Caldesmon weakens the bonding between myosin heads and actin in ghost fibers

Earlier studies using polarized microphotometry have shown that caldesmon inhibits the alterations in structure and flexibility of actin in ghost fibers that take place upon the binding of myosin heads (Ga?azkiewicz et al. (1987) Biochim. Biophys. Acta 916, 368-375). The present investigations, performed with an IAEDANS label attached to myosin subfragment 1 (S-1), revealed that this inhibition results from the weakening of the binding between myosin heads and actin as indicated by the caldesmon-induced increase in the random movement of S-1. Parallel experiments with actin labeled at Cys-374 demonstrated that this effect of caldesmon is transmitted to the C-terminus of the actin molecule resulting in a conformational adjustment in this region of the molecule.     

Motion of actin filaments in the presence of myosin heads and ATP.

We measured, by fluorescence correlation spectroscopy, the motion of actin filaments in solution during hydrolysis of ATP by acto-heavy meromyosin (acto-HMM). The method relies on the fact that the intensity of fluorescence fluctuates as fluorescently labeled actin filaments enter and leave a small sample volume. The rapidity of these number fluctuations is characterized by the autocorrelation function, which decays to 0 in time that is related to the average velocity of translation of filaments. The time of decay of the autocorrelation function of bare actin filaments in solution was 10.59 +/- 0.85 s. Strongly bound (rigor) heads slowed down the diffusion. Direct observation of filaments under an optical microscope showed that addition of HMM did not change the average length or flexibility of actin filaments, suggesting that the decrease in diffusion was not due to a HMM-induced change in the shape of filaments. Rather, slowing down of translational motion was caused by an increase in the volume of the diffusing complex. Surprisingly, the addition of ATP to acto-HMM accelerated the motion of actin filaments. The acceleration was the greatest at the low molar ratios of HMM:actin. Direct observation of filaments under an optical microscope showed that in the presence of ATP the average length of filaments did not change and that the filaments became stiffer, suggesting that acceleration of diffusion was not due to an ATP-induced increase in flexibility of filaments. These results show that some of the energy of splitting of ATP is impaired to actin filaments and suggest that 0.06 +/- 0.02 of HMM interferes with the diffusion of actin filaments during hydrolysis of ATP.     

The binding of myosin heads on heavy meromyosin and assembled myosin to actin in the presence of nucleotides. Measurements by the proteolytic rates method

The initial rates of tryptic digestion at the 50/20-kDa junction in myosin and myosin subfragment 1 were determined for the free proteins and their complexes with actin in the presence and absence of MgATP. The proteolytic reactions were carried out at 24 degrees C and under ionic strength conditions (mu) adjusted to 35, 60, and 130 mM. The percentages of myosin heads and myosin subfragment 1 bound to actin in the presence of MgATP were calculated from the rates of proteolysis for each set of digestion experiments. In all cases, the myosin heads in the synthetic filaments showed greater binding to actin than myosin subfragment 1. This binding difference was most prominent (3-fold) at mu = 130 mM. The binding of heavy meromyosin (HMM) to actin in the presence of MgADP was measured at 4 degrees C by ultracentrifugation and the proteolytic rates methods. Ultracentrifugation experiments determined the fraction of HMM molecules bound to actin in the presence of MgADP, whereas the proteolytic measurements yielded the information on the fraction of HMM heads bound to actin. Taken together, these measurements show that a significant fraction of HMM is bound to actin with only one head in the presence of MgADP under ionic conditions of 180 and 280 mM.     

The interaction of actin monomers with myosin heads and other muscle proteins.

The simplest interacting unit of actomyosin, viz., single myosin heads (subfragment 1) with actin monomers, has been studied at physiological ionic strength, by isolating the actin molecules from each other on a solid support. The interaction is characterized by a binding constant of 10(5) to 10(6) M-1 in the temperature range 4-30degrees C. It is endothermic with a standard enthalpy of 24 +/- 10 kcal mol-1, and a standard entropy of 110 +/- 40 eu. It is thus, like many protein-protein association processes, entropy-driven. Despite the high affinity of the association, which is comparable in its binding constant to that of subfragment 1 with F-actin, there is only very small activation of myosin ATPase. The ionic-strength dependence of the interaction shows unusual features. Binding of the proteins of the relaxing system to the monomeric actin was also examined: troponin binds both in the presence and absence of calcium ions, but neither tropomyosin nor the tropomyosin-troponin complex was found to bind significantly. Monomeric actin has also been examined as a function of ionic strength by spectroscopic methods; it appears that conformational differences between the G and the F state are the consequence of polymerization, and not of the change in ionic strength required to being the conversion about.     

