Simulation of calcium sparks in cut skeletal muscle fibers of the frog

Spark mass, the volume integral of Delta F/F, was investigated theoretically and with simulations. These studies show that the amount of Ca2+ bound to fluo-3 is proportional to mass times the total concentration of fluo-3 ([fluo-3T]); the proportionality constant depends on resting Ca2+ concentration ([Ca2+]R). In the simulation of a Ca2+ spark in an intact frog fiber with [fluo-3T] = 100 microM, fluo-3 captures approximately one-fourth of the Ca2+ released from the sarcoplasmic reticulum (SR). Since mass in cut fibers is several times that in intact fibers, both with similar values of [fluo-3T] and [Ca2+]R, it seems likely that SR Ca2+ release is larger in cut fiber sparks or that fluo-3 is able to capture a larger fraction of the released Ca2+ in cut fibers, perhaps because of reduced intrinsic Ca2+ buffering. Computer simulations were used to identify these and other factors that may underlie the differences in mass and other properties of sparks in intact and cut fibers. Our spark model, which successfully simulates calcium sparks in intact fibers, was modified to reflect the conditions of cut fiber measurements. The results show that, if the protein Ca2+-buffering power of myoplasm is the same as that in intact fibers, the Ca2+ source flux underlying a spark in cut fibers is 5-10 times that in intact fibers. Smaller source fluxes are required for less buffer. In the extreme case in which Ca2+ binding to troponin is zero, the source flux needs to be 3-5 times that in intact fibers. An increased Ca2+ source flux could arise from an increase in Ca2+ flux through one ryanodine receptor (RYR) or an increase in the number of active RYRs per spark, or both. These results indicate that the gating of RYRs, or their apparent single channel Ca2+ flux, is different in frog cut fibers--and, perhaps, in other disrupted preparations--than in intact fibers.     

Block of contracture in skinned frog skeletal muscle fibers by calcium antagonists

The ability of a number of calcium antagonistic drugs including nitrendipine, D600, and D890 to block contractures in single skinned (sarcolemma removed) muscle fibers of the frog Rana pipiens has been characterized. Contractures were initiated by ionic substitution, which is thought to depolarize resealed transverse tubules in this preparation. Depolarization of the transverse tubules is the physiological trigger for the release of calcium ion from the sarcoplasmic reticulum and thus of contractile protein activation. Since the transverse tubular membrane potential cannot be measured in this preparation, tension development is used as a measure of activation. Once stimulated, fibers become inactivated and do not respond to a second stimulus unless allowed to recover or reprime (Fill and Best, 1988). Fibers exposed to calcium antagonists while fully inactivated do not recover from inactivation (became blocked or paralyzed). The extent of drug-induced block was quantified by comparing the height of individual contractures. Reprimed fibers were significantly less sensitive to block by both nitrendipine (10 degrees C) and D600 (10 and 22 degrees C) than were inactivated fibers. Addition of D600 to fibers recovering from inactivation stopped further recovery, confirming preferential interaction of the drug with the inactivated state. A concerted model that assumed coupled transitions of independent drug-binding sites from the reprimed to the inactivated state adequately described the data obtained from reprimed fibers. Photoreversal of drug action left fibers inactivated even though the drug was initially added to fibers in the reprimed state. This result is consistent with the prediction from the model. The estimated KI for D600 (at 10 degrees and 22 degrees C) and for D890 (at 10 degrees C) was approximately 10 microM. The estimated KI for nitrendipine paralysis of inactivated fibers at 10 degrees C was 16 nM. The sensitivity of reprimed fibers to paralysis by D600 and D890 was similar. However, inactivated fibers were significantly less sensitive to the membrane-impermeant derivative (D890) than to the permeant species (D600), which suggests a change in the drug-binding site or its environment during the inactivation process. The enantomeric dihydropyridines (+) and (-) 202-791, reported to be calcium channel agonists and antagonists, respectively, both caused paralysis, which suggests that blockade of a transverse tubular membrane calcium flux is not the mechanism responsible for antagonist-induced paralysis. The data support a model of excitation-contraction coupling involving transverse tubular proteins that bind calcium antagonists.     

