Orientation of spin labels attached to cross-bridges in contracting muscle fibres

Effects of AMPPNP on the orientation and rotational dynamics of spin-labeled muscle cross-bridges

We have used electron paramagnetic resonance (EPR) to investigate the orientation, rotational motion, and actin-binding properties of rabbit psoas muscle cross-bridges in the presence of the nonhydrolyzable nucleotide analogue, 5'-adenylylimido-diphosphate (AMPPNP). This analogue is known to decrease muscle tension without affecting its stiffness, suggesting an attached cross-bridge state different from rigor. We spin-labeled the SH1 groups on myosin heads and performed conventional EPR to obtain high-resolution information about the orientational distribution, and saturation transfer EPR to measure microsecond rotational motion. At 4 degrees C and 100 mM ionic strength, we find that AMPPNP increases both the orientational disorder and the microsecond rotational motion of myosin heads. However, computer analysis of digitized spectra shows that no new population of probes is observed that does not match either rigor or relaxation in both orientation and motion. At 4 degrees C, under nearly saturating conditions of 16 mM AMPPNP (Kd = 3.0 mM, determined from competition between AMPPNP and an ADP spin label), 47.5 +/- 2.5% of myosin heads are dynamically disoriented (as in relaxation) without a significant decrease in rigor stiffness, whereas the remainder are rigidly oriented as in rigor. The oriented heads correspond to actin-attached heads in a ternary complex, and the disoriented heads correspond to detached heads, as indicated by EPR experiments with spin-labeled subfragment 1 (S1) that provide independent measurements of orientation and binding. We take these findings as evidence for a single-headed cross-bridge that is as stiff as the double-headed rigor cross-bridge. The data are consistent with a model in which, in the presence of saturating AMPPNP, one head of each cross-bridge binds actin about 10 times more weakly, whereas the remaining head binds at least 10 times more strongly, than extrinsic S1. Thus, although there is no evidence for heads being attached at nonrigor angles, the attached cross-bridge differs from that of rigor. The heterogeneous behavior of heads is probably due to steric effects of the filament lattice.

Energetics of the actomyosin bond in the filament array of muscle fibers

The interaction between actin and myosin in the filament array of glycerinated muscle fibers has been monitored using paramagnetic probes and mechanical measurements. Both fiber stiffness and the spectra of probes bound to a reactive sulfydral on the myosin head were measured as the actomyosin bond was weakened by addition of magnesium pyrophosphate (MgPPi) and glycerol. In the absence of MgPPi, all myosin heads are attached to actin with oriented probes. When fibers were incubated in buffers containing MgPPi, a fraction of the probes became disordered, and this effect was greater in the presence of glycerol. To determine whether the heads with disordered probes were detached from actin, spin-labeled myosin subfragment-1 (MSL-S1) was diffused into unlabeled fibers, and the fractions bound to actin and free in the medium were correlated with the oriented and disordered spectral components. These experiments showed that the label was oriented when MSL-S1 was attached to actin in a ternary complex with the ligand and that all heads with disordered probes were detached from actin. Thus the fraction of oriented labels could be used to determine the fraction of heads attached to actin in a fiber in the presence of ligand. The fraction of myosin heads attached to actin decreased with increasing [MgPPi], and in the absence of glycerol approximately 50% of the myosin heads were dissociated at 3.3 mM ligand with little change in fiber stiffness. In the presence of 37% glycerol plus ligand, up to 80% of the heads could be detached with a 50% decrease in fiber stiffness. The data indicate that there are two populations of myosin heads in the fiber. All the data could be fit with a model in which one population of myosin heads (comprising approximately 50% of the total) sees an apparent actin concentration of 0.1 mM and can be released from actin with little change in fiber stiffness. A second population of myosin heads (approximately 50%) sees a higher actin concentration (5 mM) and is only released in the presence of both glycerol and ligand.

Ionic effects on the rotational dynamics of cross-bridges in myosin filaments, measured by triplet absorption anisotropy

We have measured the rotational motion of myosin heads in synthetic thick filaments at 4 degrees C in the time range from 10(-7) to 10(-4) seconds, by measuring transient absorption anisotropy of an eosin probe attached to a reactive sulfhydryl on the myosin head. Under conditions that result in monomeric myosin (500 mM ionic strength), the anisotropy decay is independent of pH in the range from 7.0 to 8.2 and [Mg2+] in the range from 0.1 to 10 mM; the anisotropy decays bi-exponentially with correlation times of 0.4 and 2 microseconds to a constant value of 0.016. Under more physiological conditions (115 mM ionic strength), resulting in filament formation, the anisotropy decay is sensitive to both pH and [Mg2+]. The anisotropy at pH 8.2 and 0.1 mM-Mg2+ decays with correlation times of 0.5 and 3.8 microseconds to a constant limiting anisotropy of 0.038. When the [Mg2+] is increased to 10 mM, the correlation times are 0.6 and 5.7 microseconds and the limiting anisotropy value is 0.055. Identical changes in the anisotropy decay are caused by an increase in [H+] to pH 7.0, in the presence of 0.1 mM-Mg2+. Increasing the total ionic strength to 187 mM decreases the amplitude of the cation effects. These results provide direct evidence that the rotational dynamics of myosin heads in thick filaments are influenced by physiological concentrations of cations. The results are qualitatively consistent with the proposal that these and other ionic conditions regulate transitions between "spread" and "compact" cross-bridge conformations, but the quantitative results indicate that cross-bridges undergo large-amplitude microsecond rotations even under conditions where the compact state should predominate.

Influence of Mg2+ and Ca2+ bound to 1,5-IAEDANS-labeled phosphorylated and dephosphorylated heavy meromyosin complexed with F-actin on polarized fluorescence of the fluorophore

Dephosphorylated and phosphorylated heavy meromyosin, fluorescently labeled with 1,5-IAEDANS attached at the SH1 group, was introduced into myosin-free ghost fibres and the polarized fluorescence of the bound label was measured. The results depended on whether the divalent cation binding sites on heavy meromyosin were saturated with Mg2+ or Ca2+. The calculated angles of absorption and emission dipoles and the amount of random fluorophores were significantly changed, indicating that the random mobility and orientation of the fluorophores of phosphorylated and dephosphorylated heavy meromyosin heads complexed with F-actin in the ghost fibre depend on saturation of heavy meromyosin with Ca2+ or Mg2+. The presence of bound Ca2+ has an opposite effect on the polarized fluorescence of phosphorylated and dephosphorylated 1,5-IAEDANS-heavy meromyosin.

