An improved vaseline gap voltage clamp for skeletal muscle fibers

A Vaseline gap potentiometric recording and voltage clamp method is developed for frog skeletal muscle fibers. The method is based on the Frankenhaeuser-Dodge voltage clamp for myelinated nerve with modifications to improve the frequency response, to compensate for external series resistance, and to compensate for the complex impedance of the current-passing pathway. Fragments of single muscle fibers are plucked from the semitendinosus muscle and mounted while depolarized by a solution like CsF. After Vaseline seals are formed between fluid pools, the fiber ends are cut once again, the central region is rinsed with Ringer solution, and the feedback amplifiers are turned on. Errors in the potential and current records are assessed by direct measurements with microelectrodes. The passive properties of the preparation are simulated by the "disk" equivalent circuit for the transverse tubular system and the derived parameters are similar to previous measurements with microelectrodes. Action potentials at 5 degrees C are long because of the absence of delayed rectification. Their shape is approximately simulated by solving the disk model with sodium permeability in the surface and tubular membranes. Voltage clamp currents consist primarily of capacity currents and sodium currents. The peak inward sodium current density at 5 degrees C is 3.7 mA/cm2. At 5 degrees C the sodium currents are smoothly graded with increasing depolarization and free of notches suggesting good control of the surface membrane. At higher temperatures a small, late extra inward current appears for small depolarizations that has the properties expected for excitation in the transverse tubular system. Comparison of recorded currents with simulations shows that while the transverse tubular system has regenerative sodium currents, they are too small to make important errors in the total current recorded at the surface under voltage clamp at low temperature. The tubules are definitely not under voltage clamp control.     

Kinetics of contractile activation in voltage clamped frog skeletal muscle fibers.

Excitation-contraction coupling events leading to the onset of contraction were studied in single skeletal frog muscle fibers. This entailed the simultaneous measurement of the changes in intracellular calcium concentration using antipyrylazo III and fura-2, isometric force, and clamp voltage in a modified single vaseline gap chamber for the first time. The calcium transients were incorporated into an analysis of calcium binding to regulatory sites of troponin C (TnC) that permitted both a linear and a cooperative interaction. The analysis assumed that the onset of mechanical activation corresponds with a particular TnC saturation with calcium setting constraints for the calcium binding parameters of the regulatory sites. Using a simple model that successfully reproduced both the time course and the relative amplitudes of the measured isometric force transients over a wide membrane potential range, k(off) of TnC was calculated to be 78 s(-1) for the cooperative model at 10 degrees C. Together with the above constraints this gave a dissociation constant of 8.8 +/- 2.5 microM and a relative TnC saturation at the threshold (Sth) that would cause just detectable movement of 0.17 +/- 0.03 (n = 13; mean +/- SE). The predictions were found to be independent of the history of calcium binding to the regulatory sites. The observed delay between reaching Sth and the onset of fiber movement (8.7 +/- 1.0 ms; mean +/- SE, n = 37; from seven fibers) was independent of the membrane potential giving an upper estimate for the delay in myofilament activation. We thus emerge with quantitative values for the calcium binding to the regulatory sites on TnC under maintained structural conditions close to those in vivo.     

Calcium release in frog cut twitch fibers exposed to different ionic environments under voltage clamp.

Calcium release was measured in highly stretched frog cut twitch fibers mounted in a double Vaseline-gap voltage clamp chamber, with the internal solution containing 20 mM EGTA plus 0.4 or 1.8 mM added calcium. Rise in myoplasmic [Ca(2+)] was monitored with antipyrylazo III as the indicator at a temperature of 13 to 14 degrees C. The waveform of calcium release rate (Rel) computed from the absorbance change showed an early peak (Rel(p)) followed by a maintained phase (Rel(m)). Each Rel(p)-versus-V plot was fitted with a Boltzmann distribution function. The maximum value of Rel(p) (Rel(p,max)) was compared in various calcium-containing external solutions. The average value in a Cl(-) solution was about one-third larger than those in a CH(3)SO(3)(-) or gluconate solution, whereas the values in the CH(3)SO(3)(-) and gluconate solutions had no statistically significant difference. In external solutions containing CH(3)SO(3)(-) or gluconate, a replacement of the Ca(2+) with Mg(2+) reduced Rel(p,max) by 30 to 50%, on average. The values of Rel(p, max) also had no statistically significant difference among calcium-free external solutions containing different impermeant anions. An increase of the nominal free [Ca(2+)] in the end-pool solution from a reduced to the normal physiological level increased the value of Rel(p,max), and also slowed the decay of the maintained phase of the Rel waveform. The Rel waveforms in the Cl(-) and CH(3)SO(3)(-) solutions were compared in the same fiber at a fixed potential. CH(3)SO(3)(-) increased the time to peak, reduced Rel(p), and increased Rel(m), and the effects were partially reversible. Under the hypothesis that the decay of the peak was due to calcium inactivation of calcium release, the inactivation was larger in Cl(-) than in CH(3)SO(3)(-), in qualitative agreement with the ratio of Rel(p) in the two solutions. Under the alternative hypothesis that the peak and the maintained phase were separately gated by calcium and depolarization, respectively, then CH(3)SO(3)(-) appeared to decrease the calcium-gated component and increase the voltage-gated component.     

