Praveen D. Chowdary, Daphne L. Che, Kai Zhang, Bianxiao Cui 

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Retrograde NGF Axonal Transport—Motor Coordination in the Unidirectional Motility Regime  Praveen D. Chowdary, Daphne L. Che, Kai Zhang, Bianxiao Cui  Biophysical Journal  Volume 108, Issue 11, Pages 2691-2703 (June 2015) DOI: 10.1016/j.bpj.2015.04.036 Copyright © 2015 Biophysical Society Terms and Conditions

Figure 1 (A) Retrograde QD-NGF endosome trajectories at 24°C, shown as the motion along microtubules, Q||(t). (Black) Parsed constant velocity segments are also shown superimposed. (Red/gray) The periods (B and C, insets) are pauses identified by transient motion analysis with a 1-s sliding window. (D, inset) Anterograde direction reversals. (E) Distribution of diffusion constant for endosome pauses >1.5 s. (F) Distributions of microtubule curvature obtained from endosome tracks using sliding window quadratic fitting (red/gray, N = 22,399) and the curvature at pause locations (black, N = 1566). See Fig. S2. (G) Distribution of pause duration at 24°C fits to a double-exponential (χ2 = 1.01). We fit the bins with pause duration >1.1 s and counts >5. To see this figure in color, go online. Biophysical Journal 2015 108, 2691-2703DOI: (10.1016/j.bpj.2015.04.036) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 2 Probability distributions of transport metrics for retrograde NGF-endosomes at 24°C (black) and 37°C (red/gray). (A) Average speed of directed motion. (B) Retrograde (+) and anterograde (−) run velocities. (C) Retrograde (+) and anterograde (−) run lengths shown on a log-linear scale. (Inset) Same figure on linear scale. (D) Duration of parsed pauses. To see this figure in color, go online. Biophysical Journal 2015 108, 2691-2703DOI: (10.1016/j.bpj.2015.04.036) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 3 Distributions of net-directionality (A), pause propensity (B), and reversal propensity (C) from the experimental trajectories at 24°C. (D) Scatter plot demonstrating the correlation between reversal and pause propensities. Biophysical Journal 2015 108, 2691-2703DOI: (10.1016/j.bpj.2015.04.036) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 4 (A–C) In vitro model simulation (red/gray) with Poisson-distributed dyneins (mean = 5) and kinesins (mean = 1.5) on endosomes. The kinesin binding rate is reduced by 10 times to 0.5/s. Experiments (black) at 24°C. The parameter set is summarized in Table S1 and the model performance is quantified in Table 1 G. To see this figure in color, go online. Biophysical Journal 2015 108, 2691-2703DOI: (10.1016/j.bpj.2015.04.036) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 5 Dynamics of QD-NGF-endosomes under load in axons. (A, Inset) The 2-μm reversal confirming the activity of opposite polarity motors on the endosome. (B, Inset) Repeated stalling, detachment, and relaunch of the endosomal motors working against load. (B, Arrows) The shoulders that are typical of stochastic load sharing and multimotor stall profiles. Two of the nine detachments result in direction reversals of the endosome (green/dashed arrows). (C, Inset) Zoomed-in view of one such reversal showing TStall, the stall duration before detachment. To see this figure in color, go online. Biophysical Journal 2015 108, 2691-2703DOI: (10.1016/j.bpj.2015.04.036) Copyright © 2015 Biophysical Society Terms and Conditions