Effects of tetracaine on voltage-activated calcium sparks in frog intact skeletal muscle fibers

The properties of Ca(2+) sparks in frog intact skeletal muscle fibers depolarized with 13 mM [K(+)] Ringer's are well described by a computational model with a Ca(2+) source flux of amplitude 2.5 pA (units of current) and duration 4.6 ms (18 degrees C; Model 2 of Baylor et al., 2002). This result, in combination with the values of single-channel Ca(2+) current reported for ryanodine receptors (RyRs) in bilayers under physiological ion conditions, 0.5 pA (Kettlun et al., 2003) to 2 pA (Tinker et al., 1993), suggests that 1-5 RyR Ca(2+) release channels open during a voltage-activated Ca(2+) spark in an intact fiber. To distinguish between one and greater than one channel per spark, sparks were measured in 8 mM [K(+)] Ringer's in the absence and presence of tetracaine, an inhibitor of RyR channel openings in bilayers. The most prominent effect of 75-100 microM tetracaine was an approximately sixfold reduction in spark frequency. The remaining sparks showed significant reductions in the mean values of peak amplitude, decay time constant, full duration at half maximum (FDHM), full width at half maximum (FWHM), and mass, but not in the mean value of rise time. Spark properties in tetracaine were simulated with an updated spark model that differed in minor ways from our previous model. The simulations show that (a) the properties of sparks in tetracaine are those expected if tetracaine reduces the number of active RyR Ca(2+) channels per spark, and (b) the single-channel Ca(2+) current of an RyR channel is 相似文献   

Furosemide-sensitive cation transport in frog skeletal muscle fibers

Furosemide-inhibitable components in unidirectional cation fluxes have been identified in frog skeletal muscle. In sodium loaded muscles, placed in sodium-free rubidium lithium media, furosemide (1 mM) inhibits partially rubidium and lithium influxes as well as potassium and sodium outfluxes. The furosemide-inhibitable components were found to depend on the presence of ouabain. They were greatly diminished in sodium-free magnesium media and were present in chloride-free nitrate containing media. The dependence of furosemide-inhibitable sodium efflux on internal sodium content was also described.     

Resting myoplasmic free calcium in frog skeletal muscle fibers estimated with fluo-3.

Fluo-3 is an unusual tetracarboxylate Ca2+ indicator. For recent lots supplied by Molecular Probes Inc. (Eugene, OR), FMAX, the fluorescence intensity of the indicator in its Ca(2+)-bound form, is approximately 200 times that of FMIN, the fluorescence intensity of the indicator in its Ca(2+)-free form. (For earlier lots, impurities may account for the smaller reported values of FMAX/FMIN, 36-40). We have injected fluo-3 from a high-purity lot into intact single fibers from frog muscle and measured the indicator's absorbance and fluorescence signals at rest (A and F, respectively) and changes in absorbance and fluorescence following action potential stimulation (delta A and delta F signals substantially lagged behind that of the myoplasmic free Ca2+ transient. Our analysis of fluo-3's signals from myoplasm therefore focused on information about the level of resting myoplasmic free [Ca2+] ([Ca2+]r). From A, delta A, and in vitro estimates of fluo-3's molar extinction coefficients, the change in the fraction of fluo-3 in the Ca(2+)-bound form during activity (delta f) was estimated. From delta f, delta F, and F, the fraction of the indicator in the Ca(2+)-bound form in the resting fiber (fr) was estimated by fr = (delta f x F/delta F) + (1-FMAX/FMIN)-1. Since FMAX/FMIN is large, the contribution of the second term to the estimate of fr is small. At 16 degrees C, the mean value (mean +/- S.E.) of fr was 0.086 +/- 0.004 (N = 15). From two estimates of the apparent dissociation constant of fluo-3 for Ca2+ in the myoplasm, 1.09 and 2.57 microM, the average value of [Ca2+]r is calculated to be 0.10 and 0.24 microM, respectively. The smaller of these estimates lies near the upper end of the range of values for [Ca2+]r in frog fibers (0.02-0.12 microM) estimated by others with aequorin and Ca(2+)-selective electrodes. The larger of the estimates lies within the range of values (0.2-0.3 microM) previously estimated in this laboratory with fura red. We conclude that [Ca2+]r in frog fibers is at least 0.1 microM and possibly as large as 0.3 microM.     

