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.     

Ca2+ and ionic strength dependencies of S1-ADP binding to actin-tropomyosin-troponin: regulatory implications

Skeletal and cardiac muscle contraction are inhibited by the actin-associated complex of tropomyosin-troponin. Binding of Ca(2+) to troponin or binding of ATP-free myosin to actin reverses this inhibition. Ca(2+) and ATP-free myosin stabilize different tropomyosin-actin structural arrangements. The position of tropomyosin on actin affects the binding of ATP-free myosin to actin but does not greatly affect myosin-ATP binding. Ca(2+) and ATP-free myosin alter both the affinity of ATP-free myosin for actin and the kinetics of that binding. A parallel pathway model of regulation simulated the effects of Ca(2+) and ATP-free myosin binding on both equilibrium binding of myosin-nucleotide complexes to actin and the general features of ATPase activity. That model was recently shown to simulate the kinetics of myosin-S1 binding but the analysis was limited to a single condition because of the limited data available. We have now measured equilibrium binding and binding kinetics of myosin-S1-ADP to actin at a series of ionic strengths and free Ca(2+) concentrations. The parallel pathway model of regulation is consistent with those data. In that model the interaction between adjacent regulatory complexes fully saturated with Ca(2+) was destabilized and the inactive state of actin was stabilized at high ionic strength. These changes explain the previously observed change in binding kinetics with increasing ionic strength.     

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.     

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+).     

Ca(2+)- and S1-induced movement of troponin T on reconstituted skeletal muscle thin filaments observed by fluorescence energy transfer spectroscopy

Troponin T (TnT) is an essential component of troponin (Tn) for the Ca(2+)-regulation of vertebrate striated muscle contraction. TnT consists of an extended NH(2)-terminal domain that interacts with tropomyosin (Tm) and a globular COOH-terminal domain that interacts with Tm, troponin I (TnI), and troponin C (TnC). We have generated two mutants of a rabbit skeletal beta-TnT 25-kDa fragment (59-266) that have a unique cysteine at position 60 (N-terminal region) or 250 (C-terminal region). To understand the spatial rearrangement of TnT on the thin filament in response to Ca(2+) binding to TnC, we measured distances from Cys-60 and Cys-250 of TnT to Gln-41 and Cys-374 of F-actin on the reconstituted thin filament by using fluorescence resonance energy transfer (FRET). The distances from Cys-60 and Cys-250 of TnT to Gln-41 of F-actin were 39.5 and 30.0 A, respectively in the absence of Ca(2+), and increased by 2.6 and 5.8 A, respectively upon binding of Ca(2+) to TnC. The rigor binding of myosin subfragment 1 (S1) further increased these distances by 4 and 5 A respectively, when the thin filaments were fully decorated with S1. This indicates that not only the C-terminal but also the N-terminal region of TnT showed the Ca(2+)- and S1-induced movement, and the C-terminal region moved more than N-terminal region. In the absence of Ca(2+), the rigor S1 binding also increased the distances to the same extent as the presence of Ca(2+) when the thin filaments were fully decorated with S1. The addition of ATP completely reversed the changes in FRET induced by rigor S1 binding both in the presence and absence of Ca(2+). However, plots of the extent of S1-induced conformational change vs. molar ratio of S1 to actin showed hyperbolic curve in the presence of Ca(2+) but sigmoidal curve in the absence of Ca(2+). FRET measurement of the distances from Cys-60 and Cys-250 of TnT to Cys-374 of actin showed almost the same results as the case of Gln-41 of actin. The present FRET measurements demonstrated that not only TnI but also TnT change their positions on the thin filament corresponding to three states of thin filaments (relaxed, Ca(2+)-induced or closed, and S1-induced or open states).     

