Mechanism of force generation studied by neutron scattering

Neutron scattering has been used to compare the structure of myosin S1 that is free in solution to that when it is bound to F-actin. To achieve this, deuterated actin was obtained from D. discoideum that had been fed deuterated E. coli. This deuterated actin was rendered “invisible” to neutrons when dissolved in 94% D₂O. The neutron scattering patterns obtained from S1 bound to deuterated actin were identical to those of free S1 except for oscillations due to S1's bound to the same actin filament. At low S1 to actin stoichiometrics, these oscillations diminish and the patterns become indistinguishable. The apparent radius of gyration of S1 bound to actin is identical to that of free S1 when the stoichiometry is low. Thus, no changes in the structure of S1 were observed to a resolution of 2.5 nm. Computer modelling studies were used to evaluate the compatibility of models for the mechanism of force generation with the neutron data. These studies show that for powerstrokes greater than 5.0 nm, the data are consistent with more than 80% of the crossbridge maintaining a rigid conformation during force generation.     

Recent neutron scattering studies of muscle contraction and its control

We have presented two applications of the method of neutron scattering utilizing selective deuteration of actin. In these experiments the actin was rendered effectively invisible to neutrons by matching the scattering-length densities of deuterated actin and the solvent. The scattering of neutrons by myosin S1 and by Tm bound to this actin was studied.     

Bundling of actin filaments by alpha-actinin depends on its molecular length

Cross-linking of actin filaments (F-actin) into bundles and networks was investigated with three different isoforms of the dumbbell-shaped alpha-actinin homodimer under identical reaction conditions. These were isolated from chicken gizzard smooth muscle, Acanthamoeba, and Dictyostelium, respectively. Examination in the electron microscope revealed that each isoform was able to cross-link F-actin into networks. In addition, F-actin bundles were obtained with chicken gizzard and Acanthamoeba alpha-actinin, but not Dictyostelium alpha-actinin under conditions where actin by itself polymerized into disperse filaments. This F-actin bundle formation critically depended on the proper molar ratio of alpha-actinin to actin, and hence F-actin bundles immediately disappeared when free alpha-actinin was withdrawn from the surrounding medium. The apparent dissociation constants (Kds) at half-saturation of the actin binding sites were 0.4 microM at 22 degrees C and 1.2 microM at 37 degrees C for chicken gizzard, and 2.7 microM at 22 degrees C for both Acanthamoeba and Dictyostelium alpha-actinin. Chicken gizzard and Dictyostelium alpha-actinin predominantly cross-linked actin filaments in an antiparallel fashion, whereas Acanthamoeba alpha-actinin cross-linked actin filaments preferentially in a parallel fashion. The average molecular length of free alpha-actinin was 37 nm for glycerol-sprayed/rotary metal-shadowed and 35 nm for negatively stained chicken gizzard; 46 and 44 nm, respectively, for Acanthamoeba; and 34 and 31 nm, respectively, for Dictyostelium alpha-actinin. In negatively stained preparations we also evaluated the average molecular length of alpha-actinin when bound to actin filaments: 36 nm for chicken gizzard and 35 nm for Acanthamoeba alpha-actinin, a molecular length roughly coinciding with the crossover repeat of the two-stranded F-actin helix (i.e., 36 nm), but only 28 nm for Dictyostelium alpha-actinin. Furthermore, the minimal spacing between cross-linking alpha-actinin molecules along actin filaments was close to 36 nm for both smooth muscle and Acanthamoeba alpha-actinin, but only 31 nm for Dictyostelium alpha-actinin. This observation suggests that the molecular length of the alpha-actinin homodimer may determine its spacing along the actin filament, and hence F-actin bundle formation may require "tight" (i.e., one molecule after the other) and "untwisted" (i.e., the long axis of the molecule being parallel to the actin filament axis) packing of alpha-actinin molecules along the actin filaments.     

