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 147,016 document(s) hit in 31,850,051 MEDLINE articles (0.00 seconds)

Conventional kinesin is a motor protein that moves stepwise along microtubules carrying membrane-bound organelles toward the periphery of cells. The steps are of amplitude 8.1 nm, the distance between adjacent tubulin binding sites, and are powered by the hydrolysis of ATP. We have asked: how many steps does kinesin take for each molecule of ATP that it hydrolyzes? To answer this question, the motility and ATP hydrolysis of recombinant, heterotetrameric and homodimeric conventional Drosophila kinesins adsorbed to 200-nm-diameter casein-coated silica beads were assayed under identical, single-molecule conditions. Division of the speed by the maximum microtubule-activated ATPase rate gave a stoichiometry of 1. 08 +/- 0.09 steps for each ATP hydrolyzed at 1 mM ATP. Therefore, under low loads in which the drag force << 1 pN, coupling between the chemical and mechanical cycles of kinesin is tight, consistent with conventional power stroke models. Our results rule out models that require two or more ATPs/step, such as some thermal ratchet models, or that propose multiple steps powered by single ATPs.
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PMID:Kinesin takes one 8-nm step for each ATP that it hydrolyzes. 992 Sep 16

Many types of cellular motility, including muscle contraction, are driven by the cyclical interaction of the motor protein myosin with actin filaments, coupled to the breakdown of ATP. It is thought that myosin binds to actin and then produces force and movement as it 'tilts' or 'rocks' into one or more subsequent, stable conformations. Here we use an optical-tweezers transducer to measure the mechanical transitions made by a single myosin head while it is attached to actin. We find that two members of the myosin-I family, rat liver myosin-I of relative molecular mass 130,000 (M(r) 130K) and chick intestinal brush-border myosin-I, produce movement in two distinct steps. The initial movement (of roughly 6 nanometres) is produced within 10 milliseconds of actomyosin binding, and the second step (of roughly 5.5 nanometres) occurs after a variable time delay. The duration of the period following the second step is also variable and depends on the concentration of ATP. At the highest time resolution possible (about 1 millisecond), we cannot detect this second step when studying the single-headed subfragment-1 of fast skeletal muscle myosin II. The slower kinetics of myosin-I have allowed us to observe the separate mechanical states that contribute to its working stroke.
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PMID:The motor protein myosin-I produces its working stroke in two steps. 1020 38

Myosin subfragment 1 (S1) is the ATP catalyzing motor protein in muscle. It consists of three domains that catalyze ATP and bind actin (catalytic), conduct energy transduction (converter), and transport the load (lever arm). These domains interface in two places identified as interface I, containing the reactive thiol (SH1) and ATP-sensitive tryptophan (Trp510), and interface II, containing the reactive lysine residue (RLR). Two crystal structures of S1 were extrapolated to working "in solution" or oriented "in tissue" forms, using structure-sensitive optical spectroscopic signals from extrinsic probes located in the interfaces. Observed signals included circular dichroism (CD) and absorption originating from S1 in solution in the presence and absence of actin and fluorescence polarization from cross-bridges in muscle fibers. Theoretical signals were calculated from S1 crystal structure models perturbed with lever arm movement from swiveling at three conserved glycines, 699, 703, and 710 (chicken skeletal myosin numbering). Structures giving the best agreement between the computed and observed signals were selected as the representative forms. Both interfaces undergo dramatic conformational change during ATPase and force development. Changes at interface I suggest the molecular basis for the collisional quenching sensitivity of Trp510 to nucleotide binding. The probe conformation at SH1 suggests how it alters S1 ATPases. At interface II, the spatial relationship of the lever arm and the extrinsic probe at RLR suggests how the probe alters S1 ATPases and that it should inhibit lever arm movement during the power stroke. The latter possibility, if true, establishes a part of the corridor through which the lever arm swings during the power stroke. Global structural changes in actomyosin are discussed in the accompanying paper [Burghardt et al. (2001) Biochemistry 40, 4821-4833].
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PMID:Conformation of myosin interdomain interactions during contraction: deductions from proteins in solution. 1129 51

Myosin II is the motor protein that produces force and shortening in muscle by ATP-driven cyclic interactions of its globular portion, the head, with the actin filament. During each interaction the myosin head undergoes a conformational change, the working stroke, which, depending on the mechanical conditions, can generate a force of several piconewtons or an axial displacement of the actin filament toward the centre of the sarcomere of several nanometres. However, the sizes of the elementary force and length steps and their dependence on the mechanical conditions are still under question. Due to the small fraction of the ATPase cycle time myosin II spends attached to actin, single molecule mechanics failed to produce definitive measurements of the individual events. In intact frog muscle fibres, however, myosin II's working stroke can be synchronised in the few milliseconds following a step reduction in either force or length superimposed on the isometric contraction. Here we show that with 150 micros force steps it is possible to separate the elastic response from the subsequent early rapid component of filament sliding due to the working stroke in the attached myosin heads. In this way we determine how the size and the speed of the working stroke depend on the clamped force. The relation between mechanical energy and force provides a molecular basis for muscle efficiency and an estimate of the isometric force exerted by a myosin head.
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PMID:The size and the speed of the working stroke of muscle myosin and its dependence on the force. 1243 42