Ca-Dependent Photocrosslinking of Tropomyosin Residue 146 to Residues 157-163 in the C-Terminal Domain of Troponin I in Reconstituted Skeletal Muscle Thin Filaments

The Ca²⁺-dependent interaction of troponin I (TnI) with actin·tropomyosin (Tm) in muscle thin filaments is a critical step in the regulation of muscle contraction. Previous studies have suggested that, in the absence of Ca²⁺, TnI interacts with Tm and actin in reconstituted muscle thin filaments, maintaining Tm at the outer domain of actin and blocking myosin-actin interaction. To obtain direct evidence for this Tm-TnI interaction, we performed photochemical crosslinking studies using Tm labeled with 4-maleimidobenzophenone at position 146 or 174 (Tm*146 or Tm*174, respectively), reconstituted with actin and troponin [composed of TnI, troponin T (TnT), and troponin C] or with actin and TnI. After near-UV irradiation, SDS gels of the Tm*146-containing thin filament showed three new high-molecular-weight bands determined to be crosslinked products Tm*146-TnI, Tm*146-troponin C, and Tm*146-TnT using fluorescence-labeled TnI, mass spectrometry, and Western blot analysis. While Tm*146-TnI was produced only in the absence of Ca²⁺, the production of other crosslinked species did not show Ca²⁺ dependence. Tm*174 mainly crosslinked to TnT. In the absence of actin, a similar crosslinking pattern was obtained with a much lower yield. A tryptic peptide from Tm*146-TnI with a molecular mass of 2601.2 Da that was not present in the tryptic peptides of Tm*146 or TnI was identified using HPLC and matrix-assisted laser desorption/ionization time-of-flight. This was shown, using absorption and fluorescence spectroscopy, to be the 4-maleimidobenzophenone-labeled peptide from Tm crosslinked to TnI peptide 157-163. These data, which show that a region in the C-terminal domain of TnI interacts with Tm in the absence of Ca²⁺, support the hypothesis that a TnI-Tm interaction maintains Tm at the outer domain of actin and will help efforts to localize troponin in actin·Tm muscle thin filaments.     

Calmidazolium selectively inhibits exocytotic glutamate release evoked by P2X7 receptor activation

We previously observed that activation of presynaptic P2X7 receptors located on rat cerebrocortical nerve terminals induced the release of glutamate through different modes: the channel conformation allowing Ca(2+) entry triggered exocytotic release, while the receptor itself functioned as a permeation pathway for the non-exocytotic glutamate release. Considering that exocytotic and non-exocytotic glutamate release evoked by the activation of P2X7 receptors might play a role in the control of glutamatergic synapses, we investigated whether calmidazolium (which has been found to inhibit small cation currents through recombinant P2X7 receptors, but not organic molecule permeation) could distinguish between P2X7-related exocytotic and non-exocytotic modes of glutamate release. We found that calmidazolium inhibited the intrasynaptosomal Ca(2+) response to P2X7 receptor activation and the Ca(2+)-dependent exocytotic glutamate release from rat cerebrocortical nerve terminals, but was ineffective against the Ca(2+)-independent glutamate release. The P2X7 competitive antagonist A-438079 eliminated both exocytotic and non-exocytotic P2X7 receptor-evoked glutamate release. Selective inhibition of exocytotic glutamate release indicates that calmidazolium inhibits events dependent on the function of native rat P2X7 receptors as Ca(2+) channels, and suggests that it can be used as a tool to dissociate P2X7-evoked exocytotic from non-exocytotic glutamate release.     

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.     

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.     

Bi-directional regulation of emodin and quercetin on smooth muscle myosin of gizzard

This study is to reveal the characteristics of bidirectional regulation of emodin (1,3,8-trihydroxy-6-methyl-anthraquinone) and quercetin on gizzard smooth muscle myosin. Our results indicate that: (a) emodin demonstrates stimulatory effects, and quercetin produces inhibitory effects on myosin phosphorylation and Mg(2+)-ATPase activities of Ca(2+)/calmodulin-dependent phosphorylated myosin in a dose-dependent manner; (b) a combination of emodin and quercetin enhances phosphorylation and Mg(2+)-ATPase activities for partially phosphorylated myosin and inhibits those activities for fully phosphorylated myosin; (c) 1-(5-Chloronaphthalene-1-sulfonyl)-1H2-hexahydro-1,4-diazepine inhibits myosin phosphorylation in the presence of emodin and/or quercetin. A combination of emodin and quercetin indicates its potential for modulating gastric-intestinal smooth muscle.     