ATP induces microsecond rotational motions of myosin heads crosslinked to actin.

We have used saturation transfer electron paramagnetic resonance (ST-EPR) to study the effect of ATP on the rotational dynamics of spin-labeled myosin heads crosslinked to actin (XLAS1). We have previously shown that ATP induces microsecond rotational motions in activated myofibrils or muscle fibers, but the possibility remained that the motion occurred only in the detached phase of the cross-bridge cycle. The addition of ATP to the crosslinked preparation has been shown to be a model system for active cross-bridges, presumably providing an opportunity to measure the motion in the attached state, without interference from unattached heads. In the absence of ATP, XLAS1 had very little microsecond rotational mobility, yielding a spectrum identical to that observed for uncrosslinked acto-S1. This suggests that all of the labeled S1 forms normal rigor complexes when crosslinked to actin. The addition of 5 mM ATP greatly increased the microsecond rotational mobility of XLAS1, and the effects were reversed upon depletion of ATP. The most plausible explanation for these results is that myosin heads undergo microsecond rotational motion while attached actively to actin during steady state ATPase activity. These results have important implications for the interpretation of spectroscopic data obtained during muscle contraction.     

ADP binding induces an asymmetry between the heads of unphosphorylated myosin

Light chain phosphorylation is the key event that regulates smooth and non-muscle myosin II ATPase activity. Here we show that both heads of smooth muscle heavy meromyosin (HMM) bind tightly to actin in the absence of nucleotide, irrespective of the state of light chain phosphorylation. In striking contrast, only one of the two heads of unphosphorylated HMM binds to actin in the presence of ADP, and the heads have different affinities for ADP. This asymmetry suggests that phosphorylation alters the mechanical coupling between the heads of HMM. A model that incorporates strain between the two heads is proposed to explain the data, which have implications for how one head of a motor protein can gate the response of the other.     

The binding of actin to phosphorylated and dephosphorylated myosin

The binding of actin to myosin containing phosphorylated and dephosphorylated light chains (LC2) was investigated by studying the influence of actin on Mg2+- and K+-stimulated ATPase of phosphorylated and dephosphorylated myosin and by comparing the influence of PPi on actomyosin formed from pure actin and phosphorylated or dephosphorylated myosin. The concentration of actin producing inhibition of one half of myosin K+-ATPase activity was 4.1 micro M and 7.7 micro M for phosphorylated and dephosphorylated myosin, respectively. Actomyosin formed from dephosphorylated myosin dissociated at lower PPi concentration than did that from the phosphorylated form. The extrapolated values of Km obtained from studies of the influence of actin on Mg2+-ATPase activity of dephosphorylated myosin were about twice as high as for the phosphorylated form. Thus, the affinity of phosphorylated myosin for actin was significantly higher under conditions studied.     

Proteolysis and binding of myosin subfragment 1 to actin

Rates of proteolytic cleavage of myosin subfragment 1 were measured in the absence and presence of different amounts of actin. The rates of tryptic digestion at the 50K/20K junction and papain digestion at the 25K/50K junction of the myosin head were progressively inhibited with increasing substoichiometric molar ratios of actin to myosin subfragment 1. The percentage inhibitions of digestion reactions corresponded precisely to the molar compositions of actin-subfragment 1 solutions and demonstrated that equimolar complexes of these proteins were responsible for the observed changes in the proteolysis of myosin heads.     

Shift of binding site at the interface between actin and myosin

The molar ratio dependent change in the binding manner between actin and the lysine-rich sequence at the junction between 50K and 20K domains of subfragment 1 was studied by both protease digestion and cross-linking with 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide. The tryptic cleavage site at the function between 50K and 20K was found to be located between the third and fourth lysine residues in the lysine-rich sequence -KKGGKKK-. This site was not protected by actin when the molar ratio of actin to subfragment 1 was 1:1 but was protected at 2:1 and 3:1. The V8 protease cleavage site of chicken subfragment 1 and the elastase cleavage site of rabbit subfragment 1 were found to be located four residues away from the N-terminus of the lysine-rich sequence. Unlike the tryptic cleavage site, this site was protected by actin more when the molar ratio of actin to subfragment 1 was 1:1 than when it was 2:1 and 3:1. To understand the reason for the opposite effect of the molar ratio observed at the middle of and at four residues away from the lysine-rich sequence, actual cross-linked residue(s) was (were) determined by subjecting cross-linked product to a protein sequencer. It was found that the cross-linked sites were mainly at the first and second lysine residues of the lysine-rich sequence when the molar ratio of actin to subfragment 1 was 1:1.(ABSTRACT TRUNCATED AT 250 WORDS)     

Site-specific mutations in the myosin binding sites of actin affect structural transitions that control myosin binding.