Effect of ATP depletion on the isolated thick filament of limulus striated muscle

With the dynamic light scattering method, we have shown that calcium ions increase the high-frequency internal motions of isolated thick filaments of Limulus striated muscle in the presence of ATP (Kubota, K., B. Chu, Shih-fang Fan, M.M. Dewey, P. Brink, and D. Colflesh. J. Mol. Biol. 1983. 166:329 and Fan, S.-f., M.M. Dewey, D. Colflesh, B. Gaylinn, R. Greguski, and B. Chu. Biophys. J. 1985. 47:809). If ATP is removed from the suspending medium, an increase of high-frequency internal motions also has been observed with characteristics different from those of filaments suspended in a medium containing ATP and calcium ions. These internal motions appear whether calcium ions are present or not and are suppressed by trifluoperazine (TFP). The motions differ from the calcium ion-induced motions in that (a) an energy supply is not required; (b) they are insensitive to heat treatment (42 degrees C, 10 min) and (c) they are also insensitive to phenylmethylsulfonyl fluoride which blocks the motions in the presence of ATP and calcium ions (Fan, Shih-fang, M.M. Dewey, D. Colflesh, B. Gaylinn, R. Greguski, and B. Chu. 1985. Biochim. Biophys. Acta. 827:101). Electron micrographs of negatively stained thick filaments in an ATP-free medium show that the majority of crossbridges extend out from the backbone of the filament and optical diffraction patterns from these filaments lack layer lines arising from the crossbridges. The flexibility of the thick filaments suspended in ATP-free media increases.

Location of the ATPase site of myosin determined by three-dimensional electron microscopy

Both ATP hydrolysis by myosin and the accompanying cyclic association-dissociation of actin and myosin are essential for muscle contraction. It is important for understanding the molecular mechanism of contraction to know the three-dimensional locations of the two major functional sites of myosin: the ATPase site and the actin-binding site. We have determined the position of the ATPase site of myosin using three-dimensional image reconstruction from electron micrographs and site-specific labelling with the avidin-biotin system. The ATPase site is about 5 nm from the tip of the myosin head and is about 4 nm away from the actin-binding site of myosin. This is the first report of the three-dimensional location of an enzyme active site by electron microscopy.

Conformational changes of F-actin in myosin-free ghost single fibre induced by either phosphorylated or dephosphorylated heavy meromyosin

The changes in F-actin conformation of myosin-free single ghost fibre induced by binding of phosphorylated or dephosphorylated heavy meromyosin have been studied by measuring polarized fluorescence of F-actin intrinsic tryptophan and of phalloidin-rhodamine bound to F-actin. The changes of polarization of both fluorescences were found to be dependent on low or high Ca2+ concentration and on the phosphorylated or dephosphorylated form of heavy meromyosin. Computer analysis of polarized fluorescence has shown that binding of phosphorylated heavy meromyosin with divalent ion binding sites saturated with Mg2 (in the presence of 1 mM MgCl2 and 1 mM EGTA) and dephosphorylated heavy meromyosin with divalent ion binding sites saturated with Ca2+ (in the presence of 1 mM MgCl2 and 0.1 mM Ca2+) decreases the angles of emission and absorption dipoles and the angle between the F-actin axis and the fibre axis, thus suggesting that F-actin in ghost fibre becomes more flexible. On the other hand, the above-mentioned angles increase when phosphorylated heavy meromyosin at high and dephosphorylated heavy meromyosin at low Ca2+ concentration were bound to thin filaments, thus showing the decrease of F-actin flexibility under these conditions.

X-ray study of myosin heads in contracting frog skeletal muscle

Using synchrotron radiation, the behaviour of the diffuse X-ray scatter was investigated in the relaxed and active phases of auxotonic and isometric contractions. Muscles were stimulated tetanically for 0.75 of a second, leaving intervals of three minutes between successive contractions. In isometric contractions the scatter is very asymmetric, which means that the myosin heads have a strongly preferred orientation. During tension rise the scatter expands in the meridional direction and contracts in the equatorial direction, the maximal local intensity change being about 20%. The shape change indicates that on average the myosin heads become oriented more perpendicularly to the fibre axis. The distribution of orientations at peak tension is quite different from that we found previously in X-ray scattering data from rigor muscles. In auxotonic contractions where muscles shorten against an increasing tension the scatter is practically circularly symmetrical. This suggests that during shortening the myosin heads go evenly through a wide range of orientations. It is concluded that the results from both the auxotonic and isometric experiments provide strong support for the rotating myosin head model. In isometric contractions the transition between the relaxed phase and peak tension is accompanied by an overall increase in scattering intensity of about 10%: this corresponds to a relative increase in the fraction of disordered myosin heads by almost 30%.

Fluorescence resonance energy transfer measurements of distances in actin and myosin. A critical evaluation

The contractile proteins actin and myosin are of considerable biological interest. They are essential for muscle contraction and in eukaryotic cells they play a crucial role in most contractile phenomena. Over the years since the first fluorescence resonance energy transfer (FRET) paper appeared, an extensive body of literature has accumulated on this technique using actin, myosin and the actomyosin complex. These papers are reviewed with several aims in mind: we assess the reliability and consistency of intra- and inter-molecular distances measured between the fluorescent probes attached to specific sites on these proteins; we determine whether the measurements can be assembled into an internally consistent model which can be fitted to the known dimensions of the actomyosin complex; several of the FRET distances are consistent with the available structural data from crystallographic and electron microscopic dimensions; the modelled FRET distances suggest that the assumed value of the orientation factor (k2 = 2/3) is reasonable; we conclude that the model has a predictive value, i.e. it suggests that a small number of the published dimensions may be incorrect and predicts the magnitude of a larger number of measurements which have not yet been reported; and finally (vi) we discuss the contribution of FRET determinations to the current debate on the molecular mechanism of contraction.

Movement of myosin fragments in vitro: domains involved in force production

We have used the Nitella-based movement assay to localize the site of force production in myosin. Methods were developed to use nonfilamentous myosin or proteolytic fragments of myosin in place of the thick filaments used in the original assay. In the experiments described here, the tail of myosin or its subfragments is anchored via antibodies to the surface of small particles. Nonfilamentous myosin or its subfragments move along Nitella actin cables at speeds similar to those obtained with filamentous myosin. We generated short HMM, a myosin fragment containing the heads and only 400 A of the tail. Although short HMM lacks the "hinge" region proposed by Harrington to be the site of force generation, and is incapable of forming thick filaments, it moves along actin at speeds above 1 micron/sec. Therefore, neither a thick filament nor the carboxy-terminal 1100 A of the tail is required for movement along actin. The results indicate that force production occurs in or near the myosin heads.

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.