Localization of acid organelles in frog skeletal muscle fibers

By means of fluorescent and phase-contrast microscopy the distribution of acid membrane organelles in normal and vacuolated frog skeletal muscle fibers has been studied. The vacuolation of the T-system was produced by loading and subsequent removal of glycerol (80-110 mM), or it appeared as a result of Zenker's necrosis. Acridine orange (AO) was used as a marker for acid intracellular compartments. AO accumulated in granules localized near the nuclear poles (more seldom around the nucleus)' and in the intermyofibrillar spaces. Typically the AO granules make up short longitudinal chains or regular pairs, where the distances between neighboring granules are short-dated to sarcomere lengths. Almost all granules emit in red, but about one third of them simultaneously emit in green, which is characteristic of AO monomers. In the vicinity of necrotic boundary or under the influence of brefeldin A, a green component of fluorescence appears in most granules. Treatment with monensin leads to granule disappearance. Vacuoles accompanying the glycerol treatment or developing of necrosis do not accumulate AO and exert no effect on the localization of AO-granules. The nature of cellular organelles accumulating AO in skeletal muscle fibers is discussed.     

Comparison of simulated and measured calcium sparks in intact skeletal muscle fibers of the frog

Calcium sparks in frog intact skeletal muscle fibers were modeled as stereotypical events that arise from a constant efflux of Ca(2+) from a point source for a fixed period of time (e.g., 2.5 pA of Ca(2+) current for 4.6 ms; 18 degrees C). The model calculates the local changes in the concentrations of free Ca(2+) and of Ca(2+) bound to the major intrinsic myoplasmic Ca(2+) buffers (troponin, ATP, parvalbumin, and the SR Ca(2+) pump) and to the Ca(2+) indicator (fluo-3). A distinctive feature of the model is the inclusion of a binding reaction between fluo-3 and myoplasmic proteins, a process that strongly affects fluo-3's Ca(2+)-reaction kinetics, its apparent diffusion constant, and hence the morphology of sparks. DeltaF/F (the change in fluo-3's fluorescence divided by its resting fluorescence) was estimated from the calculated changes in fluo-3 convolved with the microscope point-spread function. To facilitate comparisons with measured sparks, noise and other sources of variability were included in a random repetitive fashion to generate a large number of simulated sparks that could be analyzed in the same way as the measured sparks. In the initial simulations, the binding of Ca(2+) to the two regulatory sites on troponin was assumed to follow identical and independent binding reactions. These simulations failed to accurately predict the falling phase of the measured sparks. A second set of simulations, which incorporated the idea of positive cooperativity in the binding of Ca(2+) to troponin, produced reasonable agreement with the measurements. Under the assumption that the single channel Ca(2+) current of a ryanodine receptor (RYR) is 0.5-2 pA, the results suggest that 1-5 active RYRs generate an average Ca(2+) spark in a frog intact muscle fiber.     

Use of fura red as an intracellular calcium indicator in frog skeletal muscle fibers.

Fura red, a fluorescent Ca2+ indicator with absorbance bands at visible wavelengths, was injected into intact single muscle fibers that had been stretched to a long sarcomere length (approximately 3.8 microns) and bathed in a 'high-Ca2+' Ringer ([Ca2+] = 11.8 mM). From fura red's slow diffusion coefficient in myoplasm, 0.16 (+/- 0.01, SEM) x 10(-6) cm2 s-1 (N = 5; 16 degrees C), it is estimated that approximately 85% of the indicator molecules are bound to muscle constituents of large molecular weight. Binding appears to elevate, by 3- to 4-fold, the indicator's apparent dissociation constant for Ca2+ (KD), which is estimated to be 1.1-1.6 microM in myoplasm. Fura red's myoplasmic absorbance spectrum was used to estimate fr, the fraction of fura red molecules in the Ca2+-bound form at rest. In 3 fibers thought to be minimally damaged by the micro-injection, fr was estimated to be 0.15 (+/- 0.01). Thus, resting myoplasmic free [Ca2+] ([Ca2+]r) is estimated to be 0.19-0.28 microM. For fibers in normal Ringer solution ([Ca2+] = 1.8 mM), at shorter sarcomere length (approximately 2.7 microns), and containing a nonperturbing concentration of indicator (< or = 0.2 mM), [Ca2+]r is estimated to be 0.18-0.27 microM. This range is higher than estimated previously in frog fibers with other techniques. In 6 fibers, R, the indicator's fluorescence ratio signal (equal to the emission intensity measured with 420 nm excitation divided by that measured with 480 nm excitation), was measured at rest and following electrical stimulation and compared with absorbance measurements made from the same fiber region. The analysis implies that RMIN and RMAX (the values of R that would be measured if all indicator molecules were in the Ca(2+)-free and Ca(2+)-bound states, respectively) were substantially smaller in myoplasm than in calibration solutions lacking muscle proteins. Several methods for estimation of [Ca2+]r from R are analyzed and discussed.     

