Pharmacological separation of charge movement components in frog skeletal muscle

The relationship between form and function throughout the history of excitation-contraction coupling

Franzini-Armstrong reviews the development of the excitation–contraction coupling field over time.

The concept of excitation–contraction coupling is almost as old as Journal of General Physiology. It was understood as early as the 1940s that a series of stereotyped events is responsible for the rapid contraction response of muscle fibers to an initial electrical event at the surface. These early developments, now lost in what seems to be the far past for most young investigators, have provided an endless source of experimental approaches. In this Milestone in Physiology, I describe in detail the experiments and concepts that introduced and established the field of excitation–contraction coupling in skeletal muscle. More recent advances are presented in an abbreviated form, as readers are likely to be familiar with recent work in the field.

Reciprocal dihydropyridine and ryanodine receptor interactions in skeletal muscle activation

Dihydropyridine (DHPR) and ryanodine receptors (RyRs) are central to transduction of transverse (T) tubular membrane depolarisation initiated by surface action potentials into release of sarcoplasmic reticular (SR) Ca2+ in skeletal muscle excitation-contraction coupling. Electronmicroscopic methods demonstrate an orderly positioning of such tubular DHPRs relative to RyRs in the SR at triad junctions where their membranes come into close proximity. Biochemical and genetic studies associated expression of specific, DHPR and RyR, isoforms with the particular excitation-contraction coupling processes and related elementary Ca2+ release events found respectively in skeletal and cardiac muscle. Physiological studies of intramembrane charge movements potentially related to voltage triggering of Ca2+ release demonstrated a particular qγ charging species identifiable with DHPRs through its T-tubular localization, pharmacological properties, and steep voltage-dependence paralleling Ca2+ release. Its nonlinear kinetics implicated highly co-operative conformational events in its transitions in response to voltage change. The effects of DHPR and RyR agonists and antagonists upon this intramembrane charge in turn implicated reciprocal rather than merely unidirectional DHPR-RyR interactions in these complex reactions. Thus, following membrane potential depolarization, an orthograde qγ-DHPR-RyR signaling likely initiates conformational alterations in the RyR with which it makes contact. The latter changes could then retrogradely promote further qγ-DHPR transitions through reciprocal co-operative allosteric interactions between receptors. These would relieve the resting constraints on both further, delayed, nonlinear qγ-DHPR charge transfers and on RyR-mediated Ca2+ release. They would also explain the more rapid charging and recovery qγ transients following larger depolarizations and membrane potential repolarization to the resting level.

Action of perchlorate on the voltage dependent inactivation of excitation-contraction coupling in frog skeletal muscle fibres

Perchlorate is an agonist of excitation-contraction coupling (ECC) in skeletal muscle displacing charge movement and release activation towards more negative voltages. Contradictory effects of this compound on the voltage dependent inactivation (VDI) of ECC ranging from no effect to a negative shift have been previously reported. In this study we report the effect of the extracellular application of 8 mM perchlorate to cut frog fibres on: (1) the charge movement that activates release (Q(1)), (2) the charge movement measured in fibres inactivated by depolarization (Q(2)) and (3) on the steady state VDI of Q(1) and Ca(2+) release. Our findings were: (1) The central voltage of Q(1) was negatively displaced by perchlorate from -29.0 +/- 1.6 to -38.4 +/- 1.7 mV (n = 4). The maximum Q(1) was not significantly affected while the slope of the Q(1) vs. V was increased by perchlorate. (2) The central voltage of Q(2) was shifted from -91.6 +/- 1.4 to -102.3 +/- 1.5 mV (n = 4). (3) The central voltage of the steady state inactivation curve of Q(1) went from -39.3 +/- 1.8 to -48.6 +/- 1.2 mV (mean +/- SEM, n = 6). Perchlorate had a paradoxical effect on Ca(2+) release, while potentiated the release flux in fibres held at -90 mV (peak release flux increased from 3.9 +/- 1.1 to 6.8 +/- 1.9 microM/ms, n = 5) it had an inhibitory effect when applied to fibres at a depolarized holding potential (peak release flux decreased from 3.9 +/- 0.9 to 2.0 +/- 0.5 microM/ms, n = 9). The above findings suggest that the effect on the steady state inactivation is a direct consequence of the negative shift in Q(1) activation. The negative shift in the steady state inactivation of Q(1) correlated well with the effect on Ca(2+) release.

Effects of sphingosine 1-phosphate on excitation-contraction coupling in mammalian skeletal muscle

Sphingosine 1-phosphate (S1P) activates a subset of plasma membrane receptors of the endothelial differentiation gene family (EdgRs) in many cell types. In C2C12 myoblasts, exogenous S1P elicits Ca2+ transients by activating voltage-independent plasma membrane Ca2+ channels and intracellular Ca2+-release channels. In this study, we investigated the effects of exogenous S1P on voltage-dependent L-type Ca2+ channels in skeletal muscle fibers from adult mice. To this end, intramembrane charge movements (ICM) and L-type Ca2+ current (I(Ca)) were measured in single cut fibers using the double Vaseline-gap technique. Our data showed that submicromolar concentrations of S1P (100 nM) caused a approximately 10-mV negative shift of the voltage threshold and transition voltages of q(gamma) and q(h) components of ICM, and of I(Ca) activation and inactivation. Biochemical studies showed that EdgRs are expressed in skeletal muscles. The involvement of EdgRs in the above S1P effects was tested with suramin, a specific inhibitor of Edg-3Rs. Suramin (200 microM) significantly reduced, by approximately 90%, the effects of S1P on ICM and I(Ca), suggesting that most of S1P action occurred via Edg-3Rs. Moreover, SIP at concentration above 10 microM elicited intracellular Ca2+ transients in muscle fibers loaded with the fluorescent Ca2+ dye Fluo-3, as detected by confocal laser scanning microscopy.

Association of the Igamma and Idelta charge movement with calcium release in frog skeletal muscle

Charge movement and calcium transient were measured simultaneously in stretched frog cut twitch fibers under voltage clamp, with the internal solution containing 20 mM EGTA plus added calcium and antipyrylazo III. When the nominal free [Ca2+]i was 10 nM, the shape of the broad I(gamma) hump in the ON segments of charge movement traces remained invariant when the calcium release rate was greatly diminished. When the nominal free [Ca2+]i was 50 nM, which was close to the physiological level, the I(gamma) humps were accelerated and a slow calcium-dependent I(delta) component (or state) was generated. The peak of ON I(delta) synchronized perfectly with the peak of the calcium release rate whereas the slow decay of ON I(delta) followed the same time course as the decay of calcium release rate. Suppression of calcium release by TMB-8 reduced the amount of Q(delta) concomitantly but not completely, and the effects were partially reversible. The same simultaneous suppression effects were achieved by depleting the sarcoplasmic reticulum calcium store with repetitive stimulation. The results suggest that the mobility of Q(delta) needs to be primed by a physiological level of resting myoplasmic Ca2+. Once the priming is completed, more I(delta) is mobilized by the released Ca2+ during depolarization.

FPL-64176 alters both charge movement and Ca2+ release properties in amphibian muscle fibres

A number of recent reports have suggested that ryanodine receptor (RyR)-Ca2+ release channels are gated by tubular depolarization in skeletal muscle through their direct coupling to intramembrane dihydropyridine receptor (DHPR)-voltage sensors. The qgama charge movement, which is inhibited by DHPR antagonists, is often regarded as the electrical signature for the voltage sensing process, yet pharmacological modifications of the RyR produce reciprocal upstream kinetic effects on an otherwise conserved qgamma charge. This study investigates the effect of DHPR-specific agonists upon intramembrane charge and the release of intracellularly stored Ca2+. We empirically demonstrate kinetic effects of FPL-64176 upon charge movements that closely resemble the consequences of previous interventions directed instead at the RyR. Increases in extracellular FPL-64176 concentration from 10 to 40 microM converted delayed qgamma transients to monotonic decays indistinguishable from the exponential qbeta current component. Yet total steady-state intramembrane charge and the steepness of its dependence upon test potential closely resembled previous reports from untreated fibres. These changes accompanied an appearance of transient cytosolic [Ca2+] elevations in confocal line-scans in fluo-3-loaded fibres studied in 10mM K+ and 40, but not 10 microM, FPL-64176 that resembled elementary Ca2+ release events ('sparks'). Pharmacological manipulations of the DHPR whose effects on intramembrane charge resembled those from manoeuvres directed at the RyR can thus produce downstream effects upon Ca2+ release.

L-type Ca2+ channel and ryanodine receptor cross-talk in frog skeletal muscle

The dihydropyridine receptors (DHPRs)/L-type Ca2+ channels of skeletal muscle are coupled with ryanodine receptors/Ca2+ release channels (RyRs/CRCs) located in the sarcoplasmic reticulum (SR). The DHPR is the voltage sensor for excitation-contraction (EC) coupling and the charge movement component q gamma has been implicated as the signal linking DHPR voltage sensing to Ca2+ release from the coupled RyR. Recently, a new charge component, qh, has been described and related to L-type Ca2+ channel gating. Evidence has also been provided that the coupled RyR/CRC can modulate DHPR functions via a retrograde signal. Our aim was to investigate whether the newly described qh is also involved in the reciprocal interaction or cross-talk between DHPR/L-type Ca2+ channel and RyR/CRC. To this end we interfered with DHPR/L-type Ca2+ channel function using nifedipine and 1-alkanols (heptanol and octanol), and with RyR/CRC function using ryanodine and ruthenium red (RR). Intramembrane charge movement (ICM) and L-type Ca2+ current (ICa) were measured in single cut fibres of the frog using the double-Vaseline-gap technique. Our records showed that nifedipine reduced the amount of q gamma and qh moved by approximately 90% and approximately 55%, respectively, whereas 1-alkanols completely abolished them. Ryanodine and RR shifted the transition voltages of q gamma and qh and of the maximal conductance of ICa by approximately 4-9 mV towards positive potentials. All these interventions spared q beta. These results support the hypothesis that only q gamma; and qh arise from the movement of charged particles within the DHPR/L-type Ca2+ channel and that these charge components together with ICa are affected by a retrograde signal from RyR/CRC.