Observation of two orientations from rigor cross-bridges in glycerinated muscle fibers

The fluorescence polarization from rhodamine labels specifically attached to the fast-reacting thiol of the myosin cross-bridge in glycerinated muscle fibers has been measured to determine the angular distribution of the cross-bridges in different physiological states of the fibers as a function of temperature. To investigate the fibers at temperatures below 0 degree C, we have added glycerol to the bathing solution as an anti-freezing agent. We find that the fluorescence polarization from the rhodamine probe detects distinct angular distributions of the cross-bridges in isometric-active, rigor, MgADP, and low ionic strength relaxed fibers at 4 degrees C. We also find that the rigor cross-bridges in the presence of glycerol can maintain at least two distinct orientations relative to the actin filament, one dominant at temperatures T greater than 2 degrees C and another dominant at T less than -10 degrees C. MgADP cross-bridges in the presence of glycerol maintain approximately the same orientation for all temperatures investigated. The rigor cross-bridge orientation at T less than -10 degrees C is similar to both the MgADP cross-bridge orientation in the presence of glycerol and the active muscle cross-bridge orientation at 4 degrees C. These findings show that the rigor cross-bridge in the presence of glycerol has at least two distinct orientations while attached to actin: one of them dominant at high temperature, the other dominant at low temperature or when MgADP is present. The latter orientation resembles that present in isometric-active fibers.(ABSTRACT TRUNCATED AT 250 WORDS)

The role of tropomyosin-troponin in the regulation of skeletal muscle contraction

Steric blocking of actin-myosin interaction by tropomyosin has been a working hypothesis in the study of the regulation of skeletal muscle contraction, yet the simple movement of actin-associated tropomyosin from a myosin-blocking position (relaxation) to a nonblocking position (contraction) cannot adequately account for all of the biophysical and biochemical observations which have been made to date. Ambiguous assignment of tropomyosin positions on actin during contraction, due in part to the limited resolution of reconstruction techniques, may also hint at a real lack of clearcut 'on' and 'off' positioning of tropomyosin and tropomyosin-troponin complex. Recent biochemical evidence suggests processes relatively independent of tropomyosin-troponin may have a governing effect on contraction, involving kinetic constraints on actin-myosin interaction influenced by the binding of ATP and the intermediates of ATP hydrolysis. Based on our current understanding put forth in this review, it is clear that regulatory interactions in muscle contraction do not consist solely of steric effects but involve kinetic factors as well. Where the latter are being defined in systems reconstituted from purified proteins and their fragments, the steric components of regulation are most clearly observed in studies of structurally more intact physiologic systems (e.g. intact or skinned whole muscle fibres). The fine detail of the processes and their interplay remains an intriguing question. Likewise, the precise physical relationship of myosin with actin in the crossbridge cycle continues to elude definition. Refinement of several methodologies (X-ray crystallography, three-dimensional reconstruction, time-resolved X-ray diffraction) will increase the potential for detailing the molecular basis of the regulation of muscle contraction.

Structure of the actin-myosin complex produced by crosslinking in the presence of ATP

The structure of the actin-myosin complex during ATP hydrolysis was studied by covalently crosslinking myosin subfragment 1 (S1) to F-actin in the presence of nucleotides (especially ATP) using 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide. The fluorescence energy transfer was measured between N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine and 6-(iodoacetamide)fluorescein bound to the SH1 thiol of S1 and the Cys374 thiol of actin. The covalent acto-S1, produced by crosslinking in the absence of nucleotide or in the presence of ADP, showed transfer efficiency of 0.50 to 0.52 and intersite distance of 4.5 to 4.7 nm, which were equal to those obtained with non-crosslinked acto-S1 in the absence of nucleotide. However, the covalent acto-S1, produced by crosslinking in the presence of either 5'-adenylyl imidodiphosphate (AMPPNP) at high ionic strength or ATP, showed a significant decrease in the efficiency to 0.26 to 0.34 and hence an increase in the distance to 5.2 to 5.5 nm. These results suggest that AM-ATP and/or AM-ADP-P (formed during ATP hydrolysis) and AM-AMPPNP have a very different conformation from AM and AM-ADP (in which A is actin and M is myosin).

Local melting in the subfragment-2 region of myosin in activated muscle and its correlation with contractile force

Local melting within the subfragment-2 region of activated rabbit skeletal glycerinated muscle fibers has been investigated over the temperature range 5 to 37 degrees C, using an enzyme (chymotrypsin)-probe method. The cleavage rates were determined from the time-course of formation of digestion products by electrophoresis on sodium dodecyl sulfate-containing polyacrylamide gels. We found the cleavage sites to be localized in a restricted region Mr = 64,000 to 90,000/polypeptide chain, measured from the C terminus of the myosin rod (the subfragment-2 hinge domain). The cleavage rate constant for activated muscle fibers in the presence of an ATP-regenerating system was about 100 times larger at each temperature than that for rigor or for relaxed muscle fibers and showed a marked increase in magnitude with increasing temperature. Comparative plots of the apparent rate-constant for cleavage within the subfragment-2 hinge domain and the isometric force generated by active fibers versus MgATP concentration gave closely similar profiles suggesting a strong positive correlation. Thus, there appears to be a close coupling between the conformational transition within the subfragment-2 hinge domain and contractile force when the cross-bridges undergo cycling.

Actin-attached and detached crossbridges in myofibrils: segregation into two populations according to their sensitivity to proteolytic digestion of myosin heavy chain

Tryptic digestion of myofibrils was used to assess the interaction of crossbridges with thin filaments in the presence of ATP analogues. The relative amounts of 200 kDa fragment produced by trypsin from myosin heavy chain when the crossbridge is attached to actin, and of 160 kDa fragment produced when the crossbridge is detached from actin, served as a measure of crossbridge-actin interaction. In rigor only the 200 kDa fragment was produced suggesting that a great majority of the crossbridges were strongly attached to actin; in the presence of MgPPi at 0 degrees C only the 160 kDa fragment was finally produced suggesting that eventually all crossbridges detached from actin. In the presence of MgPPi or MgAMPPNP at 25 degrees C both 200 and 160 kDa fragments were present for several minutes after myosin heavy chain had been completely digested, suggesting that two populations of crossbridges (attached and detached) co-existed at the same time within the myofibril. It is concluded that the addition of ATP analogues to muscle does not simply affect the chemical equilibrium of binding of myosin heads to actin but that it causes rapid dissociation of one crossbridge population without significant effect on binding to actin of the remaining crossbridge population.