We have examined the effects of actin mutations on myosin binding, detected by cosedimentation, and actin structural dynamics, detected by spectroscopic probes. Specific mutations were chosen that have been shown to affect the functional interactions of actin and myosin, two mutations (4Ac and E99A/E100A) in the proposed region of weak binding to myosin and one mutation (I341A) in the proposed region of strong binding. In the absence of nucleotide and salt, S1 bound to both wild-type and mutant actins with high affinity (K(d) < microM), but either ADP or increased ionic strength decreased this affinity. This decrease was more pronounced for actins with mutations that inhibit functional interaction with myosin (E99A/E100A and I341A) than for a mutation that enhances the interaction (4Ac). The mutations E99A/E100A and I341A affected the microsecond time scale dynamics of actin in the absence of myosin, but the 4Ac mutation did not have any effect. The binding of myosin eliminated these effects of mutations on structural dynamics; i.e., the spectroscopic signals from mutant actins bound to S1 were the same as those from wild-type actin. These results indicate that mutations in the myosin binding sites affect structural transitions within actin that control strong myosin binding, without affecting the structural dynamics of the strongly bound actomyosin complex.     

Structural dynamics of actin during active interaction with myosin: different effects of weakly and strongly bound myosin heads

We have used optical spectroscopy (transient phosphorescence anisotropy, TPA, and fluorescence resonance energy transfer, FRET) to detect the effects of weakly bound myosin S1 on actin during the actomyosin ATPase cycle. The changes in actin were reported by (a) a phosphorescent probe (ErIA) attached to Cys 374 and (b) a FRET donor-acceptor pair, IAEDANS attached to Cys 374 and a nucleotide analogue (TNPADP) in the nucleotide-binding cleft. Strong interactions were detected in the absence of ATP, and weak interactions were detected in the presence of ATP or its slowly hydrolyzed analogue ATP-gamma-S, under conditions where a significant fraction of weakly bound acto-S1 complex was present and the rate of nucleotide hydrolysis was low enough to enable steady-state measurements. The results show that actin in the weakly bound complex with S1 assumes a new structural state in which (a) the actin filament has microsecond rotational dynamics intermediate between that of free actin and the strongly bound complex and (b) S1-induced changes are not propagated along the actin filament, in contrast to the highly cooperative changes due to the strongly bound complex. We propose that the transition on the acto-myosin interface from weak to strong binding is accompanied by transitions in the structural dynamics of actin parallel to transitions in the dynamics of interacting myosin heads.     

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.     

Localisation of light chain and actin binding sites on myosin

A gel overlay technique has been used to identify a region of the myosin S-1 heavy chain that binds myosin light chains (regulatory and essential) and actin. The 125I-labelled myosin light chains and actin bound to intact vertebrate skeletal or smooth muscle myosin, S-1 prepared from these myosins and the C-terminal tryptic fragments from them (i.e. the 20-kDa or 24-kDa fragments of skeletal muscle myosin chymotryptic or Mg2+/papain S-1 respectively). MgATP abolished actin binding to myosin and to S-1 but had no effect on binding to the C-terminal tryptic fragments of S-1. The light chains and actin appeared to bind to specific and distinct regions on the S-1 heavy chain, as there was no marked competition in gel overlay experiments in the presence of 50-100 molar excess of unlabelled competing protein. The skeletal muscle C-terminal 24-kDa fragment was isolated from a tryptic digest of Mg2+/papain S-1 by CM-cellulose chromatography, in the presence of 8 M urea. This fragment was characterised by retention of the specific label (1,5-I-AEDANS) on the SH1 thiol residue, by its amino acid composition, and by N-terminal and C-terminal sequence analyses. Electron microscopical examination of this S-1 C-terminal fragment revealed that: it had a strong tendency to form aggregates with itself, appearing as small 'segment-like' structures that formed larger aggregates, and it bound actin, apparently bundling and severing actin filaments. Further digestion of this 24-kDa fragment with Staphylococcus aureus V-8 protease produced a 10-12-kDa peptide, which retained the ability to bind light chains and actin in gel overlay experiments. This 10-12-kDa peptide was derived from the region between the SH1 thiol residue and the C-terminus of S-1. It was further shown that the C-terminal portion, but not the N-terminal portion, of the DTNB regulatory light chain bound this heavy chain region. Although at present nothing can be said about the three-dimensional arrangement of the binding sites for the two kinds of light chain (regulatory and essential) and actin in S-1, it appears that these sites are all located within a length of the S-1 heavy chain of about 100 amino acid residues.     

