This research identifies hook stiffness as a key factor in torque asymmetry during counter-clockwise and clockwise rotation in bacterial motors.
The bacterial flagellar motor (BFM) drives cell motility by rotating the flagellar filament and converting ion flux into mechanical work. At low counter-clockwise (CCW) rotational speeds, the motor operates near the thermodynamic–reversible limit, where torque remains nearly constant against rotation speed for an extended range. With thermodynamic–reversibility previous model study predicts similar behavior in the clockwise (CW) directions independent of the details of torque generation. Structural studies further support this symmetry by showing that the torque-generation machinery in the two directions is essentially mirror-reversed. However, single-molecule measurements reveal a striking asymmetry: CCW rotation shows a torque plateau, whereas CW rotation displays a linear decrease in torque with increasing speed. Here, we identify that this asymmetry has a mechanical origin in the rotation-dependent elasticity of the hook rather than in the motor’s torque-generating units. In CCW rotation, the hook remains bent and compliant, maintaining a separation of time scales between motor stepping and load response and thereby preserving the torque plateau in the nearly thermodynamic reversible region. In CW rotation, the hook straightens and stiffens, collapsing the time-scale separation and generating the observed linear torque–speed relationship. A mathematical model that varies only the hook’s bending stiffness quantitatively reproduces the experimental torque–speed curves in both directions. These results resolve the long-standing puzzle of torque–speed asymmetry and identify hook elasticity as a key physical regulator of torque transmission in rotary molecular machines.
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Das et al. (2026) studied this question.
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