Effect of nucleotides and actin on the orientation of the light chain-binding domain in myosin subfragment 1

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 S1^∗-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.

Asymmetric myosin binding to the thin filament as revealed by a fluorescent nanocircuit

The interplay between myosin, actin, and striated muscle regulatory proteins involves complex cooperative interactions that propagate along the thin filament. A repeating unit of the tropomyosin dimer, troponin heterotrimer, and the actin protofilament heptamer is sometimes assumed to be able to bind myosin at any of its seven actins when activated even though the regulatory proteins are asymmetrically positioned along this repeating unit. Analysis of the impact of this asymmetry on actin and myosin interactions by sensitized emission luminescence resonance energy transfer spectroscopy and a unique fluorescent nanocircuit design reveals that the troponin affects the structure and function of myosin heads bound nearby in a different manner than myosin heads bound further away from the troponin. To test this hypothesis, a fluorescent nanocircuit reported the position of the myosin lever arm only when the myosin was bound adjacent to the troponin, or in controls, only when the myosin was bound distant from the troponin. Confirming the hypothesis, the myosin lever arm is predominantly in the pre powerstroke orientation when bound near troponin, but is predominantly in the post powerstroke orientation when bound distant from troponin. These data are consistent with the hypothesis that troponin is responsible for the formation of myosin binding target zones along the thin filament.

Response of rigor cross-bridges to stretch detected by fluorescence lifetime imaging microscopy of myosin essential light chain in skeletal muscle fibers

We applied fluorescence lifetime imaging microscopy to map the microenvironment of the myosin essential light chain (ELC) in permeabilized skeletal muscle fibers. Four ELC mutants containing a single cysteine residue at different positions in the C-terminal half of the protein (ELC-127, ELC-142, ELC-160, and ELC-180) were generated by site-directed mutagenesis, labeled with 7-diethylamino-3-((((2-iodoacetamido)ethyl)amino)carbonyl)coumarin, and introduced into permeabilized rabbit psoas fibers. Binding to the myosin heavy chain was associated with a large conformational change in the ELC. When the fibers were moved from relaxation to rigor, the fluorescence lifetime increased for all label positions. However, when 1% stretch was applied to the rigor fibers, the lifetime decreased for ELC-127 and ELC-180 but did not change for ELC-142 and ELC-160. The differential change of fluorescence lifetime demonstrates the shift in position of the C-terminal domain of ELC with respect to the heavy chain and reveals specific locations in the lever arm region sensitive to the mechanical strain propagating from the actin-binding site to the lever arm.

Green fluorescent protein impairs actin-myosin interactions by binding to the actin-binding site of myosin

Green fluorescent proteins (GFP) are widely used in biology for tracking purposes. Although expression of GFP is considered to be innocuous for the cells, deleterious effects have been reported. We recently demonstrated that expression of eGFP in muscle impairs its contractile properties (Agbulut, O., Coirault, C., Niederlander, N., Huet, A., Vicart, P., Hagege, A., Puceat, M., and Menasche, P. (2006) Nat. Meth. 3, 331). This prompted us to identify the molecular mechanisms linking eGFP expression to contractile dysfunction and, particularly, to test the hypothesis that eGFP could inhibit actin-myosin interactions. Therefore, we assessed the cellular, mechanical, enzymatic, biochemical, and structural properties of myosin in the presence of eGFP and F-actin. In vitro motility assays, the maximum actin-activated ATPase rate (V(max)) and the associated constant of myosin for actin (K(m)) were determined at 1:0.5, 1:1, and 1:3 myosin:eGFP molar ratios. At a myosin:eGFP ratio of 1:0.5, there was a nearly 10-fold elevation of K(m). As eGFP concentration increased relative to myosin, the percentage of moving filaments, the myosin-based velocity, and V(max) significantly decreased compared with controls. Moreover, myosin co-precipitated with eGFP. Crystal structures of myosin, actin, and GFP indicated that GFP and actin exhibited similar electrostatic surface patterns and the ClusPro docking model showed that GFP bound preferentially to the myosin head and especially to the actin-binding site. In conclusion, our data demonstrate that expression of eGFP in muscle resulted in the binding of eGFP to myosin, thereby disturbing the actin-myosin interaction and in turn the contractile function of the transduced cells. This potential adverse effect of eGFP should be kept in mind when using this marker to track cells following transplantation.