Functional characterization of the secondary actin binding site of myosin II

The role of the interaction between actin and the secondary actin binding site of myosin (segment 565-579 of rabbit skeletal muscle myosin, referred to as loop 3 in this work) has been studied with proteolytically generated smooth and skeletal muscle myosin subfragment 1 and recombinant Dictyostelium discoideum myosin II motor domain constructs. Carbodiimide-induced cross-linking between filamentous actin and myosin loop 3 took place only with the motor domain of skeletal muscle myosin and not with those of smooth muscle or D. discoideum myosin II. Chimeric constructs of the D. discoideum myosin motor domain containing loop 3 of either human skeletal muscle or nonmuscle myosin were generated. Significant actin cross-linking to the loop 3 region was obtained only with the skeletal muscle chimera both in the rigor and in the weak binding states, i.e., in the absence and in the presence of ATP analogues. Thrombin degradation of the cross-linked products was used to confirm the cross-linking site of myosin loop 3 within the actin segment 1-28. The skeletal muscle and nonmuscle myosin chimera showed a 4-6-fold increase in their actin dissociation constant, due to a significant increase in the rate for actin dissociation (k(-)(A)) with no significant change in the rate for actin binding (k(+A)). The actin-activated ATPase activity was not affected by the substitutions in the chimeric constructs. These results suggest that actin interaction with the secondary actin binding site of myosin is specific for the loop 3 sequence of striated muscle myosin isoforms but is apparently not essential either for the formation of a high affinity actin-myosin interface or for the modulation of actomyosin ATPase activity.     

Unphosphorylated calponin enhances the binding force of unphosphorylated myosin to actin

Background

Smooth muscle has the distinctive ability to maintain force for long periods of time and at low energy costs. While it is generally agreed that this property, called the latch-state, is due to the dephosphorylation of myosin while attached to actin, dephosphorylated-detached myosin can also attach to actin and may contribute to force maintenance. Thus, we investigated the role of calponin in regulating and enhancing the binding force of unphosphorylated tonic muscle myosin to actin.

Methods

To measure the effect of calponin on the binding of unphosphorylated myosin to actin, we used the laser trap assay to quantify the average force of unbinding (F_unb) in the absence and presence of calponin or phosphorylated calponin.

Results

F_unb from F-actin alone (0.12 ± 0.01 pN; mean ± SE) was significantly increased in the presence of calponin (0.20 ± 0.02 pN). This enhancement was lost when calponin was phosphorylated (0.12 ± 0.01 pN). To further verify that this enhancement of F_unb was due to the cross-linking of actin to myosin by calponin, we repeated the measurements at high ionic strength. Indeed, the F_unb obtained at a [KCl] of 25 mM (0.21 ± 0.02 pN; mean ± SE) was significantly decreased at a [KCl] of 150 mM, (0.13 ± 0.01 pN).

Conclusions

This study provides direct molecular level-evidence that calponin enhances the binding force of unphosphorylated myosin to actin by cross-linking them and that this is reversed upon calponin phosphorylation. Thus, calponin might play an important role in the latch-state.

General significance

This study suggests a new mechanism that likely contributes to the latch-state, a fundamental and important property of smooth muscle that remains unresolved.     

Measurement of the fraction of myosin heads bound to actin in rabbit skeletal myofibrils in rigor

Tryptic digestion of rabbit skeletal myofibrils at physiological ionic strength and pH results in cleavage of the myosin heavy chain at one site giving two bands (M_r = 200,000 and 26,000) on sodium dodecyl sulfate/polyacrylamide gels. Following addition of sodium pyrophosphate (to 1 mm) to dissociate the myosin heads from actin, tryptic proteolysis results in production of three bands, 160K², 51K and 26K, with a 74K band appearing as a precursor of the 51K and 26K species. Under these conditions, there is insignificant cleavage of heavy chain to the heavy and light meromyosins. Trypsin-digested myofibrils yield the same amount of rod as native myofibrils when digested with papain. These results indicate that actin blocks tryptic cleavage of the myosin heavy chain at a site 74K from the N terminus. From measurements of the amount of 51K species formed by digestion of rigor fibers at various sarcomere lengths, we estimate that at least 95% of the myosin heads are bound to actin at 100% overlap of thick and thin filaments. Hence all myosin molecules can bind to actin, and consequently both heads of a myosin molecule can interact simultaneously with actin filaments under rigor conditions.