Current clamp and voltage clamp study of the inhibitory action of DNP on membrane electrical properties of frog auricular heart muscle.

Current clamp studies showed that after 10 minutes under DNP 10(-4) M the membrane potential does not change significantly while an important shortening of the action potential duration and a diminished amplitude are observed. Voltage clamp studies have been performed on the slow inward and delayed outward currents. DNP 10(-4) M induced a marked decrease of the slow inward current related to the reduction in both conductance and driving force, and a decrease in the amplitude of the delayed current. The decrease of the slow inward current seems to be mainly responsible for the suppression of the plateau of the action potential during metabolic inhibition.     

Excitation-contraction coupling in a barnacle muscle fiber as examined with voltage clamp technique

Relations between the membrane potential and the tension associated with changes in membrane potential were analyzed in barnacle giant muscle fibers by using voltage clamp techniques. With a step change in membrane potential the tension reaches its final level with a time course which is expressed by the difference of two exponential functions. The time constants τ₁ (0.2–0.4 sec at 23°C) and τ₂ (0.07–0.12 sec at 23°C) are independent of the new membrane potential at least for a relatively small membrane potential change while the final level of tension is a function of the potential. Decreasing the temperature increases both τ₁ and τ₂ (Q₁₀ = -2 to -3) and the increase of the tonicity of the external medium increases τ₁ but not τ₂. The final level of tension is related by an S-shaped curve to the membrane potential. The slope of the final tension-membrane potential curve increases with increasing external Ca concentration and is reduced when a small amount of transition metal ions is added to the medium. This suggests that the influx of Ca ions through the membrane is an important factor in the development of tension.     

Calcium currents of frog and insect skeletal muscle fibres measured during voltage clamp

Both vertebrate and invertebrate skeletal muscle fibres have Ca2+ permeability mechanisms which are turned on by depolarization of the surface membrane. In frog muscle, Ca currents are extremely slow and will be scarcely activated during the action potential that normally elicits a twitch. This Ca permeability cannot therefore play any substantial, direct role in excitation--contraction coupling. In insect (Carausius morosus) muscle, Ca currents activate within milliseconds of depolarization, even at low temperature, and may well play at least a triggering role in excitation--contraction coupling. These Ca currents show saturation with increasing [Ca]0, while the instantaneous current--voltage relation rectifies inwards, as expected from a very low [Ca]i. The Ca channel is permeable to Sr2+ and Ba2+. Inactivation of Ca currents under a maintained depolarization depends on Ca2+ carrying inward current, however, rather than on the depolarization itself.     

Effects of sulfhydryl inhibitors on depolarizations-contraction coupling in frog skeletal muscle fibers

We have studied the effects of the sulfhydryl reagents on contractile responses, using either electrically stimulated single muscle fibers or short muscle fibers that were voltage-clamped with a two-microelectrode voltage-clamp technique that allows the fiber tension in response to membrane depolarization to be recorded. The sulfhydryl inhibitors para- chloromercuribenzoic acid (PCMB) and parahydroximercuriphenyl sulfonic acid (PHMPS), at concentrations from 0.5 to 2 mM, cause loss of the contractile ability; however, before this effect is completed, they change the fiber contractile behavior in a complex way. After relatively short exposure to the compounds, < 20 min, before the fibers lose their contractile capacity, secondary tension responses may appear after electrically elicited twitches or tetani. After losing their ability to contract in response to electrical stimulation, the fibers maintain their capacity to develop caffeine contractures, even after prolonged periods (120 min) of exposure to PHMPS. In fibers under voltage-clamp conditions, contractility is also lost; however, before this happens, long-lasting (i.e., minutes) episodes of spontaneous contractile activity may occur with the membrane polarized at -100 mV. After more prolonged exposure (> 30 min), the responses to membrane depolarization are reduced and eventually disappear. The agent DTT at a concentration of 2 mM appears to protect the fibers from the effects of PCMB and PHMPS. Furthermore, after loss of the contractile responses by the action of PCMB or PHMPS, addition of 2 mM DTT causes recovery of tension development capacity.     