Skeletal muscle myosin subfragment-1 induces bundle formation by actin filaments

As is well known, the light scattering intensity of F-actin solutions increases immediately upon formation of the rigor complex with subfragment-1 (S-1). We have found that after the initial rise in scattering, there is a further gradual increase in scattering (we call it "super-opalescence"). Fluorescence and electron microscopic observations of acto-S-1 solutions showed that super-opalescence results from formation of actin filament bundles once S-1 binds to F-actin. The actin bundles possessed transverse stripes with a periodicity of about 350 A, which suggested that in the bundles actin filaments are arranged in parallel register. The rate of the initial process of bundle formation (i.e. side-by-side dimerization) could be approximately estimated by measuring the initial rate of super-opalescence (V0). V0 had a maximum (V0m) at a molar ratio of S-1 to actin of 1;6-1;7, regardless of the actin concentration, pH (6-8.5), Mg2+ concentration (up to 5 mM), or ionic strength (up to 0.3 M KC1). Lower pH, higher Mg2+ concentration, and higher ionic strength increased V0m; V0 was proportional to the square of the actin concentration, regardless of the solution conditions.     

Proteolytic cleavage of actin within the DNase-I-binding loop changes the conformation of F-actin and its sensitivity to myosin binding

Effects of subtilisin cleavage of actin between residues 47 and 48 on the conformation of F-actin and on its changes occurring upon binding of myosin subfragment-1 (S1) were investigated by measuring polarized fluorescence from rhodamine-phalloidin- or 1, 5-IAEDANS-labeled actin filaments reconstructed from intact or subtilisin-cleaved actin in myosin-free muscle fibers (ghost fibers). In separate experiments, polarized fluorescence from 1, 5-IAEDANS-labeled S1 bound to non-labeled actin filaments in ghost fibers was measured. The measurements revealed differences between the filaments of cleaved and intact actin in the orientation of rhodamine probe on the rhodamine-phalloidin-labeled filaments, orientation and mobility of the C-terminus of actin, filament flexibility, and orientation and mobility of the myosin heads bound to F-actin. The changes in the filament flexibility and orientation of the actin-bound fluorophores produced by S1 binding to actin in the absence of ATP were substantially diminished by subtilisin cleavage of actin. The results suggest that loop 38-52 plays an important role, not only in maintaining the F-actin structure, but also in the conformational transitions in actin accompanying the strong binding of the myosin heads that may be essential for the generation of force and movement during actin-myosin interaction.     

Multiple supramolecular structures formed by interaction of actin with protamine

When protamine is added to actin, different supramolecular structures are formed depending on the molar ratio of the two proteins and of the ionic strength of the medium. At low ionic strength, and going from a molar ratio of protamine to G-actin of 4:1, 2:1 and 1:1, globular aggregates are first converted into extended structures and then to long threads in which the constituent ATP–G-actin is rapidly exchangeable with the actin of the medium. At high ionic strength {Tyrode [(1910) Arch. Int. Pharmacodyn. Ther. 20, 205–212] solution}, starting from G-actin and protamine in the 1:1 molar ratio, long ropes are formed that can be resolved into intertwining filaments of 4–5nm diameter. The addition of protamine in a 1:1 molar ratio to a solution of F-actin in Tyrode solution causes the breakage of the actin filaments, which is also revealed by the decrease of the viscosity of the solution and the formation of ordered latero-lateral aggregates. The structures formed by reaction of protamine with G-actin can be separated from free G-actin and protamine by filtration through 0.45μm-pore-size Millipore filters. This technique has been exploited to study the exchange reaction between free actin and the actin–protamine complexes. For these studies the 1:1 actin–protamine complex formed at low ionic strength and the 2:1 actin–protamine complex formed in the presence of 23nm-free Mg²⁺ have been selected. In the first case the exchange reaction is practically complete in the dead time of the experiment (20s). In the second case, where the complex operates like a true ATPase, the rate of the exchange is initially comparable with the rate of the ATP cleavage. Later on, however, the complex undergoes a change and the rate of the exchange between free actin and the actin bound to protamine becomes lower than the rate of the ATPase reaction. It is proposed that the ATP exchanges for ADP directly on the G-actin bound in the complex.     