Saturation transfer electron paramagnetic resonance study of the mobility of myosin heads in myofibrils under conditions of partial dissociation

The rotational motion of rigidly spin-labeled myosin heads of glycerinated myofibrils as reflected in saturation-transfer EPR spectra behaves to a first approximation as though the heads consist of two populations with different rotational motions. An immobilized fraction has a correlation time (tau 2) of approximately 0.5 ms, comparable to that of spin-labeled subfragment-1 (S1) bound to thin filaments, while a mobile fraction has a tau 2 of 10 microseconds, comparable to that of the heads of purified myosin filaments. The effects of nonhydrolyzable ATP analogues, potassium pyrophosphate (PPi), or adenylyl imidodiphosphate, Ca2+, temperature, or ionic strength on the spectra can be analyzed in terms of the fraction of myosin heads immobilized by attachment to thin filaments, without requiring changes in the motion of either attached or detached heads.

The mechanism of muscle contraction

Knowledge of the mechanism of contraction has been obtained from studies of the interaction of actin and myosin in solution, from an elucidation of the structure of muscle fibers, and from measurements of the mechanics and energetics of fiber contraction. Many of the states and the transition rates between them have been established for the hydrolysis of ATP by actin and myosin subfragments in solution. A major goal is to now understand how the kinetics of this interaction are altered when it occurs in the organized array of the myofibril. Early work on the structure of muscle suggested that changes in the orientation of myosin cross-bridges were responsible for the generation of force. More recently, fluorescent and paramagnetic probes attached to the cross-bridges have suggested that at least some domains of the cross-bridges do not change orientation during force generation. A number of properties of active cross-bridges have been defined by measurements of steady state contractions of fibers and by the transients which follow step changes in fiber length or tension. Taken together these studies have provided firm evidence that force is generated by a cyclic interaction in which a myosin cross-bridge attaches to actin, exerts force through a "powerstroke" of 12 nm, and is then released by the binding of ATP. The mechanism of this interaction at the molecular level remains unknown.

Fraction of myosin cross-bridges bound to actin in active muscle fibers: estimation by fluorescence anisotropy measurements

Time-resolved and steady-state fluorescence anisotropy measurements from fluorescence-labeled myosin cross-bridges in single glycerinated skeletal muscle fibers in rigor, relaxed, MgADP-induced, and contracting states have been made in order to estimate the fraction of actin-bound cross-bridges in active muscle. When the plane of polarization of the excitation light is perpendicular to the fiber axis and its propagation vector has a component parallel to this axis, actin-bound cross-bridge states, such as rigor and MgADP-induced, have time-zero and steady-state anisotropies that are substantially lower than has the relaxed state. This difference provides a means of determining the fraction of cross-bridges bound to actin in active isometric fibers, by comparing the fluorescence anisotropy from active fibers with the anisotropy from bound and unbound cross-bridges in static states. By assuming that the active cross-bridges are either bound (in the manner of rigor or MgADP-induced states) or relaxed, we estimate that greater than 80% of the cross-bridges are actin-bound in active isometric fibers.

Critical dependence of calcium-activated force on width in highly compressed skinned fibers of the frog

Force development by skinned frog semitendinosus fibers was studied at various levels of lateral compression to compare the results with intact fibers and to evaluate the limits on cross-bridge movements during isometric contraction. The skinned fibers were compressed osmotically using a high molecular weight polymer, dextran T500. Ca-activated force remained constant down to 58% of the fiber width (w0) after skinning, corresponding to a nearly twofold change in separation between the thin and thick filaments in the myofilament lattice. This agrees with the earlier result on intact fibers, and gives additional evidence that the cross-bridge mechanism for force generation is relatively insensitive to large changes in interfilament separation. Further compression, below 0.58 w0, produced a sharp drop in force, and the force was practically zero at a fiber width of 50%. The effect at high compression was the same at all pCa's, which indicates that the Ca sensitivity of the myofilaments is unaffected by radial compression. The stiffness of the fiber remained high in rigor in the presence of dextran, which indicates that the rigor cross-bridge attachment is not inhibited, and actually may be improved, with decreases in the interfilament space. Also, the drop in active force with the highest compression was similar when the compressed fibers were put in rigor before contraction, which suggests that the force drop also was not due to a hindrance to cross-bridge attachment. The results appear to exclude large motions such as tilting and rocking of the bridge as a rigid molecule, but suggest that at least some molecular movement is essential for force development; they also raise the possibility that there is a critical interfilament separation in the fiber, below which the cross-bridge cannot function.

Model-independent electron spin resonance for measuring order of immobile components in a biological assembly

A model-independent description of the angular orientation distribution of elements in an ordered biological assembly is applied to the electron spin resonance (ESR) technique. As in a previous model-independent treatment of fluorescence polarization (Burghardt, T.P., 1984, Biopolymers, 23:2383-2406) the elemental order is described by an angular distribution of molecular frames with one frame fixed in each element of the assembly. The distribution is expanded in a complete orthonormal set of functions. The coefficients of the series expansion (the order parameters) describe the orientation distribution of the elements in the assembly without reference to a model and can be obtained from the observed spectrum. The method establishes the limitations of ESR in detecting order in the assembly by determining which distribution coefficients the technique can detect. A method of determining the order parameters from an ESR spectra, using a set of ESR basis spectra, is developed. We also describe a treatment that incorporates the actual line shape measured from randomly oriented, immobile elements. In this treatment, no model-dependent assumptions about the line shape are required. We have applied the model-independent analysis to ESR spectra from spin-labeled myosin cross-bridges in muscle fibers. The results contain detailed information on the spin-probe angular distribution and differ in interesting ways from previous model-dependent interpretations of the spectra.

Resonance energy transfer evidence for two attached states of the actomyosin complex

Resonance energy transfer measurements were made between a donor fluorophore, N-(bromacetyl)-N'-(1-sulpho-5-naphthyl)ethylenediamine, located on the single cysteine of the Al light chain of myosin (S1(A1), and an acceptor fluorophore, 5-(iodoacetamido)fluorescein, sited on Cys-374 of actin. In the binary rigor complex a transfer efficiency of 24% was noted, representing a spatial separation of about 6 nm. When the same measurements were made using a stable analogue of S1 X ATP, in which the fast reacting SH1 thiol group is crosslinked to another thiol group in the 20 kDa domain of S1, the 2 fluorophores were found to have moved closer together by greater than or equal to 3 nm. This provides, for the first time, direct experimental evidence for a change in structure of the myosin crossbridge that could account for tension generation.

