Ca(2+)-induced movement of tropomyosin in skeletal muscle thin filaments observed by multi-site FRET

To obtain information on Ca(2+)-induced tropomyosin (Tm) movement in Ca(2+)-regulated muscle thin filaments, frequency-domain fluorescence energy transfer data were collected between 5-(2-iodoacetyl-amino-ethyl-amino)naphthalene-1-sulfonic acid at Cys-190 of Tm and phalloidin-tetramethylrhodamine B isothiocyanate bound to F-actin. Two models were used to fit the experimental data: an atomic coordinate (AC) model coupled with a search algorithm that varies the position and orientation of Tm on F-actin, and a double Gaussian distance distribution (DD) model. The AC model showed that little or no change in transfer efficiency is to be expected between different sites on F-actin and Tm if Ca(2+) causes azimuthal movement of Tm of the magnitude suggested by structural data (C. Xu, R. Craig, L. Tobacman, R. Horowitz, and W. Lehman. 1999. Biophys. J. 77:985-992). However, Ca(2+) produced a small but significant change in our phase/modulation versus frequency data, showing that changes in lifetime decay can be detected even when a change of the steady-state transfer efficiency is very small. A change in Tm azimuthal position of 17 on the actin filament obtained with the AC model indicates that solution data are in reasonable agreement with EM image reconstruction data. In addition, the data indicate that Tm also appears to rotate about its axis, resulting in a rolling motion over the F-actin surface. The DD model showed that the distance from one of the two chains of Tm to F-actin was mainly affected, further verifying that Ca(2+) causes Tm to roll over the F-actin surface. The width of the distance distributions indicated that the position of Tm in absence and in presence of Ca(2+) is well defined with appreciable local flexibility.     

Movement of smooth muscle tropomyosin by myosin heads.

It has been proposed that during the activation of muscle contraction the initial binding of myosin heads to the actin thin filament contributes to switching on the thin filament and that this might involve the movement of actin-bound tropomyosin. The movement of smooth muscle tropomyosin on actin was investigated in this work by measuring the change in distance between specific residues on tropomyosin and actin by fluorescence resonance energy transfer (FRET) as a function of myosin head binding to actin. An energy transfer acceptor was attached to Cys374 of actin and a donor to the tropomyosin heterodimer at either Cys36 of the beta-chain or Cys190 of the alpha-chain. FRET changed for the donor at both positions of tropomyosin upon addition of skeletal or smooth muscle myosin heads, indicating a movement of the whole tropomyosin molecule. The changes in FRET were hyperbolic and saturated at about one head per seven actin subunits, indicating that each head cooperatively affects several tropomyosin molecules, presumably via tropomyosin's end-to-end interaction. ATP, which dissociates myosin from actin, completely reversed the changes in FRET induced by heads, whereas in the presence of ADP the effect of heads was the same as in its absence. The results indicate that myosin with and without ADP, intermediates in the myosin ATPase hydrolytic pathway, are effective regulators of tropomyosin position, which might play a role in the regulation of smooth muscle contraction.     

Ca(2+)-dependent, myosin subfragment 1-induced proximity changes between actin and the inhibitory region of troponin I.