Membrane-associated actin in the rhabdomeral microvilli of crayfish photoreceptors

Infiltration of compound eyes of crayfish, Cherax destructor, with the thiol protease inhibitor Ep-475 or with trifluoperazine prior to fixation for electron microscopy was found to stabilize an axial filament of 6-12 nm diam within each rhabdomeral microvillus of the photoreceptors. Rhabdoms isolated from retinal homogenates by sucrose gradient centrifugation under conditions that stabilize cytoskeletal material contained large amounts of a 42-kd polypeptide that co- migrated with insect flight muscle actin in one- and two-dimensional PAGE, inhibited pancreatic DNase l, and bound to vertebrate myosin. Vertebrate skeletal muscle actin added to retinal homogenates did not co-purify with rhabdoms, implying that actin was not a contaminant from nonmembranous structures. DNase l inhibition assays of detergent-lysed rhabdoms indicated the presence of large amounts of filamentous actin provided ATP was present. Monomeric actin in such preparations was completely polymerizable only after 90 min incubation with equimolar phalloidin. More than half of the actin present could be liberated from the membrane by sonication, indicating a loose association with the membrane. However, a large proportion of the actin was tightly bound to the rhabdomeral membrane, and washing sonicated membrane fractions with solutions of a range of ionic strengths and nonionic detergents failed to remove it. Antibodies to scallop actin only bound to frozen sections of rhabdoms after gentle permeabilization and very long incubation periods, probably because of steric hindrance and the hydrophobicity of the structure. The F-actin probe nitrobenzoxadiazol phallacidin bound to rhabdoms and labeled F-actin aggregates in other retinal components, but rhabdom fluorescence was not abolished by preincubation with phalloidin. The biochemical data indicate the existence of two distinct actin-based cytoskeletal systems, one being closely membrane associated. The other may possibly constitute the axial filament, although the evidence for this is equivocal.     

The amino-terminal domain of the B subunit of vacuolar H+-ATPase contains a filamentous actin binding site

Vacuolar H(+)-ATPase (V-ATPase) binds actin filaments with high affinity (K(d) = 55 nm; Lee, B. S., Gluck, S. L., and Holliday, L. S. (1999) J. Biol. Chem. 274, 29164-29171). We have proposed that this interaction is an important mechanism controlling transport of V-ATPase from the cytoplasm to the plasma membrane of osteoclasts. Here we show that both the B1 (kidney) and B2 (brain) isoforms of the B subunit of V-ATPase contain a microfilament binding site in their amino-terminal domain. In pelleting assays containing actin filaments and partially disrupted V-ATPase, B subunits were found in greater abundance in actin pellets than were other V-ATPase subunits, suggesting that the B subunit contained an F-actin binding site. In overlay assays, biotinylated actin filaments also bound to the B subunit. A fusion protein containing the amino-terminal half of B1 subunit bound actin filaments tightly, but fusion proteins containing the carboxyl-terminal half of B1 subunit, or the full-length E subunit, did not bind F-actin. Fusion proteins containing the amino-terminal 106 amino acids of the B1 isoform or the amino-terminal 112 amino acids of the B2 isoform bound filamentous actin with K(d) values of 130 and 190 nm, respectively, and approached saturation at 1 mol of fusion protein/mol of filamentous actin. The B1 and B2 amino-terminal fusion proteins competed with V-ATPase for binding to filamentous actin. In summary, binding sites for F-actin are present in the amino-terminal domains of both isoforms of the B subunit, and likely are responsible for the interaction between V-ATPase and actin filaments in vivo.     