The active cross-bridge motions of isolated thick filaments from myosin-regulated muscles detected by quasi-elastic light scattering

Intensity fluctuation spectroscopy has been used successfully as a probe that can detect an increase in high-frequency internal motions of isolated thick filaments of Limulus muscle upon the addition of calcium ions. We have attributed such motions to cross-bridge motion instead of to an increase in the flexibility of the filament backbone. Here we show that after cleavage of the S-1 and then the S-2 moieties with papain, cross-linking the myosin heads to the filament backbone, or heat denaturation (42 degrees C, 10 min), the increase in the high frequency internal motions in the thick filaments no longer occurs. Congo Red, which has been shown to induce shortening of isolated myofibrils, also increases the high-frequency motions of the isolated filaments. Furthermore, the increase is suppressed by treating the filaments with a myosin ATPase inhibitor such as vanadate ions (10 mM) or by replacing ATP with either an equimolar CrADP or the nonhydrolyzable ATP analogue beta, gamma-imido-adenine-5'-triphosphate (AMP-PNP). Calcium ions have a similar effect on isolated thick filaments from scallop muscle, where the myosin is known to be regulatory. Calcium ions have no such effect on thick filaments isolated from frog muscle, which is believed not to be regulated by calcium binding to myosin. These results confirm our earlier supposition that the additional high frequency internal motions of the thick filaments isolated from striated muscle of Limulus are related to the energy dependent, active cross-bridge motions.

On the mechanism of muscular contraction

A thermodynamic analysis is presented for the energy conversion by muscle contraction. During the cyclic processes the major change in energy of the myosin-actin system is due to bond formation between myosin heads and actin. To account for the high efficiency of a working muscle the work done is connected directly to the formation of myosin-actin bond. It is suggested that successively stronger bonds are formed by a stepwise movement of myosin heads over an interval between two troponin molecules on the actin filament. At the end of the interval, where the bond has maximum strength, energy is supplied to break the bond. Here the work is not primarily connected to the 45 degrees rotation of myosin heads as is commonly done. A way of separating the different kinds of energy losses is presented.

The rate of MgADP binding to and dissociation from acto-S1

The rate of binding and dissociation of MgADP from its ternary complex with actin and S1 was measured by following the extent to which fixed concentrations of MgADP slow down MgATP-induced dissociation of acto-S1. The solution of the equations describing this process shows that at any MgADP concentration the apparent rate of acto-S1 dissociation should be proportional to a square root of the equilibrium constant for MgADP dissociation and to MgATP concentration. By measuring the apparent rate of acto-S1 dissociation as a function of MgATP concentration, the rate of MgADP binding and dissociation were determined as 5 X 10(6) M-1 X s-1 and 1400 s-1, respectively. These rates were unchanged by modification of SH1 thiol of S1 by a variety of fluorescence and spin-labels, but dissociation rate was drastically reduced when SH1 was labelled with 5-iodoacetamidofluorescein.

Crossbridge behaviour during muscle contraction

A number of recent observations by probe and X-ray methods on the behaviour of crossbridges during contraction is considered in relation to the energetics of the process. It is shown that a self-consistent picture of the crossbridge cycle, compatible with these observations and involving strongly and weakly attached crossbridges, can be obtained providing that the tension-generating part of the crossbridge stroke is only about 40 A i.e. about one-third of the usually accepted value. The myosin head subunits in the tension-generating bridges could have a configuration close to that of rigor. A mechanism is suggested whereby rapid tension recovery after quick releases up to 120 A could still be produced by such a system.

Angle of active site of myosin heads in contracting muscle during sudden length changes

The change in orientation of myosin crossbridges in contracting muscle during sudden length changes was examined by fluorescence polarization. This study used a fluorescent ATP analogue, 1,N6-etheno-2-aza-ATP(epsilon-2-aza-ATP) as a probe. Its fluorescence is considerably enhanced upon binding with myosin and is dependent on the chemical state of the myosin-nucleotide complex in muscle. The results showed that nucleotides bound to crossbridges in the intermediate attached state (presumably AM-epsilon-2-aza-ADP-Pi) during isometric contraction are highly oriented at the same angle as that of AM in rigor with bound epsilon-2-aza-ADP. Furthermore the orientation of nucleotides bound to crossbridges in the attached state is not altered during sudden changes in length of isometrically contracting muscle. The results of this time-resolved measurement support the conclusion obtained from a previous steady-state experiment that change in axial orientation of the active site of the myosin head is not involved in force generation.

Microsecond rotational motions of eosin-labeled myosin measured by time-resolved anisotropy of absorption and phosphorescence

We have studied submicrosecond and microsecond rotational motions within the contractile protein myosin by observing the time-resolved anisotropy of both absorption and emission from the long-lived triplet state of eosin-5-iodoacetamide covalently bound to a specific site on the myosin head. These results, reporting anisotropy data up to 50 microseconds after excitation, extend by two orders of magnitude the time range of data on time-resolved site-specific probe motion in myosin. Optical and enzymatic analyses of the labeled myosin and its chymotryptic digests show that more than 95% of the probe is specifically attached to sulfhydryl-1 (SH1) on the myosin head. In a solution of labeled subfragment-1 (S-1) at 4 degrees C, absorption anisotropy at 0.1 microseconds after a laser pulse is about 0.27. This anisotropy decays exponentially with a rotational correlation time of 210 ns, in good agreement with the theoretical prediction for end-over-end tumbling of S-1, and with times determined previously by fluorescence and electron paramagnetic resonance. In aqueous glycerol solutions, this correlation time is proportional to viscosity/temperature in the microsecond time range. Furthermore, binding to actin greatly restricts probe motion. Thus the bound eosin is a reliable probe of myosin-head rotational motion in the submicrosecond and microsecond time ranges. Our submicrosecond data for myosin monomers (correlation time 400 ns) also agree with previous results using other techniques, but we also detect a previously unresolvable slower decay component (correlation time 2.6 microseconds), indicating that the faster motions are restricted in amplitude. This restriction is not consistent with the commonly accepted free-swivel model of S-1 attachment in myosin. In synthetic thick filaments of myosin, both fast (700 ns) and slow (5 microseconds) components of anisotropy decay are observed. In contrast to the data for monomers, the anisotropy of filaments has a substantial residual component (26% of the initial anisotropy) that does not decay to zero even at times as long as 50 microseconds, implying significant restriction in overall rotational amplitude. This result is consistent with motion restricted to a cone half-angle of about 50 degrees. The combined results are consistent with a model in which myosin has two principal sites of segmental flexibility, one giving rise to submicrosecond motions (possibly corresponding to the junction between S-1 and S-2) and the other giving rise to microsecond motions (possibly corresponding to the junction between S-2 and light meromyosin).(ABSTRACT TRUNCATED AT 400 WORDS)

Saturation transfer electron paramagnetic resonance of spin-labeled muscle fibers. Dependence of myosin head rotational motion on sarcomere length

