Interferometric Scattering Microscopy for the Study of Molecular Motors.

Our understanding of molecular motor function has been greatly improved by the development of imaging modalities, which enable real-time observation of their motion at the single-molecule level. Here, we describe the use of a new method, interferometric scattering microscopy, for the investigation of motor protein dynamics by attaching and tracking the motion of metallic nanoparticle labels as small as 20nm diameter. Using myosin-5, kinesin-1, and dynein as examples, we describe the basic assays, labeling strategies, and principles of data analysis. Our approach is relevant not only for motor protein dynamics but also provides a general tool for single-particle tracking with high spatiotemporal precision, which overcomes the limitations of single-molecule fluorescence methods.

Distinct cytoplasmic dynein complexes are transported by different mechanisms in axons.

In neurons, cytoplasmic dynein is synthesized in the cell body, but its function is to move cargo from the axon back to the cell body. Dynein must therefore be delivered to the axon and its motor activity must be regulated during axonal transport. Cytoplasmic dynein is a large protein complex composed of a number of different subunits. The dynein heavy chains contain the motor domains and the intermediate chains are involved in binding the complex to cargo. Five different intermediate chain polypeptides, which are the result of the alternative splicing of the two intermediate chain genes, have been identified. We have characterized two distinct pools of dynein that are transported from the cell body along the axon by different mechanisms. One pool, which contains the ubiquitous intermediate chain, is associated with the membranous organelles transported by kinesin in the fast transport component. The other pool, which contains the other developmentally regulated intermediate chains, is transported in slow component b. The mechanism of dynein regulation will therefore depend on which pool of dynein is recruited to function as the retrograde motor. In addition, the properties of the large pool of dynein associated with actin in slow component b are consistent with the hypothesis that this dynein may be the motor for microtubule transport in the axon.

Kinesin's tail domain is an inhibitory regulator of the motor domain.

When not bound to cargo, the motor protein kinesin is in an inhibited state that has low microtubule-stimulated ATPase activity. Inhibition serves to minimize the dissipation of ATP and to prevent mislocalization of kinesin in the cell. Here we show that this inhibition is relieved when kinesin binds to an artificial cargo. Inhibition is mediated by kinesin's tail domain: deletion of the tail activates the ATPase without need of cargo binding, and inhibition is re-established by addition of exogenous tall peptide. Both ATPase and motility assays indicate that the tail does not prevent kinesin from binding to microtubules, but rather reduces the motor's stepping rate.

Kinesin's processivity results from mechanical and chemical coordination between the ATP hydrolysis cycles of the two motor domains.

Kinesin is a processive motor protein: A single molecule can walk continuously along a microtubule for several micrometers, taking hundreds of 8-nm steps without dissociating. To elucidate the biochemical and structural basis for processivity, we have engineered a heterodimeric one-headed kinesin and compared its biochemical properties to those of the wild-type two-headed molecule. Our construct retains the functionally important neck and tail domains and supports motility in high-density microtubule gliding assays, though it fails to move at the single-molecule level. We find that the ATPase rate of one-headed kinesin is 3-6 s(-1) and that detachment from the microtubule occurs at a similar rate (3 s(-1)). This establishes that one-headed kinesin usually detaches once per ATP hydrolysis cycle. Furthermore, we identify the rate-limiting step in the one-headed hydrolysis cycle as detachment from the microtubule in the ADP.P(i) state. Because the ATPase and detachment rates are roughly an order of magnitude lower than the corresponding rates for two-headed kinesin, the detachment of one head in the homodimer (in the ADP.P(i) state) must be accelerated by the other head. We hypothesize that this results from internal strain generated when the second head binds. This idea accords with a hand-over-hand model for processivity in which the release of the trailing head is contingent on the binding of the forward head. These new results, together with previously published ones, allow us to propose a pathway that defines the chemical and mechanical cycle for two-headed kinesin.

Processivity of the motor protein kinesin requires two heads.

