The power stroke causes changes in the orientation and mobility of the termini of essential light chain 1 of myosin.

Binding of ATP to the catalytic domain of myosin induces a local conformational change which is believed to cause a major rotation of an 8.5 nm alpha-helix that is stabilized by the regulatory and essential light chains. Here we attempt to follow this rotation by measuring the mobility and orientation of a fluorescent probe attached near the C- or N-terminus of essential light chain 1 (LC1). Cysteine 178 of wild-type LC1, or Cys engineered near the N-terminus of mutant LC1, was labeled with tetramethylrhodamine and exchanged into skeletal subfragment-1 (S1) or into striated muscle fibers. In the absence of ATP, the fluorescence anisotropy (r) and the rotational correlation time (rho) of S1 reconstituted with LC1 labeled near the C-terminus were 0.195 and 66.6 ns, respectively. In the presence of ATP, r and rho increased to 0.233 and 233 ns, indicating considerable immobilization of the probe. A related parameter indicating the degree of order of cross-bridges in muscle fibers, Deltar, was small in rigor fibers (-0.009) and increased in relaxed fibers (0.030). For S1 reconstituted with LC1 labeled near the N-terminus, the steady-state anisotropy was 0.168 in rigor, and increased to 0.223 in relaxed state. In fibers, the difference in rigor was large (Deltar = 0.080), because of binding to the thin filaments, and decreased to 0.037 in relaxed fibers. These results suggest that before the power stroke, in the presence of ATP or its products of hydrolysis, the termini of LC1 are immobilized and ordered, and after the stroke, they become more mobile and partially disordered. The results are consistent with crystallographic structures that show that the level of putative stabilizing interactions of LC1 with the heavy chain of S1 in the transition state is reduced as the regulatory domain rotates to its post-power stroke position.

Evidence for cleft closure in actomyosin upon ADP release.

Structural insights into the interaction of smooth muscle myosin with actin have been provided by computer-based fitting of crystal structures into three-dimensional reconstructions obtained by electron cryomicroscopy, and by mapping of structural and dynamic changes in the actomyosin complex. The actomyosin structures determined in the presence and absence of MgADP differ significantly from each other, and from all crystallographic structures of unbound myosin. Coupled to a complex movement ( approximately 34 A) of the light chain binding domain upon MgADP release, we observed a approximately 9 degrees rotation of the myosin motor domain relative to the actin filament, and a closure of the cleft that divides the actin binding region of the myosin head. Cleft closure is achieved by a movement of the upper 50 kDa region, while parts of the lower 50 kDa region are stabilized through strong interactions with actin. This model supports a mechanism in which binding of MgATP at the active site opens the cleft and disrupts the interface, thereby releasing myosin from actin.

Functional consequences of mutations in the smooth muscle myosin heavy chain at sites implicated in familial hypertrophic cardiomyopathy.

Familial hypertrophic cardiomyopathy (FHC) is frequently associated with mutations in the beta-cardiac myosin heavy chain. Many of the implicated residues are located in highly conserved regions of the myosin II class, suggesting that these mutations may impair the basic functions of the molecular motor. To test this hypothesis, we have prepared recombinant smooth muscle heavy meromyosin with mutations at sites homologous to those associated with FHC by using a baculovirus/insect cell expression system. Several of the heavy meromyosin mutants, in particular R403Q, showed an increase in actin filament velocity in a motility assay and an enhanced actin-activated ATPase activity. Single molecule mechanics, using a laser trap, gave unitary displacements and forces for the mutants that were similar to wild type, but the attachment times to actin following a unitary displacement were markedly reduced. These results suggest that the increases in activity are due to a change in kinetics and not due to a change in the intrinsic mechanical properties of the motor. In contrast to earlier reports, we find that mutations in residues implicated in FHC affect motor function by enhancing myosin activity rather than by a loss of function.

Two heads of myosin are better than one for generating force and motion.