We have investigated the orientation and rotational mobility of spin-labeled myosin heads in muscle fibers as a function of the sarcomere length in the absence of ATP. An iodoacetamide spin label was used to label selectively two-thirds of the sulfhydryl-1 groups in glycerinated rabbit psoas muscle. Conventional electron paramagnetic resonance experiments were used to determine the orientation distribution of the probes relative to the fiber axis, and saturation transfer experiments were used to detect sub-millisecond rotational motion. When fibers are at sarcomere length 2.3 microns (full overlap), spin-labeled heads have a high degree of orientational order. The probes are in a single, narrow orientation distribution (full width 15 degrees), and they exhibit no detectable sub-millisecond rotational motion. When fibers are stretched (sarcomere length increased), either before or after labeling, disorder and microsecond mobility increase greatly, in proportion to the fraction of myosin heads that are no longer in the overlap zone between the thick and thin filaments. Saturation transfer difference spectra show that a fraction of myosin heads equal to the fraction outside the overlap zone have much more rotational mobility than those in fibers at full overlap, and almost as much as in synthetic myosin filaments. The most likely interpretation is that some of the probes, corresponding approximately to the fraction of heads in the overlap zone, remain oriented and immobile, while the rest are highly disordered (angular spread greater than 90 degrees) and mobile (microsecond rotational motion). Thus, it appears that myosin heads are rigidly immobilized by actin, but they rotate through large angles on the microsecond time-scale when detached from actin, even in the absence of ATP.

Initiation of active contraction by photogeneration of adenosine-5'-triphosphate in rabbit psoas muscle fibres

Mechanical and biochemical descriptions of the muscle cross-bridge cycle have been correlated. Skinned muscle fibres of rabbit psoas muscle in rigor were incubated in solutions containing approximately equal to 30 microM-Ca2+ ions and P3-1-(2-nitro)phenylethyladenosine-5'-triphosphate, 'caged ATP', an inert photolabile precursor of ATP. ATP was liberated from caged ATP within the fibres by pulses of 347 nm radiation from a frequency-doubled ruby laser. The mechanical responses of muscle fibres to the rapid increase of ATP concentration were monitored. Tension dropped briefly and then rose above the rigor value to the level characteristic of a steady active contraction. Liberation of ATP decreased in-phase stiffness (measured at 500 Hz) from the rigor level to a maintained value intermediate between rigor and relaxed values. Out-of-phase stiffness increased to a maintained level indicating a phase lead of tension with respect to imposed length oscillations. Rigor tension was varied prior to photolysis by slight alterations of fibre length. Tension traces starting at different rigor tensions converged to a common tension level at the same rate, whether or not Ca2+ was included in the medium. These data suggest that the rate of cross-bridge detachment by ATP from the rigor state is not influenced by Ca2+. Analysis of the tension records, in terms of sequential detachment and reattachment reactions, provided a measure of cross-bridge reattachment rate and an alternate measure of the detachment rate. Detachment from the rigor state was approximately proportional to the ATP concentration, with a second-order rate constant of at least 5 X 10(5) M-1 S-1. Reattachment with force generation had no detectable dependence on the concentration of ATP liberated by photolysis. A simple kinetic model of the cross-bridge cycle in terms of chemically defined intermediates was compatible with most of the experimental data. The ATP dependence of cross-bridge detachment, the kinetics of maintained cross-bridge reattachment in the presence of Ca2+, and transient reattachment and final relaxation in the absence of Ca2+ were explained. In this model, reversibility of cross-bridge attachment and the steps leading to force production allow the relatively high observed detachment rate to be accommodated with other data relating to active contraction. These data include the steady ATPase rate of active muscle fibres and the fewer attached cross-bridges in active contractions compared to rigor.

Predominant attached state of myosin cross-bridges during contraction and relaxation at low ionic strength

The chemical states of a cross-bridge--nucleotide complex were studied using a fluorescent ATP analogue, 1-N6-etheno-2-aza-ATP(epsilon-2-aza-ATP). The fluorescence of epsilon-2-aza-ATP at specific emission wavelengths was enhanced by 12.5 times upon binding to myosin in a relaxed muscle and the fluorescence from the resultant myosin(M)-epsilon-2-aza-ADP-Pi intermediate was 2.5 times greater than that from a M-epsilon-2-aza-ADP complex. Similar enhancements of the fluorescence of epsilon-2-aza-ATP and epsilon-2-aza-ADP were observed upon binding to heavy meromyosin in solution. Binding of F-actin did not change the fluorescence of epsilon-2-aza-ATP or epsilon-2-aza-ADP bound to heavy meromyosin. When a muscle went from a relaxed state to a state of isometric contraction or contraction with shortening, the fluorescence intensity decreased only slightly or not at all, i.e. the fluorescence of nucleotides bound to most of the myosin heads during contraction is the same as that of the M-epsilon-2-aza-ADP-Pi intermediate. These results suggest that an actomyosin(AM)-epsilon-2-aza-ADP-Pi intermediate is the predominant attached state during contraction. When the ionic strength of the relaxing solution was decreased, cross-bridges formed at 6 degrees C without tension generation. At 20 degrees C, a large tension was produced although the shortening velocity was negligibly small or zero. The fluorescence intensity decreased by 15% at 20 degrees C but only a small decrease of 3% was observed at 6 degrees C, suggesting that the predominant complexes in the attached state were AM-epsilon-2-aza-ATP and/or AM-2-aza-ADP-Pi at 6 degrees C and AM-epsilon-2-aza-ADP at 20 degrees C. Thus, the identification of the actomyosin-nucleotide complexes existing before and after the force-generating step lent further support to the conclusion that the sliding force is generated by conformational changes in actomyosin when the (epsilon-2-aza-)ADP-Pi complex is bound to it.

Fluorescence energy transfer between probes on actin and probes on myosin

The structural relationship between F-actin filaments and the biologically active fragments of myosin (either as myosin subfragment-1 or heavy meromyosin) has been investigated using the technique of fluorescence energy transfer. Donor and acceptor probes were used to obtain the following inter- and intramolecular distances. Energy transfer was measured: (1) from the SH1 groups of the myosin 'heads' to the nucleotide sites of F-actin (in the absence of free nucleotide); (2) from the SH1 groups of myosin to multiple probes on the surface of the actin filament; (3) from the nucleotide-binding sites of F-actin to the ATPase sites of myosin; (4) from the ATPase sites of myosin to the nucleotide-binding sites of F-actin; (5) from the SH1 sites of myosin to the nucleotide-binding sites of F-actin; and (6) from the Cys-373 residues of F-actin to the nucleotide binding sites of F-actin. We observed very little energy transfer between the probes on actin and the probes on myosin (10% or less) and we observed a large transfer between the actin Cys-373 and the actin nucleotide. These data strongly suggest that both the SH1 moiety and the ATPase site of myosin are located more than 6 nm from the actin sites. When these distances are combined with similar measurements by other authors and inserted into the most recent three-dimensional reconstruction of electron micrographs of the acto-subfragment-1 complex, it is apparent that the SH1 and the ATPase sites on myosin are not located adjacent to actin and are most probably located in the half of the myosin head that is distal from actin in the actomyosin complex.