Mechanism of formation of actomyosin interface

Force generation in muscle results from binding of myosin to F-actin. ATP binding to myosin provides energy to dissociate actomyosin complex while the hydrolysis of ATP is needed for re-binding of myosin to F-actin. At the end of each cycle myosin and actin form a tight complex with a substantial interface area. We investigated the dynamics of formation of actomyosin interface in presence and absence of nucleotides by quenched flow cross-linking technique. We showed previously that myosin head (subfragment 1, S1) directly interacts with at least two monomers in the actin filament. The quenched flow cross-linking experiments revealed that the initial contact (in presence or absence of nucleotides) occurs between loop 635-647 of S1 and 1-12 N-terminal residues of one actin and, then, the second contact forms between loop 567-574 of S1 and the N terminus of the second actin. The distance between these two loops in S1 corresponds to the distance between N termini of two actins in the same strand (53 A) but is smaller than that between two actins from the different strands (102 A). The formation of the actomyosin complex proceeds in ordered sequence: S1 initially binds to one actin then binds with the second actin located in the same strand but probably closer to the barbed end of F-actin. The presence of nucleotides slows down the interaction of S1 with the second actin, which correlates with recently proposed cleft movement in a 50 kDa domain of S1. The sequential mechanism of formation of actomyosin interface starting from one end and developing towards the barbed end might be involved in force generation and directional movement in actin-myosin system.     

Distances between tropomyosin sites across the muscle thin filament using luminescence resonance energy transfer: evidence for tropomyosin flexibility

To obtain information about the interaction of tropomyosin (Tm) with actin associated with the regulatory states of the muscle thin filament, we used luminescence resonance energy transfer (LRET) between Tb(3+) as a donor and rhodamine as an acceptor. A novel Tb(3+) chelator, S-(2-nitro-5-thiobenzoate)cysteaminyl-DTPA-Cs124, was synthesized, which specifically labels Cys groups in proteins. With the Tb chelate as the donor and tetramethylrhodamine-5-maleimide as the acceptor, both bound to specific Cys groups of Tm, we obtained 67 A as the distance between Tm's across the actin filament, a much shorter value than that obtained from structural studies (72-86 A). The difference appears to be due to submillisecond motion associated with Tm flexibility, which brings the probes closer during the millisecond lifetime of the donor. Ca(2+) did not change the energy transfer with the reconstituted thin filament, but myosin subfragment 1 decreased the transfer, consistent with either a 5-6 A increase in distance or, more likely, a decrease in flexibility.     

The role of PML in the control of apoptotic cell fate: a new key player at ER-mitochondria sites

The development of malignant tumors results from deregulated proliferation or an inability of cells to undergo apoptotic cell death. Experimental works of the past decade have highlighted the importance of calcium (Ca(2+)) in the regulation of apoptosis. Several studies indicate that the Ca(2+) content of the endoplasmic reticulum (ER) determines the cell's sensitivity to apoptotic stress and perturbation of ER Ca(2+) homeostasis appears to be a key component in the development of several pathological situations. Sensitivity to apoptosis depends on the ability of cells to transfer Ca(2+) from the ER to the mitochondria. The physical platform for the interplay between the ER and mitochondria is a domain of the ER called the mitochondria-associated membranes (MAMs). The disruption of these contact sites has profound consequences for cellular function, such as imbalances of intracellular Ca(2+) signaling, cellular stress, and disrupted apoptosis progression. The promyelocytic leukemia (PML) protein has been previously recognized as a critical and essential regulator of multiple apoptotic response. Nevertheless, how PML would exert such broad and fundamental role in apoptosis remained for long time a mystery. In this review, we will discuss how recent results demonstrate that the elusive mechanism whereby the PML tumor suppressor exerts its essential role in apoptosis triggered by Ca(2+)-dependent stimuli can be attributed to its unexpected and fundamental role at MAMs in the control of the functional cross-talk between ER and mitochondria.     

