The regulatory domain of the myosin head behaves as a rigid lever.

The regulatory domain of the myosin head is believed to serve as a lever arm that amplifies force generated in the catalytic domain and transmits this strain to the thick filament. The lever arm itself either can be passive or may have a more active role storing some of the energy created by hydrolysis of ATP. A structural correlate which might distinguish between these two possibilities (a passive or an active role) is the stiffness of the domain in question. To this effect we have examined the motion of the proximal (ELC) and distal (RLC) subdomains of the regulatory domain in reconstituted myosin filaments. Each subdomain was labeled with a spin label at a unique cysteine residue, Cys-136 of ELC or Cys-154 of mutant RLC, and its mobility was determined using saturation transfer electron paramagnetic resonance spectroscopy. The mobility of the two domains was similar; the effective correlation time (tau(eff)) for ELC was 17 micros and that for RLC was 22 micros. Additionally, following a 2-fold change of the global dynamics of the myosin head, effected by decreasing the interactions with the filament surface (or the other myosin head), the coupling of the intradomain dynamics remained unchanged. These data suggest that the regulatory domain of the myosin head acts as a single mechanically rigid body, consistent with the regulatory domain serving as a passive lever.     

Modification of interface between regulatory and essential light chains hampers phosphorylation-dependent activation of smooth muscle myosin

We examined the regulatory importance of interactions between regulatory light chain (RLC), essential light chain (ELC), and adjacent heavy chain (HC) in the regulatory domain of smooth muscle heavy meromyosin. After mutating the HC, RLC, and/or ELC to disrupt their predicted interactions (using scallop myosin coordinates), we measured basal ATPase, V(max), and K(ATPase) of actin-activated ATPase, actin-sliding velocities, rigor binding to actin, and kinetics of ATP binding and ADP release. If unphosphorylated, all mutants were similar to wild type showing turned-off behaviors. In contrast, if phosphorylated, mutation of RLC residues smM129Q and smG130C in the F-G helix linker, which interact with the ELC (Ca(2+) binding in scallop), was sufficient to abolish motility and diminish ATPase activity, without altering other parameters. ELC mutations within this interacting ELC loop (smR20M and smK25A) were normal, but smM129Q/G130C-R20M or -K25A showed a partially recovered phenotype suggesting that interaction between the RLC and ELC is important. A molecular dynamics study suggested that breaking the RLC/ELC interface leads to increased flexibility at the interface and ELC-binding site of the HC. We hypothesize that this leads to hampered activation by allowing a pre-existing equilibrium between activated and inhibited structural distributions (Vileno, B., Chamoun, J., Liang, H., Brewer, P., Haldeman, B. D., Facemyer, K. C., Salzameda, B., Song, L., Li, H. C., Cremo, C. R., and Fajer, P. G. (2011) Broad disorder and the allosteric mechanism of myosin II regulation by phosphorylation. Proc. Natl. Acad. Sci. U.S.A. 108, 8218-8223) to be biased strongly toward the inhibited distribution even when the RLC is phosphorylated. We propose that an important structural function of RLC phosphorylation is to promote or assist in the maintenance of an intact RLC/ELC interface. If the RLC/ELC interface is broken, the off-state structures are no longer destabilized by phosphorylation.     

Role of the essential light chain in the activation of smooth muscle myosin by regulatory light chain phosphorylation

The activity of smooth and non-muscle myosin II is regulated by phosphorylation of the regulatory light chain (RLC) at serine 19. The dephosphorylated state of full-length monomeric myosin is characterized by an asymmetric intramolecular head–head interaction that completely inhibits the ATPase activity, accompanied by a hairpin fold of the tail, which prevents filament assembly. Phosphorylation of serine 19 disrupts these head–head interactions by an unknown mechanism. Computational modeling (Tama et al., 2005. J. Mol. Biol. 345, 837–854) suggested that formation of the inhibited state is characterized by both torsional and bending motions about the myosin heavy chain (HC) at a location between the RLC and the essential light chain (ELC). Therefore, altering relative motions between the ELC and the RLC at this locus might disrupt the inhibited state. Based on this hypothesis we have derived an atomic model for the phosphorylated state of the smooth muscle myosin light chain domain (LCD). This model predicts a set of specific interactions between the N-terminal residues of the RLC with both the myosin HC and the ELC. Site directed mutagenesis was used to show that interactions between the phosphorylated N-terminus of the RLC and helix-A of the ELC are required for phosphorylation to activate smooth muscle myosin.     