Several classes of the myosin superfamily are distinguished by their "double-headed" structure, where each head is a molecular motor capable of hydrolyzing ATP and interacting with actin to generate force and motion. The functional significance of this dimeric structure, however, has eluded investigators since its discovery in the late 1960s. Using an optical-trap transducer, we have measured the unitary displacement and force produced by double-headed and single-headed smooth- and skeletal-muscle myosins. Single-headed myosin produces approximately half the displacement and force (approximately 6 nm; 0.7 pN) of double-headed myosin (approximately 10 nm; 1.4 pN) during a unitary interaction with actin. These data suggest that muscle myosins require both heads to generate maximal force and motion.

Interaction of the N-terminus of chicken skeletal essential light chain 1 with F-actin.

Skeletal myosin has two isoforms of the essential light chain (ELC), called LC1 and LC3, which differ only in their N-terminal amino acid sequence. The LC1 has 41 additional residues containing seven pairs of Ala-Pro, which form an elongated structure, and two pairs of lysines located near the N-terminus. When myosin subfragment-1 (S1) binds to actin, these lysines may interact with the C-terminus of actin and be responsible for the isoform specific properties of myosin. Here we employ cross-linking to identify the LC1 residues that are in contact with actin. S1 was reconstituted with various LC1 mutants and reacted with the zero-length cross-linker 1-ethyl-3-[3-dimethyl-aminopropyl]-carbodiimide (EDC). Cross-linking occurred only when actin was in molar excess over S1. Wild-type LC1 could be cross-linked through the terminal alpha-NH2 group, as well as via the two pairs of lysines. In a mutant ELC, where the lysines were deleted but two arginines were introduced near the N-terminus, the light chain could still be cross-linked via the terminal alpha-NH2 group. When the charge was reduced in the N-terminal region while retaining the Ala-Pro rich region, the mutant could not be cross-linked. These results suggest that as long as the N-terminus contains charged residues and an Ala-Pro rich extension, the binding between LC1 and actin can occur.

Myosin conformational states determined by single fluorophore polarization.

Muscle contraction is powered by the interaction of the molecular motor myosin with actin. With new techniques for single molecule manipulation and fluorescence detection, it is now possible to correlate, within the same molecule and in real time, conformational states and mechanical function of myosin. A spot-confocal microscope, capable of detecting single fluorophore polarization, was developed to measure orientational states in the smooth muscle myosin light chain domain during the process of motion generation. Fluorescently labeled turkey gizzard smooth muscle myosin was prepared by removal of endogenous regulatory light chain and re-addition of the light chain labeled at cysteine-108 with the 6-isomer of iodoacetamidotetramethylrhodamine (6-IATR). Single myosin molecule fluorescence polarization data, obtained in a motility assay, provide direct evidence that the myosin light chain domain adopts at least two orientational states during the cyclic interaction of myosin with actin, a randomly disordered state, most likely associated with myosin whereas weakly bound to actin, and an ordered state in which the light chain domain adopts a finite angular orientation whereas strongly bound after the powerstroke.

Subunit interactions within an expressed regulatory domain of chicken skeletal myosin. Location of the NH2 terminus of the regulatory light chain by fluorescence resonance energy transfer.

The regulatory domain (RD), or neck region of the myosin head, consists of two classes of light chains that stabilize an alpha-helical segment of the heavy chain. RD from chicken skeletal muscle myosin was prepared in Escherichia coli by coexpression of a 9-kDa heavy chain fragment with the essential light chain. Recombinant regulatory light chain (RLC), wild type or mutant, was added separately to reconstitute the complex. The affinity of RD for divalent cations was determined by measuring the change in fluorescence of a pair of heavy chain tryptophans upon addition of calcium or magnesium. The complex bound divalent cations with high affinity, similar to the association constants determined for native myosin. The intrinsic fluorescence of the tryptophans could be used as a donor to measure the fluorescence resonance energy transfer distance to a single labeled cysteine engineered at position 2 on RLC. Dansylated Cys2 could also serve as a donor by preparing RLC with a second cysteine at position 79 which was labeled with an acceptor probe. These fluorescence resonance energy transfer distances (24-30 A), together with a previous measurement between Cys2 and Cys155 (Wolff-Long, V. L., Tao, T., and Lowey, S. (1995) J. Biol. Chem. 270, 31111-31118) suggest a location for the NH2 terminus of RLC that appears to preclude a direct interaction between the phosphorylatable serine and specific residues in the COOH-terminal domain.