A non-cross-bridge stiffness in activated frog muscle fibers

Force responses to fast ramp stretches of various amplitude and velocity, applied during tetanic contractions, were measured in single intact fibers from frog tibialis anterior muscle. Experiments were performed at 14 degrees C at approximately 2.1 microm sarcomere length on fibers bathed in Ringer's solution containing various concentrations of 2,3-butanedione monoxime (BDM) to greatly reduce the isometric tension. The fast tension transient produced by the stretch was followed by a period, lasting until relaxation, during which the tension remained constant to a value that greatly exceeded the isometric tension. The excess of tension was termed "static tension," and the ratio between the force and the accompanying sarcomere length change was termed "static stiffness." The static stiffness was independent of the active tension developed by the fiber, and independent of stretch amplitude and stretching velocity in the whole range tested; it increased with sarcomere length in the range 2.1-2.8 microm, to decrease again at longer lengths. Static stiffness increased well ahead of tension during the tetanus rise, and fell ahead of tension during relaxation. These results suggest that activation increased the stiffness of some sarcomeric structure(s) outside the cross-bridges.     

Excitation-contraction coupling in intact frog skeletal muscle fibers injected with mmolar concentrations of fura-2.

Experiments were carried out to test the hypothesis that mM concentrations of fura-2, a high-affinity Ca2+ buffer, inhibit the release of Ca2+ from the sarcoplasmic reticulum (SR) of skeletal muscle fibers. Intact twitch fibers from frog muscle, stretched to a long sarcomere length and pressure-injected with fura-2, were activated by an action potential. Fura-2's absorbance and fluorescence signals were measured at different distances from the site of fura-2 injection; thus, the myoplasmic free Ca2+ transient (delta [Ca2+]) and the amount and rate of SR Ca2+ release could be estimated at different myoplasmic concentrations of fura-2 ([fura-2T]). At [fura-2T] = 2-3 mM, the amplitude and half-width of delta [Ca2+] were reduced to approximately 25% of the values measured at [fura-2T] less than 0.15 mM, whereas the amount and rate of SR Ca2+ release were enhanced by approximately 50% (n = 5; 16 degrees C). Similar results were observed in experiments carried out at low temperature (n = 2; 8.5-10.5 degrees C). The finding of an enhanced rate of Ca2+ release at 2-3 mM [fura-2T] is opposite to that reported by Jacquemond et al. (Jacquemond, V., L. Csernoch, M. G. Klein, and M. F. Schneider. 1991. Biophys. J. 60:867-873) from analogous experiments carried out on cut fibers. In two experiments involving the injection of larger amounts of fura-2, reductions in SR Ca2+ release were observed; however, we were unable to decide whether these reductions were due to [fura-2T] or to some nonspecific effect of the injection itself. These experiments do, however, suggest that if large [fura-2T] inhibits SR Ca2+ release in intact fibers, [fura-2T] must exceed 6 mM to produce an effect comparable to that reported by Jacquemond et al. in cut fibers. Our clear experimental result that 2-3 mM [fura-2T] enhances SR Ca2+ release supports the proposal that delta [Ca2+] triggered by an action potential normally feeds back to inhibit further release of Ca2+ from the SR (Baylor, S.M., and S. Hollingworth. 1988. J. Physiol. [Lond.]. 403:151-192). Our results provide no support for the hypothesis that Ca(2+)-induced Ca2+ release plays a significant role in excitation-contraction coupling in amphibian skeletal muscle.     

Acetylcholine-induced current fluctuations in tissue-cultured muscle cells under voltage clamp.