In order to help understand the spatial rearrangements of thin filament proteins during the regulation of muscle contraction, we used fluorescence resonance energy transfer (FRET) to measure Ca(2+)-dependent, myosin-induced changes in distances and fluorescence energy transfer efficiencies between actin and the inhibitory region of troponin I (TnI). We labeled the single Cys-117 of a mutant TnI with N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine (IAEDANS) and Cys-374 of actin with 4-dimethylaminophenylazophenyl-4'-maleimide (DABmal). These fluorescent probes were used as donor and acceptor, respectively, for the FRET measurements. We reconstituted a troponin-tropomyosin (Tn-Tm) complex which contained the AEDANS-labeled mutant TnI, together with natural troponin T (TnT), troponin C (TnC) and tropomyosin (Tm) from rabbit fast skeletal muscle. Fluorescence titration of the AEDANS-labeled Tn-Tm complex with DABmal-labeled actin, in the presence and absence of Ca(2+), resulted in proportional, linear increases in energy transfer efficiency up to a 7:1 molar excess of actin over Tn-Tm. The distance between AEDANS on TnI Cys-117 and DABmal on actin Cys-374 increased from 37.9 A to 44.1 A when Ca(2+) bound to the regulatory sites of TnC. Titration of reconstituted thin filaments, containing AEDANS-labeled Tn-Tm and DABmal-labeled actin, with myosin subfragment 1 (S1) decreased the energy transfer efficiency, in both the presence and absence of Ca(2+). The maximum decrease occurred at well below stoichiometric levels of S1 binding to actin, showing a cooperative effect of S1 on the state of the thin filaments. S1:actin molar ratios of approximately 0.1 in the presence of Ca(2+), and approximately 0.3 in the absence of Ca(2+), were sufficient to cause a 50% reduction in normalized transfer efficiency. The distance between AEDANS on TnI Cys-117 and DABmal on actin Cys-374 increased by approximately 7 A in the presence of Ca(2+) and by approximately 2 A in the absence of Ca(2+) when S1 bound to actin. Our results suggest that TnI's interaction with actin inhibits actomyosin ATPase activity by modulating the equilibria among active and inactive states of the thin filament. Structural rearrangements caused by myosin S1 binding to the thin filament, as detected by FRET measurements, are consistent with the cooperative behavior of the thin filament proteins.     

Fluorescence properties of acrylodan-labeled tropomyosin and tropomyosin-actin: evidence for myosin subfragment 1 induced changes in geometry between tropomyosin and actin

The Cys groups of rabbit skeletal tropomyosin (Tm) and rabbit skeletal alpha alpha Tm were specifically labeled with acrylodan (AC). The probe on Tm is quite immobile yet exposed to solvent as indicated by its limiting polarization (P0 = 0.38) and fluorescence emission spectrum (lambda max = 520 nm) and its accessibility to solute quenching. Changes in the shape of the excitation spectrum with temperature correlated with the helix thermal pretransition and main transition without much spectral change of the emission spectrum. The probe environment of ACTm did not significantly change on binding to F-actin, but fluorescence energy transfer between tryptophan in actin and AC on Tm was indicated by a 15-20% increase in AC fluorescence and a few percent decrease in tryptophan fluorescence. This energy transfer increased when myosin subfragment 1 (S1) was bound to the ACTm-actin filament, in quantitative agreement with the postulated shift in state of Tm associated with the cooperative binding of S1 to actin (Hill et al., 1980). The increase in energy transfer shows that there is a change in the spatial relationship between Tm and actin associated with the S1-induced change in state of Tm.     

A three-dimensional FRET analysis to construct an atomic model of the actin-tropomyosin complex on a reconstituted thin filament

Fluorescence resonance energy transfer (FRET) was used to construct an atomic model of the actin–tropomyosin (Tm) complex on a reconstituted thin filament. We generated five single-cysteine mutants in the 146–174 region of rabbit skeletal muscle α-Tm. An energy donor probe was attached to a single-cysteine Tm residue, while an energy acceptor probe was located in actin Gln41, actin Cys374, or the actin nucleotide binding site. From these donor–acceptor pairs, FRET efficiencies were determined with and without Ca²⁺. Using the atomic coordinates for F-actin and Tm, we searched all possible arrangements for Tm segment 146–174 on F-actin to calculate the FRET efficiency for each donor–acceptor pair in each arrangement. By minimizing the squared sum of deviations for the calculated FRET efficiencies from the observed FRET efficiencies, we determined the location of the Tm segment on the F-actin filament. Furthermore, we generated a set of five single-cysteine mutants in each of the four Tm regions 41–69, 83–111, 216–244, and 252–279. Using the same procedures, we determined each segment's location on the F-actin filament. In the best-fit model, Tm runs along actin residues 217–236, which were reported to compose the Tm binding site. Electrostatic, hydrogen-bonding, and hydrophobic interactions are involved in actin and Tm binding. The C-terminal region of Tm was observed to contact actin more closely than did the N-terminal region. Tm contacts more residues on actin without Ca²⁺ than with it. Ca²⁺-induced changes on the actin–Tm contact surface strongly affect the F-actin structure, which is important for muscle regulation.     