Connectin filaments in stretched skinned fibers of frog skeletal muscle

Indirect immunofluorescence microscopy of highly stretched skinned frog semi-tendinous muscle fibers revealed that connectin, an elastic protein of muscle, is located in the gap between actin and myosin filaments and also in the region of myosin filaments except in their centers. Electron microscopic observations showed that there were easily recognizable filaments extending from the myosin filaments to the I band region and to Z lines in the myofibrils treated with antiserum against connectin. In thin sections prepared with tannic acid, very thin filaments connected myosin filaments to actin filaments. These filaments were also observed in myofibrils extracted with a modified Hasselbach-Schneider solution (0.6 M KCl, 0.1 M phosphate buffer, pH 6.5, 2 mM ATP, 2 mM MgCl2, and 1 mM EGTA) and with 0.6 M Kl. SDS PAGE revealed that connectin (also called titin) remained in extracted myofibrils. We suggest that connectin filaments play an important role in the generation of tension upon passive stretch. A scheme of the cytoskeletal structure of myofibrils of vertebrate skeletal muscle is presented on the basis of our present information of connectin and intermediate filaments.     

A-band shortening in single fibers of frog skeletal muscle.

The question of whether A-bands shorten during contraction was investigated using two methods: high-resolution polarization microscopy and electron microscopy. During shortening from extended sarcomere lengths in the passive state, sarcomere-length changes were essentially accounted for by I-band shortening. During active shortening under otherwise identical conditions, the sarcomere length change was taken up approximately equally by A- and I-bands. Several potential artifacts that could give rise to apparent A-band shortening were considered and judged unlikely. Results obtained with polarization microscopy were similar to those obtained with electron microscopy. Thus, modest but significant thick filament shortening appears to occur during active sarcomere shortening under physiological conditions.     

Stiffness and force in activated frog skeletal muscle fibers.

Single fibers, isolated intact from frog skeletal muscles, were held firmly very near to each end by stiff metal clasps fastened to the tendons. The fibers were then placed horizontally between two steel hooks inserted in eyelets of the tendon clasps. One hook was attached to a capacitance gauge force transducer (resonance frequency up to approximately 50 kHz) and the other was attached to a moving-coil length changer. This allowed us to impose small, rapid releases (complete in less than 0.15 ms) and high frequency oscillations (up to 13 kHz) to one end of a resting or contracting fiber and measure the consequences at the other end with fast time resolution at 4 to 6 degrees C. The stiffness of short fibers (1.8-2.6 mm) was determined directly from the ratio of force to length variations produced by the length changer. The resonance frequency of short fibers was so high (approximately 40 kHz) that intrinsic oscillations were not detectably excited. The stiffness of long fibers, on the other hand, was calculated from measurement of the mechanical resonance frequency of a fiber. Using both short and long fibers, we measured the sinusoids of force at one end of a contracting fiber that were produced by relatively small sinusoidal length changes at the other end. The amplitudes of the sinusoidal length changes were small compared with the size of step changes that produce nonlinear force-extension relations. The sinusoids of force from long fibers changed amplitude and shifted phase with changes in oscillation frequency in a manner expected of a transmission line composed of mass, compliance, and viscosity, similar to that modelled by (Ford, L. E., A. F. Huxley, and R. M. Simmons, 1981, J. Physiol. (Lond.), 311:219-249). A rapid release during the plateau of tetanic tension in short fibers caused a fall in force and stiffness, a relative change in stiffness that putatively was much smaller than that of force. Our results are, for the most part, consistent with the cross-bridge model of force generation proposed by Huxley, A. F., and R. M. Simmons (1971, Nature (Lond.), 213:533-538). However, stiffness in short fibers developed markedly faster than force during the tetanus rise. Thus our findings show the presence of one or more noteworthy cross-bridge states at the onset and during the rise of active tension towards a plateau in that attachment apparently is followed by a relatively long delay before force generation occurs.(ABSTRACT TRUNCATED AT 400 WORDS)     

Myoplasmic calcium transients monitored with purpurate indicator dyes injected into intact frog skeletal muscle fibers

