Dynamic electron microscopy of ATP-induced myosin head movement in living muscle thick filaments

Although muscle contraction is known to result from movement of the myosin heads on the thick filaments while attached to the thin filaments, the myosin head movement coupled with ATP hydrolysis still remains to be investigated. Using a gas environmental (hydration) chamber, in which biological specimens can be kept in wet state, we succeeded in recording images of living muscle thick filaments with gold position markers attached to the myosin heads. The position of individual myosin heads did not change appreciably with time in the absence of ATP, indicating stability of the myosin head mean position. On application of ATP, the position of individual myosin heads was found to move by ≈20 nm along the filament axis, whereas no appreciable movement of the filaments was detected. The ATP-induced myosin head movement was not observed in filaments in which ATPase activity of the myosin heads was eliminated. Application of ADP produced no appreciable myosin head movement. These results show that the ATP-induced myosin head movement takes place in the absence of the thin filaments. Because ATP reacts rapidly with the myosin head (M) to form the complex (MADPP_i) with an average lifetime of >10 s, the observed myosin head movement may be mostly associated with reaction, M + ATP → MADPP_i. This work will open a new research field to study dynamic structural changes of individual biomolecules, which are kept in a living state in an electron microscope.     

Reverse actin sliding triggers strong myosin binding that moves tropomyosin

Actin/myosin interactions in vertebrate striated muscles are believed to be regulated by the “steric blocking” mechanism whereby the binding of calcium to the troponin complex allows tropomyosin (TM) to change position on actin, acting as a molecular switch that blocks or allows myosin heads to interact with actin. Movement of TM during activation is initiated by interaction of Ca²⁺ with troponin, then completed by further displacement by strong binding cross-bridges. We report x-ray evidence that TM in insect flight muscle (IFM) moves in a manner consistent with the steric blocking mechanism. We find that both isometric contraction, at high [Ca²⁺], and stretch activation, at lower [Ca²⁺], develop similarly high x-ray intensities on the IFM fourth actin layer line because of TM movement, coinciding with x-ray signals of strong-binding cross-bridge attachment to helically favored “actin target zones.” Vanadate (Vi), a phosphate analog that inhibits active cross-bridge cycling, abolishes all active force in IFM, allowing high [Ca²⁺] to elicit initial TM movement without cross-bridge attachment or other changes from relaxed structure. However, when stretched in high [Ca²⁺], Vi-“paralyzed” fibers produce force substantially above passive response at pCa ~ 9, concurrent with full conversion from resting to active x-ray pattern, including x-ray signals of cross-bridge strong-binding and TM movement. This argues that myosin heads can be recruited as strong-binding “brakes” by backward-sliding, calcium-activated thin filaments, and are as effective in moving TM as actively force-producing cross-bridges. Such recruitment of myosin as brakes may be the major mechanism resisting extension during lengthening contractions.     

Tension relaxation induced by pulse photolysis of caged ATP in partially crosslinked fibers from rabbit psoas muscle.

Muscle contractile force is thought to be generated by ATP-induced conformational changes in myosin crossbridges. In the present study, we investigated the response to ATP binding of force-bearing, attached cross-bridges. For this investigation, skinned fibers, in which myosin heads were in part covalently crosslinked to thin filaments with a zero-length crosslinker, were prepared. Caged ATP [the P3-1-(2-nitro)phenylethyl ester of ATP] was then pulse-photolyzed in these crosslinked fibers, which retained ATP-induced "rigor" tension, and then the subsequent tension changes were followed at 14-16 degrees C and ionic strengths of 0.1-2 M. A rapid tension decrease was observed after the photolysis in the partially crosslinked fibers. The rate of the decrease was not any different from that in the uncrosslinked fibers compared at ionic strength of 0.2 M. This and other results thus indicate a kinetic similarity in the crosslinked and uncrosslinked crossbridges in response to ATP binding. These findings also suggest that ATP-induced structural changes take place in the attached crossbridges at a rate similar to that of the ATP-induced dissociation of crossbridges from thin filaments.     

Determination of the myosin step size from mechanical and kinetic data.