Binding of actin filaments to connectin

The binding of actin filaments to connectin, a muscle elastic protein, was investigated by means of turbidity and sedimentation measurements and electron microscopy. In the presence of less than 0.12 M KCl at pH 7.0, actin filaments bound to connectin. Long actin filaments formed bundles. Short actin filaments also aggregated into irregular bundles or a meshwork, and were frequently attached perpendicularly to long bundles. The binding of F-actin to connectin was saturated at an equal weight ratio (molar ratio, 50 : 1), as determined by a cosedimentation assay. Larger amounts of sonicated short actin filaments appeared to bind to connectin than intact F-actin. Myosin S1-decorated actin filaments did not bind to connectin. The addition of S1 to connectin-induced actin bundles resulted in partial disaggregation. Thus, connectin does not appear to interfere with actin-myosin interactions, since myosin S1 binds to actin more strongly than connectin.     

Influence of the bound nucleotide on the molecular dynamics of actin

Rotational dynamics of actin spin-labelled with maleimide probes at the reactive thiol Cys-374 were studied. Replacement of the bound nucleotide by Br8ATP in G-actin and Br8ADP in F-actin causes significant increase of the rotational correlation time of the spin probe, indicating reduced motion in both G and F-actin. The orientation dependence of the electron paramagnetic resonance spectra in oriented F-actin filaments revealed an altered molecular order of the probe when the nucleotide was a Br-substituted one. The bound nucleotide affects the myosin S1 ATPase activation by actin; both Vmax and K(actin) decreased significantly when the bound nucleotide of actin was Br8ADP.     

The C0C1 fragment of human cardiac myosin binding protein C has common binding determinants for both actin and myosin

The N-terminal domains of cardiac myosin binding protein C (MyBP-C) play a regulatory role in modulating interactions between myosin and actin during heart muscle contraction. Using NMR spectroscopy and small-angle neutron scattering, we have determined specific details of the interaction between the two-module human C0C1 cMyBP-C fragment and F-actin. The small-angle neutron scattering data show that C0C1 spontaneously polymerizes monomeric actin (G-actin) to form regular assemblies composed of filamentous actin (F-actin) cores decorated by C0C1, similar to what was reported in our earlier four-module mouse cMyBP-C actin study. In addition, NMR titration analyses show large intensity changes for a subset of C0C1 peaks upon addition of G-actin, indicating that human C0C1 interacts specifically with actin and promotes its assembly into filaments. During the NMR titration, peaks corresponding to cardiac-specific C0 domain are the first to be affected, followed by those from the C1 domain. No peak intensity or position changes were detected for peaks arising from the disordered proline/alanine-rich (P/A) linker connecting C0 with C1, despite previous suggestions of its involvement in binding actin. Of considerable interest is the observation that the actin-interaction “hot-spots” within the C0 and C1 domains, revealed in our NMR study, overlap with regions previously identified as binding to the regulatory light chain of myosin and to myosin ΔS2. Our results suggest that C0 and C1 interact with myosin and actin using a common set of binding determinants and therefore support a cMyBP-C switching mechanism between myosin and actin.     

A synthetic peptide of the N-terminus of actin interacts with myosin

Research reported from numerous laboratories suggested that the N-terminal region of actin contained one of the binding sites between actin and myosin. A synthetic peptide corresponding to residues 1-28 of skeletal actin was prepared by solid-phase peptide methodology. The formation of a complex between this peptide and myosin subfragment 1 (S1) was demonstrated by high-performance size-exclusion chromatography (pH 6.8). The actin peptide precipitated S1 at higher pH (7.4-8.2) but remained soluble when bound to heavy meromyosin (HMM) or S1 in the presence of F-actin. The actin peptide 1-28 bound to S1 and HMM and activated the ATPase activity in a manner similar to that of F-actin. These results demonstrate that the N-terminal region of actin, residues 1-28, contains a biologically important binding site for myosin.     