Intact single twitch fibers from frog muscle were studied on an optical bench apparatus after microinjection with tetramethylmurexide (TMX) or purpurate-3,3' diacetic acid (PDAA), two compounds from the purpurate family of absorbance Ca2+ indicators previously used in cut muscle fibers (Maylie, J., M. Irving, N. L. Sizto, G. Boyarsky, and W. K. Chandler. 1987. J. Gen. Physiol. 89:145-176; Hirota, A., W. K. Chandler, P. L. Southwick, and A. S. Waggoner. 1989. J. Gen. Physiol. 94:597-631.) The apparent longitudinal diffusion constant of PDAA (mol wt 380) in myoplasm was 0.99 (+/- 0.04, SEM) x 10(-6) cm2 s-1 (16-17 degrees C), a value which suggests that 24-43% of the PDAA molecules were bound to myoplasmic constituents of large molecular weight. The corresponding values for TMX (mol wt 322) were 0.98 (+/- 0.05) x 10(-6) cm2 s-1 and 44-50%, respectively. Muscle membranes (surface and/or transverse-tubular) appear to be permeable to TMX and, to a lesser extent, to PDAA, since the total amount of indicator contained within a fiber decreased with time after injection. The average time constants for disappearance of indicator were 46 (+/- 7, SEM) min for TMX and 338 (+/- 82) min for PDAA. The fraction of indicator in the Ca2(+)-bound state in resting fibers was significantly different from zero for TMX (0.070 +/- 0.008) but not for PDAA (0.026 +/- 0.009). In in vitro calibrations PDAA but not TMX appeared to react with Ca2+ with 1:1 stoichiometry. In agreement with Hirota et al. (Hirota, A., W. K. Chandler, P. L. Southwick, and A. S. Waggoner. 1989. J. Gen. Physiol. 94:597-631), we conclude that PDAA is probably a more reliable myoplasmic Ca2+ indicator than TMX. In fibers that contained PDAA and were stimulated by a single action potential, the calibrated peak value of the myoplasmic free [Ca2+] transient (delta[Ca2+]) averaged 9.4 (+/- 0.6) microM, a value about fivefold larger than that calibrated with antipyrylazo III under otherwise identical conditions (Baylor, S. M., and S. Hollingworth. 1988. J. Physiol. 403:151-192). The fivefold difference is similar to that previously reported in cut fibers with antipyrylazo III and PDAA. Since in both intact and cut fibers the percentage of PDAA bound to myoplasmic constituents is considerably smaller than that found for antipyrylazo III, the PDAA calibration of delta[Ca2+] is likely to be more accurate. Interestingly, in intact fibers the peak value of delta[Ca2+] calibrated with either PDAA or antipyrylazo III is about half that calibrated in cut fibers.(ABSTRACT TRUNCATED AT 400 WORDS)     

Imaging of calcium transients in skeletal muscle fibers.

Epifluorescence images of Ca2+ transients elicited by electrical stimulation of single skeletal muscle fibers were studied with fast imaging techniques that take advantage of the large fluorescence signals emitted at relatively long wavelengths by the dyes fluo-3 and rhod-2 in response to binding of Ca2+ ions, and of the suitable features of a commercially available CCD video camera. The localized release of Ca2+ in response to microinjection of InsP3 was also monitored to demonstrate the adequate space and time resolutions of the imaging system. The time resolution of the imager system, although limited to the standard video frequency response, still proved to be adequate to investigate the fast Ca2+ release process in skeletal muscle fibers at low temperatures.     

Low myoplasmic Mg2+ potentiates calcium release during depolarization of frog skeletal muscle fibers.

The role of intracellular free magnesium concentration ([Mg2+]) in modulating calcium release from the sarcoplasmic reticulum (SR) was studied in voltage-clamped frog cut skeletal muscle fibers equilibrated with cut end solutions containing two calcium indicators, fura-2 and antipyrylazo III (AP III), and various concentrations of free Mg2+ (25 microM-1 mM) obtained by adding appropriate total amounts of ATP and magnesium to the solutions. Changes in AP III absorbance were used to monitor calcium transients, whereas fura-2 fluorescence was used to monitor resting calcium. The rate of release (Rrel) of calcium from the SR was calculated from the calcium transient and found to be increased in low internal [Mg2+]. After correcting for effects of calcium depletion from the SR and normalization to SR content, the mean values of the inactivatable and noninactivatable components of Rrel were increased by 163 and 46%, respectively, in low Mg2+. Independent of normalization to SR content, the ratio of inactivatable to noninactivatable components of Rrel was increased in low internal [Mg2+]. Both observations suggest that internal [Mg2+] preferentially modulates the inactivatable component of Rrel, which is thought to be due to calcium-induced calcium release from the SR. This could also explain the observation that, in low internal [Mg2+], the time to the peak of the calcium transient for a 5-ms depolarizing pulse was not very different from the time to the peak of the delta [Ca2+] for a 10-ms pulse of the same amplitude. Finally, in low internal [Mg2+], the calcium transient elicited by a short depolarizing pulse was in some cases clearly followed by a very slow rise of calcium after the end of the pulse. The observed effects of reduced [Mg2+] on calcium release are consistent with a removal of the inhibition that the normal 1 mM myoplasmic [Mg2+] exerts on calcium release in skeletal muscle fibers.     