Orientation changes of fluorescent probes at five sites on the myosin regulatory light chain during contraction of single skeletal muscle fibres.

Changes in the orientation of the myosin regulatory light chain (RLC) in single muscle fibres were measured using polarised fluorescence from acetamidotetramethylrhodamine (ATR). Mutants of chicken skeletal RLC containing single cysteine residues at positions 2, 73, 94, 126 and 155 were labelled with either the 5 or 6-isomer of iodo-ATR, giving ten different probes. The labelled RLCs were exchanged into demembranated fibres from rabbit psoas muscle without significant effect on active force generation. Fluorescence polarisation measurements showed that nine out of the ten probe dipoles were more perpendicular to the fibre axis in the absence of ATP (in rigor) than in either relaxation or active contraction. The orientational distribution of the RLC region of the myosin head in active contraction is closer to the relaxed than to the rigor orientation, and is not equivalent to a linear combination of the relaxed and rigor orientations. Rapid length steps were applied to the fibres to synchronise the motions of myosin heads attached to actin. In active contraction the fluorescence polarisation changed both during the step, indicating elastic distortion of the RLC region of the myosin head, and during the subsequent rapid force recovery that is thought to signal the working stroke. The peak change in fluorescence polarisation produced by an active release of 5 nm per half sarcomere indicates an axial tilt of less than 5 degrees for all ten probes, if all the myosin heads in the fibre respond to the length step. This tilting was towards the rigor orientation for all ten probes, and could be explained by 14% of the heads moving to the rigor orientation. An active stretch tilted the heads away from the rigor conformation by a similar extent.

Proximity relationships between engineered cysteine residues in chicken skeletal myosin regulatory light chain. A resonance energy transfer study.

Resonance energy transfer was used to measure the distances between pairs of cysteines, Cys2 and Cys155 and Cys73 and Cys155, in recombinant chicken skeletal myosin regulatory light chains in the free and bound states. The fluorescent and nonfluorescent probes N-iodoacetyl-N'-(5-sulfo-1-naphthyl) ethylenediamine and N-(4-dimethylamino-3,5-dinitrophenyl)maleimide were used as the donor and the acceptor, respectively. The distance between Cys2 and Cys155 was measured to be 35 and 30 A in the absence and presence of myosin heavy chain, respectively, suggesting a slightly more compact structure for the light chain in the bound state. The distance between Cys73 and Cys155 measured in a similar manner was 31 and 30 A in the free and bound states, respectively; this latter value is in good agreement with that derived from crystallographic structures. For heavy chain-bound light chains, no measurable distance changes were detected with the binding of ATP or actin. These results show that no gross structural changes occur within the regulatory light chain during the contraction cycle, but that resonance energy transfer between other sites could be used to monitor potential changes in the myosin head upon the binding of nucleotides and actin.

A minimal motor domain from chicken skeletal muscle myosin.

The myosin head (S1) consists of a wide, globular region that contains the actin- and nucleotide-binding sites and an alpha-helical, extended region that is stabilized by the presence of two classes of light chains. The essential light chain abuts the globular domain, whereas the regulatory light chain lies near the head-rod junction of myosin. Removal of the essential light chain by a mild denaturant exposes the underlying heavy chain to proteolysis by chymotrypsin. The cleaved fragment, or "motor domain" (MD), migrates as a single band on SDS-polyacrylamide gel electrophoresis, with a slightly greater mobility than S1 prepared by papain or chymotrypsin. Three-dimensional image analysis of actin filaments decorated with MD reveals a structure similar to S1, but shorter by an amount consistent with the absence of a light chain-binding domain. The actin-activated MgATPase activity of MD is similar to that of S1 in Vmax and Km. But the ability of MD to move actin filaments in a motility assay is considerably reduced relative to S1. We conclude that the globular, active site region of the myosin head is a stable, independently folded domain with intrinsic motor activity, but the coupling efficiency between ATP hydrolysis and movement declines markedly as the light chain binding region is truncated.