Biomolecular dynamics. A report from a workshop in Gysinge, Sweden, October 4-7, 1982

From the results of X-ray crystallography a wealth of information is now available concerning the detailed molecular structure of proteins, nucleic acids, and membrane components. This has made it possible to apply successfully various spectroscopie techniques for time resolved studies as well as theoretical simulations of internal molecular dynamics in the biological macromolecules and molecular aggregates. We were particularly pleased to see professor Ivar Waller among the participants of the workshop since new use of the wellknown Debye–Waller factor has greatly contributed to this development. A molecular picture is presently emerging including the dimension of time which ultimately will give us a detailed understanding of the functional interactions between biomolecules in general, and in particular enzyme catalysis, nucleic acid functions, and transport of matter and information through membranes.

The effect of myosin sulphydryl modification on the mechanics of fibre contraction

Glycerinated rabbit psoas fibres have been modified with paramagnetic probes ( IASL and MSL) which react selectively with the reactive sulphydryl on the myosin head. The extent of SH-1 modification was monitored by extracting myosin and measuring its ATPase activity in the presence of EDTA and of Ca2+. The isometric tension, stiffness, maximum velocity of contraction (slack test), and the force-velocity relation was measured as a function of the degree of SH-1 modification. Reaction of up to 50% of SH-1, i.e. 50% reduction in the K+-EDTA ATPase activity of extracted myosin, produced little change (less than 10%) in any of the fibre parameters. Modification of 75% of the SH-1 sites produced small decreases (15-30%) in the magnitude of all parameters, while reaction of more than 90% of SH-1 required long reaction times and produced decreases of 40-75%. In all cases the velocities of contraction decreased in parallel with the decrease in tension, while the decrease in stiffness was less pronounced. We conclude that a large fraction of muscle fibre SH-1 groups can be modified without greatly affecting the mechanical performance of the fibre. At least a portion of the decrease in fibre parameters that is observed at high levels of SH-1 modification can be attributed to modification of other sulphydryls by the probes. The reaction of both SH-1 and nonspecific sulphydryls abolishes myosin ATPase activity, and can account for approximately one half of the decrease in fibre parameters that is observed at high degrees of sulphydryl modification. We conclude that the modification of SH-1 does not greatly affect the function of a myosin head in the filament array of a fibre. This is in contrast to results obtained in vitro where SH-1 modification alters several rates in the interaction of myosin with ATP and decreases the actin-activated ATPase activity of myosin subfragments.

The characterization of vanadate-trapped nucleotide complexes with spin-labelled myosins

The properties of spin-labelled myosin, prepared from rabbit skeletal and scallop adductor muscle, on forming a long-lived complex with ADP and vanadate (M.ADP.Vi), have been investigated. In the case of an iodoacetamide-based label attached to rabbit myosin or subfragment 1, M.ADP.Vi formation is characterized by a marked increase in the mobility of the probe, similar to that seen during steady-state ATPase activity. Hence, this complex appears to be a good analogue of the M**ADP.Pi state. The kinetics of M.ADP.Vi formation were determined by following the electron paramagnetic resonance (e.p.r.) signal with time and were analysed according to the scheme: (formula; see text) After correction for Vi polymerization, K'4 = 3.2 X 10(-4)M, k'-3 = 8.7 X 10(-3) s-1 and k'3 = 1.5 X 10(-4) s-1. The major effect of spin-labelling the reactive SH1 thiol is to increase k'3, so that M.ADP.Vi dissociates over a period of hours rather than days. In contrast, a maleimide-based spin-label attached to rabbit myosin does not exhibit a large change in mobility, on formation of the M.ADP.Vi complex. However, the small change observed in both the conventional and saturation transfer spectra questions the assumption that this probe is completely insensitive to librational motion during ATPase activity. The immobilized spectrum of the iodoacetamide-based spin label attached to scallop myosin is insensitive to M.ADP.Vi formation in the presence or absence of Ca2+. Under these conditions, the label appears to reflect gross head motion and hence this observation lends no support to the idea that, in the myosin-linked regulatory system, Ca2+ operates by controlling the flexibility of the subfragment 1-subfragment 2 joint.

Intrinsic shortening speed of temperature-jump-activated intact muscle fibers. Effects of varying osmotic pressure with sucrose and KCl

Effects of intracellular ionic strength on the isotonic contraction properties of both intact fibers and skinned fibers give insights into the cross-bridge mechanism, but presently there is fundamental disagreement in the results on the two fiber preparations. This paper, which studies the effects on contraction of varying the osmotic pressure of the bathing medium with impermeant and permeant solutes, explains the above controversy and establishes the physiological significance of the previous results on skinned fibers. Fast-twitch fibers, isolated singly from tibialis and semitendinosus muscles of frogs, were activated by a temperature-jump technique in hyperosmotic solutions with either 100 or 150 mM sucrose (impermeant), or 50 or 75 mM KCl (permeant). Intracellular ionic strength was expected to rise in these solutions from the standard value of approximately 190 to 265 mM. Cell volume and the speed of unloaded shortening both decreased with sucrose and were constant with KCl. On the other hand, isometric force decreased equally with equiosmolar addition of either solute; this is additional evidence that contractile force decreases with ionic strength and is independent of fiber volume. Therefore, for the main cross-bridges, force per bridge is constant with changes in the lateral separation between the myofilaments. The next finding, that at a fixed cell volume the contraction speed is constant with KCl, provides clear evidence in intact fibers that the intrinsic speed of shortening is insensitive to increased ionic strength. The data with KCl are in agreement with the results on skinned fibers. The results suggest that in the cross-bridge kinetics in vivo the rate-limiting step is different for force than that for shortening. On the other hand, the decrease in speed with sucrose is associated with the shrinkage in cell volume, and is explained by the possibility of an increased internal load. A major fraction of the internal load may arise from unusual interactions between the sliding filaments; these interactions are enhanced in the fibers compressed with sucrose, but this does not affect the intrinsic kinetics of the main cross-bridges.

A comparison of order and orientation of crossbridges in rigor and relaxed muscle fibres using fluorescence polarization

Information has been obtained concerning the spatial disposition of the fluorescent reagent 5-(iodoacetamidoethylaminonaphthalene)-1-sulphonic acid bound covalently to muscle proteins in chemically skinned fibres of rabbit psoas muscle, using a novel time-gated fluorescence detection system to reject scattered incident light selectively. The results are consistent with a model of muscle crossbridge organization in which a particular crossbridge axial angle is strongly favoured in the rigor state. The structure in relaxation is less well ordered, but the favoured axial angle appears to be very close to that in rigor. This conclusion does not depend upon which of the models of crossbridge organization considered here is chosen, and is essentially unchanged if results obtained using a different fluorophore are analysed in the same way.