A damped oscillation in the intramembranous charge movement and calcium release flux of frog skeletal muscle fibers

Asymmetric membrane currents and calcium transients were recorded simultaneously from cut segments of frog skeletal muscle fibers voltage clamped in a double Vaseline-gap chamber in the presence of high concentration of EGTA intracellularly. An inward phase of asymmetric currents following the hump component was observed in all fibers during the depolarization pulse to selected voltages (congruent to -45 mV). The average value of the peak inward current was 0.1 A/F (SEM = 0.01, n = 18), and the time at which it occurred was 34 ms (SEM = 1.8, n = 18). A second delayed outward phase of asymmetric current was observed after the inward phase, in those experiments in which hump component and inward phase were large. It peaked at more variable time (between 60 and 130 ms) with amplitude 0.02 A/F (SEM = 0.003, n = 11). The transmembrane voltage during a pulse, measured with a glass microelectrode, reached its steady value in less than 10 ms and showed no oscillations. The potential was steady at the time when the delayed component of asymmetric current occurred. ON and OFF charge transfers were equal for all pulse durations. The inward phase moved 1.4 nC/microF charge (SEM = 0.8, n = 6), or about one third of the final value of charge mobilized by these small pulses, and the second outward phase moved 0.7 nC/microF (SEM = 0.8, n = 6), bringing back about half of the charge moved during the inward phase. When repolarization intersected the peak of the inward phase, the OFF charge transfer was independent of the repolarization voltage in the range -60 to -90 mV. When both pre- and post-pulse voltages were changed between -120 mV and -60 mV, the equality of ON and OFF transfers of charge persisted, although they changed from 113 to 81% of their value at -90 mV. The three delayed phases in asymmetric current were also observed in experiments in which the extracellular solution contained Cd2+, La3+ and no Ca2+. Large increases in intracellular [Cl-] were imposed, and had no major effect on the delayed components of the asymmetric current. The Ca2+ transients measured optically and the calculated Ca2+ release fluxes had three phases whenever a visible outward phase followed the inward phase in the asymmetric current. Several interventions intended to interfere with Ca release, reduced or eliminated the three delayed phases of the asymmetric current.(ABSTRACT TRUNCATED AT 400 WORDS)     

Calcium sparks in intact skeletal muscle fibers of the frog.

Calcium sparks were studied in frog intact skeletal muscle fibers using a home-built confocal scanner whose point-spread function was estimated to be approximately 0.21 microm in x and y and approximately 0.51 microm in z. Observations were made at 17-20 degrees C on fibers from Rana pipiens and Rana temporaria. Fibers were studied in two external solutions: normal Ringer's ([K(+)] = 2.5 mM; estimated membrane potential, -80 to -90 mV) and elevated [K(+)] Ringer's (most frequently, [K(+)] = 13 mM; estimated membrane potential, -60 to -65 mV). The frequency of sparks was 0.04-0.05 sarcomere(-1) s(-1) in normal Ringer's; the frequency increased approximately tenfold in 13 mM [K(+)] Ringer's. Spark properties in each solution were similar for the two species; they were also similar when scanned in the x and the y directions. From fits of standard functional forms to the temporal and spatial profiles of the sparks, the following mean values were estimated for the morphological parameters: rise time, approximately 4 ms; peak amplitude, approximately 1 DeltaF/F (change in fluorescence divided by resting fluorescence); decay time constant, approximately 5 ms; full duration at half maximum (FDHM), approximately 6 ms; late offset, approximately 0.01 DeltaF/F; full width at half maximum (FWHM), approximately 1.0 microm; mass (calculated as amplitude x 1.206 x FWHM(3)), 1.3-1.9 microm(3). Although the rise time is similar to that measured previously in frog cut fibers (5-6 ms; 17-23 degrees C), cut fiber sparks have a longer duration (FDHM, 9-15 ms), a wider extent (FWHM, 1.3-2.3 microm), and a strikingly larger mass (by 3-10-fold). Possible explanations for the increase in mass in cut fibers are a reduction in the Ca(2+) buffering power of myoplasm in cut fibers and an increase in the flux of Ca(2+) during release.     