Role of skeletal and smooth muscle myosin light chains.

A persistent problem with the rotating cross-bridge model for muscle contraction has been the inability to detect any large conformational changes within the myosin molecule to account for a working stroke of 5-10 nm. The recent crystal structure of myosin subfragment-1 suggests a solution to this problem by showing the presence of two distinct domains: a catalytic or motor domain, from which extends a long, 8.5-nm alpha-helix that is stabilized by the regulatory and essential light chains. Rayment et al. (1993) proposed that closure of a cleft in the motor domain could rotate the light chain-binding domain by a sufficient distance to account for the power stroke. With the development of new in vitro motility assays, and the ability to prepare unusual myosins by biochemical and molecular biological methods, we can now examine this hypothesis and explore the role of the light chains in generating force and movement. Here we will review some of these recent data and outline a possible mechanism for how light chains regulate contractile properties.

The essential light chain is required for full force production by skeletal muscle myosin.

Myosin, a molecular motor that is responsible for muscle contraction, is composed of two heavy chains each with two light chains. The crystal structure of subfragment 1 indicates that both the regulatory light chains (RLCs) and the essential light chains (ELCs) stabilize an extended alpha-helical segment of the heavy chain. It has recently been shown in a motility assay that removal of either light chain markedly reduces actin filament sliding velocity without a significant loss in actin-activated ATPase activity. Here we demonstrate by single actin filament force measurements that RLC removal has little effect on isometric force, whereas ELC removal reduces isometric force by over 50%. These data are interpreted with a simple mechanical model where subfragment 1 behaves as a torque motor whose leyer arm length is sensitive to light-chain removal. Although the effect of removing RLCs fits within the confines of this model, altered crossbridge kinetics, as reflected in a reduced unloaded duty cycle, probably contributes to the reduced velocity and force production of ELC-deficient myosins.

Cysteine mutants of light chain-2 form disulfide bonds in skeletal muscle myosin.

Multiple disulfide bonds form in recombinant myosin light chain-2 mutants that contain an engineered cysteine at positions 2, 73, or 94, in addition to the endogenous cysteines at residues 126 and 155 (Saraswat, L.D., and Lowey, S. (1991) J. Biol. Chem. 266, 1977). By replacing one of the native cysteines with an alanine, mutants with a single pair of thiols were created: Cys2/Cys155, Cys2/Cys126, Cys73/Cys155 and Cys94/Cys155. Oxidation of these mutants resulted in a fast migrating band on nonreducing SDS gels, which was attributed to an intramolecular disulfide bond. To determine if disulfide formation could also occur when the light chains (LC) are bound to the myosin heavy chains, LCs were added to myosin which had been depleted of its native LC2 by an immunoadsorbent. When the reconstituted myosin was reacted with 5,5'-dithiobis(2-nitrobenzoic acid) in the absence of divalent cations, intramolecular disulfide bonds formed in the mutant and wild type LCs, but the LCs did not remain bound to the myosin heavy chains. Addition of magnesium ions prevented LC dissociation, but intramolecular disulfide bonds no longer formed. Instead, mutants containing cysteines in the NH2-terminal domain formed intermolecular disulfide bonds between the two heads of myosin. The ability to cross-link the heads demonstrates the existence of close head/head interactions in the myosin molecule, a feature that may be essential for regulation.

Function of skeletal muscle myosin heavy and light chain isoforms by an in vitro motility assay.

The functional significance of the large number of myosin isoforms in skeletal muscles is poorly understood. Myosin molecules that have the same heavy chain, but differ in their essential or alkali light chains, have the same actin-activated ATPase activity. Similarly, the many heavy chain isoforms that appear during the course of muscle development do not show any significant differences in enzymatic activity. By means of an in vitro motility assay, we have measured the analogue of unloaded shortening velocity for myosin isoforms in a reconstituted actomyosin system. We find that both light and heavy chain isoforms translocate actin filaments at distinct velocities. These results support the hypothesis that myosin isoforms are the primary determinant for the range of shortening velocities adopted by a muscle in response to changing functional demands.