Acetylcholine applied ionophoretically to chick skeletal muscle cells grown in tissue culture produces membrane current fluctuations. Cells treated with vinblastine are transformed to a roughly spherical shape. Such transformed cells can be voltage-clamped with microelectrodes. The frequency spectrum of the current fluctuations at fixed voltage obeys a relation of the Lorentz form. From analysis of the current noise, the conductance of a single ionic channel is estimated to be 39 pmho at a temperature of 28 degrees C, and increases with increasing temperature, exhibiting a Q10 of 1.7. The relaxation time for the channel conductance is more sharply temperature dependent, showing a Q10 of approximately 5. These results are in agreement with the picture of acetylcholine-activated ionic channels determined from experiments on frog end plate (Anderson and Stevens, 1973). The relaxation time for carbachol activation is shorter than for acetylcholine, and appears to be more temperature sensitive.     

Membrane currents in a calcium type muscle membrane under voltage clamp.

Four ionic current components were identified in the total membrane current recorded under voltage clamp conditions from the muscle membrane of the crayfish (Astacus fluviatilis). The early inward current component is dependent on the presence of Ca2+ ions, disappears in Ca2+ free solutions and is insensitive to variaton of external Na+ ions and to tetrodotoxin. The outward current consists of at least three components, an early, a late and a slow outward current. The outward currents are sensitive to TEA and their reversal potentials differ. The early potassium current may be separated in a proportion of fibres by a hump from the later potassium current. An insufficient space clamp as a cause of the hump was excluded by comparing the size of the clamped membrane area with the distribution of large membrane clefts in the fibre. The early outward current is critically dependent on the presence of Ca2+ ions and is relatively more sensitive to TEA ions and to conditioning depolarisation than the late outward current.     

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)     

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.     

Calcium release and its voltage dependence in frog cut muscle fibers equilibrated with 20 mM EGTA

Sarcoplasmic reticulum (SR) Ca release was studied at 13-16 degrees C in cut fibers (sarcomere length, 3.4-3.9 microns) mounted in a double Vaseline-gap chamber. The amplitude and duration of the action- potential stimulated free [Ca] transient were reduced by equilibration with end-pool solutions that contained 20 mM EGTA with 1.76 mM Ca and 0.63 mM phenol red, a maneuver that appeared to markedly reduce the amount of Ca complexed by troponin. A theoretical analysis shows that, under these conditions, the increase in myoplasmic free [Ca] is expected to be restricted to within a few hundred nanometers of the SR Ca release sites and to have a time course that essentially matches that of release. Furthermore, almost all of the Ca that is released from the SR is expected to be rapidly bound by EGTA and exchanged for protons with a 1:2 stoichiometry. Consequently, the time course of SR Ca release can be estimated by scaling the delta pH signal measured with phenol red by -beta/2. The value of beta, the buffering power of myoplasm, was determined in fibers equilibrated with a combination of EGTA, phenol red, and fura-2; its mean value was 22 mM/pH unit. The Ca content of the SR (expressed as myoplasmic concentration) was estimated from the total amount of Ca released by either a train of action potentials or a depleting voltage step; its mean value was 2,685 microM in the action-potential experiments and 2,544 microM in the voltage- clamp experiments. An action potential released, on average, 0.14 of the SR Ca content with a peak rate of release of approximately 5%/ms. A second action potential, elicited 20 ms later, released only 0.6 times as much Ca (expressed as a fraction of the SR content), probably because Ca inactivation of Ca release was produced by the first action potential. During a depolarizing voltage step to 60 mV, the rate of Ca release rapidly increased to a peak value of approximately 3%/ms and then decreased to a quasi-steady level that was only 0.6 times as large; this decrease was also probably due to Ca inactivation of Ca release. SR Ca release was studied with small step depolarizations that open no more than one SR Ca channel in 7,000 and increase the value of spatially averaged myoplasmic free [Ca] by only 0.2 nM.     

Helicoids in the T system and striations of frog skeletal muscle fibers seen by high voltage electron microscopy.

Reconstruction from thick serial transverse slices of frog skeletal muscle fibers stained with peroxidase and examined by high-voltage electron microscopy has revealed that the T system networks at successive sarcomeres are connected together in a helicoidal fashion. From zero to eight helicoids have been found in each of a group of 21 fibers reconstructed in cross section. Helicoids can have either right- or left-handed screw senses, and both senses can be found in one fiber cross section. Because the T system maintains a relatively precise alignment with the myofibrillar striations, it follows that the striations must also have a helicoidal arrangement. This has been found before, but has not been widely accepted in recent times. The presence of helicoids in the bands and membrane networks is not thought per se to alter very much our thinking about excitation and contraction mechanisms in skeletal muscle fibers.     

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.