During muscle contraction, work is generated when a myosin cross-bridge attaches to an actin filament and exerts a force on it through some power-stroke distance, h. At the end of this power stroke, attached myosin heads are carried into regions where they exert a negative force on the actin filament (the drag stroke) and where they are released rapidly from actin by ATP binding. Although the length of the power stroke remains controversial, average distance traversed in the drag-stroke region can be determined when one knows both rate of cross-bridge dissociation and filament-sliding velocity. At maximum contraction velocity, the average force exerted in the drag stroke must balance that exerted in the power stroke. We discuss here a simple model of cross-bridge interaction that allows one to calculate the force exerted in the drag stroke and to relate this to the power-stroke distance h traversed by cross-bridges in the positive-force region. Both the rate at which myosin can be dissociated from actin and the velocity at which an actin filament can be translated have been measured for a series of myosin isozymes and for different substrates, producing a wide range of values for each. Nonetheless, we show here that the rate of myosin dissociation from actin correlates well with the velocity of filament sliding, providing support for the simple model presented and suggesting that the power stroke is approximately 10 nm in length.     

Cardiac myosin binding protein-C modulates actomyosin binding and kinetics in the in vitro motility assay

The modulatory role of whole cardiac myosin binding protein-C (cMyBP-C) on myosin force and motion generation was assessed in an in vitro motility assay. The presence of cMyBP-C at an approximate molar ratio of cMyBP-C to whole myosin of 1:2, resulted in a 25% reduction in thin filament velocity (P < 0.002) with no effect on relative isometric force under maximally activated conditions (pCa 5). Cardiac MyBP-C was capable of inhibiting actin filament velocity in a concentration-dependent manner using either whole myosin, HMM or S1, indicating that the cMyBP-C does not have to bind to myosin LMM or S2 subdomains to exert its effect. The reduction in velocity by cMyBP-C was independent of changes in ionic strength or excess inorganic phosphate. Co-sedimentation experiments demonstrated S1 binding to actin is reduced as a function of cMyBP-C concentration in the presence of ATP. In contrast, S1 avidly bound to actin in the absence of ATP and limited cMyBP-C binding, indicating that cMyBP-C and S1 compete for actin binding in an ATP-dependent fashion. However, based on the relationship between thin filament velocity and filament length, the cMyBP-C induced reduction in velocity was independent of the number of cross-bridges interacting with the thin filament. In conclusion, the effects of cMyBP-C on velocity and force at both maximal and submaximal activation demonstrate that cMyBP-C does not solely act as a tether between the myosin S2 and LMM subdomains but likely affects both the kinetics and recruitment of myosin cross-bridges through its direct interaction with actin and/or myosin head.     

Kinetics of cardiac sarcomeric processes and rate-limiting steps in contraction and relaxation

The sarcomere is the core structure responsible for active mechanical heart function. It is formed primarily by myosin, actin, and titin filaments. Cyclic interactions occur between the cross-bridges of the myosin filaments and the actin filaments. The forces generated by these cyclic interactions provide the molecular basis for cardiac pressure, while the motion produced by these interactions provides the basis for ejection. The cross-bridge cycle is controlled by upstream mechanisms located in the membrane and by downstream mechanisms inside the sarcomere itself. These downstream mechanisms involve the Ca²⁺-controlled conformational change of the regulatory proteins troponin and tropomyosin and strong cooperative interactions between neighboring troponin-tropomyosin units along the actin filament. The kinetics of upstream and downstream processes have been measured in intact and demembranated myocardial preparations. This review outlines a conceptual model of the timing of these processes during the individual mechanical heart phases. Particular focus is given to kinetic data from studies on contraction-relaxation cycles under mechanical loads. Evidence is discussed that the dynamics of cardiac contraction and relaxation are determined mainly by sarcomeric downstream mechanisms, in particular by the kinetics of the cross-bridge cycle. The rate and extent of ventricular pressure development is essentially subjected to the mechanistic principles of cross-bridge action and its upstream and downstream regulation. Sarcomere relengthening during myocardial relaxation plays a key role in the rapid decay of ventricular pressure and in early diastolic filling.     

Millisecond time-resolved changes in x-ray reflections from contracting muscle during rapid mechanical transients, recorded using synchrotron radiation.