Extra activation component of calcium release in frog muscle fibres

In addition to activating more Ca(2+) release sites via voltage sensors in the t-tubular membranes, it has been proposed that more depolarised voltages enhance activation of Ca(2+) release channels via a voltage-dependent increase in Ca-induced Ca(2+) release (CICR). To test this, release permeability signals in response to voltage-clamp pulses to two voltages, -60 and -45 mV, were compared when Delta[Ca(2+)] was decreased in two kinds of experiments. (1) Addition of 8 mM of the fast Ca(2+) buffer BAPTA to the internal solution decreased release permeability at -45 mV by > 2-fold and did not significantly affect Ca(2+) release at -60 mV. Although some of this decrease may have been due to a decrease in voltage activation at -45 mV - as assessed from measurements of intramembranous charge movement - the results do tend to support a Ca-dependent enhancement with greater depolarisations. (2) Decreasing SR (sarcoplasmic reticulum) Ca content ([Ca(SR)]) should decrease the Ca(2+) flux through an open channel and thereby Delta[Ca(2+)]. Decreasing [Ca(SR)] from > 1000 microM (the physiological range) to < 200 microM decreased release permeability at -45 mV relative to that at -60 mV by > 6-fold, an effect shown to be reversible and not attributable to a decrease in voltage activation at -45 mV. These results indicate a Ca-dependent triggering of Ca(2+) release at more depolarised voltages in addition to that expected by voltage control alone. The enhanced release probably involves CICR and appears to involve another positive feedback mechanism in which Ca(2+) release speeds up the activation of voltage sensors.

Differential effects of sarcoplasmic reticular Ca(2+)-ATPase inhibition on charge movements and calcium transients in intact amphibian skeletal muscle fibres

A hypothesis in which intramembrane charge reflects a voltage sensing process allosterically coupled to transitions in ryanodine receptor (RyR)-Ca(2+) release channels as opposed to one driven by release of intracellularly stored Ca(2+) would predict that such charging phenomena should persist in skeletal muscle fibres unable to release stored Ca(2+). Charge movement components were accordingly investigated in intact voltage-clamped amphibian fibres treated with known sarcoplasmic reticular (SR) Ca(2+)-ATPase inhibitors. Cyclopiazonic acid (CPA) pretreatment abolished Ca(2+) transients in fluo-3-loaded fibres following even prolonged applications of caffeine (10 mM) or K(+) (122 mM). Both CPA and thapsigargin (TG) transformed charge movements that included delayed (q(gamma)) "hump" components into simpler decays. However, steady-state charge-voltage characteristics were conserved to values (maximum charge, Q(max) approximately equal to 20-25 nC microF(-1); transition voltage, V* approximately equal to -40 to-50 mV; steepness factor, k approximately equal to 6-9 mV; holding voltage -90 mV) indicating persistent q(gamma) charge. The features of charge inactivation similarly suggested persistent q(beta) and q(gamma) charge contributions in CPA-treated fibres. Perchlorate (8.0 mM) restored the delayed kinetics shown by "on" q(gamma) charge movements, prolonged their "off" decays, conserved both Q(max) and k, yet failed to restore the capacity of such CPA-treated fibres for Ca(2+) release. Introduction of perchlorate (8.0 mM) or caffeine (0.2 mM) to tetracaine (2.0 mM)-treated fibres, also known to restore q(gamma) charge, similarly failed to restore Ca(2+) transients. Steady-state intramembrane q(gamma) charge thus persists with modified kinetics that can be restored to its normally complex waveform by perchlorate, even in intact muscle fibres unable to release Ca(2+). It is thus unlikely that q(gamma) charge movement is a consequence of SR Ca(2+) release rather than changes in tubular membrane potential.

Calcium release and intramembranous charge movement in frog skeletal muscle fibres with reduced (< 250 microM) calcium content

It is generally accepted that activation of voltage sensors in the T-tubular membranes is a critical step of excitation-contraction coupling in skeletal muscle. The purpose of this study was to evaluate further whether the Qgamma component (delayed 'hump' component) of the intramembranous charge movement current (I(cm)) results from movement of these voltage sensors. Ca2+ release and I(cm) were measured in voltage-clamped frog cut fibres mounted in a double Vaseline-gap chamber. In order to reduce effects of Ca2+ feedback mechanisms, the calcium content of the sarcoplasmic reticulum (SR) during rest was reduced to < 250 microM (referred to volume of myoplasm) and maintained approximately constant. The early (Qbeta) and Qgamma components of charge movement were estimated by fitting the sum of two Boltzmann functions to the total steady-state intramembranous charge vs. voltage data. The average voltage steepness factor (k) and half-maximal voltage (V-) for Qgamma were 4.3 and -57.4 mV (n = 6), respectively. The SR membrane permeability for Ca2+ release was assessed when a constant amount of calcium remained in the SR (usually about 60 microM). A single Boltzmann function fitted to these data gave values on average for k and V- of 4.7 and -45.3 mV, respectively. The similarity of the values of k for Qgamma and Ca2+ release supports the idea that Qgamma reflects movement of voltage sensors for Ca2+ release. The greater value of V- for Ca2+ release compared to Qgamma is consistent with multi-state models of the voltage sensor involving movement of Qgamma charge during non-activating transitions.

Separation of charge movement components in mammalian skeletal muscle fibres

1. Intramembrane charge movements, I(ICM), were measured in rat skeletal muscle fibres in response to voltage steps from a -90 mV holding potential to a wide test voltage range (-85 to 30 mV), using a double Vaseline-gap voltage-clamp technique. Solutions were designed to minimise ionic currents. Ca(2+) current was blocked by adding Cd(2+) (0.8 mM) to the external solution. In a subset of experiments Cd(2+) was omitted to determine which components of the charge movement best correlated with L-type Ca(2+) channel gating. 2. Detailed kinetic analysis of I(ICM) identified two major groups of charges. The first two components, designated Q(a) and Q(b), were the only charges moved by small depolarising steps. The second group of components, Q(c) and Q(d), showed a more positive voltage threshold, -35.6 +/- 2.0 mV, (n = 6) in external solution with Cd(2+), and -41.1 +/- 2.0 mV (n = 12) in external solution without Cd(2+). Notably, in external solution without Cd(2+) the voltage threshold of Ca(2+) current, I(Ca), activation had a similar value, being -38.1 +/- 2.4 mV. 3. The sum of three Boltzmann functions, Q(1), Q(2) and Q(3), showing progressively more positive transition voltages, could be fitted to charge versus voltage, Q(ICM)-V, plots. The three Boltzmann terms identified three charge components: Q(1) described the shallow voltage-dependent Q(a) and Q(b) charges, Q(2) and Q(3) described the steep voltage-dependent Q(c) and Q(d) charges. 4. In external solution without Cd(2+) the charge kinetics changed: a slow decaying phase was replaced by a pronounced delayed hump. Moreover, the transition voltages of the individual steady-state charge components were shifted towards negative potentials (from 6.3 to 8.2 mV). Nevertheless, the overall charge and steepness factors were conserved. 5. In conclusion, these experiments allowed a clear separation of four components of intramembrane charge movements in rat skeletal muscle, showing that there are no fundamental differences with respect to charge movement components between amphibian and mammalian twitch muscle. Moreover, Q(c) and Q(d) charge are correlated with L-type Ca(2+) channel gating.

Charge movements in intact amphibian skeletal muscle fibres in the presence of cardiac glycosides

1. Intramembrane charge movements were examined in intact voltage-clamped amphibian muscle fibres following treatment with cardiac glycosides in the hypertonic gluconate-containing solutions hitherto reported to emphasise the features of q(gamma) at the expense of q(beta) charge. 2. The application of chlormadinone acetate (CMA) at concentrations known selectively to block Na(+)-K(+)-ATPase conserved the steady-state voltage dependence of intramembrane charge, contributions from delayed (q(gamma)) charging transients, and their inactivation characteristics brought about by shifts in holding potential. 3. The addition of either ouabain (125, 250 or 500 nM) or digoxin (5 nM) at concentrations previously reported additionally to influence excitation-contraction coupling similarly conserved the steady-state charge-voltage relationships, Q(V), in fully polarised fibres to give values of maximum charge, Q(max), transition voltage, V*, and steepness factor, k, that were consistent with a persistent q component as reported on earlier occasions (Q(max) approximately = 25-27 nC F-1, V* approximately = -45 to -50 mV, k approximately = 7-9 mV). 4. In both cases shifts in holding potential from -90 to -50 mV produced a partial inactivation that separated steeply and more gradually voltage-dependent charge components in agreement with previous characterisations. 5. However, charge movements that were observed in the presence of either digoxin or ouabain were monotonic decays in which delayed (q(gamma)) transients could not be distinguished from the early charging records. These features persisted despite the further addition of chlormadinone acetate over a 10-fold concentration range (5-50 microM) known to displace ouabain from the Na(+)-K(+)-ATPase. 6. Ouabain (500 nM) restored the steady-state charge movement that was previously abolished by the addition of 2.0 mM tetracaine in common with previous results of using ryanodine receptor (RyR)-specific agents. 7. Perchlorate (8.0 mM) restored the delayed 'on' relaxations and increased the prominence of the 'off' decays produced by q(gamma) charge following treatment with cardiac glycosides. This was accompanied by a negative (approximately 10-15 mV) shift in the steady-state charge-voltage relationship but an otherwise conserved maximum charge, Q(max), and steepness factor, k, in parallel with previously reported effects of perchlorate following treatments with RyR-specific agents. 8. The features of cardiac glycoside action thus parallel those of other agents that act on RyR-Ca(2+) release channels yet influence the kinetics but spare the steady-state properties of intramembrane charge.