Cross-linked long-pitch actin dimer forms stoichiometric complexes with gelsolin segment 1 and/or deoxyribonuclease I that nonproductively interact with myosin subfragment 1

Actin dimer cross-linked along the long pitch of the F-actin helix by N-(4-azido)-2-nitrophenyl (ANP) was purified by gel filtration. Purified dimers were found to polymerize on increasing the ionic strength, although at reduced rate and extent in comparison with native actin. Purified actin dimer interacts with the actin-binding proteins (ABPs) deoxyribonuclease I (DNase I) and gelsolin segment-1 (G1) as analyzed by gel filtration and native gel electrophoresis. Complex formation of the actin dimer with these ABPs inhibits its ability to polymerize. The interaction with rabbit skeletal muscle myosin subfragment 1 (S1) was analyzed for polymerized actin dimer and dimer complexed with gelsolin segment 1 or DNase I by measurement of the actin-stimulated myosin S1-ATPase and gel filtration. The data obtained indicate binding of subfragment 1 to actin dimer, albeit with considerably lower affinity than to F-actin. Polymerized actin dimer was able to stimulate the S1-ATPase activity to about 50% of the level of native F-actin. In contrast, the actin dimer complexed to DNase I or gelsolin segment 1 or to both proteins was unable to significantly stimulate the S1-ATPase. Similarly, G1:dimer complex at 20 microM stimulated the rate of release of subfragment 1 bound nucleotide (mant-ADP) only 1.6-fold in comparison to about 9-fold by native F-actin at a concentration of 0.5 microM. Using rapid kinetic techniques, a dissociation constant of 2.4 x 10 (-6) M for subfragment 1 binding to G1:dimer was determined in comparison to 3 x 10 (-8) M for native F-actin under identical conditions. Since the rate of association of subfragment 1 to G1:dimer was considerably lower than to native F-actin, we suspect that the ATP-hydrolysis by S1 was catalyzed before its association to the dimer. These data suggest an altered, nonproductive mode for the interaction of subfragment 1 with the isolated long-pitch actin dimer.     

Intermolecular coupling between loop 38-52 and the C-terminus in actin filaments.

The recently reported structural connectivity in F-actin between the DNase I binding loop on actin (residues 38-52) and the C-terminus region was investigated by fluorescence and proteolytic digestion methods. The binding of copper to Cys-374 on F- but not G-actin quenched the fluorescence of dansyl ethylenediamine (DED) attached to Gin-41 by more than 50%. The blocking of copper binding to DED-actin by N-ethylmaleimide labeling of Cys-374 on actin abolished the fluorescence quenching. The quenching of DED-actin fluorescence was restored in copolymers (1:9) of N-ethylmaleimide-DED-actin with unlabeled actin. The quenching of DED-actin fluorescence by copper was also abolished in copolymers (1:4) of DED-actin and N-ethylmaleimide-actin. These results show intermolecular coupling between loop 38-52 and the C-terminus in F-actin. Consistent with this, the rate of subtilisin cleavage of actin at loop 38-52 was increased by the bound copper by more than 10-fold in F-actin but not in G-actin. Neither acto-myosin subfragment-1 (S1) ATPase activity nor the tryptic digestion of G-actin and F-actin at the Lys-61 and Lys-69 sites were affected by the bound copper. These observations suggest that copper binding to Cys-374 does not induce extensive changes in actin structure and that the perturbation of loop 38-52 environment results from changes in the intermolecular contacts in F-actin.     