Low-angle x-ray diffraction diagrams have been recorded from frog sartorius muscles by using synchrotron radiation as a high-intensity x-ray source. This has enabled changes in some of the principal reflections of interest to be followed with a time resolution of 1 ms, during small but very rapid length changes imposed on a contracting muscle. The 143-A meridional reflection, which is believed to arise from a repeating pattern of myosin cross-bridges along the length of the muscle, shows large changes in intensity in these circumstances. During both rapid releases and rapid stretches, by amounts that produce a translation of actin and myosin filaments past each other by about 100 A and that are completed in about a millisecond (i.e., before significant cross-bridge detachment would be expected), an almost synchronous decrease in 143-A intensity occurs, by 50% or more. This is followed, in the case of quick releases, by a rapid partial recovery of intensity lasting 5--6 ms (which may represent cross-bridge release and reattachment) and then by a more gradual return to the normal isometric value. Quick stretches show only the slower return of intensity. Immediately after the length change, the initial drop in 143-A intensity can be reversed if the release (or stretch) is reversed. These changes provide evidence of a more direct kind than has hitherto been available that the active sliding of actin filaments past myosin filaments during contraction is produced by longitudinal movement of attached cross-bridges.     

Mutation of the myosin converter domain alters cross-bridge elasticity

Elastic distortion of a structural element of the actomyosin complex is fundamental to the ability of myosin to generate motile forces. An elastic element allows strain to develop within the actomyosin complex (cross-bridge) before movement. Relief of this strain then drives filament sliding, or more generally, movement of a cargo. Even with the known crystal structure of the myosin head, however, the structural element of the actomyosin complex in which elastic distortion occurs remained unclear. To assign functional relevance to various structural elements of the myosin head, e.g., to identify the elastic element within the cross-bridge, we studied mechanical properties of muscle fibers from patients with familial hypertrophic cardiomyopathy with point mutations in the head domain of the beta-myosin heavy chain. We found that the Arg-719 --> Trp (Arg719Trp) mutation, which is located in the converter domain of the myosin head fragment, causes an increase in force generation and fiber stiffness under isometric conditions by 48-59%. Under rigor and relaxing conditions, fiber stiffness was 45-47% higher than in control fibers. Yet, kinetics of active cross-bridge cycling were unchanged. These findings, especially the increase in fiber stiffness under rigor conditions, indicate that cross-bridges with the Arg719Trp mutation are more resistant to elastic distortion. The data presented here strongly suggest that the converter domain that forms the junction between the catalytic and the light-chain-binding domain of the myosin head is not only essential for elastic distortion of the cross-bridge, but that the main elastic distortion may even occur within the converter domain itself.     

Protein kinase A mediated modulation of acto-myosin kinetics

The effects of protein kinase A (PKA) mediated phosphorylation on thin filament and cross-bridge function is not fully understood. To delineate the effects of troponin I (TnI) phosphorylation by PKA on contractile protein performance, reconstituted thin filaments were treated with PKA. With the use of the in vitro motility assay, PKA treated thin filament function was assessed relative to non-phosphorylated thin filaments in a calcium-regulated system. At maximal calcium activation, unloaded shortening velocity and force did not differ between the groups. However, at submaximal activation, an increase in calcium sensitivity of the thin filament was observed for velocity but a decrease in calcium sensitivity was observed for force. Activation of the thin filament by myosin strong-binding did not elicit a calcium-independent effect. The rightward shift in calcium sensitivity for force and the leftward shift in calcium sensitivity for velocity indicate that PKA phosphorylation of TnI directly modulates the kinetics of the myosin cross-bridge. In addition, the altered velocity dependence on thin filament length implicates reduced myosin cross-bridge binding with PKA treatment. These data highlight the importance of TnI serine 23 and 24 phosphorylation in the modulation of cardiac function.     

Protein kinase A-mediated phosphorylation of cMyBP-C increases proximity of myosin heads to actin in resting myocardium

Protein kinase A-mediated (PKA) phosphorylation of cardiac myosin binding protein C (cMyBP-C) accelerates the kinetics of cross-bridge cycling and may relieve the tether-like constraint of myosin heads imposed by cMyBP-C. We favor a mechanism in which cMyBP-C modulates cross-bridge cycling kinetics by regulating the proximity and interaction of myosin and actin. To test this idea, we used synchrotron low-angle x-ray diffraction to measure interthick filament lattice spacing and the equatorial intensity ratio, I(11)/I(10), in skinned trabeculae isolated from wild-type and cMyBP-C null (cMyBP-C(-/-)) mice. In wild-type myocardium, PKA treatment appeared to result in radial or azimuthal displacement of cross-bridges away from the thick filaments as indicated by an increase (approximately 50%) in I(11)/I(10) (0.22+/-0.03 versus 0.33+/-0.03). Conversely, PKA treatment did not affect cross-bridge disposition in mice lacking cMyBP-C, because there was no difference in I(11)/I(10) between untreated and PKA-treated cMyBP-C(-/-) myocardium (0.40+/-0.06 versus 0.42+/-0.05). Although lattice spacing did not change after treatment in wild-type (45.68+/-0.84 nm versus 45.64+/-0.64 nm), treatment of cMyBP-C(-/-) myocardium increased lattice spacing (46.80+/-0.92 nm versus 49.61+/-0.59 nm). This result is consistent with the idea that the myofilament lattice expands after PKA phosphorylation of cardiac troponin I, and when present, cMyBP-C, may stabilize the lattice. These data support our hypothesis that tethering of cross-bridges by cMyBP-C is relieved by phosphorylation of PKA sites in cMyBP-C, thereby increasing the proximity of cross-bridges to actin and increasing the probability of interaction with actin on contraction.     

