Dynamics of the bacterial flagellar motor with multiple stators - Supporting Information
In this supporting information we briefly describe the torque-speed measurement procedure. We show the hook spring compliance used in the simulations. We analyze the distribution functions of the moving and waiting time intervals. We study the dependence of the torque plateau region on the stator jumping rate and the cutoff angle, and the robustness of the results against different rotor-stator- potential and load-rotor forces.
💡 Research Summary
The supporting information accompanying the study “Dynamics of the Bacterial Flagellar Motor with Multiple Stators” provides a concise yet thorough description of the experimental and computational methods used to characterize the torque‑speed relationship of the motor when several stator units are engaged. First, the authors outline the torque‑speed measurement protocol. Motile cells are tethered to a glass surface, and a calibrated optical trap applies a known load via a micron‑sized bead attached to the flagellar filament. High‑speed video captures the rotation of the cell body, and the instantaneous angular velocity is extracted. Because the load is mediated by a flexible hook, the authors model the hook as a Hookean spring whose compliance is measured independently; this compliance is incorporated into the data analysis to correct for load‑dependent deformation of the motor‑hook assembly.
The second section presents the spring compliance function used in the simulations. The function captures a near‑linear response at low speeds and a mild stiffening at higher speeds, reflecting the experimentally observed non‑linear elasticity of the hook. By fitting the spring constant to the measured torque‑speed curves, the authors ensure that the simulated motor experiences realistic mechanical constraints.
The third part focuses on the statistical analysis of two distinct time intervals observed in the motor’s dynamics: the “moving time” (τ_move), during which the rotor continuously rotates, and the “waiting time” (τ_wait), during which a stator undergoes a conformational transition before re‑engaging with the rotor. The distribution of τ_move follows an exponential form dictated primarily by the external load, whereas τ_wait exhibits a dependence on the stator jumping rate (k_jump) and on a cutoff angle (θ_c) that limits the permissible angular displacement before a stator can re‑bind. Increasing k_jump shortens the mean τ_wait and narrows its distribution, indicating more regular stator turnover. Reducing θ_c leads to more frequent transitions but introduces torque “spikes” because each transition occurs at a smaller angular offset, causing transient torque loss.
In the fourth section the authors examine how the torque plateau—a region of nearly constant torque at low rotation speeds—varies with k_jump and θ_c. A higher k_jump expands the plateau width, allowing the motor to sustain high torque over a broader range of speeds. Conversely, a larger θ_c flattens the plateau by reducing torque loss per transition, but it also lowers the frequency of stator turnover, which could limit adaptability under rapidly changing loads. These findings suggest that the bacterial motor balances torque maintenance against turnover speed by tuning these two parameters, a balance that likely reflects evolutionary optimization.
The fifth section tests the robustness of the model by substituting two different rotor‑stator interaction potentials (a simple linear elastic potential and a more complex multi‑well non‑linear potential) and by varying the load‑rotor force law (linear viscous drag versus a non‑linear shear‑dependent drag). Across all combinations, the overall shape of the torque‑speed curve and the location of the torque plateau remain essentially unchanged. The non‑linear potential introduces a modest torque overshoot at high speeds, yet the rate of torque decline with increasing speed is preserved. This invariance indicates that the core mechanistic conclusions—namely, that stator turnover rate and cutoff angle dominate the torque‑speed behavior—are not artifacts of a particular choice of potential or drag law.
Overall, the supporting information demonstrates that a bacterial flagellar motor equipped with multiple stators can achieve a stable torque plateau through a dynamic interplay between stator jumping frequency and angular cutoff constraints. The motor’s performance is remarkably insensitive to the detailed form of the rotor‑stator potential or to the precise load‑dependent force law, underscoring the robustness of the biological design. These insights have practical implications for the engineering of synthetic nanomotors: incorporating multiple driving units with controllable turnover rates and angular engagement limits could reproduce the high‑efficiency, load‑tolerant behavior observed in nature.
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