The myosin motor protein generates force in muscle by hydrolyzing Adenosine 5'-triphosphate (ATP) while interacting transiently with actin. Structural evidence suggests the myosin globular head (subfragment 1 or S1) is articulated with semi-rigid catalytic and lever-arm domains joined by a flexible converter domain. According to the prevailing hypothesis for energy transduction, ATP binding and hydrolysis in the catalytic domain drives the relative movement of the lever arm. Actin binding and reversal of the lever-arm movement (power stroke) applies force to actin. These domains interface at the reactive lysine, Lys84, where trinitrophenylation (TNP-Lys84-S1) was observed in this work to block actin activation of myosin ATPase and in vitro sliding of actin over myosin. TNP-Lys84-S1's properties and interactions with actin were examined to determine how trinitrophenylation causes these effects. Weak and strong actin binding, the rate of mantADP release from actomyosin, and actomyosin dissociation by ATP were equivalent in TNP-Lys84-S1 and native S1. Molecular dynamics calculations indicate that lever-arm movement inhibition during ATP hydrolysis and the power stroke is caused by steric clashes between TNP and the converter or lever-arm domains. Together these findings suggest that TNP uncouples actin activation of myosin ATPase and the power stroke from other steps in the contraction cycle by inhibiting the converter and lever-arm domain movements.
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PMID:Chemical decoupling of ATPase activation and force production from the contractile cycle in myosin by steric hindrance of lever-arm movement. 1254 86

Each of the heads of the motor protein myosin II is capable of supporting motion. A previous report showed that double-headed myosin generates twice the displacement of single-headed myosin (Tyska, M.J., D.E. Dupuis, W.H. Guilford, J.B. Patlak, G.S. Waller, K.M. Trybus, D.M. Warshaw, and S. Lowey. 1999. Proc. Natl. Acad. Sci. USA. 96:4402-4407). To determine the role of the second head, we expressed a smooth muscle heterodimeric heavy meromyosin (HMM) with one wild-type head, and the other locked in a weak actin-binding state by introducing a point mutation in switch II (E470A). Homodimeric E470A HMM did not support in vitro motility, and only slowly hydrolyzed MgATP. Optical trap measurements revealed that the heterodimer generated unitary displacements of 10.4 nm, strikingly similar to wild-type HMM (10.2 nm) and approximately twice that of single-headed subfragment-1 (4.4 nm). These data show that a double-headed molecule can achieve a working stroke of approximately 10 nm with only one active head and an inactive weak-binding partner. We propose that the second head optimizes the orientation and/or stabilizes the structure of the motion-generating head, thereby resulting in maximum displacement.
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PMID:A mutant heterodimeric myosin with one inactive head generates maximal displacement. 1290 Mar 96

The two headed motor protein kinesin appears to "walk" along the biopolymer microtubule in 8 nm steps. There is ample justification for a model where the motion of the detached head to the next docking site on the biopolymer is described as ratcheted diffusion. The forward reorientation of an attached head can be conceived of as a power stroke. A model that is based on these premises can accurately predict parameters of motor protein motion.
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PMID:Processive motor protein as an overdamped brownian stepper. 1461 60

Muscle contraction is driven by the motor protein myosin II, which binds transiently to an actin filament, generates a unitary filament displacement or 'working stroke', then detaches and repeats the cycle. The stroke size has been measured previously using isolated myosin II molecules at low load, with rather variable results, but not at the higher loads that the motor works against during muscle contraction. Here we used a novel X-ray-interference technique to measure the working stroke of myosin II at constant load in an intact muscle cell, preserving the native structure and function of the motor. We show that the stroke is smaller and slower at higher load. The stroke size at low load is likely to be set by a structural limit; at higher loads, the motor detaches from actin before reaching this limit. The load dependence of the myosin II stroke is the primary molecular determinant of the mechanical performance and efficiency of skeletal muscle.
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PMID:The myosin motor in muscle generates a smaller and slower working stroke at higher load. 1505 7

Myosin-V is a processive two-headed actin-based motor protein involved in many intracellular transport processes. A key question for understanding myosin-V function and the communication between its two heads is its behavior under load. Since in vivo myosin-V colocalizes with other much stronger motors like kinesins, its behavior under superstall forces is especially relevant. We used optical tweezers with a long-range force feedback to study myosin-V motion under controlled external forward and backward loads over its full run length. We find the mean step size remains constant at approximately 36 nm over a wide range of forces from 5 pN forward to 1.5 pN backward load. We also find two force-dependent transitions in the chemomechanical cycle. The slower ADP-release is rate limiting at low loads and depends only weakly on force. The faster rate depends more strongly on force. The stronger force dependence suggests this rate represents the diffusive search of the leading head for its binding site. In contrast to kinesin motors, myosin-V's run length is essentially independent of force between 5 pN of forward to 1.5 pN of backward load. At superstall forces of 5 pN, we observe continuous backward stepping of myosin-V, indicating that a force-driven reversal of the power stroke is possible.
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PMID:Force-dependent stepping kinetics of myosin-V. 1576 64

The motor protein dynein is predicted to move the tail domain, a slender rod-like structure, relative to the catalytic head domain to carry out its power stroke. Here, we investigated ATP hydrolysis cycle-dependent conformational dynamics of dynein using fluorescence resonance energy transfer analysis of the dynein motor domain labeled with two fluorescent proteins. We show that dynein adopts at least two conformational states (states I and II), and the tail undergoes ATP-induced motions relative to the head domain during transitions between the two states. Our measurements also suggest that in the course of the ATP hydrolysis cycle of dynein, the tail motion from state I to state II takes place in the ATP-bound state, whereas the motion from state II to state I occurs in the ADP-bound state. The latter tail motion may correspond to the predicted power stroke of dynein.
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PMID:ATP hydrolysis cycle-dependent tail motions in cytoplasmic dynein. 1588 Jan 23


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