ2 angle, in which Ealarge and Easmall are the activation energies for the large-angle ring-flips and small-angle fluctuations, respectively.