Skeletal muscle myosin light chains are essential for physiological speeds of shortening.

In muscle each myosin head contains a regulatory light chain (LC2) that is wrapped around the head/rod junction, and an alkali light chain that is distal to LC2 (ref. 1). The role of these light chains in vertebrate skeletal muscle myosin has remained obscure. Here we prepare heavy chains that are free of both light chains in order to determine by a motility assay whether the light chains are necessary for movement. We find that removal of light chains from myosin reduces the velocity of actin filaments from 8.8 microns s-1 to 0.8 microns s-1 without significantly decreasing the ATPase activity. Reconstitution of myosin with LC2 or alkali light chain increases filament velocity to intermediate rates, and readdition of both classes of light chains fully restores the original sliding velocity. We conclude that even though the light chains are not essential for enzymatic activity, light-chain/heavy-chain interactions play an important part in the conversion of chemical energy into movement.

Distribution of developmental myosin isoforms in isolated A-segments.

Immunogold labelling was used to determine the distribution of myosin isoforms within the A-bands of developing chicken pectoralis muscles. Previous localization studies led to the suggestion that neonatal myosin is preferentially located in the centre of heterogeneous thick filaments that contain either embryonic or adult myosin in addition to neonatal myosin. To further explore the possibility that neonatal myosin may serve to nucleate thick filament assembly, a method was developed to isolate A-segments (arrays of myosin filaments) from myofibrils in the presence of MgATP. A-bands usually dissociate into thick and thin filaments in a relaxing buffer, but the inclusion of an antibody against M-line protein prevented separation of the thick filament array. Well-ordered A-segments, approximately 1.5 microns in length, were prepared from muscles 12, 29, 40 days, and approximately 1 year after hatching. After reaction with monoclonal antibodies specific for neonatal and adult myosins, the A-segments were labelled with gold-conjugated secondary antibodies prior to negative staining. An antibody which cross-reacts with embryonic myosin was used to localize that epitope in A-bands of myofibrils from day 1 and day 3 posthatch muscles. At ages where expression of neonatal myosin was high, extensive gold labelling of A-segments was observed in the electron microscope. However, no preferential distribution of antibodies was observed at any age, independent of whether embryonic or adult myosin was coexpressed with the neonatal myosin, suggesting that neonatal myosin is not segregated to any particular region in the A-bands of developing muscles.

Mapping single cysteine mutants of light chain 2 in chicken skeletal myosin.

The NH2- and COOH-terminal regions of the regulatory light chain (LC2) have been mapped to the head/rod junction by immunoelectron microscopy, using monoclonal and anti-fluorescyl antibodies as probes. In order to map the entire length of the light chain, we have engineered and purified mutants that contain a single cysteine residue at positions 2, 73, 94, 126, or 155. The single cysteine residues were labeled with either 5-iodoacetamido fluorescein or N-ethylmaleimide-biotin. We observed that the reactivity of Cys126 is far greater than that of Cys155, confirming that cysteine 126 is the fast-reacting thiol in wild-type light chain. The labeled light chains were exchanged into myosin stripped of its native LC2 by immunoaffinity chromatography, and the reconstituted myosin was reacted with anti-fluorescein antibody or avidin prior to rotary shadowing for electron microscopy. The position of the antibody or avidin was found to be near the head/rod junction for all mutants. These mapping studies, together with our finding that cysteines widely separated in the primary sequence can form multiple disulfide bonds (Saraswat, L.D., and Lowey, S. (1991) J. Biol. Chem. 226, 19777-19785), support a model for LC2 as a flexible, globular molecule localized mainly in the vicinity of the head/rod junction of myosin.

Engineered cysteine mutants of myosin light chain 2. Fluorescent analogues for structural studies.