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.

The influence of caffeine on intramembrane charge movements in intact frog striated muscle

1. The influence of caffeine, applied over a 25-fold range of concentrations, on intramembrane charge movements was examined in intact voltage-clamped amphibian muscle fibres studied in the hypertonic gluconate-containing solutions that were hitherto reported to emphasize the features of qgamma at the expense of those of qbeta charge. 2. The total charge, Qmax, the transition voltage, V*, and the steepness factor, k, of the steady-state charge-voltage relationships, Q(V), were all conserved to values expected with significant contributions from the steeply voltage-dependent qgamma species (Qmax approximately 20 nC microF-1, V* approximately -50 mV, k approximately 8 mV) through all the applications of caffeine concentrations between 0.2 and 5.0 mM. This differs from recent reports from studies in cut as opposed to intact fibres. 3. The delayed transients that have been attributed to transitions within the qgamma charge persisted at low (0.2 mM) and intermediate (1.0 mM) caffeine concentrations. 4. In contrast, the time courses of such qgamma currents became more rapid and their waveforms consequently merged with the earlier qbeta decays at higher (5.0 mM) reagent concentrations. The charging records became single monotonic decays from which individual contributions could not be distinguished. This suggests that caffeine modified the kinetic properties of the qgamma system but preserved its steady-state properties. These findings thus differ from earlier reports that high caffeine concentrations enhanced the prominence of delayed transient components in cut fibres. 5. Caffeine (5.0 mM) and ryanodine (0.1 mM) exerted antagonistic actions upon qgamma charge movements. The addition of caffeine restored the delayed time courses that were lost in ryanodine-containing solutions, reversed the shift these produced in the steady-state charge-voltage relationship but preserved both the maximum charge, Qmax, and the steepness, k, of the steady-state Q(V) relationships. 6. Caffeine also antagonized the actions of tetracaine on the total available qgamma charge, but did so only at the low and not at the high applied concentrations. Thus, 0.2 mM caffeine restored the steady-state qgamma charge, the steepness of the overall Q(V) function and the appearance of delayed qgamma charge movements that had been previously abolished by the addition of 2.0 mM tetracaine. 7. In contrast, the higher applied (1.0 and 5.0 mM) caffeine concentrations paradoxically did not modify these actions of tetracaine. The total charge and voltage dependence of the Q(V) curves, and the amplitude and time course of charge movements remained at the reduced values expected for the tetracaine-resistant qbeta charge. 8. These results permit a scheme in which caffeine acts directly upon ryanodine receptor (RyR)-Ca2+ release channels whose consequent activation then dissociates them from the tubular dihydropyridine receptor (DHPR) voltage sensors that produce qgamma charge movement, with which they normally are coupled in reciprocal allosteric contact.

Fast voltage gating of Ca2+ release in frog skeletal muscle revealed by supercharging pulses

1. In single frog skeletal muscle fibres, we utilized supercharging voltage clamp command pulses to boost the rate of depolarization in the transverse tubular system (T-system) such that 95 % of steady-state potential is achieved in < 2 ms (as indicated by fluorescent potentiometric dye signals detected from a global illumination region). Signals detected near the edge of muscle fibres indicate that peripheral regions of the T-system are not significantly overcompensated under these conditions. 2. We explored the impact of accelerating T-system depolarization on voltage-dependent events of excitation-contraction (E-C) coupling by measuring charge movement currents (CMCs) and Ca2+ fluorescence transients in response to both supercharging and conventional step pulses. 3. When compared with CMCs elicited by step pulses, supercharging CMCs are larger, and their kinetics more closely resemble those of gating current records reported for ionic channels. Furthermore, they decay bi-exponentially (tau fast range, 1.3-1.8 ms; tau slow range, 7.3-11.9 ms), whereas step CMCs fall with a single exponential time course (tau range, 12.5-26.7 ms). 4. Similarly, supercharging produces a distinct acceleration in Ca2+ release transients, which show little evidence of the voltage-dependent onset latencies previously encountered using step pulses. 5. The use of this novel methodology in skeletal muscle unveils a previously undetected component of charge movement, the rapid, voltage-dependent recruitment of which may provide the basis for understanding the fast gating of physiological E-C coupling.

A slow calcium-dependent component of charge movement in Rana temporaria cut twitch fibres

1. Charge movement was studied in highly stretched frog cut twitch fibres in a double Vaseline-gap voltage-clamp chamber, with the internal solution containing either 0.1 mM EGTA or 20 mM EGTA plus 1. 8 mM total Ca2+. 2. Fibres were stimulated with TEST pulses lasting 100-400 ms. Replacement of the external Cl- with an 'impermeant' anion, such as SO42-, CH3SO3-, gluconate or glutamate, greatly reduced the calcium-dependent Cl- current in the ON segment and generated a slowly decaying inward OFF current in charge movement traces. 3. Application of 20 mM EGTA to the internal solution abolished the slow inward OFF current, implying that the activation of the current depended on the presence of Ca2+ in the myoplasm. The possibility that the slow inward OFF current was carried by cations flowing inwards or anions flowing outwards was studied and determined to be unlikely. 4. During a long (2000 ms) TEST pulse, a slowly decaying ON current was also observed. When the slow ON and OFF currents were included as parts of the total charge movement, ON-OFF charge equality was preserved. This slow capacitive current is named Idelta. 5. When Cl- was the major anion in the external solution, the OFF Idelta was mostly cancelled by a slow outward current carried by the inflow of Cl-. 6. The OFF Idelta component showed a rising phase. The average values of the rising time constants in CH3SO3- and SO42- were similar and about half of that in gluconate. 7. The OFF Idelta component in CH3SO3- had a larger magnitude and longer time course than that in SO42-. The maximum amount of Qdelta in CH3SO3- was about three times as much as that in SO42-, whereas the voltage dependence of Qdelta was similar in the two solutions. 8. Since the existence of Qdelta depends on the presence of Ca2+ in the myoplasm, it is speculated that Qdelta could be a function of intracellular calcium release.

The influence of perchlorate ions on complex charging transients in amphibian striated muscle

1. The effects of perchlorate ions on intramembrane charge movements were examined under different conditions of ryanodine receptor (RyR) modification in intact voltage-clamped amphibian skeletal muscle fibres studied in the gluconate-containing solutions previously reported to emphasize the features of q gamma at the expense of those of the q beta charge. 2. The introduction of graded increases in perchlorate concentration to the experimental solutions selectively shifted the threshold of appearance of the q gamma 'hump' currents to more negative test potentials at which they actually appeared in the absence of prior q beta transients at perchlorate concentrations of 4.0-8.0 mM. Such findings suggested that the delayed (q gamma) transitions can take place independently of any previous exponential (q beta) decay. 3. These kinetic effects were accompanied by hyperpolarizing shifts in the transition potentials (V*) of the steady-state voltage dependences of either the overall or the isolated q gamma charge. These shifts were graded with concentration and reached their maximum effects at 4.0-8.0 mM perchlorate. However, both the total charge (Qmax) and the steepness factor (k) remained conserved at values consistent with a system that included significant contributions from the steeply voltage-sensitive q gamma component (overall charge: Qmax approximately 19-21 nC microF-1, k approximately 7-9 mV; q gamma component alone: Qmax approximately 10-12 nC microF-1, k approximately 4-6 mV). This contrasts with earlier reports on the effects of perchlorate in fibres that were studied in sulphate- or methanesulphonate-containing extracellular solutions. 4. Perchlorate (8.0 mM) restored the 'hump' waveform associated with q gamma charge movements that had previously been obliterated by the prior application of fully effective (0.1 mM) concentrations of either ryanodine or daunorubicin. 5. Perchlorate similarly reversed the positive shift in the transition potential of the q gamma component that was brought about by such RyR modification (from V* approximately -40 mV back to V* approximately -60 mV). In contrast, the values of either Qmax (overall charge, 19-21 nC microF-1; q gamma component, 10-13 nC microF-1) or k (overall charge, 7-9 mV; q gamma component, 4-6 mV) remained conserved through all these experimental manoeuvres. 6. The inclusion of perchlorate also reversed the action of 2 mM tetracaine and restored delayed q gamma transients to an extent that was graded with concentration (0.5-8.0 mM perchlorate). There was an accompanying recovery of the steeply voltage-dependent steady-state (q gamma) component consistent with a competitive interaction between these agents upon the q gamma intramembrane charge. 7. The present findings suggest that perchlorate exerts a specific action upon the q gamma charge in independent transitions that are driven by the tubular membrane field. Its interactions with the known RyR inhibitors that nevertheless conserve both the charge and its voltage sensitivity suggest a primary action upon the RyR that in turn exerts reciprocal actions upon the voltage sensor.