Voltage- and calcium-dependent inactivation of calcium channels in Lymnaea neurons.

Ca(2+) channel inactivation in the neurons of the freshwater snail, Lymnaea stagnalis, was studied using patch-clamp techniques. In the presence of a high concentration of intracellular Ca(2+) buffer (5 mM EGTA), the inactivation of these Ca(2+) channels is entirely voltage dependent; it is not influenced by the identity of the permeant divalent ions or the amount of extracellular Ca(2+) influx, or reduced by higher levels of intracellular Ca(2+) buffering. Inactivation measured under these conditions, despite being independent of Ca(2+) influx, has a bell-shaped voltage dependence, which has often been considered a hallmark of Ca(2+)-dependent inactivation. Ca(2+)-dependent inactivation does occur in Lymnaea neurons, when the concentration of the intracellular Ca(2+) buffer is lowered to 0.1 mM EGTA. However, the magnitude of Ca(2+)-dependent inactivation does not increase linearly with Ca(2+) influx, but saturates for relatively small amounts of Ca(2+) influx. Recovery from inactivation at negative potentials is biexponential and has the same time constants in the presence of different intracellular concentrations of EGTA. However, the amplitude of the slow component is selectively enhanced by a decrease in intracellular EGTA, thus slowing the overall rate of recovery. The ability of 5 mM EGTA to completely suppress Ca(2+)-dependent inactivation suggests that the Ca(2+) binding site is at some distance from the channel protein itself. No evidence was found of a role for serine/threonine phosphorylation in Ca(2+) channel inactivation. Cytochalasin B, a microfilament disrupter, was found to greatly enhance the amount of Ca(2+) channel inactivation, but the involvement of actin filaments in this effect of cytochalasin B on Ca(2+) channel inactivation could not be verified using other pharmacological compounds. Thus, the mechanism of Ca(2+)-dependent inactivation in these neurons remains unknown, but appears to differ from those proposed for mammalian L-type Ca(2+) channels.     

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.     

Functional coupling of Ca(2+) channels to ryanodine receptors at presynaptic terminals. Amplification of exocytosis and plasticity

Ca(2+)-induced Ca(2+) release (CICR) enhances a variety of cellular Ca(2+) signaling and functions. How CICR affects impulse-evoked transmitter release is unknown. At frog motor nerve terminals, repetitive Ca(2+) entries slowly prime and subsequently activate the mechanism of CICR via ryanodine receptors and asynchronous exocytosis of transmitters. Further Ca(2+) entry inactivates the CICR mechanism and the absence of Ca(2+) entry for >1 min results in its slow depriming. We now report here that the activation of this unique CICR markedly enhances impulse-evoked exocytosis of transmitter. The conditioning nerve stimulation (10-20 Hz, 2-10 min) that primes the CICR mechanism produced the marked enhancement of the amplitude and quantal content of end-plate potentials (EPPs) that decayed double exponentially with time constants of 1.85 and 10 min. The enhancement was blocked by inhibitors of ryanodine receptors and was accompanied by a slight prolongation of the peak times of EPP and the end-plate currents estimated from deconvolution of EPP. The conditioning nerve stimulation also enhanced single impulse- and tetanus-induced rises in intracellular Ca(2+) in the terminals with little change in time course. There was no change in the rate of growth of the amplitudes of EPPs in a short train after the conditioning stimulation. On the other hand, the augmentation and potentiation of EPP were enhanced, and then decreased in parallel with changes in intraterminal Ca(2+) during repetition of tetani. The results suggest that ryanodine receptors exist close to voltage-gated Ca(2+) channels in the presynaptic terminals and amplify the impulse-evoked exocytosis and its plasticity via CICR after Ca(2+)-dependent priming.     