Conformational and dynamic differences between actin filaments polymerized from ATP- or ADP-actin monomers

Conformational and dynamic properties of actin filaments polymerized from ATP- or ADP-actin monomers were compared by using fluorescence spectroscopic methods. The fluorescence intensity of IAEDANS attached to the Cys(374) residue of actin was smaller in filaments from ADP-actin than in filaments from ATP-actin monomers, which reflected a nucleotide-induced conformational difference in subdomain 1 of the monomer. Radial coordinate calculations revealed that this conformational difference did not modify the distance of Cys(374) from the longitudinal filament axis. Temperature-dependent fluorescence resonance energy transfer measurements between donor and acceptor molecules on Cys(374) of neighboring actin protomers revealed that the inter-monomer flexibility of filaments assembled from ADP-actin monomers were substantially greater than the one of filaments from ATP-actin monomers. Flexibility was reduced by phalloidin in both types of filaments.     

The flexibility of actin filaments as revealed by fluorescence resonance energy transfer. The influence of divalent cations

The temperature profile of the fluorescence resonance energy transfer efficiency normalized by the fluorescence quantum yield of the donor in the presence of acceptor, f', was measured in a way allowing the independent investigation of (i) the strength of interaction between the adjacent protomers (intermonomer flexibility) and (ii) the flexibility of the protein matrix within actin protomers (intramonomer flexibility). In both cases the relative increase as a function of temperature in f' is larger in calcium-F-actin than in magnesium-F-actin in the range of 5-40 degrees C, which indicates that both the intramonomer and the intermonomer flexibility of the actin filaments are larger in calcium-F-actin than those in magnesium-F-actin. The intermonomer flexibility was proved to be larger than the intramonomer one in both the calcium-F-actin and the magnesium-F-actin. The distance between Gln41 and Cys374 residues was found to be cation-independent and did not change during polymerization at 21 degrees C. The steady-state fluorescence anisotropy data of fluorophores attached to the Gln41 or Cys374 residues suggest that the microenvironments around these regions are more rigid in the magnesium-loaded actin filament than in the calcium-loaded form.     

Detection of actin assembly by fluorescence energy transfer

Fluorescence energy transfer was used to measure the assembly and disassembly of actin filaments. Actin was labeled at cysteine 373 with an energy donor (5-iodoacetamidofluorescein) or an energy acceptor (tetramethylrhodamine iodoacetamide or eosin iodoacetamide). Donor- labeled actin and acceptor-labeled actin were coassembled. The dependence of the transfer efficiency on the mole fraction of acceptor- labeled actin showed that the radial coordinate of the label at cysteine 373 is approximately 35 A, which means that this site is located near the outer surface of the filament. The distance between a donor and the closest acceptor in such a filament is 58 A. The increase in fluorescence after the mixing of actin filaments containing both donor and acceptor with unlabeled filaments showed that there is a slow continuous exchange of actin units. The rate of exchange was markedly accelerated when the filaments were sonicated. The rapid loss of energy transfer caused by mechanical shear probably resulted from an increase in the number of filament ends, which in turn accelerated the exchange of monomeric actin units. Energy transfer promises to be a valuable tool in characterizing the assembly and dynamics of actin and other cytoskeletal and contractile proteins in vitro and in intact cells.     

Calcium-induced flexibility changes in the troponin C-troponin I complex

The contraction of vertebrate striated muscle is modulated by Ca(2+) binding to the regulatory protein troponin C (TnC). Ca(2+) binding causes conformational changes in TnC which alter its interaction with the inhibitory protein troponin I (TnI), initiating the regulatory process. We have used the frequency domain method of fluorescence resonance energy transfer (FRET) to measure distances and distance distributions between specific sites in the TnC-TnI complex in the presence and absence of Ca(2+) or Mg(2+). Using sequences based on rabbit skeletal muscle proteins, we prepared functional, binary complexes of wild-type TnC and a TnI mutant which contains no Cys residues and a single Trp residue at position 106 within the TnI inhibitory region. We used TnI Trp-106 as the FRET donor, and we introduced energy acceptor groups into TnC by labeling at Met-25 with dansyl aziridine or at Cys-98 with N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine. Our distance distribution measurements indicate that the TnC-TnI complex is relatively rigid in the absence of Ca(2+), but becomes much more flexible when Ca(2+) binds to regulatory sites in TnC. This increased flexibility may be propagated to the whole thin filament, helping to release the inhibition of actomyosin ATPase activity and allowing the muscle to contract. This is the first report of distance distributions between TnC and TnI in their binary complex.     