Charge movement in cut twitch fibres of Rana temporaria containing 0.1 mM EGTA

1. Charge movement was studied in the cut twitch fibres of Rana temporaria with a double Vaseline-gap voltage-clamp technique. 2. In fibres containing 0.1 mM EGTA, the I gamma hump component of charge movement was either unresolvable or had a brief duration at all potentials. In the steady-state charge-voltage (Q-V) plots that were separable into the less voltage dependent (Q beta) and more voltage dependent (Q gamma) components, the amount of Q gamma was 0.9 +/- 0.1 nC microF-1. (mean +/- S.E.M., n = 18). 3. Fibres containing 20 mM EGTA showed broad I gamma humps at about -45 mV. The addition of 1.8 mM total Ca2+ to the end-pools accelerated the rising phase and abbreviated the duration of the hump. 4. I gamma in fibres containing 0.1 mM EGTA resembled those in intact fibres when recorded at similar low temperatures. 5. These results explain the controversy concerning the variable appearance of I gamma humps in cut fibres.

Dual actions of tetracaine on intramembrane charge in amphibian striated muscle

1. The effects of graded concentrations of tetracaine on the steady-state and kinetic properties of intramembrane charge were examined in intact voltage-clamped amphibian muscle fibres. 2. The micromolar tetracaine concentrations that were hitherto reported to abolish Ca2+ transients in skeletal muscle failed to affect significantly the steady-state charge. Maximal reductions of such intramembrane charge required relatively high, 1-2 mM, concentrations of tetracaine. 3. The plots of maximum charge against tetracaine concentration suggested a saturable 1:1 drug binding that spared a fixed amount of tetracaine-resistant (q beta) charge but inhibited a discrete fraction of susceptible (q gamma) charge with a KD between 0.1 and 0.2 mM. 4. The q beta charge thus isolated by 2 mM tetracaine was conserved through a wide range of applied test voltages and pulse durations and regardless of whether the imposed transition from the holding potential (-90 mV) to the test potential took place in one or more steps. 5. Similarly, 'on' and 'off' q beta currents that were elicited by voltage steps from fixed conditioning to varying test levels mapped onto non-linear phase-plane trajectories that nevertheless depended uniquely upon voltage. In contrast, the currents that followed voltage steps made from varying prepulse levels to fixed -90 or -20 mV test potentials mapped onto identical q beta phase-plane trajectories that were independent of the prepulse history. 6. The charge movements that followed strong depolarizing voltage clamp steps to test potentials in the range -50 to 0 mV approximated simple monotonic decays that could empirically be described by a single time constant. Nevertheless, a complete inhibition of a tetracaine-sensitive (q gamma) charge movement by 2 mM tetracaine that left only q beta charge, sharply altered both the magnitude and the voltage dependence of these time constants. This establishes a distinct contribution of the q gamma species to overall charge kinetics even at such test voltages. 7. Under such a criterion for the voltage dependence of charging kinetics, even the micromolar (0.05-0.2 mM) tetracaine concentrations that failed to markedly alter the steady-state charge consistently increased the charging time constants yet did not influence their voltage sensitivity. 8. These findings demonstrate the existence of separate kinetic and steady-state effects of tetracaine on intramembrane charge movements, at micromolar and millimolar anaesthetic concentrations, respectively. These parallel earlier effects of tetracaine that have been reported upon the transient and sustained components of sarcoplasmic reticular Ca2+ release. They also establish that maximally effective concentrations of tetracaine isolate a single distinct species of conserved (q beta) intramembrane charge.

Kinetic isoforms of intramembrane charge in intact amphibian striated muscle

The effects of the ryanodine receptor (RyR) antagonists ryanodine and daunorubicin on the kinetic and steady-state properties of intramembrane charge were investigated in intact voltage-clamped frog skeletal muscle fibers under conditions that minimized time-dependent ionic currents. A hypothesis that RyR gating is allosterically coupled to configurational changes in dihydropyridine receptors (DHPRs) would predict that such interactions are reciprocal and that RyR modification should influence intramembrane charge. Both agents indeed modified the time course of charging transients at 100-200-microM concentrations. They independently abolished the delayed charging phases shown by q gamma currents, even in fibers held at fully polarized, -90-mV holding potentials; such waveforms are especially prominent in extracellular solutions containing gluconate. Charge movements consistently became exponential decays to stable baselines in the absence of intervening inward or other time-dependent currents. The steady-state charge transfers nevertheless remained equal through the ON and the OFF parts of test voltage steps. The charge-voltage function, Q(VT), shifted by approximately +10 mV, particularly through those test potentials at which delayed q gamma currents normally took place but retained steepness factors (k approximately 8.0 to 10.6 mV) that indicated persistent, steeply voltage-dependent q gamma contributions. Furthermore, both RyR antagonists preserved the total charge, and its variation with holding potential, Qmax (VH), which also retained similarly high voltage sensitivities (k approximately 7.0 to 9.0 mV). RyR antagonists also preserved the separate identities of q gamma and q beta species, whether defined by their steady-state voltage dependence or inactivation or pharmacological properties. Thus, tetracaine (2 mM) reduced the available steady-state charge movement and gave shallow Q(VT) (k approximately 14 to 16 mV) and Qmax (VH) (k approximately 14 to 17 mV) curves characteristic of q beta charge. These features persisted with exposure to test agent. Finally, q gamma charge movements showed steep voltage dependences with both activation (k approximately 4.0 to 6.5 mV) and inactivation characteristics (k approximately 4.3 to 6.6 mV) distinct from those shown by the remaining q beta charge, whether isolated through differential tetracaine sensitivities, or the full approximation of charge-voltage data to the sum of two Boltzmann distributions. RyR modification thus specifically alters q gamma kinetics while preserving the separate identities of steady-state q beta and q gamma charge. These findings permit a mechanism by which transverse tubular voltage provides the primary driving force for configurational changes in DHPRs, which might produce q gamma charge movement. However, they attribute its kinetic complexities to the reciprocal allosteric coupling by which DHPR voltage sensors and RyR-Ca2+ release channels might interact even though these receptors reside in electrically distinct membranes. RyR modification then would still permit tubular voltage change to drive net q gamma charge transfer but would transform its complex waveforms into simple exponential decays.

Differential suppression of charge movement components by gluconate in cut twitch fibres of Rana temporaria

1. Charge movement was studied in cut twitch fibres of Rana temporaria using a double Vaseline-gap voltage-clamp technique. 2. Replacement of Cl- by gluconate in the external solution reduced the magnitude of the early current component (I beta) substantially but affected the magnitude and slowed the kinetics of the hump current component (I gamma) slightly. 3. The early (Q beta) and hump (Q gamma) charge components in the gluconate solution were 11.8 +/- 2.3 and 88.0 +/- 4.8% (mean +/- S.E.M., n = 9), respectively, of those in the Cl- solution. 4. These results suggest that Q beta cannot be a precursor of Q gamma. Moreover, since fibres bathed in a gluconate solution can release calcium, Q beta is probably not involved in triggering calcium release.

Kinetic separation of charge movement components in intact frog skeletal muscle

1. Procedures for a complete charge movement separation employed a combination of its steady-state inactivation and activation properties in intact frog skeletal muscle fibres in gluconate-containing solutions. 2. Holding potential shifts from -70 to -50 mV reduced the total charge available between -90 and -20 mV from 16.76 +/- 1.70 nC microF-1 (mean +/- S.E.M.; n = 4 fibres) to 9.25 +/- 1.43 nC microF-1 without significant loss of tetracaine-resistant charge (q beta). 3. The steady-state and kinetic properties of tetracaine-sensitive charge (q gamma) persisted through holding potential changes from -90 to -70 mV in the presence of gluconate and generally resembled activation properties established hitherto in sulphate-containing solutions. 4. Further holding potential displacement to -50 mV abolished q gamma charge movements and depressed the charge-voltage curve. 5. Test voltage steps applied from a -70 mV prepulse level gave rapid monotonic q beta decays and similarly depressed activation functions in 2 mM tetracaine unchanged by holding potential shifts between -70 and -50 mV. 6. The isolated 'on' q gamma charge movements, I(t), always included early transients that preceded any prolonged charging phases and which increased with depolarization. They decayed to stable baselines in the absence of prolonged time-dependent or inward-current phases and yielded integrals, Q(t), that monotonically increased with test voltage. 7. 'Off' steps always elicited rapid monotonic q gamma decays that fully returned the 'on' charge. 8. 'On' and 'off' q gamma currents, I(t), following voltage steps from fixed conditioning to varying test levels mapped onto topologically distinct higher-order phase-plane trajectories, I(Q), that steeply varied with test voltage. 9. In contrast, voltage steps to fixed test potentials of either -70 or -20 mV elicited identical q gamma phase-plane trajectories independent of prepulse history. 10. The q gamma current thus reflects an independent, capacitative process driven uniquely by higher-order dependences upon charge distribution, Q(t), and test voltage, V(t), autonomous of prepulse history or time, t.