Evidence for cross-bridge order in contraction of glycerinated skeletal muscle

The linear dichroism of iodoacetylrhodamine labels attached to the single reactive thiol groups of myosin heads was measured to determine the spatial orientation of myosin cross-bridges in single glycerinated skeletal muscle fibers. We have shown previously that in rigor the chromophoric labels are well ordered and assume an orientation nearly perpendicular to the fiber axis; in the presence of MgADP, a large fraction of probe remains well ordered but the probe attitude assumes a more slanted orientation; in relaxed muscle, the probe order is largely lost, implying a high degree of cross-bridge disorder. In this paper, we report that during isometric contraction a large fraction of the probe shows a high degree of order, suggesting the attachment of approximately equal to 65% of the cross-bridges to actin. These ordered cross-bridges have a probe attitude similar to that of the MgADP-induced static state and hence are in a mechanical state quite distinct from rigor.

Studies on conformation of F-actin in muscle fibers in the relaxed state, rigor, and during contraction using fluorescent phalloidin

F-actin in a glycerinated muscle fiber was specifically labeled with fluorescent phalloidin-(fluorescein isothiocyanate) FITC complex at 1:1 molar ratio. Binding of phalloidin-FITC to F-actin affected neither contraction of the fiber nor its regulation by Ca2+. Comparison of polarized fluorescence from phalloidin-FITC bound to F-actin in the relaxed state, rigor, and during isometric contraction of the fiber revealed that the changes in polarization accompanying activation are quantitatively as well as qualitatively different from those accompanying transition of the fiber from the relaxed state to rigor. The extent of the changes of polarized fluorescence during isometric contraction increased with decreasing ionic strength, in parallel with increase in isometric tension. On the other hand, polarized fluorescence was not affected by addition of ADP or by stretching of the fiber in rigor solution. It is concluded from these observations that conformational changes in F-actin are involved in the process of active tension development.

Fluorescence energy transfer between the myosin subfragment-1 isoenzymes and F-actin in the absence and presence of nucleotides

The unique fast-reacting cysteine residue (SH1) of myosin subfragment 1 (S1), prepared by chymotryptic digestion, and cysteine 373 of actin have been labelled selectively with the fluorescent probes, N-(bromoacetyl)-N'-(1-sulpho-5-naphthyl)ethylenediamine (1,5-BrAEDANS) and 5-(iodoacetamido)fluorescein (5-IAF), whose spectral properties render them a particularly effective donor-acceptor pair in fluorescence energy transfer studies. The transfer efficiency of 40-45% represented a spatial separation of the chromophores of about 5 nm, which is in reasonable agreement with the value of 6 nm reported earlier for similarly labelled S1, prepared by papain digestion, and actin [Takashi, R. (1979) Biochemistry, 18, 5164-5169]. This transfer efficiency did not change when the doubly-labelled binary complex was formed: (1) with acto-S1(A1) or acto-S1(A2) at 10-200 mM KCl, pH 7-8 and different buffer conditions; (2) with either S1 isoenzyme and regulated actin (i.e. actin with tropomyosin and troponin) both in the presence and absence of Ca2+ or when the donor and acceptor attachment sites were reversed. Analysis of donor and acceptor polarized fluorescence showed that the chromophores are not randomly orientated (i.e. chi 2 not equal to 2/3), but they do have some motion relative to either protein. From a knowledge of the limiting values for chi 2, the intersite distance for donor and acceptor chromophores was calculated to be in the range 3.9-6.7 nm. Addition of MgATP to the doubly-labelled acto-S1 complex eliminated energy transfer but this was recovered when ATP hydrolysis was completed. By utilizing the known binding constants between S1, actin and either MgADP or MgAdoPP[NH]P (magnesium adenosine 5'-[beta, gamma-imido]triphosphate) [Konrad, M. and Goody, K. (1982) Eur. J. Biochem. 128, 547-555; Greene, L. E. and Eisenberg, E. (1980) J. Biol. Chem. 255, 543-548], the concentrations of all species present at equilibrium were determined. Experimental conditions were chosen to maximise the amount of ternary acto-S1-nucleotide complex (approximately equal to 50%) and minimise the amount of binary complex (less than or equal to 2%). The spatial separation of the chromophore interaction sites in the ternary complex was found to be the same with both nucleotides and indistinguishable from that found with the binary complex. A similar strategy was employed to compare the conformations of the binary and ternary complexes by 1H-NMR spectroscopy. In these experiments about 90% of the S1 was in the form of the ternary complex. There was no noticeable change in the acto-S1 spectra upon addition of either MgAdoPP[NH]P or MgADP. These observations support the conclusion that there is no large change in structure in the 'rigor' binary acto-S1 complex when it binds either ADP or AdoPP[NH]P.

Saturation transfer EPR spectroscopy on spin-labeled muscle fibers using a loop-gap resonator

Previously, saturation transfer (ST-EPR) studies of biomolecular dynamics have involved the use of a resonant cavity and the V'2 display (absorption, second harmonic, out of phase). In the present study, we replaced the resonant cavity with a loop-gap resonator and used the U'1 display (dispersion, first harmonic, out of phase) to study spin-labeled muscle fibers. The new resonator and display showed several advantages over those previously used. It produced virtually noiseless U'1 spectra on a 0.4 microliter sample using a 4 min scan; previous U'1 experiments on spin-labeled muscle, using a conventional rectangular cavity, resulted in an unacceptably low signal-to-noise ratio. The high filling factor of the resonator facilitated the study of these extremely small fiber bundles and permitted high microwave field intensities to be achieved at much lower incident microwave power levels, thus greatly enhancing the signal-to-noise ratio in U'1 experiments. This reduction in the noise level made it possible to benefit from the other advantages of U'1 over V'2, such as stronger signals, simpler line shapes, and simpler data analysis. For these muscle fiber samples, the resulting sensitivity (signal/noise/sample volume) of the U'1 signals was greater than 100 times that of V'2 signals obtained in a conventional cavity. Another advantage of the U'1 display is that signals from weakly immobilized probes, i.e., probes that have nanosecond rotational mobility relative to the labeled protein (myosin), are greatly suppressed relative to strongly immobilized probes. This reduces the ambiguity of spectral analysis, and eliminates the need for chemical treatments [e.g., using K3Fe(CN)6] that were previously required in muscle fibers and other systems. Further suppression of this weakly immobilized component was achieved in U'1 spectra by increasing the microwave power and decreasing the field modulation frequency.