Modification of Lys-237 on actin by 2,4-pentanedione. Alteration of the interaction of actin with tropomyosin

It has been possible to specifically label rabbit skeletal muscle actin at Lys-237 with 2,4-pentanedione, producing an enamine. This reaction can be reversed with hydroxylamine. The modification can be carried out with actin in either the G- or F-forms and does not affect polymerization-depolymerization. The modification does affect, however, the interaction of tropomyosin (Tm) with the modified F-actin. In the absence of Ca2+ and Mg2+ (mu = 0.12), Tm failed to bind to the modified F-actin whereas it did bind to unmodified F-actin (1 Tm:7 actins). Tm binding could be restored under these conditions by the addition of either troponin (Tn), Mg2+, or Mg2+ and Ca2+. Under certain conditions, Tm alone has been shown to inhibit actin-activated heavy meromyosin (HMM)-Mg2+-ATPase. This inhibition did not occur with the modified F-actin even though Tm was bound (approximately 1 Tm:7 actins). Even when Tn was added to this system (in the absence of Ca2+), no inhibition of ATPase could be observed. Thus, this modification appears to prevent F-actin X Tm from assuming the "blocking" inhibitory position (conformation). In addition, Tn appears to enhance the activation of heavy meromyosin-Mg2+-ATPase by the modified F-actin X Tm complex whether Ca2+ is present or not. This state may be analogous to the potentiated state (Murray, J. M., Knox, M. K., Trueblood, C. E., and Weber, A. (1982) Biochemistry 27, 906-915) seen with myosin subfragment 1-saturated actin at low ATP levels. Thus, using modified and unmodified F-actin, it is possible to produce three Tm X actin states: off (F-actin X Tm), on (modified F-actin X Tm), and "potentiated" (modified F-actin X Tm X Tn).     

Dilated cardiomyopathy mutations in α-tropomyosin inhibit its movement during the ATPase cycle

The Glu40Lys and Glu54Lys mutations in α-tropomyosin cause dilated cardiomyopathy (DCM). Functional analysis has demonstrated that both mutations decrease thin filament Ca²⁺-sensitivity and that Glu40Lys reduces maximum activation. To understand the molecular mechanism underlying these changes, we labeled wild type α-tropomyosin and both mutants at Cys190 with 5-iodoacetamide-fluorescein and incorporated the labeled proteins into ghost muscle fibers. Using the polarized fluorimetry, the position of the labeled tropomyosins on the thin filament and their affinity for actin were measured and the change in these parameters at different stages of the ATPase cycle determined. Both DCM mutations were found to shift tropomyosin towards the periphery of thin filament and to change the affinity of tropomyosin for actin; during the ATPase cycle the amplitude of tropomyosin movement was reduced and at some stages of the cycle even reversed. The correlation of these structural changes with the observed function effects is discussed.     

Ca2+-induced structural changes in phosphorylase kinase detected by small-angle X-ray scattering

Phosphorylase kinase (PhK), a 1.3-MDa (alphabetagammadelta)(4) hexadecameric complex, is a Ca(2+)-dependent regulatory enzyme in the cascade activation of glycogenolysis. PhK comprises two arched (alphabetagammadelta)(2) octameric lobes that are oriented back-to-back with overall D(2) symmetry and joined by connecting bridges. From chemical cross-linking and electron microscopy, it is known that the binding of Ca(2+) by PhK perturbs the structure of all its subunits and promotes redistribution of density throughout both its lobes and bridges; however, little is known concerning the interrelationship of these effects. To measure structural changes induced by Ca(2+) in the PhK complex in solution, small-angle X-ray scattering was performed on nonactivated and Ca(2+)-activated PhK. Although the overall dimensions of the complex were not affected by Ca(2+), the cation did promote a shift in the distribution of the scattering density within the hydrated volume occupied by the PhK molecule, indicating a Ca(2+)-induced conformational change. Computer-generated models, based on elements of the known structure of PhK from electron microscopy, were constructed to aid in the interpretation of the scattering data. Models containing two ellipsoids and four cylinders to represent, respectively, the lobes and bridges of the PhK complex provided theoretical scattering profiles that accurately fit the experimental data. Structural differences between the models representing the nonactivated and Ca(2+)-activated conformers of PhK are consistent with Ca(2+)-induced conformational changes in both the lobes and the interlobal bridges.