Anatomical distribution of voltage-dependent membrane capacitance in frog skeletal muscle fibers

Components of nonlinear capacitance, or charge movement, were localized in the membranes of frog skeletal muscle fibers by studying the effect of 'detubulation' resulting from sudden withdrawal of glycerol from a glycerol-hypertonic solution in which the muscles had been immersed. Linear capacitance was evaluated from the integral of the transient current elicited by imposed voltage clamp steps near the holding potential using bathing solutions that minimized tubular voltage attenuation. The dependence of linear membrane capacitance on fiber diameter in intact fibers was consistent with surface and tubular capacitances and a term attributable to the capacitance of the fiber end. A reduction in this dependence in detubulated fibers suggested that sudden glycerol withdrawal isolated between 75 and 100% of the transverse tubules from the fiber surface. Glycerol withdrawal in two stages did not cause appreciable detubulation. Such glycerol-treated but not detubulated fibers were used as controls. Detubulation reduced delayed (q gamma) charging currents to an extent not explicable simply in terms of tubular conduction delays. Nonlinear membrane capacitance measured at different voltages was expressed normalized to accessible linear fiber membrane capacitance. In control fibers it was strongly voltage dependent. Both the magnitude and steepness of the function were markedly reduced by adding tetracaine, which removed a component in agreement with earlier reports for q gamma charge. In contrast, detubulated fibers had nonlinear capacitances resembling those of q beta charge, and were not affected by adding tetracaine. These findings are discussed in terms of a preferential localization of tetracaine-sensitive (q gamma) charge in transverse tubule membrane, in contrast to a more even distribution of the tetracaine-resistant (q beta) charge in both transverse tubule and surface membranes. These results suggest that q beta and q gamma are due to different molecules and that the movement of q gamma in the transverse tubule membrane is the voltage-sensing step in excitation-contraction coupling.     

Modulation by caffeine of calcium-release microdomains in frog skeletal muscle fibers

The effects of caffeine on the process of excitation-contraction coupling in amphibian skeletal muscle fibers were investigated using the confocal spot detection technique. This method permits to carefully discriminate between caffeine effects on the primary sources of Ca2+ release at the Z-lines where the triads are located and secondary actions on other potential Ca Release sources. Our results demonstrate that 0.5 mM caffeine potentiates and prolongs localized action-potential evoked Ca2+ transients recorded at the level of the Z-lines, but that 1mM only prolongs them. The effects at both doses are reversible. At the level of the M-line, localized Ca2+ transients displayed more variability in the presence of 1 mM caffeine than in control conditions. At this dose of caffeine, extra-junctional sources of Ca2+ release also were observed occasionally.     

Cooperative binding of calcium to glycerinated skeletal muscle fibers

The binding of ⁴⁵Ca²⁺ to glycerinated rabbit psoas fibers was measured by means of a double isotope technique. With 5 mM Mg²⁺ (no ATP) binding was half-maximal at 1.4 · 10^?6M Ca²⁺ and the maximal amount bound was 1.6 μmol/g protein. At < 50% saturation, the Scatchard plot had a positive slope and the Hill coefficient was 2.2. At greater than 50% saturation, the Scatchard plot was linear with a negative slope (K′ = 0.8 · 10⁶ M^?1) and the Hill coefficient was 1.0. In the absence of Mg²⁺, binding was half-maximal at 3 · 10^?7 M Ca²⁺ and the maximal amount bound was 2.9 μmol/g protein. The Scatchard plot indicated two classes of sites with K′ values of about 2 · 10⁷ and 2 · 10⁶ M^?1. The Hill coefficient in the mid-saturation range was approx. 0.6. The data indicate that in the presence of Mg²⁺ binding to about half of the total Ca²⁺ binding sites is suppressed and there is a strong positive cooperativity involving half of the remaining sites.