Fluorescence resonance energy transfer between points on actin and the C-terminal region of tropomyosin in skeletal muscle thin filaments

Fluorescence resonance energy transfer between points on tropomyosin (positions 87 and 190) and actin (Gln-41, Lys-61, Cys-374, and the ATP-binding site) showed no positional change of tropomyosin relative to actin on the thin filament in response to changes in Ca2+ concentration (Miki et al. (1998) J. Biochem. 123, 1104-1111). This is consistent with recent electron cryo-microscopy analysis, which showed that the C-terminal one-third of tropomyosin shifted significantly towards the outer domain of actin, while the N-terminal half of tropomyosin shifted only a little (Narita et al. (2001) J. Mol. Biol. 308, 241-261). In order to detect any significant positional change of the C-terminal region of tropomyosin relative to actin, we generated mutant tropomyosin molecules with a unique cysteine residue at position 237, 245, 247, or 252 in the C-terminal region. The energy donor probe was attached to these positions on tropomyosin and the acceptor probe was attached to Cys-374 or Gln-41 of actin. These probe-labeled mutant tropomyosin molecules retain the ability to regulate the acto-S1 ATPase activity in conjunction with troponin and Ca2+. Fluorescence resonance energy transfer between these points of tropomyosin and actin showed a high transfer efficiency, which should be very sensitive to changes in distance between probes attached to actin and tropomyosin. However, the transfer efficiency did not change appreciably upon removal of Ca2+ ions, suggesting that the C-terminal region of tropomyosin did not shift significantly relative to actin on the reconstituted thin filament in response to the change of Ca2+ concentration.     

Myosin-induced movement of alphaalpha, alphabeta, and betabeta smooth muscle tropomyosin on actin observed by multisite FRET

The interaction of the alphaalpha, betabeta, and alphabeta smooth muscle tropomyosin (Tm) isoforms with F-actin was systematically studied in the absence and in the presence of myosin subfragment 1 (S1) using multifrequency phase/modulation F?rster resonance energy transfer (FRET). A Gaussian double distance distribution model was adopted to fit FRET data between a 5-(2-iodoacetyl-amino-ethyl-amino)naphthalene-1-sulfonic acid donor at either Cys-36 of the beta-chain or Cys-190 of the alpha-chain and a 4-dimethylaminophenylazophenyl 4'-maleimide acceptor at Cys-374 of F-actin. Experimental data were obtained for singly and doubly labeled alphabeta Tm (donor only at alpha, only at beta, or both) and for doubly labeled alphaalpha or betabeta Tm. Data for singly labeled alphabetaTm were combined in a global analysis with doubly labeled alphabetaTm. In all doubly labeled isoforms, upon S1 binding, one donor-acceptor "apparent" distance increased slightly by 0.5-2 A, whereas the other decreased by 6-9 A. These changes are consistent with a uniform "rolling" motion of Tm over the F-actin surface. The analysis indicates that Tm occupies relatively well-defined positions, with some flexibility, in both the predominantly closed (-S1) and open (+S1) thin-filament states. The results for the alphabetaTm heterodimer indicate that the local twofold symmetry of alphaalpha or betabeta Tm is effectively broken in alphabetaTm bound to F-actin, which implies a difference between the alpha- and beta-chains in terms of their interaction with F-actin.     