Change in the actin-myosin subfragment 1 interaction during actin polymerization

To better characterize the conformational differences of G- and F-actin, we have compared the interaction between G- and F-actin with myosin subfragment 1 (S1) which had part of its F-actin binding site (residues 633-642) blocked by a complementary peptide or "antipeptide" (Chaussepied, P., and Morales, M. F. (1988) Proc. Natl. Acad. Sci. U.S.A. 85, 7471-7475). Light scattering, sedimentation, and electron microscopy measurements showed that, with the antipeptide covalently attached to the S1 heavy chain, S1 was not capable of inducing G-actin polymerization in the absence of salt. Moreover, the antipeptide-carrying S1 did not change the fluorescence polarization of 5-[2-(iodoacetyl)-aminoethyl]aminonaphthalene-1-sulfonic acid (1,5-IAEDANS)-labeled G-actin or of 1,5-IAEDANS-labeled actin dimer, compared to the control S1. This result, interpreted as a lack of interaction between G-actin and antipeptide-carrying S1, was confirmed further by the following experiments: in the presence of G-actin, antipeptide.S1 heavy chain was not protected against trypsin and papain proteolysis, and G-actin could not be cross-linked to antipeptide.S1 by 1-ethyl-3[-3-(dimethylamino)propyl]carbodiimide. In contrast, similar experiments showed that antipeptide.S1 was able to interact with nascent F-actin and with F-actin. Thus, blocking the stretch 633-642 of S1 heavy chain by the antipeptide strongly inhibits G-actin-S1 interaction but only slightly alters F-actin-S1 contact. We, therefore postulate that this stretch of skeletal S1 heavy chain is essential for G-actin-S1 interaction and that the G-F transformation generates new S1 binding site(s) on the actin molecule.     

Ca2+ regulation of gelsolin activity: binding and severing of F-actin.

Regulation of the F-actin severing activity of gelsolin by Ca2+ has been investigated under physiologic ionic conditions. Tryptophan fluorescence intensity measurements indicate that gelsolin contains at least two Ca2+ binding sites with affinities of 2.5 x 10(7) M-1 and 1.5 x 10(5) M-1. At F-actin and gelsolin concentrations in the range of those found intracellularly, gelsolin is able to bind F-actin with half-maximum binding at 0.14 microM free Ca2+ concentration. Steady-state measurements of gelsolin-induced actin depolymerization suggest that half-maximum depolymerization occurs at approximately 0.4 microM free Ca2+ concentration. Dynamic light scattering measurements of the translational diffusion coefficient for actin filaments and nucleated polymerization assays for number concentration of actin filaments both indicate that severing of F-actin occurs slowly at micromolar free Ca2+ concentrations. The data suggest that binding of Ca2+ to the gelsolin-F-actin complex is the rate-limiting step for F-actin severing by gelsolin; this Ca2+ binding event is a committed step that results in a Ca2+ ion bound at a high-affinity, EGTA-resistant site. The very high affinity of gelsolin for the barbed end of an actin filament drives the binding reaction equilibrium toward completion under conditions where the reaction rate is slow.     

The recovery of the polymerizability of Lys-61-labelled actin by the addition of phalloidin. Fluorescence polarization and resonance-energy-transfer measurements

Modification of Lys-61 in actin with fluorescein-5-isothiocyanate (FITC) blocks actin polymerization [Burtnick, L. D. (1984) Biochim. Biophys. Acta 791, 57-62]. FITC-labelled actin recovered its ability to polymerize on addition of phalloidin. The polymers had the same characteristic helical thread-like structure as normal F-actin and the addition of myosin subfragment-1 to the polymers formed the characteristic arrowhead structure in electron microscopy. The polymers activated the ATPase activity of myosin subfragment-1 as efficiently as normal F-actin. These results indicate that Lys-61 is not directly involved in an actin-actin binding region nor in myosin binding site. From static fluorescence polarization measurements, the rotational relaxation time of FITC-labelled actin filaments was calculated to be 20 ns as the value reduced in water at 20 degrees C, while any rotational relaxation time of 1,5-IAEDANS bound to Cys-374 on F-actin in the presence of a twofold molar excess of phalloidin could not be detected by static polarization measurements under the same conditions. This indicates that the Lys-61 side chain is extremely mobile even in the filamentous structure. Fluorescence resonance energy transfer between the donor 1,5-IAEDANS bound to SH1 of myosin subfragment-1 and the acceptor fluorescein-5-isothiocyanate bound to Lys-61 of actin in the rigor complex was measured. The transfer efficiency was 0.39 +/- 0.05 which corresponds to the distance of 5.2 +/- 0.1 nm, assuming that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime and that the transfer occurs between a single donor and an acceptor.     

