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. 2017 Dec 19;6:e32742. doi: 10.7554/eLife.32742

Figure 5. Structural importance of R788 at the converter/Nter/lever junction.

(A) Relay helix angle as a function of MD simulation time, as monitored by the angle between Cα atoms of residues S489, M510, and E521 along the trajectories. The relay helix straightens in NM2C with a steady increase in the angle of the relay helix from approximately 145° to 150°, while the angle does not change significantly in R788E and fluctuates around 145° throughout the 100 ns time course of the simulation. Values for the relay helix angle observed in crystal structures of pre-power stroke (PPS) and post-rigor (PR) are indicated by dotted lines. (B) Population of hydrogen bonds (HB) between R788 (NM2C) or E788 (R788E) and surrounding structural elements over the simulation time of 100 ns. The abbreviations s and m indicate side chain and main chain. (C) Dynamics and conformational changes in NM2C during MD simulations. Snapshots from the start (0 ns simulation time) and end conformations (100 ns simulation time) are shown in light cyan and colored cartoon representation, respectively. The relay helix is shown in red, the SH1-SH2 helix in purple and the converter in grey. Relay loop W525 is shown in red in stick representation. The insets show a close-up view of the conformational changes of W525 along the simulation trajectory. (D) Tryptophan fluorescence emission spectrum of 4 µM NM2C in the absence of nucleotide or the presence of 0.5 mM ATP or 0.5 mM ADP. (E) Dynamics and conformational changes in R788E during MD simulations. Snapshots from the start (0 ns simulation time) and end conformations (100 ns simulation time) are shown in light cyan and colored cartoon representation, respectively. The relay helix is shown in red, the SH1-SH2 helix in purple and the converter in grey. Relay loop W525 is shown in red in stick representation. The insets show a close-up view of the conformational changes of W525 along the simulation trajectory. (F) Tryptophan fluorescence emission spectrum of 4 µM R788E in the absence of nucleotide or presence of 0.5 mM ATP or 0.5 mM ADP.

Figure 5.

Figure 5—figure supplement 1. Stability of the salt bridge between switch-1 and switch-2 in MD simulations of NM2C, R788K, and R788E.

Figure 5—figure supplement 1.

(A) Monitored number of hydrogen bond (#HB) interactions between R261 (switch-1) and E483 (switch-2) along the simulation time of NM2C. (B) Monitored number of hydrogen bond (#HB) interactions between R261 (switch-1) and E483 (switch-2) along the simulation time of R788E (B). Hydrogen bonds were detected with cutoff values for the donor-acceptor distance and angle of 3.5 Å and 30°. Note the intermediate breaking of the salt-bridge in R788E (B). (C) Distance between main chain of G481 of switch-2 with the γ-phosphate of ATP during the 100 ns simulation time for NM2C. (D) Population of hydrogen bonds (HB) between structural elements of the active site of NM2C and ATP along the 100 ns simulation. The abbreviations s and m indicate side chain and main chain, respectively. (E) Population of hydrogen bonds (HB) between R788 (NM2C) or K788 (R788K) and surrounding structural elements along the simulation time. The abbreviations s and m indicate side chain and main chain, respectively. (F) Monitored number of hydrogen bond (#HB) interactions between R261 (switch-1) and E483 (switch-2) along the simulation trajectory of R788K. Simulations for NM2C, R788K, and R788E were performed in the presence of ATP in the active site.