A single kinesin molecule can move for hundreds of steps along a microtubule without dissociating. One hypothesis to account for this processive movement is that the binding of kinesin's two heads is coordinated so that at least one head is always bound to the microtubule. To test this hypothesis, the motility of a full-length single-headed kinesin heterodimer was examined in the in vitro microtubule gliding assay. As the surface density of single-headed kinesin was lowered, there was a steep fall both in the rate at which microtubules landed and moved over the surface, and in the distance that microtubules moved, indicating that individual single-headed kinesin motors are not processive and that some four to six single-headed kinesin molecules are necessary and sufficient to move a microtubule continuously. At high ATP concentration, individual single-headed kinesin molecules detached from microtubules very slowly (at a rate less than one per second), 100-fold slower than the detachment during two-headed motility. This slow detachment directly supports a coordinated, hand-over-hand model in which the rapid detachment of one head in the dimer is contingent on the binding of the second head.

Models of calcium activation account for differences between skeletal and cardiac force redevelopment kinetics.

To explain observed differences in the activation dependence of force redevelopment kinetics between cardiac and skeletal muscle, two numerical models of contractile regulation by Ca2+ were investigated. Ca2+ binding and force production were each modelled as two-state processes with forward and reverse rate constants taken from the literature. The first model incorporates four possible thin-filament states. In the second model Ca2+ is assumed not to dissociate from a thin-filament unit in the force-generating state, resulting in three states. The four-state model can account for the activation dependence of the rate constant of tension redevelopment (ktr) seen in skeletal muscle, without requiring that Ca2+ directly modulates the kinetics of any step in the cross-bridge cycle. Using identical kinetic parameters, the three-state model shows no activation dependence of ktr, consistent with our results in cardiac muscle. Following a step increase in [Ca2+], the rate of rise in tension (as described by the rate constant kCa) varies with the final [Ca2+] for both models, consistent with experimental results from skeletal and cardiac muscle. These numerical models demonstrate that experimental measurements thought to reveal changes in kinetic parameters may simply reflect coupling between the two kinetic processes of Ca2+ binding and force generation. Furthermore, the models present possible differences in the Ca2+ activation scheme between cardiac and skeletal muscle which can account for the contrasting activation dependencies of force redevelopment kinetics.

Influence of Ca2+ on force redevelopment kinetics in skinned rat myocardium.

The influence of Ca2+ on isometric force kinetics was studied in skinned rat ventricular trabeculae by measuring the kinetics of force redevelopment after a transient decrease in force. Two protocols were employed to rapidly detach cycling myosin cross-bridges: a large-amplitude muscle length ramp followed by a restretch back to the original length or a 4% segment length step. During the recovery of force, the length of the central region of the muscle was controlled by using a segment marker technique and software feedback control. Tension redevelopment was fit by a rising exponential governed by the rate constant ktr for the ramp/restretch protocol and kstep for the step protocol. ktr and kstep averaged 7.06 s-1 and 15.7 s-1, respectively, at 15 degrees C; neither ktr nor kstep increased with the level of Ca2+ activation. Similar results were found at submaximum Ca2+ levels when sarcomere length control by laser diffraction was used. The lack of activation dependence of ktr contrasts with results from fast skeletal fibers, in which ktr varies 10-fold from low to high activation levels, and suggests that Ca2+ does not modulate the kinetics of cross-bridge attachment or detachment in mammalian cardiac muscle.

Ca2+ and segment length dependence of isometric force kinetics in intact ferret cardiac muscle.

The influence of Ca2+ and sarcomere length on myocardial crossbridge kinetics was studied in ferret papillary muscle by measuring the rate of force redevelopment following a rapid length step that dropped the force to zero. Tetanic stimulation with 5 mumol/L ryanodine was used to obtain a steady-state contraction, and segment length was measured and controlled using a sense-coil technique that measures changes in the cross-sectional area of the central region of the muscle. The rate constant for the recovery of force (ktr) following a rapid length release was obtained by fitting the data with a single exponential function. Contrary to results from skinned skeletal fibers in which ktr increases almost 10-fold from low to maximal activation levels, ktr was found not to increase at higher activation levels in this study. Similarly, although force increased with segment length under all conditions, ktr never increased with length. Data presented here are consistent with a model of myocardial Ca2+ activation in which Ca2+ modulates the number of crossbridges interacting with the thin filament and are inconsistent with a model in which Ca2+ modulates the kinetics of transitions to force producing states within the actomyosin cycle. Differences in the activation dependence of the force redevelopment rate between cardiac and skeletal muscle suggest that there are fundamental differences in the mechanism of Ca2+ activation between these two muscle types.