The use of FRET in the analysis of motor protein structure

Fluorescence resonance energy transfer (FRET) is a spectroscopic phenomenon that consists of long-range dipole-dipole interaction between two chromophores. This method can be employed to gain quantitative distance information on macromolecules. FRET is particularly useful to characterize structural states of motor proteins, because the spatial relationship between various mechanical elements of the motor undergoing its mechanical cycle is essential to understand how force and movement are generated. In this chapter, we describe the technique, including the equations, methods of introducing fluorescence probes in specific loci of the protein, and data analysis. Practical guidelines and hints are also provided for protein preparation, labeling, and measuring FRET efficiency. The protocol is presented for interhead distance measurements in the dimeric kinesin-like motor, Ncd. However, it can easily be adapted to many other motor proteins.

Effect of nucleotides and their analogues on essential light chains in myosin head

The domain movement in myosin head plays a decisive role in the energy transduction process of the muscle contraction. During hydrolysis of ATP, the specific formation of strong binding of myosin head for actin causes conformational changes. As a consequence, the light chain-binding motif generates the powerstroke. In our work maleimide spin labels were covalently attached to Cys-177 residue of ELC in subfragment-1 (S1). Our goal was to study the orientation dependence and the motion of S1, which were incorporated into glycerinated skeletal muscle fibres. The electron paramagnetic resonance spectroscopy (EPR) spectra of the probes depended strongly on the orientation of the fibre axis relative to the magnetic field, indicating that the essential light chain (ELC) and the neck were ordered. The probes were undergoing rapid motion within a cone. The half-width of the cone was estimated to be 65+/-5 degrees (SD, n=8). Addition of ADP affected little the hyperfine splitting and the angular spread of the probe distribution. In the presence of ADP and orthovanadate the intensity of the spectra decreased, which showed the dissociation of S1 and this was accompanied with the disappearance of the orientation dependence.

Conformational selection during weak binding at the actin and myosin interface

The molecular mechanism of the powerstroke in muscle is examined by resonance energy transfer techniques. Recent models suggesting a pre-cocking of the myosin head involving an enormous rotation between the lever arm and the catalytic domain were tested by measuring separation distances among myosin subfragment-2, the nucleotide site, and the regulatory light chain in the presence of nucleotide transition state analogs. Only small changes (<0.5 nm) were detected that are consistent with internal conformational changes of the myosin molecule, but not with extreme differences in the average lever arm position suggested by some atomic models. These results were confirmed by stopped-flow resonance energy transfer measurements during single ATP turnovers on myosin. To examine the participation of actin in the powerstroke process, resonance energy transfer between the regulatory light chain on myosin subfragment-1 and the C-terminus of actin was measured in the presence of nucleotide transition state analogs. The efficiency of energy transfer was much greater in the presence of ADP-AlF(4), ADP-BeF(x), and ADP-vanadate than in the presence of ADP or no nucleotide. These data detect profound differences in the conformations of the weakly and strongly attached cross-bridges that appear to result from a conformational selection that occurs during the weak binding of the myosin head to actin.

A FRET-based sensor reveals large ATP hydrolysis-induced conformational changes and three distinct states of the molecular motor myosin

The molecular motor myosin is proposed to bind to actin and swing its light-chain binding region through a large angle to produce an approximately 10 nm step in motion coupled to changes in the nucleotide state at the active site. To date, however, direct dynamic measurements have largely failed to show changes of that magnitude. Here, we use a cysteine engineering approach to create a high resolution, FRET-based sensor that reports a large, approximately 70 degree nucleotide-dependent angle change of the light-chain binding region. The combination of steady-state and time-resolved fluorescence resonance energy transfer measurements unexpectedly reveals two distinct prestroke states. The measurements also show that bound Mg.ADP.Pi, and not bound Mg.ATP, induces the myosin to adopt the prestroke states.