A three-dimensional FRET analysis to construct an atomic model of the actin-tropomyosin-troponin core domain complex on a muscle thin filament

It is essential to know the detailed structure of the thin filament to understand the regulation mechanism of striated muscle contraction. Fluorescence resonance energy transfer (FRET) was used to construct an atomic model of the actin-tropomyosin (Tm)-troponin (Tn) core domain complex. We generated single-cysteine mutants in the 167-195 region of Tm and in TnC, TnI, and the β-TnT 25-kDa fragment, and each was attached with an energy donor probe. An energy acceptor probe was located at actin Gln41, actin Cys374, or the actin nucleotide-binding site. From these donor-acceptor pairs, FRET efficiencies were determined with and without Ca(2+). Using the atomic coordinates for F-actin, Tm, and the Tn core domain, we searched all possible arrangements for Tm or the Tn core domain on F-actin to calculate the FRET efficiency for each donor-acceptor pair in each arrangement. By minimizing the squared sum of deviations for the calculated FRET efficiencies from the observed FRET efficiencies, we determined the location of Tm segment 167-195 and the Tn core domain on F-actin with and without Ca(2+). The bulk of the Tn core domain is located near actin subdomains 3 and 4. The central helix of TnC is nearly perpendicular to the F-actin axis, directing the N-terminal domain of TnC toward the actin outer domain. The C-terminal region in the I-T arm forms a four-helix-bundle structure with the Tm 175-185 region. After Ca(2+) release, the Tn core domain moves toward the actin outer domain and closer to the center of the F-actin axis.     

Fluorescence resonance energy transfer between residues on troponin and tropomyosin in the reconstituted thin filament: modeling the troponin-tropomyosin complex

Troponin (Tn), in association with tropomyosin (Tm), plays a central role in the calcium regulation of striated muscle contraction. Fluorescence resonance energy transfer (FRET) between probes attached to the Tn subunits (TnC, TnI, TnT) and to Tm was measured to study the spatial relationship between Tn and Tm on the thin filament. We generated single-cysteine mutants of rabbit skeletal muscle α-Tm, TnI and the β-TnT 25-kDa fragment. The energy donor was attached to a single-cysteine residue at position 60, 73, 127, 159, 200 or 250 on TnT, at 98 on TnC and at 1, 9, 133 or 181 on TnI, while the energy acceptor was located at 13, 146, 160, 174, 190, 209, 230, 271 or 279 on Tm. FRET analysis showed a distinct Ca²⁺-induced conformational change of the Tm-Tn complex and revealed that TnT60 and TnT73 were closer to Tm13 than Tm279, indicating that the elongated N-terminal region of TnT extends beyond the beginning of the next Tm molecule on the actin filament. Using the atomic coordinates of the crystal structures of Tm and the Tn core domain, we searched for the disposition and orientation of these structures by minimizing the deviations of the calculated FRET efficiencies from the observed FRET efficiencies in order to construct atomic models of the Tn-Tm complex with and without bound Ca²⁺. In the best-fit models, the Tn core domain is located on residues 160-200 of Tm, with the arrowhead-shaped I-T arm tilting toward the C-terminus of Tm. The angle between the Tm axis and the long axis of TnC is ∼ 75° and ∼ 85° with and without bound Ca²⁺, respectively. The models indicate that the long axis of TnC is perpendicular to the thin filament without bound Ca²⁺, and that TnC and the I-T arm tilt toward the filament axis and rotate around the Tm axis by ∼ 20° upon Ca²⁺ binding.     

Phosphorylation of tropomyosin extends cooperative binding of myosin beyond a single regulatory unit

Tropomyosin (Tm) is one of the major phosphoproteins comprising the thin filament of muscle. However, the specific role of Tm phosphorylation in modulating the mechanics of actomyosin interaction has not been determined. Here we show that Tm phosphorylation is necessary for long-range cooperative activation of myosin binding. We used a novel optical trapping assay to measure the isometric stall force of an ensemble of myosin molecules moving actin filaments reconstituted with either natively phosphorylated or dephosphorylated Tm. The data show that the thin filament is cooperatively activated by myosin across regulatory units when Tm is phosphorylated. When Tm is dephosphorylated, this "long-range" cooperative activation is lost and the filament behaves identically to bare actin filaments. However, these effects are not due to dissociation of dephosphorylated Tm from the reconstituted thin filament. The data suggest that end-to-end interactions of adjacent Tm molecules are strengthened when Tm is phosphorylated, and that phosphorylation is thus essential for long range cooperative activation along the thin filament.     

