Bidirectional Power Stroke by Ncd Kinesin

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Presentation transcript:

Bidirectional Power Stroke by Ncd Kinesin Anthony E. Butterfield, Russell J. Stewart, Christoph F. Schmidt, Mikhail Skliar  Biophysical Journal  Volume 99, Issue 12, Pages 3905-3915 (December 2010) DOI: 10.1016/j.bpj.2010.10.045 Copyright © 2010 Biophysical Society Terms and Conditions

Figure 1 (A) Experimental setup. (B) Two-bead model. Refer to Table S1 in the Supporting Material for the nomenclature and the definition of all variables. (C) Single-bead model. Biophysical Journal 2010 99, 3905-3915DOI: (10.1016/j.bpj.2010.10.045) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 2 Validation of the Kalman filters in simulations. The time series of true motor head displacements was used in the two-bead model to produce synthetic measurements, y, of the right bead position (shown in gray). Ktotal, identified by the single-bead Kalman filter, is shown in red. Orange line shows Ktotal identified using Eq. 12. The identified xAT and the filtered xR (green line) were obtained using the two-bead Kalman filter (Filter 1 in Fig. S1). Biophysical Journal 2010 99, 3905-3915DOI: (10.1016/j.bpj.2010.10.045) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 3 Examples of ncd-MT events. (Vertical arrows) Peak motor head displacements due to terminal motor action. (A–D) Minus-end power strokes against a loading force due to attachment displacement, xeq. (E) Power stroke toward the minus-end starts with assisting force, due to small negative xeq, ending with loading force. (F) Event with a stroke-assisting force due to binding location. (G and H) Events without detected stroke. (I and J) Events with the power stroke toward MT's plus-end and a loading force due to equilibrium displacement. Biophysical Journal 2010 99, 3905-3915DOI: (10.1016/j.bpj.2010.10.045) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 4 (A) Distribution of equilibrium displacements, xeq, due to binding location. (B) Distribution of the identified terminal displacements, xtm, due to motor action. Biophysical Journal 2010 99, 3905-3915DOI: (10.1016/j.bpj.2010.10.045) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 5 Results of ensemble averaging. (A) Average of all 675 detected motor events. (B) All 675 events in the y axis. (C) All 322 events with a positive equilibrium displacement (333 events based on NN classification). (D) All 353 events with a negative equilibrium displacement (286 events based on NN classification). (E) All 418 events with a positive (minus-end directed) terminal motor action (414 events based on NN classification). (F) All 216 events with a negative (plus-end directed) terminal motor action (205 events based on NN classification). (Dashed vertical lines) Event start and stop times. Biophysical Journal 2010 99, 3905-3915DOI: (10.1016/j.bpj.2010.10.045) Copyright © 2010 Biophysical Society Terms and Conditions

Figure 6 ATP dependence of the duration of positive and negative terminal displacements. (A) Histograms and exponential fits for 2 μM ATP concentration. (B) The same for 5 μM ATP concentration. Biophysical Journal 2010 99, 3905-3915DOI: (10.1016/j.bpj.2010.10.045) Copyright © 2010 Biophysical Society Terms and Conditions