Evidence for the non-existence of a negative phase in the hump charge movement component (I gamma) in Rana temporaria

1. Charge movement was studied in cut twitch fibres of Rana temporaria with a double Vaseline-gap voltage-clamp technique. 2. When charge movement was measured from stretched fibres (3.5 microns sarcomere length) bathed in a TEA-Cl Ringer solution, the ON transients in the appropriate potential range showed an early I beta component followed by an I gamma hump. The late I gamma hump generally decayed monotonically towards the maintained current level. 3. On some rare occasions, the ON transient showed an undershoot immediately following the I gamma hump before reaching the steady-state level. This dip in current, when it occurred, could only be observed in a very narrow potential range and might not persist until the end of the experiment. 4. A replacement of the Cl- in the external solution by CH3SO3- reduced the magnitude of the dip, suggesting that the dip is ionic in origin. 5. When charge movement was measured in slack fibres (2.2 microns sarcomere length, the probability of observing the dip in current was increased. 6. In some experiments in which the dip in current was very stable, the signal was studied by a sequence of TEST pulses to the same potential but with different durations. It was found that, if the dip in current was included as a negative phase of the I gamma hump, then the amount of ON charge was smaller than that of OFF charge. Also, as the pulse duration was increased progressively so that a longer portion of the dip was recorded, the OFF charge remained constant instead of being decreased.(ABSTRACT TRUNCATED AT 250 WORDS)

Charge conservation in intact frog skeletal muscle fibres in gluconate-containing solutions

1. The conservation of intramembrane charge was investigated in intact voltage-clamped frog skeletal muscle fibres under conditions that minimized time-dependent ionic currents and so facilitated precise determination of capacitative charge. 2. Prolonged (q gamma) transients were demonstrated in 3,4-diaminopyridine and tetraethyl-ammonium gluconate-containing low [Ca2+] solutions in response to 125 ms pulses that explored the voltage range -90 to -20 mV. The tetracaine-sensitive, q gamma, component then accounted for a significant proportion (over 50%) of available charge. 3. Both delayed 'on' q gamma currents and 'off' current tails decayed to steady direct current (DC) baselines without significant residual ionic current slopes in the chosen extracellular solutions. This suggested that the current transients represented capacitative decays. It was also compatible with the precise determination of effective charge by integration. 4. The advent of 'on' q gamma current was accompanied by increased 'off' charge. Thus, charge was conserved through all 'on' and 'off' steps and through test voltages that extended from the threshold appearance of q gamma as a slow transient to its full merger with the earlier q beta decay at stronger depolarizations. 5. Charge conservation persisted through a wide range of 'on' pulse durations between 60 and 370 ms and was therefore independent of the interval following the q gamma decay. 6. The quantity of q gamma charge remained a monotonic single-valued function of test voltage, whether this potential was reached directly from the -90 mV holding potential or following a prepulse to -10 mV. 7. These findings suggest that the q gamma charge movement represents the electrical signature of an intramembrane entity whose transitions are primarily driven by, and therefore conserved with, the steady-state potential.

Charge inactivation in the membrane of intact frog striated muscle fibers

1. Charge movements were compared in normally polarized and depolarized intact frog muscle fibres under voltage clamp. 2. The membrane capacitance was linear through positive control steps made consistently from a holding voltage of -10 mV, in agreement with earlier reports from cut fibres. 3. A shift in holding voltage from -90 to -10 mV reduced both the absolute amount and the voltage dependence of charge movement elicited by voltage steps imposed from a fixed conditioning voltage of -180 mV. The charge transferred by steps from -180 to -20 mV was 43.8 +/- 1.14 nC/microF in fully polarized fibres and 21.7 +/- 1.49 nC/microF in the same depolarized fibres (means +/- S.E. of the mean; four fibres). 4. Charge movement in response to steps from -90 to -20 mV increased from 10.4 +/- 1.60 nC/microF to 28.4 +/- 2.42 nC/microF (five fibres) within 30s of changing the holding voltage from -10 to -90 mV. 5. The same fibres also showed significant charge movement between voltages of -180 and -90 mV. However, shifts in holding voltage did not significantly alter the maximum value of this charge, around 10-11 nC/microF. 6. Membrane capacitance as measured by small steps to a voltage of -90 mV remained constant despite holding potential changes, or lidocaine (10 mM) treatment. 7. The same results were obtained whether the above procedures were applied to fibres exposed to normal extracellular [Ca2+], or in Ca(2+)-free media. In both cases tubular cable corrections did not affect the results. 8. These findings suggest independent charge I and charge II systems in which inactivation of charge I is not associated with its interconversion into charge II.

Extracellular Ca2+ sensing by the osteoclast

An increasing number of cell types appear to detect changes in the extracellular Ca2+ concentration and and accordingly modify their function. We review recent evidence for the existence and function of such a mechanism in the osteoclast. Elevated external [Ca2+] in the mM range reduces bone resorption and results in motile changes in the cells. These changes may partly result from elevations of cytosolic [Ca2+] triggered through activation of a surface Ca2+ receptor. Closer analyses of the increases in cytosolic [Ca2+] associated with receptor activation are hindered by the action of this ion both as extracellular agonist and intracellular second messenger. Variations in the peak cytosolic [Ca2+] response to external Ca2+ with changes in cell membrane potential by K+ and valinomycin establish a contribution from extracellular Ca2+. Use of CIO4-, Ni2+ and Cd2+ as surrogate activators in low extracellular [Ca2+] indicate a contribution from Ca2+ release from intracellular stores as well. Such agonists also modify Ca2+ redistribution in other systems, such as skeletal muscle. Thus, we may gain insights into osteoclast extracellular Ca2+ detection and transduction from known features of more well-characterised cell systems.

Effects of local anesthetics on single channel behavior of skeletal muscle calcium release channel

The effects of the two local anesthetics tetracaine and procaine and a quaternary amine derivative of lidocaine, QX314, on sarcoplasmic reticulum (SR) Ca2+ release have been examined by incorporating the purified rabbit skeletal muscle Ca2+ release channel complex into planar lipid bilayers. Recordings of potassium ion currents through single channels showed that Ca(2+)- and ATP-gated channel activity was reduced by the addition of the tertiary amines tetracaine and procaine to the cis (cytoplasmic side of SR membrane) or trans (SR lumenal) side of the bilayer. Channel open probability was lowered twofold at tetracaine and procaine concentrations of approximately 150 microM and 4 mM, respectively. Hill coefficients of 2.0 and greater indicated that the two drugs inhibited channel activity by binding to two or more cooperatively interacting sites. Unitary conductance of the K(+)-conducting channel was not changed by 1 mM tetracaine in the cis and trans chambers. In contrast, cis millimolar concentrations of the quaternary amine QX314 induced a fast blocking effect at positive holding potentials without an apparent change in channel open probability. A voltage-dependent block was observed at high concentrations (millimolar) of tetracaine, procaine, and QX314 in the presence of 2 microM ryanodine which induced the formation of a long open subconductance. Vesicle-45Ca2+ ion flux measurements also indicated an inhibition of the SR Ca2+ release channel by tetracaine and procaine. These results indicate that local anesthetics bind to two or more cooperatively interacting high-affinity regulatory sites of the Ca2+ release channel in or close to the SR membrane. Voltage-dependent blockade of the channel by QX314 in the absence of ryanodine, and by QX314, procaine and tetracaine in the presence of ryanodine, indicated one low-affinity site within the conduction pathway of the channel. Our results further suggest that tetracaine and procaine may primarily inhibit excitation-contraction coupling in skeletal muscle by binding to the high-affinity, regulatory sites of the SR Ca2+ release channel.

Effects of conditioning depolarization and repetitive stimulation on Q beta and Q gamma charge components in frog cut twitch fibers

Charge movement was measured in frog cut twitch fibers with the double Vaseline-gap technique. Steady-state inactivation of charge movement was studied by changing the holding potential from -90 mV to a level ranging from -70 to -30 mV. Q beta and Q gamma at each holding potential were separated by fitting the Q-V plot with a sum of two Boltzmann distribution functions. At -70 mV Q beta and Q gamma were inactivated to 54.0% (SEM 2.2) and 82.7% (SEM 3.0) of the amounts at -90 mV. At holding potentials greater than or equal to -60 mV, more Q gamma was inactivated than Q beta, and at -30 mV Q gamma was completely inactivated but Q beta was not. There was no holding potential at which Q beta was unaffected and Q gamma was completely inactivated. The differences between the residual fractions of Q beta and Q gamma are significant at all holding potentials (P less than 0.001-0.05). The plot of the residual fraction of Q beta or Q gamma versus holding potential can be fitted well by an inverted sigmoidal curve that is a mirror image of the activation curve of the respective charge component. The pair of curves for Q gamma correlates well with those for tension generation or Ca release obtained by other investigators. The time courses of the inactivation of Q beta and Q gamma were studied by obtaining several Q-V plots with conditioning depolarizations lasting 1-20 s and separating each Q-V plot into Q beta and Q gamma components by fitting with a sum of two Boltzmann distribution functions. The inactivation time constant of Q beta was found to be 5-10 times as large as that of Q gamma. During repetitive stimulation, prominent I gamma humps could be observed in TEST-minus-CONTROL current traces and normal Q gamma components could be separated from the Q-V plots, whether 20 or 50 mM EGTA was present in the internal solution, whether 2 or 10 stimulations were used, and whether the stimuli were separated by 400 ms or 6 s. Repetitive stimulation slowed the kinetics of the I gamma hump and could shift the Q-V curve slightly in the depolarizing direction in some cases, resulting in an apparent suppression of charge at the potentials that fall on the steep part of the Q-V curve.