Cross-helix separation of tropomyosin molecules in acto-tropomyosin as determined by neutron scattering.

The cross-helix separation of Tm molecules in acto-tropomyosin has been determined using neutron scattering. Deuterated Dictyostelium discoideum actin was density matched in a 93% D2O buffer so that effectively only the protonated tropomyosin was "visible" to neutrons. Analysis of the solution scattering pattern in the region of the first oscillation yielded a value for the cross-helix separation of 7.9 +/- 0.3 nm. The implications of this value for the mechanism of the regulation of muscle contraction are discussed in light of recent results by others.     

Conformational change in actin filament induced by the interaction with heavy meromyosin: effects of pH, tropomyosin and deoxy-ATP.

Conformational changes in pure and tropomyosin-containing F-actin during interaction with heavy meromyosin in the absence and presence of deoxy-ATP, were studied by measurements of the changes in fluorescence intensity of e-ADP² incorporated into the F-actin instead of ADP. The actin filaments were found to be stabilized by tropomyosin and were more stable at pH 7 than at pH 8. The rigor binding of HMM to F-actin caused an increase in the fluorescence intensity. The increase with F-actin containing TM was higher than that with pure F-actin at each HMM concentration. A linear relation between the fluoresence change and moles of HMM per actin was found regardless of the presence of TM, with a maximum value of 0.5 moles of HMM per actin. In the presence of deoxy-ATP, (which is a substrate for acto-HMM but cannot bind to actin) no changes in fluorescence intensity of e-ADP bound to pure F-actin were observed. In the case of F-actin containing TM, the fluorescence intensity increased with increasing HMM concentration, although the light scattering intensity of the acto-HMM solutions indicated that almost all the HMM was dissociated from the F-actin. This suggests that the conformational change in F-actin-TM induced by the interaction with HMM in the presence of deoxy-ATP has a long lifetime which continues for some time even after the detachment of the HMM.     

Conformational changes of troponin C within the thin filaments detected by neutron scattering

Regulation of skeletal and cardiac muscle contraction is associated with structural changes of the thin filament-based proteins, troponin consisting of three subunits (TnC, TnI, and TnT), tropomyosin, and actin, triggered by Ca2+-binding to TnC. Knowledge of in situ structures of these proteins is indispensable for elucidating the molecular mechanism of this Ca2+-sensitive regulation. Here, the in situ structure of TnC within the thin filaments was investigated with neutron scattering, combined with selective deuteration and the contrast matching technique. Deuterated TnC (dTnC) was first prepared, this dTnC was then reconstituted into the native thin filaments, and finally neutron scattering patterns of these reconstituted thin filaments containing dTnC were measured under the condition where non-deuterated components were rendered "invisible" to neutrons. The obtained scattering curves arising only from dTnC showed distinct difference in the absence and presence of Ca2+. These curves were analyzed by model calculations using the Monte Carlo method, in which inter-dTnC interference was explicitly taken into consideration. The model calculation showed that in situ radius of gyration of TnC was 23 A (99% confidence limits between 22 A and 23 A) and 24 A (99% confidence limits between 23 A and 25 A) in the absence and presence of Ca2+, respectively, indicating that TnC within the thin filaments assumes a conformation consistent with the extended dumbbell structure, which is different from the structures found in the crystals of various Tn complexes. Elongation of TnC by binding of Ca2+ was also suggested. Furthermore, the radial position of TnC within the thin filament was estimated to be 53 A (99% confidence limits between 49 A and 57 A) and 49 A (99% confidence limits between 44 A and 53 A) in the absence and presence of Ca2+, respectively, suggesting that this radial movement of TnC by 4A is associated with large conformational changes of the entire Tn molecule by binding of Ca2+.