Probes bound to myosin Cys-707 rotate during length transients in contraction

It is widely conjectured that muscle shortens because portions of myosin molecules (the “cross-bridges”) impel the actin filament to which they transiently attach and that the impulses result from rotation of the cross-bridges. Crystallography indicates that a cross-bridge is articulated–consisting of a globular catalytic/actin-binding domain and a long lever arm that may rotate. Conveniently, a rhodamine probe with detectable attitude can be attached between the globular domain and the lever arm, enabling the observer to tell whether the anchoring region rotates. Well-established signature effects observed in shortening are tension changes resulting from the sudden release or quick stretch of active muscle fibers. In this investigation we found that closely correlated with such tension changes are changes in the attitude of the rhodamine probes. This correlation strongly supports the conjecture about how shortening is achieved.     

Structure of the actin-myosin complex in the presence of ATP.

The structure of the complex between actin and myosin subfragment 1 (S1), designated the acto-S1 complex, in the presence of ATP was examined by electron microscopy. This was accomplished by using negative staining to study a complex of S1 covalently crosslinked to actin by the zero-length crosslinker, 1-ethyl-3-[3-(dimethylamino)-propyl]carbodiimide. Two levels of S1 binding were studied, with a molar ratio of crosslinked S1 to total actin of either 20% or 50%. The lower percentage was used to observe individual S1 molecules attached to actin, while the higher percentage was used to look at the overall pattern of S1 decoration of the actin filament. In the absence of ATP, the appearances of both the 20% and 50% crosslinked filaments closely resembled the rigor appearances obtained with noncrosslinked proteins. The arrowheads observed had the conventional structure, and individual S1 molecules were elongated and curved and appeared to make an angle of 45 degrees with the thin filament. Addition of ATP to the crosslinked acto-S1 complex caused a radical change in the structure of the cross-bridges. At both 20 and 170 mM ionic strengths, individual S1 molecules appeared to be attached at variable angles which, in contrast to rigor, did not center on 45 degrees. In addition, the S1 molecules often appeared shorter and fatter than in rigor. The 50% crosslinked acto-S1 preparation no longer showed the arrowhead pattern of S1 decoration but instead appeared to be disordered with little obvious polarity. Control experiments with ADP suggest that these effects were not due simply to a weakening of the binding of S1 to actin in the presence of nucleotide but most likely were ATP-specific. The crosslinked acto-S1 complex, which hydrolyzes ATP at about the same rate as the maximal actin-activated ATPase of S1 (Vmax), is composed of a mixture of states A X M X ATP and A X M X ADP X Pi (in which A = actin and M = myosin), with more than 50% of the crosslinked S-1 occurring in state A X M X ATP. Therefore, it appears that both states A X M X ATP and A X M X ADP X Pi have a very different conformation from the classic arrowhead conformation of the A X M state.     

UNC-45/CRO1/She4p (UCS) protein forms elongated dimer and joins two myosin heads near their actin binding region

