The 2 nanomotors of rotary ATP synthase, ionmotive FO and chemically active F1, are mechanically coupled by a central rotor and an eccentric bearing. Both motors rotate, with 3 steps in F1 and 10 -15 in FO. Simulation by statistical mechanics has revealed that an elastic power transmission is required for a high rate of coupled turnover. Here, we investigate the distribution in the FOF1 structure of compliant and stiff domains. The compliance of certain domains was restricted by engineered disulfide bridges between rotor and stator, and the torsional stiffness () of unrestricted domains was determined by analyzing their thermal rotary fluctuations. A fluorescent magnetic bead was attached to single molecules of F 1 and a fluorescent actin filament to FOF1, respectively. They served to probe first the functional rotation and, after formation of the given disulfide bridge, the stochastic rotational motion. Most parts of the enzyme, in particular the central shaft in F1, and the long eccentric bearing were rather stiff (torsional stiffness > 750 pNnm). One domain of the rotor, namely where the globular portions of subunits ␥ and of F1 contact the c-ring of FO, was more compliant ( Х 68 pNnm). This elastic buffer smoothes the cooperation of the 2 stepping motors. It is located were needed, between the 2 sites where the power strokes in FO and F1 are generated and consumed.elasticity ͉ F-ATPase ͉ nanomotor
The F(O)F(1)-ATPase is a rotary molecular motor. Driven by ATP-hydrolysis, its central shaft rotates in 80 degrees and 40 degrees steps, interrupted by catalytic and ATP-waiting dwells. We recorded rotations and halts by means of microvideography in laboratory coordinates. A correlation with molecular coordinates was established by using an engineered pair of cysteines that, under oxidizing conditions, formed zero-length cross-links between the rotor and the stator in an orientation as found in crystals. The fixed orientation coincided with that of the catalytic dwell, whereas the ATP waiting dwell was displaced from it by +40 degrees . In crystals, the convex side of the cranked central shaft faces an empty nucleotide binding site, as if holding it open for arriving ATP. Functional studies suggest that three sites are occupied during a catalytic dwell. Our data imply that the convex side faces a nucleotide-occupied rather than an empty site. The enzyme conformation in crystals seems to differ from the conformation during either dwell of the active enzyme. A revision of current schemes of the mechanism is proposed.
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