Essential light chain modulates phosphorylation-dependent regulation of smooth muscle myosin

To examine the functional role of the essential light chain (ELC) in the phosphorylation-dependent regulation of smooth muscle myosin, we replace the native light chain in smooth muscle myosin with bacterially expressed chimeric ELCs in which one or two of the four helix-loop-helix domains of chicken gizzard ELC were substituted by the corresponding domains of scallop (Aquipecten irradians) ELC. All of these myosins, regardless of the ELC mutations or regulatory light chain (RLC) phosphorylation, showed normal subunit constitutions and NH(4)(+)/EDTA-ATPase activities, both of which were similar to those of native myosin. None of the ELC mutations changed the actin-activated ATPase activity of myosin in the absence of RLC phosphorylation. However, in the presence of RLC phosphorylation, the substitution of domain 1 or 2 in the ELC significantly decreased the actin-activated ATPase activity, whereas the substitution of both of these domains did not change the activity. In contrast to myosin, the domain 2 substitution in the ELC did not affect the actin-activated ATPase activity of single-headed myosin subfragment 1. These results suggest an interhead interaction between domains 1 and 2 of ELCs which is required to attain the full actin-activated ATPase activity of smooth muscle myosin in the presence of RLC phosphorylation.     

Transient interaction between the N-terminal extension of the essential light chain-1 and motor domain of the myosin head during the ATPase cycle

The molecular mechanism of muscle contraction is based on the ATP-dependent cyclic interaction of myosin heads with actin filaments. Myosin head (myosin subfragment-1, S1) consists of two major domains, the motor domain responsible for ATP hydrolysis and actin binding, and the regulatory domain stabilized by light chains. Essential light chain-1 (LC1) is of particular interest since it comprises a unique N-terminal extension (NTE) which can bind to actin thus forming an additional actin-binding site on the myosin head and modulating its motor activity. However, it remains unknown what happens to the NTE of LC1 when the head binds ATP during ATPase cycle and dissociates from actin. We assume that in this state of the head, when it undergoes global ATP-induced conformational changes, the NTE of LC1 can interact with the motor domain. To test this hypothesis, we applied fluorescence resonance energy transfer (FRET) to measure the distances from various sites on the NTE of LC1 to S1 active site in the motor domain and changes in these distances upon formation of S1-ADP-BeF_x complex (stable analog of S1¹-AТP state). For this, we produced recombinant LC1 cysteine mutants, which were first fluorescently labeled with 1,5-IAEDANS (donor) at different positions in their NTE and then introduced into S1; the ADP analog (TNP-ADP) bound to the S1 active site was used as an acceptor. The results show that formation of S1-ADP-BeF_x complex significantly decreases the distances from Cys residues in the NTE of LC1 to TNP-ADP in the S1 active site; this effect was the most pronounced for Cys residues located near the LC1 N-terminus. These results support the concept of the ATP-induced transient interaction of the LC1 N-terminus with the S1 motor domain.     

Cardiomyopathy mutations impact the actin-activated power stroke of human cardiac myosin

Cardiac muscle contraction is driven by the molecular motor myosin, which uses the energy from ATP hydrolysis to generate a power stroke when interacting with actin filaments, although it is unclear how this mechanism is impaired by mutations in myosin that can lead to heart failure. We have applied a fluorescence resonance energy transfer (FRET) strategy to investigate structural changes in the lever arm domain of human β-cardiac myosin subfragment 1 (M2β-S1). We exchanged the human ventricular regulatory light chain labeled at a single cysteine (V105C) with Alexa 488 onto M2β-S1, which served as a donor for Cy3ATP bound to the active site. We monitored the FRET signal during the actin-activated product release steps using transient kinetic measurements. We propose that the fast phase measured with our FRET probes represents the macroscopic rate constant associated with actin-activated rotation of the lever arm during the power stroke in M2β-S1. Our results demonstrated M2β-S1 has a slower actin-activated power stroke compared with fast skeletal muscle myosin and myosin V. Measurements at different temperatures comparing the rate constants of the actin-activated power stroke and phosphate release are consistent with a model in which the power stroke occurs before phosphate release and the two steps are tightly coupled. We suggest that the actin-activated power stroke is highly reversible but followed by a highly irreversible phosphate release step in the absence of load and free phosphate. We demonstrated that hypertrophic cardiomyopathy (R723G)- and dilated cardiomyopathy (F764L)-associated mutations both reduced actin activation of the power stroke in M2β-S1. We also demonstrate that both mutations alter in vitro actin gliding in the presence and absence of load. Thus, examining the structural kinetics of the power stroke in M2β-S1 has revealed critical mutation-associated defects in the myosin ATPase pathway, suggesting these measurements will be extremely important for establishing structure-based mechanisms of contractile dysfunction.     