Mutations in actin subdomain 3 that impair thin filament regulation by troponin and tropomyosin.

Thin filament-mediated regulation of striated muscle contraction involves conformational switching among a few quaternary structures, with transitions induced by binding of Ca(2+) and myosin. We establish and exploit Saccharomyces cerevisiae actin as a model system to investigate this process. Ca(2+)-sensitive troponin-tropomyosin binding affinities for wild type yeast actin are seen to closely resemble those for muscle actin, and these hybrid thin filaments produce Ca(2+)-sensitive regulation of the myosin S-1 MgATPase rate. Yeast actin filament inner domain mutant K315A/E316A depresses Ca(2+) activation of the MgATPase rate, producing a 4-fold weakening of the apparent Ca(2+) affinity and a 50% decrease in the MgATPase rate at saturating Ca(2+) concentration. Observed destabilization of troponin-tropomyosin binding to actin in the presence of Ca(2+), a 1.4-fold effect, provides a partial explanation. Despite the decrease in apparent MgATPase Ca(2+) affinity, there was no detectable change in the true Ca(2+) affinity of the thin filament, measured using fluorophore-labeled troponin. Another inner domain mutant, E311A/R312A, decreased the MgATPase rate but did not change the apparent Ca(2+) affinity. These results suggest that charged residues on the surface of the actin inner domain are important in Ca(2+)- and myosin-induced thin filament activation.     

Smooth muscle alpha-tropomyosin crosslinks to caldesmon, to actin and to myosin subfragment 1 on the muscle thin filament

To obtain proximity information between tropomyosin (Tm) and caldesmon (CaD) on the muscle thin filament, we cloned gizzard alphaTm and created two single Cys mutants S56C/C190S (56Tm) and D100C/C190S (100Tm). They were labeled with benzophenone maleimide (BPM) and UV-irradiated on thin filaments. One chain of BPM-56Tm and two chains of BPM-100Tm crosslinked to CaD. Only BPM-100Tm crosslinked to actin in the absence and presence of CaD and binding of low ratios of myosin subfragment 1 (S1) prevented the crosslinking. Tm-S1 crosslinks were produced when actin.Tm was saturated with S1. Thus, CaD on the actin.Tm filament is located <10 A away from Tm amino acids 56 and 100; in the closed state of the actin.Tm filament, Tm residue 100 is located close to the actin surface and is moved further away in the S1-induced open state; in the open state, S1 binds close to Tm.     

Specification of actin filament function and molecular composition by tropomyosin isoforms

The specific functions of greater than 40 vertebrate nonmuscle tropomyosins (Tms) are poorly understood. In this article we have tested the ability of two Tm isoforms, TmBr3 and the human homologue of Tm5 (hTM5(NM1)), to regulate actin filament function. We found that these Tms can differentially alter actin filament organization, cell size, and shape. hTm5(NM1) was able to recruit myosin II into stress fibers, which resulted in decreased lamellipodia and cellular migration. In contrast, TmBr3 transfection induced lamellipodial formation, increased cellular migration, and reduced stress fibers. Based on coimmunoprecipitation and colocalization studies, TmBr3 appeared to be associated with actin-depolymerizing factor/cofilin (ADF)-bound actin filaments. Additionally, the Tms can specifically regulate the incorporation of other Tms into actin filaments, suggesting that selective dimerization may also be involved in the control of actin filament organization. We conclude that Tm isoforms can be used to specify the functional properties and molecular composition of actin filaments and that spatial segregation of isoforms may lead to localized specialization of actin filament function.     