Separation of Q beta and Q gamma charge components in frog cut twitch fibers with tetracaine. Critical comparison with other methods

Charge movement was measured in frog cut twitch fibers with the double Vaseline-gap technique. 25 microM tetracaine had very little effect on the maximum amounts of Q beta and Q gamma but slowed the kinetics of the I gamma humps in the ON segments of TEST-minus-CONTROL current traces, giving rise to biphasic transients in the difference traces. This concentration of tetracaine also shifted V gamma 3.7 (SEM 0.7) mV in the depolarizing direction, resulting in a difference Q-V plot that was bell-shaped with a peak at approximately -50 mV. 0.5-1.0 mM tetracaine suppressed the total amount of charge. The suppressed component had a sigmoidal voltage distribution with V = -56.6 (SEM 1.1) mV, k = 2.5 (SEM 0.5) mV, and qmax/cm = 9.2 (SEM 1.5) nC/microF, suggesting that the tetracaine-sensitive charge had a steep voltage dependence, a characteristic of the Q gamma component. An intermediate concentration (0.1-0.5 mM) of tetracaine shifted V gamma and partially suppressed the tetracaine-sensitive charge, resulting in a difference Q-V plot that rose to a peak and then decayed to a plateau level. Following a TEST pulse to greater than -60 mV, the slow inward current component during a post-pulse to approximately -60 mV was also tetracaine sensitive. The voltage distribution of the charge separated by tetracaine (method 1) was compared with those separated by three other existing methods: (a) the charge associated with the hump component separated by a sum of two kinetic functions from the ON segment of a TEST-minus-CONTROL current trace (method 2), (b) the steeply voltage-dependent component separated from a Q-V plot of the total charge by fitting with a sum of two Boltzmann distribution functions (method 3), and (c) the sigmoidal component separated from the Q-V plot of the final OFF charge obtained with a two-pulse protocol (method 4). The steeply voltage-dependent components separated by all four methods are consistent with each other, and are therefore concluded to be equivalent to the same Q gamma component. The shortcomings of each separation method are critically discussed. Since each method has its own advantages and disadvantages, it is recommended that, as much as possible, Q gamma should be separated by more than one method to obtain more reliable results.

A reconstruction of charge movement during the action potential in frog skeletal muscle

The transfer of intramembrane charge during an action potential at 4 degrees C was reconstructed for a model representing the electrical properties of frog skeletal muscle by a cylindrical surface membrane and 16 concentric annuli ("shells") of transverse tubular membrane of equal radial thickness. The lumina of the transverse tubules were separated from extracellular fluid by a fixed series resistance. The quantity, geometrical distribution and steady-state and kinetic properties of charge movement components were described by equations incorporating earlier experimental results. Introducing such nonlinear charge into the distributed model for muscle membrane diminished the maximum amplitude of the action potential within the transverse tubules by 2 mV but increased the maximum size of the after-depolarization by 3-5 mV and also its duration. However, these changes were small in comparison to the 135-mV deflection represented by the action potential. They therefore did not justify altering the values of the electrical parameters adopted by Adrian R.H., and L.D. Peachey (1973. J. Physiol. [Lond.]. 235:103-131.) and used in the present calculations. Cable properties significantly affected the time course and extent of charge movement in each shell during action potential propagation into the tubular system. Q beta charge moved relatively rapidly in all annuli, and did so without significant latency (approximately 0.3 ms) after the surface action potential upstroke. Its peak displacement varied between 53 and 58% (the range representing the difference fiber edge/fiber axis) of the total Q beta charge. This was attained at 5.4-7.3 ms after the stimulus, depending on depth within the tubules. In contrast, q gamma moved after a 1.7-2.9 ms latency and achieved a peak displacement of up to 22-34% of available charge. Both charge movement species could be driven by repetitive (47.7 Hz) action potentials without buildup of charge transfer. Such stimulus frequencies would normally cause tetanus. Latencies in q gamma charge movement in response to an action potential were resolved into (a) propagation of tubular depolarization required to gain the "threshold" of q gamma charge (0.8-1.5 ms) and (b) dielectric loss processes. The latter took consistently around 1.5 ms throughout the tubular system. Taken with (c) the earlier reports of a minimal latency in delta [Ca2+] signals attributed to tubulo-cisternal coupling following voltage sensing (approximately 2 ms: Zhu, P.H., I. Parker, and R. Miledi., 1986. Proc. R. Soc. Lond. B. Biol. Sci. 229:39-46.). these times can be reconciled to the latency (~ 4-5 ms) reported between the onset of the surface action potential and that of delta [Ca2+] signals (Vergara, J., and M. Delay. 1986. Proc. R. Soc. Lond. B. Biol. Sci. 229:97-110.). This is consistent with a relationship between the q gamma system and excitation-contraction coupling whether as an independent event (e.g.,Adrian, R.H., and C.L.-H. Huang. 1984. J. Physiol. (Lond.). 353:419-434.) or as an end reaction following earlier (q beta) transfers of charge (e.g., Horowicz, P., and M.F. Schneider. 1981. J. Physiol. (Lond.). 314:565-593.; Melzer, W., M.F. Schneider, B.J. Simon,and G. Szucs. 1986. J. Physiol. (Lond.). 373:481-512.)

Charge movement and SR calcium release in frog skeletal muscle can be related by a Hodgkin-Huxley model with four gating particles

Charge movement currents (IQ) and calcium transients (delta[Ca2+]) were measured simultaneously in frog skeletal muscle fibers, voltage clamped in a double vaseline gap chamber, using Antipyrylazo III as the calcium indicator. The rate of release of calcium from the SR (Rrel) was calculated from the calcium transients using the removal model of Melzer, W., E. Rios, and M. F. Schneider (1987. Biophys. J. 51:849-863.). IQ and delta [Ca2+] were calculated for 100 ms depolarizing test pulses to membrane potentials from -30 to +20 mV. To eliminate an inactivating component of Rrel, each test pulse was preceded by a large, fixed prepulse to +20 mV. The resulting Rrel records, which represent the noninactivating component of Rrel, were compared with integral of IQdt.(Q), the total charge that moves. The voltage dependence of the steady state Rrel was steeper then that of Q and shifted to the right. During depolarization, the Rrel waveform was similar to that of Q but was delayed by several ms, while, during repolarization, Rrel preceded Q. All of these results could be explained with a Hodgkin-Huxley type model for E-C coupling in which four voltage sensors in the t-tubule membrane which give rise to IQ must all be in their activating positions for the calcium release channel in the SR membrane to open. his model is consistent with the structural architecture of the triadic junction in which four dihydropyridine receptors (the voltage sensors for E-C coupling) in the t-tubule membrane are closely associated with each ryanodine receptor(the calcium release channel) in the SR membrane [Block, B. A., T. Imagawa, K. P. Campbell, and C. Franzini-Armstrong. 1988. J.Cell. Biol. 107:2587-2600.]). Some aspects of this work have appeared in abstract form (Simon, B. J., and D. Hill. 1991. Biophys. J.59:64a. ([Abstr.]).

Intramembrane charge movements in frog skeletal muscle in strongly hypertonic solutions

Intramembrane charge movements were studied in intact, voltage-clamped frog (Rana temporaria) skeletal muscle fibers in external solutions made increasingly hypertonic by addition of sucrose. The marked dependence of membrane capacitance on test potential persisted with increases in extracellular sucrose concentration between 350 and 500 mM. Charge movements continued to show distinguishable early monotonic (q beta) decays and the strongly voltage-dependent delayed (q gamma) charging phases reported on earlier occasions. In contrast, a further increase to 600 mM sucrose abolished the most steeply voltage-sensitive part of the membrane capacitance. It left a more gradual variation with potential that closely resembled the function that resulted when q gamma charge was abolished by tetracaine in the presence of 500 mM sucrose. Charging transients were now simple monotonic (q beta) decays and lacked delayed (q gamma) transients. Furthermore, tetracaine (2 mM) altered neither the kinetic nor the steady-state features of the charge left in 600 mM sucrose. However, Ca2+ current activation in the same fibers persisted through such tonicity increases under identical conditions of temperature, external solution, and holding voltage. Tonicity changes thus accomplish an independent separation of q gamma and q beta charge as defined hitherto through their tetracaine sensitivity. Their effects on q gamma charge correlate with earlier observations of osmotic conditions on delta[Ca2+] signals (1987. J. Physiol. (Lond.) 383:615-627.) and the parallel effects of other agents on excitation-contraction coupling and q gamma charge. In contrast, they suggest that Ca2+ current activation does not require q gamma charge transfer whether by itself or as part of the excitation-contraction coupling process.