Molecular modeling of the myosin-S1(A1) isoform

Type II myosin is the molecular motor which drives contraction upon cyclic interaction with filamentous actin while consuming ATP. The contemporary crystallographic structure of the myosin subfragment-1 (S1) of myosin covers both the motor domain of the heavy chain (MHC) as well as the essential (ELC) and regulatory light chains (RLC). A part of the N-terminus of the ELC is, however, missing in the 3D-models of Type II myosin. The N-terminal domain of the ELC comprises interesting functional features since it binds to actin thus controlling myosin motor activity. For the first time, we modeled the missing 46 N-terminal amino acid of the ELC to the contemporary actin-myosin-S1 complex. We show a rod-like 91 A structure being long enough to bridge the gap between the ELC core of myosin-S1 and the appropriate binding site of the ELC on the actin filament.     

On the relationship between distance information derived from cross-linking and from resonance energy transfer, with specific reference to sites located on myosin heads.

The techniques of fluorescence resonance energy transfer (FRET) and cross-linking can provide complementary information concerning the relative separation of a pair of sites. Cross-linking experiments provide an assessment of the distance of closest approach between a pair of sites. FRET measurements, by contrast, yield information about the average distance between the pair of sites. We have taken advantage of hybrid myosins to understand the relationship between distances obtained for a pair of equivalent sites, one on each myosin head, using both FRET (steady-state and time-decay) and cross-linking techniques. The rigid cross-linker, 4-4'-dimaleimidyl-stilbene-2-2'-disulfonic acid (DMSDS), can efficiently cross-link the two myosin regulatory light-chains, each at residue Cys50 of the Mercenaria regulatory light chain (Chantler, P.D., and S. M. Bower. 1988. J. Biol. Chem. 263:938-944), indicating that these sites can come within 18 +/- 2 A of each other. In a complementary set of experiments, steady-state and time-decay measurements using fluorescence donor/acceptor pairs located at these same sites indicate transfer efficiencies of somewhat less than 20%, suggesting an average separation of greater than 50 A between sites (Chantler, P. D., and T. Tao. 1986. J. Mol. Biol. 192:87-99). Here, we present theoretical calculations which show that efficient cross-linking can be achieved readily in dynamic systems such as the heads of myosin, even though the necessary subpopulation of proximate molecules at any instant may be below the detection limits of time-decay-FRET.(ABSTRACT TRUNCATED AT 250 WORDS)     

Luminescence resonance energy transfer measurements in myosin.

Myosin is thought to generate force by a rotation between the relative orientations of two domains. Direct measurements of distances between the domains could potentially confirm and quantify these conformational changes, but efforts have been hampered by the large distances involved. Here we show that luminescence resonance energy transfer (LRET), which uses a luminescent lanthanide as the energy-transfer donor, is capable of measuring these long distances. Specifically, we measure distances between the catalytic domain (Cys707) and regulatory light chain domain (Cys108) of the myosin head. An energy transfer efficiency of 21.2 +/- 1.9% is measured in the myosin complex without nucleotide or actin, corresponding to a distance of 73 A, consistent with the crystal structure of Rayment et al. Upon binding to actin, the energy transfer efficiency decreases by 4.5 +/- 1.0%, indicating a conformational change in myosin that involves a relative rotation and/or translation of Cys707 relative to the light chain domain. Addition of ADP also alters the energy transfer efficiency, likely through a rotation of the probe attached to Cys707. These results demonstrate that LRET is capable of making accurate measurements on the relatively large actomyosin complex, and is capable of detecting conformational changes between the catalytic and light chain domains of myosin.     

Two new modes of smooth muscle myosin regulation by the interaction between the two regulatory light chains, and by the S2 domain

Previous studies indicated that single-headed smooth muscle myosin and S1 (a single head fragment) are not regulated through phosphorylation of the regulatory light chain (RLC). To investigate the importance of the double-headedness of myosin and of the S2 region for the phosphorylation-dependent regulation, we made three types of recombinant mutant smooth muscle HMMs with one intact head and an N-terminally truncated head. The truncated head of Delta MD lacked the motor domain, that of Delta(MD+ELC) lacked the motor and essential light chain binding domains, and single-headed HMM had one intact head alone. The basal ATPase activities of the three mutants decreased as the KCl concentration became less than 0.1 M. Such a decrease was not observed for S1, which had no S2 region, suggesting that S2 is necessary for this myosin behavior. This activity decrease also disappeared when RLCs of Delta MD and Delta(MD+ELC), but that of single-headed HMM, were phosphorylated. When their RLCs were unphosphorylated, the three mutants exhibited similar actin-activated ATPase levels. However, when they were phosphorylated, the actin-activated ATPase activities of Delta MD and Delta(MD+ELC) increased to the S1 level, while that of single-headed HMM remained unchanged. Even in the phosphorylated state, the actin-activated ATPase activities of the three mutants and S1 were much lower than that of wild-type HMM. We propose that S2 has an inhibitory function that is canceled by an interaction between two phosphorylated RLCs. We also propose that a cooperative interaction between two motor domains is required for a higher level of actin activation.