The role of tropomyosin domains in cooperative activation of the actin-myosin interaction

To establish α-tropomyosin (Tm)'s structure–function relationships in cooperative regulation of muscle contraction, thin filaments were reconstituted with a variety of Tm mutants (Δ2Tm, Δ3Tm, Δ6Tm, P2sTm, P3sTm, P2P3sTm, P1P5Tm, and wtTm), and force and sliding velocity of the thin filament were studied using an in vitro motility assay. In the case of deletion mutants, Δ indicates which of the quasi-equivalent repeats in Tm was deleted. In the case of period (P) mutants, an Ala cluster was introduced into the indicated period to strengthen the Tm–actin interaction. In P1P5Tm, the N-terminal half of period 5 was substituted with that of period 1 to test the quasi-equivalence of these two Tm periods. The reconstitution included bovine cardiac troponin. Deletion studies revealed that period 3 is important for the positive cooperative effect of Tm on actin filament regulation and that period 2 also contributes to this effect at low ionic strength, but to a lesser degree. Furthermore, Tm with one extra Ala cluster at period 2 (P2s) or period 3 (P3s) did not increase force or velocity, whereas Tm with two extra Ala clusters (P2P3s) increased both force and velocity, demonstrating interaction between these periods. Most mutants did not move in the absence of Ca²⁺. Notable exceptions were Δ6Tm and P1P5Tm, which moved near at the full velocity, but with reduced force, which indicate impaired relaxation. These results are consistent with the mechanism that the Tm–actin interaction cooperatively affects actin to result in generation of greater force and velocity.     

A catalytic site of protein disulfide isomerase probed with adenosine-5'-triphosphate analogs

Anthraniloyl adenosine-5'-triphosphate (Ant-ATP) and etheno-adenosine-5'-triphosphate (epsilon-ATP) complexed to Mg(2+) ions are substrates of protein disulfide isomerase (PDI). epsilon-ATP, coordinated to Tb(3+) ions, was used as a probe of the ATPase binding site. Sensitized luminescence arising from resonance energy transfer from epsilon-adenine to Tb(3+) is quenched by PDI. The luminescence results are discussed in reference to a model in which the distance of separation between epsilon-adenine (donor) and Tb(3+) (acceptor) is increased upon binding of PDI. The interaction of a small peptide of 14 amino acid residues with the b/b' domain of the protein does not influence the ATPase activity. The phosphorescence, fluorescence and fluorescence anisotropy of bound epsilon-ATP are not perturbed by the binding of the small molecular weight peptide to PDI. It is suggested that the peptide and ATP do not share a common binding site on the b/b' domain.     

Ca(2+)- and s1-induced movement of troponin T on mutant thin filaments reconstituted with functionally deficient mutant tropomyosin

The deletion mutant (D234Tm) of rabbit skeletal muscle alpha-tropomyosin, in which internal actin-binding pseudo-repeats 2, 3, and 4 are missing, inhibits the thin filament activated myosin-ATPase activity whether Ca(2+) ion is present or not [Landis et al. (1997) J. Biol. Chem. 272, 14051-14056]. Fluorescence resonance energy transfer (FRET) showed substantial changes in distances between Cys-60 or 250 of troponin T (TnT) and Gln-41 or Cys-374 of actin on wild-type thin filaments corresponding to three states of thin filaments [Kimura et al. (2002) J. Biochem. 132, 93-102]. Troponin T movement on mutant thin filaments reconstituted with D234Tm was compared with that on wild-type thin filaments to understand from which the functional deficiency of mutant thin filaments derives. The Ca(2+)-induced changes in distances between Cys-250 of TnT and Gln-41 or Cys-374 of F-actin were smaller on mutant thin filaments than on wild-type thin filaments. On the other hand, the distances between Cys-60 of TnT and Gln-41 or Cys-374 of F-actin on mutant thin filaments did not change at all regardless of whether Ca(2+) was present. Thus, FRET showed that the Ca(2+)-induced movement of TnT was severely impaired on mutant thin filaments. The rigor binding of myosin subfragment 1 (S1) increased the distances when the thin filaments were fully decorated with S1 in the presence and absence of Ca(2+). However, plots of the extent of S1-incuced movement of TnT against molar ratio of S1 to actin in the presence and absence of Ca(2+) showed that the S1-induced movement of TnT was also impaired on mutant thin filaments. The deficiency of TnT movement on mutant thin filaments causes the altered S1-induced movement of TnI, and mutant thin filaments consequently fail to activate the myosin-ATPase activity even in the presence of Ca(2+).