UNC-45/CRO1/She4p (UCS) proteins have variously been proposed to affect the folding, stability, and ATPase activity of myosins. They are the only proteins known to interact directly with the motor domain. To gain more insight into UCS function, we determined the atomic structure of the yeast UCS protein, She4p, at 2.9 Å resolution. We found that 16 helical repeats are organized into an L-shaped superhelix with an amphipathic N-terminal helix dangling off the short arm of the L-shaped molecule. In the crystal, She4p forms a 193-Å-long, zigzag-shaped dimer through three distinct and evolutionary conserved interfaces. We have identified She4p’s C-terminal region as a ligand for a 27-residue-long epitope on the myosin motor domain. Remarkably, this region consists of two adjacent, but distinct, binding epitopes localized at the nucleotide-responsive cleft between the nucleotide- and actin-filament-binding sites. One epitope is situated inside the cleft, the other outside the cleft. After ATP hydrolysis and Pi ejection, the cleft narrows at its base from 20 to 12 Å thereby occluding the inside the cleft epitope, while leaving the adjacent, outside the cleft binding epitope accessible to UCS binding. Hence, one cycle of higher and lower binding affinity would accompany one ATP hydrolysis cycle and a single step in the walk on an actin filament rope. We propose that a UCS dimer links two myosins at their motor domains and thereby functions as one of the determinants for step size of myosin on actin filaments.     

Actin filaments mediate Dictyostelium myosin assembly in vitro.

Because myosin thick filaments form in the actin-rich cortex of nonmuscle cells, we have examined the role of Dictyostelium actin filaments in the assembly of Dictyostelium myosin (type II). Fluorescence energy transfer and light-scattering assembly assays indicate that self-association of Dictyostelium myosin into bipolar thick filaments is kinetically regulated by actin filament networks. Regulation is nucleotide dependent but does not require ATP hydrolysis. Myosin assembly is accelerated approximately 5-fold by actin filaments when either 1 mM ATP or 1 mM adenosine 5'-[beta,gamma-imido]triphosphate (AMP-P[NH]P) is present. However, actin filaments together with 1 mM ADP abolish myosin assembly. Accelerated assembly appears to require transient binding of myosin molecules to actin filaments before incorporation into thick filaments. Fluorescence energy-transfer assays demonstrate that myosin associates with actin filaments at a rate that is equivalent to the accelerated myosin assembly rate, evidence that myosin to actin binding is a rate-limiting step in accelerated thick filament formation. Actin filament networks are also implicated in regulation of thick filament formation, since fragmentation of F-actin networks by severin causes immediate cessation of accelerated myosin assembly. Electron microscopic studies support a model of actin filament-mediated myosin assembly. In ADP, myosin monomers rapidly decorate F-actin, preventing extensive formation of thick filaments. In AMP-P[NH]P, myosin assembles along actin filaments, forming structures that resemble primitive stress fibers. Taken together, these data suggest a model in which site-directed assembly of thick filaments in Dictyostelium is mediated by the interaction of myosin monomers with cortical actin filament networks.     

Torsional rigidity of single actin filaments and actin–actin bond breaking force under torsion measured directly by in vitro micromanipulation

Knowledge of the elastic properties of actin filaments is crucial for considering its role in muscle contraction, cellular motile events, and formation of cell shape. The stiffness of actin filaments in the directions of stretching and bending has been determined. In this study, we have directly determined the torsional rigidity and breaking force of single actin filaments by measuring the rotational Brownian motion and tensile strength using optical tweezers and microneedles, respectively. Rotational angular fluctuations of filaments supplied the torsional rigidity as (8.0 ± 1.2) × 10⁻²⁶ Nm². This value is similar to that deduced from the longitudinal rigidity, assuming the actin filament to be a homogeneous rod. The breaking force of the actin–actin bond was measured while twisting a filament through various angles using microneedles. The breaking force decreased greatly under twist, e.g., from 600–320 pN when filaments were turned through 90°, independent of the rotational direction. Our results indicate that an actin filament exhibits comparable flexibility in the rotational and longitudinal directions, but breaks more easily under torsional load.     

Direct measurements of the coordination of lever arm swing and the catalytic cycle in myosin V