Differential blockage of charge movement components in frog cut twitch fibres by nifedipine

1. The effect of nifedipine on charge movement was studied in cut twitch fibres of Rana temporaria with a double Vaseline-gap voltage-clamp technique. The steady-state charge-voltage (Q-V) plot, in the absence or presence of nifedipine, was separated into Q beta and Q gamma components by fitting with a sum of two Boltzmann distribution functions. 2. When a fibre was held at -90 mV, low concentrations (around 20 nM) of nifedipine suppressed a large fraction of Q beta than Q gamma. Higher concentrations of nifedipine suppressed Q gamma more effectively than Q beta, but even 2 microM-nifedipine did not suppress Q beta and Q gamma completely. Ten micromolar was required for complete suppression of Q gamma. Nifedipine thus suppressed Q beta and Q gamma with different dose dependencies. 3. When the holding potential was changed to -70 mV, some Q beta and Q gamma were inactivated. Low concentrations (around 20 nM) of nifedipine still suppressed a larger fraction of the mobile Q beta than the mobile Q gamma. Higher concentrations of nifedipine also suppressed Q gamma more effectively than Q beta, but 2 microM-nifedipine was sufficient to suppress Q gamma completely. Hence, at this slightly depolarized holding potential, nifedipine also suppressed Q beta and Q gamma with different dose dependencies. 4. A portion of Q beta appeared to be resistant to the action of nifedipine. At -70 mV, the blockage of the nifedipine-sensitive portion of Q beta appeared to saturate at 2 microM of the drug. At -90 mV, the nifedipine-resistant portion of Q beta was more difficult to identify, because the blockage of the nifedipine-sensitive portion of Q beta did not saturate at 2 microM. 5. Based on double-reciprocal plots for the dose-response relationships, the half-blocking concentration of nifedipine for Q beta was found to be 14-19 nM at -90 mV and less than 13 nM at -70 mV, whereas that for Q gamma was approximately 1.6 microM at -90 mV and 120 nM at -70 mV. Thus, nifedipine suppressed Q gamma in a voltage-dependent manner, but its suppression of Q beta was much less voltage dependent. 6. It was demonstrated that the enhancement in the blockage of charge movement by maintained depolarization could not be achieved by depolarizing pulses lasting up to hundreds of milliseconds. 7. The difference in the half-blocking concentrations of nifedipine for Q beta and Q gamma implies that Q beta and Q gamma cannot be tightly coupled.

Multiple actions of 2,3-butanedione monoxime on contractile activation in frog twitch fibres

1. The effects of 2,3-butanedione monoxime (BDM) on various steps in the excitation-contraction coupling sequence, including action potential, charge movement and twitch tension, were studied in twitch fibres of Rana temporaria. 2. The resting potential of intact fibres in whole muscle bathed in 20 mM-BDM was the same as control. The resting potential also remained stable after more than 100 min in 20 mM-BDM. 3. The action potential was measured in intact fibres of fibre bundles with an intracellular microelectrode. Applications of 5 and 7.5 mM-BDM had no effect on its amplitude, whereas 10 and 20 mM suppressed its amplitude by about 4 and 10%, respectively. Increasing concentrations of BDM prolonged the half-width and elevated the after-potential of the action potential progressively. The action potential was also measured in cut fibres mounted in a double Vaseline-gap chamber. Results were similar to those in intact fibres. 4. Charge movement was measured in intact fibres of halved muscles with the three-microelectrode voltage-clamp technique. The steady-state Q-V plot of the total charge measured in isotonic tetraethylammonium (TEA) Ringer solution with 20 mM-BDM appeared to be shifted about 10 mV in the depolarizing direction and to be slightly more shallow when compared with the control Q-V plot measured in hypertonic TEA Ringer solution with 350 mM-sucrose. After allowing for the voltage shift, 20 mM-BDM did not appear to affect the kinetics of both components of charge movement, but suppressed the maximum amount of total charge by about one-quarter. 5. Charge movement was also measured in cut fibres with the double Vaseline-gap voltage-clamp technique. In the presence of 20 mM-BDM, charge movement traces resembled those from intact fibres. Twenty millimolar BDM suppressed the maximum amount of total charge by about one-quarter, as in intact fibres. The steady-state Q-V plots from cut fibres were separated into Q beta (early current) and Q gamma (late hump current) components by least-squares fitting with a sum of two Boltzmann distribution functions. On average, 20 mM-BDM suppressed Q beta and Q gamma in roughly equal proportion, but did not affect the individual voltage distributions of Q beta and Q gamma. 6. Twitch tension was measured in single intact fibres stimulated extracellularly. BDM effectively reduced the peak amplitude, the time-to-peak and the half-width of twitch tension. The interaction of BDM with receptors appeared to follow more or less a simple 1:1 binding in fibres stretched to sarcomere lengths of about 3.6 microns.(ABSTRACT TRUNCATED AT 400 WORDS)

Interfering with calcium release suppresses I gamma, the "hump" component of intramembranous charge movement in skeletal muscle

Four manifestations of excitation-contraction (E-C) coupling were derived from measurements in cut skeletal muscle fibers of the frog, voltage clamped in a Vaseline-gap chamber: intramembranous charge movement currents, myoplasmic [Ca2+] transients, flux of calcium release from the sarcoplasmic reticulum (SR), and the intrinsic optical transparency change that accompanies calcium release. In attempts to suppress Ca release by direct effects on the SR, three interventions were applied: (a) a conditioning pulse that causes calcium release and inhibits release in subsequent pulses by Ca-dependent inactivation; (b) a series of brief, large pulses, separated by long intervals (greater than 700 ms), which deplete Ca2+ in the SR; and (c) intracellular application of the release channel blocker ruthenium red. All these reduced calcium release flux. None was expected to affect directly the voltage sensor of the T-tubule; however, all of them reduced or eliminated a component of charge movement current with the following characteristics: (a) delayed onset, peaking 10-20 ms into the pulse; (b) current reversal during the pulse, with an inward phase after the outward peak; and (c) OFF transient of smaller magnitude than the ON, of variable polarity, and sometimes biphasic. When the total charge movement current had a visible hump, the positive phase of the current eliminated by the interventions agreed with the hump in timing and size. The component of charge movement current blocked by the interventions was greater and had a greater inward phase in slack fibers with high [EGTA] inside than in stretched fibers with no EGTA. Its amplitude at -40 mV was on average 0.26 A/F (SEM 0.03) in slack fibers. The waveform of release flux determined from the Ca transients measured simultaneously with the membrane currents had, as described previously (Melzer, W., E. Ríos, and M. F. Schneider. 1984. Biophysical Journal. 45:637-641), an early peak followed by a descent to a steady level during the pulse. The time at which this peak occurred was highly correlated with the time to peak of the current suppressed, occurring on average 6.9 ms later (SEM 0.73 ms). The current suppressed by the above interventions in all cases had a time course similar to the time derivative of the release flux; specifically, the peak of the time derivative of release flux preceded the peak of the current suppressed by 0.7 ms (SEM 0.6 ms). The magnitude of the current blocked was highly correlated with the inhibitory effect of the interventions on Ca2+ release flux.(ABSTRACT TRUNCATED AT 400 WORDS)

Contraction threshold and the "hump" component of charge movement in frog skeletal muscle

The delayed component of intramembranous charge movement (hump, I gamma) was studied around the contraction threshold in cut skeletal muscle fibers of the frog (Rana esculenta) in a single Vaseline-gap voltage clamp. Charges (Q) were computed as 50-ms integrals of the ON (QON) and OFF (QOFF) of the asymmetric currents after subtracting a baseline. The hump appeared in parallel with an excess of QON over QOFF by approximately 2.5 nC/mu F. Caffeine (0.75 mM) not only shifted the contraction threshold but moved both the hump and the difference between the ON and OFF charges to more negative membrane potentials. When using 10-mV voltage steps on top of different prepulse levels, the delayed component, if present, was more readily observable. The voltage dependences of the ON and OFF charges measured with these pulses were clearly different: QON had a maximum at or slightly above the contraction threshold, while QOFF increased monotonically in the voltage range examined. Caffeine (0.75 mM) shifted this voltage dependence of QON toward more negative membrane potentials, while that of QOFF was hardly influenced. These results show that the delayed component of intramembranous charge movement either is much slower during the OFF than during the ON, or returns to the OFF position during the pulse. Tetracaine (25 microM) had similar effects on the charge movement currents, shifting the voltage dependence on the ON charge in parallel with the contraction threshold, but to more positive membrane potentials, and leaving QOFF essentially unchanged. The direct difference between the charge movement measured in the presence of caffeine and in control solution was either biphasic or resembled the component isolated by tetracaine, suggesting a common site of caffeine and tetracaine action. The results can be understood if the released Ca plays a direct role in the generation of the hump, as proposed in the first paper of this series (Csernoch et al. 1991. J. Gen. Physiol. 97:845-884).