Interaction of myosin LYS-553 with the C-terminus and DNase I-binding loop of actin examined by fluorescence resonance energy transfer

Fluorescence resonance energy transfer (FRET) experiments were carried out in the absence of nucleotide (rigor) or in the presence of MgADP between fluorescent donor probes (IAEDANS (5((((2-iodoacetyl)amino)ethyl)amino)-naphthalene-1-sulfonic acid) at Cys-374 or DANSYL (5-dimethylamino naphthalene-1-(N-(5-aminopentyl))sulfonamide) at Gln-41 of actin and acceptor molecules (FHS (6-[fluorescein-5(and 6)-carboxamido] hexanoic acid succinimidyl ester) at Lys-553 of skeletal muscle myosin subfragment 1. The critical Förster distance (R(0)) was determined to be 44 and 38 A for the IAEDANS-FHS and DANSYL-FHS donor-acceptor pairs, respectively. The efficiency of energy transfer between the acceptor molecules at Lys-553 of myosin and donor probes at Cys-374 or Gln-41 of actin was calculated to be 0.78 +/- 0.01 or 0.94 +/- 0.01, respectively, corresponding to distances of 35.6 +/- 0.4 A and 24.0 +/- 1.6 A, respectively. MgADP had no significant effect on the distances observed in rigor. Thus, rearrangements in the acto-myosin interface are likely to occur elsewhere than in the lower 50-kDa subdomain of myosin as its affinity for actin is weakened by MgADP binding.

Flexibility of myosin-subfragment-1 in its complex with actin as revealed by fluorescence resonance energy transfer

The flexibility of the acto-myosin complex in rigor conditions was characterized by measuring the temperature profile of normalized fluorescence resonance energy transfer efficiency, f' [Somogyi, B., Matkó, J., Papp, S., Hevessy, J., Welch, G.R. & Damjanovich, S. (1984) Biochemistry 23, 3403-3411]. Fluorescence acceptors were introduced to the Cys374 residues of actin and the donors were covalently attached either to Cys707 in the catalytic domain or to Cys177 in the essential light-chain of myosin S1. Fluorescence resonance energy transfer measurements revealed that the protein matrix between Cys374 of actin and Cys707 of S1 is rigid. In contrast, the link between the catalytic and light-chain-binding domains in myosin S1 is flexible. We have recently shown that the positional distribution of Cys707 was narrow relative to the actin filament, while that of the Cys177 was broad. Accordingly, the broad positional distribution of Cys177 is likely to be due to the large flexibility of the link between the catalytic and light-chain-binding domains. This flexibility is probably essential for the interdomain reorganization of the myosin head during the force generation process and for accommodating the symmetry difference between actin and myosin filaments to allow the formation of cross-bridges.

Dynamics at Lys-553 of the acto-myosin interface in the weakly and strongly bound states

Lys-553 of skeletal muscle myosin subfragment 1 (S1) was specifically labeled with the fluorescent probe FHS (6-[fluorescein-5(and 6)-carboxamido]hexanoic acid succinimidyl ester) and fluorescence quenching experiments were carried out to determine the accessibility of this probe at Lys-553 in both the strongly and weakly actin-bound states of the MgATPase cycle. Solvent quenchers of varying charge [nitromethane, (2,2,6, 6-tetramethyl-1-piperinyloxy) (TEMPO), iodide (I(-)), and thallium (Tl(+))] were used to assess both the steric and electrostatic accessibilities of the FHS probe at Lys-553. In the strongly bound rigor (nucleotide-free) and MgADP states, actin offered no protection from solvent quenching of FHS by nitromethane, TEMPO, or thallium, but did decrease the Stern-Volmer constant by almost a factor of two when iodide was used as the quencher. The protection from iodide quenching was almost fully reversed with the addition of 150 mM KCl, suggesting this effect is ionic in nature rather than steric. Conversely, actin offered no protection from iodide quenching at low ionic strength during steady-state ATP hydrolysis, even with a significant fraction of the myosin heads bound to actin. Thus, the lower 50 kD subdomain of myosin containing Lys-553 appears to interact differently with actin in the weakly and strongly bound states.