Myosins use a conserved structural mechanism to convert the energy from ATP hydrolysis into a large swing of the force-generating lever arm. The precise timing of the lever arm movement with respect to the steps in the actomyosin ATPase cycle has not been determined. We have developed a FRET system in myosin V that uses three donor–acceptor pairs to examine the kinetics of lever arm swing during the recovery and power stroke phases of the ATPase cycle. During the recovery stroke the lever arm swing is tightly coupled to priming the active site for ATP hydrolysis. The lever arm swing during the power stroke occurs in two steps, a fast step that occurs before phosphate release and a slow step that occurs before ADP release. Time-resolved FRET demonstrates a 20-Å change in distance between the pre- and postpower stroke states and shows that the lever arm is more dynamic in the postpower stroke state. Our results suggest myosin binding to actin in the ADP.Pi complex triggers a rapid power stroke that gates the release of phosphate, whereas a second slower power stroke may be important for mediating strain sensitivity.Myosins are molecular machines that use the energy from ATP hydrolysis to generate force and motion through a cyclic interaction with actin filaments. Actomyosin-based force generation is used to drive muscle contraction, organelle transport, cytokinesis, membrane tension generation, and numerous biological tasks (1). Most myosins display a conserved structural fold and ATPase mechanism, suggesting the mechanism of energy transduction is similar in the myosin superfamily. A long α-helix which extends from the motor core binds a variable number of light chains and is referred to as the “lever arm” (2). A relative sliding motion of myosin (thick) and actin (thin) filaments in muscle forms the basis of the cross-bridge hypothesis which provides a more general view of the mechanism of muscle contraction (3). The swinging lever arm hypothesis provides a more molecular basis of muscle contraction. In this hypothesis, the lever arm swing is associated with the actin-activated product release steps, in turn leading to force generation by the attached cross-bridge (4). However, the precise timing of the lever arm swing and product release steps has remained a central question since early studies of actomyosin (5).Scheme I represents a simplified actomyosin ATPase cycle that can be used to describe the kinetics of key steps in the catalytic cycle (5, 6). The weak actin-binding states of myosin are indicated in bold, and the actin-bound biochemical transitions are indicated by equilibrium constants with a prime. ATP binding to myosin occurs in two steps, an initial collision complex (K′₁) followed by a structural change that is associated with a weak actin-binding conformation (open actin-binding cleft) and high affinity for ATP (closed nucleotide-binding pocket) (K′₂). The movement of the lever arm into the prepower stroke state is thought to occur during one of the ATP-binding steps and before ATP hydrolysis. The ATP hydrolysis step (K₃) occurs while myosin remains in a weak actin-binding conformation. When myosin binds to actin with the hydrolyzed products in the active site, there is a dramatic acceleration of the product release steps, first phosphate (Pi) (K′₄) and then ADP (K′₅). It is during the actin-activated product release steps that the lever shifts from a pre- to a postpower stroke state and force generation occurs. In addition, myosin shifts from a weak to a strong actin-binding conformation as a result of actin-induced closure of the actin-binding cleft. Thus, to determine the structural mechanism of actomyosin-based force generation, it is crucial to design a method of measuring the position of the lever arm during the formation of the prepower stroke state (recovery stroke) as well as during the transition from the pre- to postpower stroke states (power stroke).Open in a separate windowScheme 1.The actomyosin ATPase cycle.In the current study we engineered myosin V (MV), a motor that is well characterized both kinetically and structurally, to contain three site-specific donor–acceptor pairs that allowed us to measure the lever arm swing directly by FRET. We provide direct evidence that the lever arm swings into the prepower stroke state (recovery stroke) when the active site is primed for ATP hydrolysis. The force-generating swing (the power stroke) occurs in two steps, with the first, fast step occurring before phosphate release. The slower power stroke step occurs before ADP release which is hypothesized to be a strain-sensitive step in the catalytic cycle of MV. Our work provides crucial insights into the structural details of lever arm swing in relation to the different steps in the catalytic cycle of myosin motors.     

Ablation of cardiac myosin-binding protein-C accelerates stretch activation in murine skinned myocardium

Cardiac myosin binding protein-C (cMyBP-C) is a thick filament accessory protein that binds tightly to myosin, but despite evidence that mutations in the cMyBP-C gene comprise a frequent cause of hypertrophic cardiomyopathy, relatively little is known about the role(s) of cMyBP-C in myocardium. Based on earlier studies demonstrating the potential importance of stretch activation in cardiac contraction, we examined the effects of cMyBP-C on the stretch activation responses of skinned ventricular preparations from wild-type (WT) and homozygous cMyBP-C knockout mice (cMyBP-C(-/-)) previously developed in our laboratory. Sudden stretch of skinned myocardium during maximal or submaximal Ca2+ activations resulted in an instantaneous increase in force that quickly decayed to a minimum and was followed by a delayed redevelopment of force (ie, stretch activation) to levels greater than prestretch force. Ablation of cMyBP-C dramatically altered the stretch activation response, ie, the rates of force decay and delayed force transient were accelerated compared with WT myocardium. These results suggest that cMyBP-C normally constrains the spatial position of myosin cross-bridges, which, in turn, limits both the rate and extent of interaction of cross-bridges with actin. We propose that ablation of cMyBP-C removes this constraint, increases the likelihood of cross-bridge binding to actin, and speeds the rate of delayed force development following stretch. Regardless of the specific mechanism, acceleration of cross-bridge cycling in cMyBP-C(-/-) myocardium could account for the abbreviation of systolic ejection in this mouse as a direct consequence of premature stretch activation of ventricular myocardium.     