Site-directed mutagenesis has been used to insert cysteine residues at specific locations in the myosin light chain 2 (LC2) sequence. The aim was to modify these cysteines with one or more spectroscopic probes and to reconstitute myosin with labeled light chains for structural studies. Native LC2 has two endogenous cysteine residues at positions 126 and 155; a third sulfhydryl was added by replacing either Pro2, Ser73, or Pro94 with cysteine. By oxidizing the endogenous cysteines to an intramolecular disulfide bond (Katoh, T., and Lowey, S., (1989) J. Cell Biol. 109, 1549), it was expected that the new cysteine could be selectively labeled with a fluorescent probe. This proved more difficult to accomplish than anticipated due to the formation of secondary disulfide bonds between the newly engineered cysteines and the native ones. Nevertheless, the unpaired cysteines were labeled with 5-(iodoacetamido)fluorescein, and singly labeled species were purified by ion-exchange chromatography. Chymotryptic digestion of the light chains, followed by high performance liquid chromatography separation of the peptides, led to the identification of the fluorescein-labeled cysteines. After light chain exchange into myosin, the position of the thiols was mapped by antifluorescyl antibodies in the electron microscope. Rotary-shadowed images showed the antibody bound at the head/rod junction of myosin for all the mutants. These mapping studies, together with the finding that widely separated cysteines can form multiple disulfide bonds, support a model for LC2 as a flexible, globular molecule that resembles other Ca/Mg-binding proteins in tertiary structure.

Neonatal and adult myosin heavy chains form homodimers during avian skeletal muscle development.

Myosin isoforms contribute to the heterogeneity and adaptability of skeletal muscle fibers. Besides the well-characterized slow and fast muscle myosins, there are those isoforms that appear transiently during the course of muscle development. At a stage of development when two different myosins are coexpressed, the possibility arises for the existence of heterodimers, molecules containing two different heavy chains, or homodimers, molecules with two identical heavy chains. The question of whether neonatal and adult myosin isoforms can associate to form a stable heterodimer was addressed by using stage-specific monoclonal antibodies in conjunction with immunological and electron microscopic techniques. We find that independent of the ratio of adult to neonatal myosin, depending on the age of the animal, the myosin heavy chains form predominantly homodimeric molecules. The small amount of hybrid species present suggests that either the rod portion of the two heavy chain isoforms differs too much in sequence to form a stable alpha-helical coiled coil, or that the biosynthesis of the heavy chains precludes the formation of heterodimeric molecules.

Mapping myosin light chains by immunoelectron microscopy. Use of anti-fluorescyl antibodies as structural probes.

The two classes of light chains in vertebrate fast muscle myosin have been selectively labeled with the thiol specific reagent 5-(iodoacetamido) fluorescein to determine their location in the myosin head. The alkali light chains (A1 and A2) were labeled at a single cysteine residue near the COOH terminus, whereas the regulatory light chain (LC2) was reacted at either cysteine 125 or 154. The two cysteines of LC2 appear to be near each other in the tertiary structure as evidenced by the ease of formation of an intramolecular disulfide bond. Besides having favorable spectral properties, fluorescein is a potent haptenic immunogen for raising high affinity antibodies. When anti-fluorescyl antibodies were added to the fluorescein-labeled light chains, the fluorescence was quenched by greater than 90%, thereby providing a simple method for determining an association constant. The interaction with antibody was the same for light chains exchanged into myosin as for free light chains. Complexes of antibody bound to light chain could be visualized in the electron microscope by rotary shadowing with platinum. By this approach we have shown that the COOH-terminal regions of the two classes of light chains are widely separated in myosin: the cysteine residues of LC2 lie close to the head/rod junction, whereas the single cysteine of A1 or A2 is located approximately 90 A distal to the junction. These sites correspond to the positions of the NH2 termini of the light chains mapped in earlier studies (Winkelmann, D. A., and S. Lowey. 1986. J. Mol. Biol. 188:595-612; Tokunaga, M., M. Suzuki, K. Saeki, and T. Wakabayashi. 1987b. J. Mol. Biol. 194:245-255). We conclude that the two classes of light chains do not lie in a simple colinear arrangement, but instead have a more complex organization in distinct regions of the myosin head.