Conformational distributions and proximity relationships in the rigor complex of actin and myosin subfragment-1

Cyclic conformational changes in the myosin head are considered essential for muscle contraction. We hereby show that the extension of the fluorescence resonance energy transfer method described originally by Taylor et al. (Taylor, D. L., Reidler, J., Spudich, J. A., and Stryer, L. (1981) J. Cell Biol. 89, 362-367) allows determination of the position of a labeled point outside the actin filament in supramolecular complexes and also characterization of the conformational heterogeneity of an actin-binding protein while considering donor-acceptor distance distributions. Using this method we analyzed proximity relationships between two labeled points of S1 and the actin filament in the acto-S1 rigor complex. The donor (N-[[(iodoacetyl)amino]ethyl]-5-naphthylamine-1-sulfonate) was attached to either the catalytic domain (Cys-707) or the essential light chain (Cys-177) of S1, whereas the acceptor (5-(iodoacetamido)fluorescein) was attached to the actin filament (Cys-374). In contrast to the narrow positional distribution (assumed as being Gaussian) of Cys-707 (5 +/- 3 A), the positional distribution of Cys-177 was found to be broad (102 +/- 4 A). Such a broad positional distribution of the label on the essential light chain of S1 may be important in accommodating the helically arranged acto-myosin binding relative to the filament axis.

Conformational changes between the active-site and regulatory light chain of myosin as determined by luminescence resonance energy transfer: the effect of nucleotides and actin

Myosin is thought to generate movement of actin filaments via a conformational change between its light-chain domain and its catalytic domain that is driven by the binding of nucleotides and actin. To monitor this change, we have measured distances between a gizzard regulatory light chain (Cys 108) and the active site (near or at Trp 130) of skeletal myosin subfragment 1 (S1) by using luminescence resonance energy transfer and a photoaffinity ATP-lanthanide analog. The technique allows relatively long distances to be measured, and the label enables site-specific attachment at the active-site with only modest affect on myosin's enzymology. The distance between these sites is 66.8 +/- 2.3 A when the nucleotide is ADP and is unchanged on binding to actin. The distance decreases slightly with ADP-BeF3, (-1.6 +/- 0.3 A) and more significantly with ADP-AlF4 (-4.6 +/- 0.2 A). During steady-state hydrolysis of ATP, the distance is temperature-dependent, becoming shorter as temperature increases and the complex with ADP.Pi is favored over that with ATP. We conclude that the distance between the active site and the light chain varies as Acto-S1-ADP approximately S1-ADP > S1-ADP-BeF3 > S1-ADP-AlF4 approximately S1-ADP-Pi and that S1-ATP > S1-ADP-Pi. The changes in distance are consistent with a substantial rotation of the light-chain binding domain of skeletal S1 between the prepowerstroke state, simulated by S1-ADP-AlF4, and the post-powerstroke state, simulated by acto-S1-ADP.

Domain motion between the regulatory light chain and the nucleotide site in skeletal myosin

Resonance energy transfer probes were attached to skeletal myosin's nucleotide site and regulatory light chain (RLC) to examine nucleotide analog-induced structural transitions. A novel chemical modification of the RLC was developed for specific labeling of the basic N-terminus without affecting myosin ATPase activity. The modification allows attachment of a terbium chelate to rabbit skeletal RLC and was mapped by tryptic digestion to an amino group on the six N-terminal RLC residues. The use of terbium as a resonance energy transfer donor allowed the determination of the efficiency of energy transfer by sensitized emission lifetime measurements that practically eliminate background from unlabeled donor and acceptor sites as well as potential orientation factor artifacts in the calculation of the critical transfer distance. The nucleotide site was labeled with a functional CY3-labeled nucleotide as an energy transfer acceptor. Of the nucleotide states examined, ADP, ADP. vanadate, ADP. A1F4, and ADP. BeFx, the difference between the ADP and ADP. vanadate states was greatest (0.4-nm change), but was not considered to be statistically significant. The binding of actin to ADP-myosin also failed to produce a statistically significant change (0.3-nm change). These results are not consistent with a number of versions of the swinging lever arm hypothesis.

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.