An introduction to the physics of the bacterial flagellar motor: A nanoscale rotary electric motor

Contemporary Physics 50:6 (2009) 617-632

Authors:

MAB Baker, RM Berry

Abstract:

Biological molecular motors show us how directed motion can be generated by nanometre-scale devices that work at the energy scale of the thermal bath. Direct and indirect observations of functioning single molecule motors allow us to see fundamental processes of statistical physics unfolding in microscopic detail at room temperature, something that was unimaginable only a few decades ago. In this review, we introduce molecular motors and the physics relevant to their mechanisms before focusing on our recent experiments on the bacterial flagellar motor, the rotary device responsible for bacterial locomotion.

Single molecule measurements of F1-ATPase reveal an interdependence between the power stroke and the dwell duration.

Biochemistry 48:33 (2009) 7979-7985

Authors:

D Spetzler, R Ishmukhametov, T Hornung, LJ Day, J Martin, WD Frasch

Abstract:

Increases in the power stroke and dwell durations of single molecules of Escherichia coli F(1)-ATPase were measured in response to viscous loads applied to the motor and inhibition of ATP hydrolysis. The load was varied using different sizes of gold nanorods attached to the rotating gamma subunit and/or by increasing the viscosity of the medium using PEG-400, a noncompetitive inhibitor of ATPase activity. Conditions that increase the duration of the power stroke were found to cause 20-fold increases in the length of the dwell. These results suggest that the order of hydrolysis, product release, and substrate binding may change as the result of external load on the motor or inhibition of hydrolysis.

A molecular brake, not a clutch, stops the Rhodobacter sphaeroides flagellar motor.

Proc Natl Acad Sci U S A 106:28 (2009) 11582-11587

Authors:

Teuta Pilizota, Mostyn T Brown, Mark C Leake, Richard W Branch, Richard M Berry, Judith P Armitage

Abstract:

Many bacterial species swim by employing ion-driven molecular motors that power the rotation of helical filaments. Signals are transmitted to the motor from the external environment via the chemotaxis pathway. In bidirectional motors, the binding of phosphorylated CheY (CheY-P) to the motor is presumed to instigate conformational changes that result in a different rotor-stator interface, resulting in rotation in the alternative direction. Controlling when this switch occurs enables bacteria to accumulate in areas favorable for their survival. Unlike most species that swim with bidirectional motors, Rhodobacter sphaeroides employs a single stop-start flagellar motor. Here, we asked, how does the binding of CheY-P stop the motor in R. sphaeroides--using a clutch or a brake? By applying external force with viscous flow or optical tweezers, we show that the R. sphaeroides motor is stopped using a brake. The motor stops at 27-28 discrete angles, locked in place by a relatively high torque, approximately 2-3 times its stall torque.

A molecular brake, not a clutch, stops the Rhodobacter sphaeroides flagellar motor

Proceedings of the National Academy of Sciences of the United States of America 106:28 (2009) 11582-11587

Authors:

T Pilizota, MT Brown, MC Leake, RW Branch, RM Berry, JP Armitage

Abstract:

Many bacterial species swim by employing ion-driven molecular motors that power the rotation of helical filaments. Signals are transmitted to the motor from the external environment via the chemotaxis pathway. In bidirectional motors, the binding of phosphorylated CheY (CheY-P) to the motor is presumed to instigate conformational changes that result in a different rotor-stator interface, resulting in rotation in the alternative direction. Controlling when this switch occurs enables bacteria to accumulate in areas favorable for their survival. Unlike most species that swim with bidirectional motors, Rhodobacter sphaeroides employs a single stopstart flagellar motor. Here,weasked,howdoes the binding of CheY-P stop the motor in R. sphaeroides - using a clutch or a brake? By applying external force with viscous flow or optical tweezers, we show that the R. sphaeroides motor is stopped using a brake. The motor stops at 27-28 discrete angles, locked in place by a relatively high torque, approximately 2-3 times its stall torque.

The mechanics of slithering locomotion.

Proceedings of the National Academy of Sciences of the United States of America 106:25 (2009) 10081-10085

Authors:

David L Hu, Jasmine Nirody, Terri Scott, Michael J Shelley

Abstract:

In this experimental and theoretical study, we investigate the slithering of snakes on flat surfaces. Previous studies of slithering have rested on the assumption that snakes slither by pushing laterally against rocks and branches. In this study, we develop a theoretical model for slithering locomotion by observing snake motion kinematics and experimentally measuring the friction coefficients of snakeskin. Our predictions of body speed show good agreement with observations, demonstrating that snake propulsion on flat ground, and possibly in general, relies critically on the frictional anisotropy of their scales. We have also highlighted the importance of weight distribution in lateral undulation, previously difficult to visualize and hence assumed uniform. The ability to redistribute weight, clearly of importance when appendages are airborne in limbed locomotion, has a much broader generality, as shown by its role in improving limbless locomotion.