Remote control of A-band cardiac thin filaments by the I-Z-I protein network of cardiac sarcomeres

A conventional view of the role of sarcomeric thin filaments in cardiac function is that they react with cross-bridges that translate them toward the center of the sarcomere in a reaction triggered by Ca(2+) and powered by ATP. However, thin filaments also engage in a complex network of protein-protein interactions in the Z-disc. Thus, in the modern context, understanding of what thin filaments do in the heart must take into account not only A-band regions that react with cross-bridges, but also I-Z-I regions that rarely, if ever, react with cross-bridges and dwell near and within the Z-disc. To highlight these multiplex functions of the thin filament, I discuss the hypothesis that physical and chemical reactions at the interface of the thin filaments with Z-disc proteins control the docking and activity of kinases and phosphatases that control the levels of phosphorylation of thin filament regulatory proteins. Testing this hypothesis has taken on new significance with the identification of multisite phosphorylation of thin filament proteins as a critical element in the control of cardiac contraction and relaxation reserve and in maladaptive mechanisms in heart failure. Moreover, multiple mutations in Z-disc proteins that link to prevalent cardiomyopathies are likely to alter this remote control of A-band thin filament function.     

Tropomyosin directly modulates actomyosin mechanical performance at the level of a single actin filament

Muscle contraction is the result of myosin cross-bridges (XBs) cyclically interacting with the actin-containing thin filament. This interaction is modulated by the thin filament regulatory proteins, troponin and tropomyosin (Tm). With the use of an in vitro motility assay, the role of Tm in myosin's ability to generate force and motion was assessed. At saturating myosin surface densities, Tm had no effect on thin filament velocity. However, below 50% myosin saturation, a significant reduction in actin-Tm filament velocity was observed, with complete inhibition of movement occurring at 12. 5% of saturating surface densities. Under similar conditions, actin filaments alone demonstrated no reduction in velocity. The effect of Tm on force generation was assessed at the level of a single thin filament. In the absence of Tm, isometric force was a linear function of the density of myosin on the motility surface. At 50% myosin surface saturation, the presence of Tm resulted in a 2-fold enhancement of force relative to actin alone. However, no further potentiation of force was observed with Tm at saturating myosin surface densities. These results indicate that, in the presence of Tm, the strong binding of myosin cooperatively activates the thin filament. The inhibition of velocity at low myosin densities and the potentiation of force at higher myosin densities suggest that Tm can directly modulate the kinetics of a single myosin XB and the recruitment of a population of XBs, respectively. At saturating myosin conditions, Tm does not appear to affect the recruitment or the kinetics of myosin XBs.     

Length-dependence of Actin–Myosin Interaction in Skinned Cardiac Muscle Fibers in Rigor

It has been suggested that the length dependence of myofilament Ca²⁺sensitivity and of Ca²⁺binding to troponin C, observed over the ascending limb of the cardiac force–length curve, is based on variation in the number of interacting cross-bridges. This interaction would be reduced at short sarcomere length as a consequence of double overlap of oppositely polarized actin filaments and increased lateral separation of actin and myosin filaments. Based on current evidence, it is not clear to what extent the actin–myosin interaction is hindered at sarcomere lengths where Ca²⁺sensitivity is reduced. We have used two biochemical assays to assess cross-bridge attachment in rigor muscle at sarcomere lengths corresponding to the ascending limb of the cardiac force–length curve. These are based on (1) the inhibition of K⁺-activated myosin ATPase by the complexation of actin with myosin, and (2) the enhancement of Ca²⁺binding to troponin C by rigor bridge attachment to actin. Measurements were made with skinned fibers from bovine ventricle. As a check on our method, measurements were also made with skinned rabbit psoas muscle fibers. With both muscle types, a reduction in sarcomere length along the ascending limb of the force–length curve was associated with an increase in K⁺-activated ATPase activity and a reduction in Ca²⁺binding to the regulatory sites of troponin C. These results indicate that actin–myosin interaction is significantly reduced at short sarcomere length.