The relationship between Q gamma and Ca release from the sarcoplasmic reticulum in skeletal muscle

Asymmetric membrane currents and fluxes of Ca2+ release were determined in skeletal muscle fibers voltage clamped in a Vaseline-gap chamber. The conditioning pulse protocol 1 for suppressing Ca2+ release and the "hump" component of charge movement current (I gamma), described in the first paper of this series, was applied at different test pulse voltages. The amplitude of the current suppressed during the ON transient reached a maximum at slightly suprathreshold test voltages (-50 to -40 mV) and decayed at higher voltages. The component of charge movement current suppressed by 20 microM tetracaine also went through a maximum at low pulse voltages. This anomalous voltage dependence is thus a property of I gamma, defined by either the conditioning protocol or the tetracaine effect. A negative (inward-going) phase was often observed in the asymmetric current during the ON of depolarizing pulses. This inward phase was shown to be an intramembranous charge movement based on (a) its presence in the records of total membrane current, (b) its voltage dependence, with a maximum at slightly suprathreshold voltages, (c) its association with a "hump" in the asymmetric current, (d) its inhibition by interventions that reduce the "hump", (e) equality of ON and OFF areas in the records of asymmetric current presenting this inward phase, and (f) its kinetic relationship with the time derivative of Ca release flux. The nonmonotonic voltage dependence of the amplitude of the hump and the possibility of an inward phase of intramembranous charge movement are used as the main criteria in the quantitative testing of a specific model. According to this model, released Ca2+ binds to negatively charged sites on the myoplasmic face of the voltage sensor and increases the local transmembrane potential, thus driving additional charge movement (the hump). This model successfully predicts the anomalous voltage dependence and all the kinetic properties of I gamma described in the previous papers. It also accounts for the inward phase in total asymmetric current and in the current suppressed by protocol 1. According to this model, I gamma accompanies activating transitions at the same set of voltage sensors as I beta. Therefore it should open additional release channels, which in turn should cause more I gamma, providing a positive feedback mechanism in the regulation of calcium release.

Existence of Q gamma in frog cut twitch fibers with little Q beta

Charge movements were measured in frog cut twitch fibers with the double Vaseline-gap voltage-clamp technique. In most fibers, when a depolarizing pulse to -60 to -40 mV was applied at 13-14 degrees C, the ON segment of a charge movement trace showed an early I beta component and a late I gamma hump component. An ongoing controversy is whether the I gamma hump component triggers calcium release from the sarcoplasmic reticulum or arises as a consequence of the release. Interestingly, a number of cut fibers showed normal I gamma components but greatly diminished, or unresolvable, I beta components. When the amount of charge associated with the current transient was plotted against the membrane potential, the steeply voltage-dependent Q gamma component appeared normal whereas the less steeply voltage-dependent Q beta component was also greatly diminished or unresolvable. These results suggest that I gamma can flow in the absence of I beta, thereby ruling out the possibility that Q beta triggers calcium release which, in turn, causes Q gamma to move. The results, however, do not rule out the positive feedback of calcium release to activate Q gamma, if calcium release is not triggered by Q beta but by Q gamma itself or by some other signal.

Differential effects of ryanodine and tetracaine on charge movement and calcium transients in frog skeletal muscle

1. Charge movement and myoplasmic calcium transients were simultaneously recorded from frog skeletal muscle fibres by using the double-seal Vaseline-gap technique. Calcium transients were monitored with the fluorescent indicator Rhod-2. 2. Ryanodine modified the kinetics and the total amount of charge moved during depolarizing pulses (Q(on)), while it did not significantly modify the charge after repolarization (Q(off)). The extracellular application of 100 microM-ryanodine elicited a temporary initial increase of the delayed component of charge movement (Q gamma) and the calcium transient. Both phenomena were later blocked with the same temporal course and to the same extent. 3. The blockade of Q gamma and the calcium transient was also observed with ryanodine concentrations of 1-10 microM. For membrane potentials positive to -10mV, the Qon measured was larger in the presence of ryanodine; Qoff was not modified. 4. Tetracaine (400-500 microM) blocked a similar delayed component of Qon, identified as Q gamma, as well as the calcium transient monitored simultaneously. This effect was observed in the first minutes after the addition of tetracaine to the extracellular solution. 5. Tetracaine blocked a faster initial component of Qon for voltages positive to -10 mV, corresponding to the voltage range of activation of the calcium current. At these same membrane potentials, Qoff was also reduced to a similar extent to Qon. 6. Ryanodine and tetracaine showed different effects on calcium current. Whereas the slow calcium current was not modified upon the addition of ryanodine, it was completely blocked in the presence of tetracaine. The blockade of the slow calcium current made evident the fast calcium current. The effects of tetracaine on the charge movement, the calcium transient and the slow calcium current were reversible. 7. These results suggest that ryanodine and tetracaine may act at different sites. Ryanodine exerts its effect on the sarcoplasmic reticulum ryanodine receptor, blocking calcium release and Q gamma, while tetracaine at these concentrations may affect the release channel and the dihydropyridine receptor, causing a blockade of the charge movement, calcium transient and calcium current.

The effects of tetracaine on charge movement in fast twitch rat skeletal muscle fibres

1. The effects of tetracaine, a local anaesthetic that inhibits muscle contraction, on membrane potential and intramembrane charge movements were investigated in fast twitch rat muscle fibres (extensor digitorum longus). 2. The resting membrane potentials of surface fibres from muscles bathed in isotonic Ringer solution containing 2 mM-tetracaine were well maintained, but higher concentrations of tetracaine caused a time-dependent fall of potential. Muscle fibres bathed in hypertonic solutions containing 2 mM-tetracaine were rapidly depolarized. In both isotonic and hypertonic solutions, the depolarizing effect of tetracaine could not be reversed. 3. Charge movement measurements were made using the middle-of-the-fibre voltage clamp technique. The voltage dependence of charge movements measured in cold isotonic solutions was well fitted by a Boltzmann distribution (Q(V) = Qmax/(1 + exp(-(V-V)/k] where Qmax = 37.3 +/- 2.8 nC muF-1, V = -17.9 +/- 1.2 mV and k = 12.6 +/- 0.8 mV (n = 6, 2 degrees C; means +/- S.E. of means). Similar values were obtained when 2 mM-tetracaine was added to the isotonic bathing fluid (Qmax = 40.6 +/- 2.3 nC microF-1, V = -14.1 +/- 1.3 mV, k = 15.3 +/- 0.8 mV; n = 8, 2 degrees C). 4. Charge movements measured around mechanical threshold in muscle fibres bathed in hypertonic solutions were reduced when 2 mM-tetracaine was added to the bathing fluid. The tetracaine-sensitive component of charge was well fitted with an unconstrained Boltzmann distribution which gave: Qmax = 7.5 nC microF-1, V = -46.5 mV, k = 5.5 mV. The e-fold rise of the foot of the curve was 9.3 mV.

The effect of phenylglyoxal on contraction and intramembrane charge movement in frog skeletal muscle

1. The effects of the arginine-specific protein-modifying reagent, phenylglyoxal, on contraction and intramembrane charge movement were studied in cut single fibres from frog skeletal muscle, using the double-Vaseline-gap voltage clamp technique. 2. The strength-duration curve for pulses which produced microscopically just-detectable contractions was shifted to more positive potentials and longer durations following treatment of fibres with phenylglyoxal. Caffeine-induced contractures were not blocked. 3. The amount of charge moved by large depolarizing pulses from -100 mV holding potential (charge 1) declined during the phenylglyoxal treatment with a single-exponential time course (tau = 7 min). Linear capacitance did not change significantly over the entire experiment. Inhibition of charge movement was predominantly irreversible. 4. Slow bumps (Q gamma) observed in charge movement current transients recorded before phenylglyoxal treatment, using either large test pulses or small steps superimposed on test pulses, were absent from currents recorded after treatment. The current removed by phenylglyoxal contained the bump (Q gamma) and a small fast transient (Q beta). 5. The amount of charge moved by large depolarizing pulses from -100 mV was reduced 20-50% following phenylglyoxal treatment. Charge moved by pulses to potentials more negative than -40 mV was relatively unaffected. The magnitude and voltage range of this inhibitory effect were the same whether the reagent was applied at -100 mV or at 0 mV holding potential. 6. A phenylglyoxal-sensitive component of charge was isolated which had a much steeper voltage dependence than the total charge movement or the charge remaining after treatment. 7. Charge recorded during hyperpolarizing pulses from 0 mV holding potential (charge 2) was reduced very little (less than 5%) at any potential by phenylglyoxal treatments at either 0 or -100 mV. 8. The phenylglyoxal reaction with charge 2 was kinetically different from the reaction with charge 1. 9. The effects of phenylglyoxal on charge 1 and charge 2 both measured in the same fibre were compared. Whether phenylglyoxal was applied at -100 mV, or at 0 mV the results were the same: charge 1 was inhibited much more (25-60%) than charge 2(2-12%). 10. The results presented here indicate that arginyl residues have a functional role in the voltage-sensing mechanism of excitation-contraction coupling and support the hypothesis that the dihydropyridine receptor is the voltage sensor molecule.

Excitation contraction coupling in normal and mdx mice

The protein dystrophin is absent from patients with Duchenne muscular dystrophy and from the muscles of mdx mice. Recent studies have shown that dystrophin is located at the surface membrane and at the triadic junction, where it is associated with the transverse tubular membrane. Since the triadic junction is the site of excitation-contraction (EC) coupling, we have investigated whether intramembrane charge movement, a step in EC coupling, is modified by the absence of dystrophin. Charge movements are thought to arise from the transverse tubular membrane and to underlie the dependence of sarcoplasmic reticulum Ca2+ release on transverse tubular membrane potential. We find no differences between intramembrane charge movements or passive membrane electrical properties measured in muscles from mdx mice compared with normal mice. If dystrophin does play a role in EC coupling, that role is likely to be subsequent to the charge movement step.

Intramembrane charge movement in guinea-pig and rat ventricular myocytes

1. Non-linear capacitative current (charge movement) was studied in isolated guinea-pig and rat ventricular myocytes. Linear capacitance was subtracted using standard procedures. Most of the experiments were done with guinea-pig myocytes, while rat myocytes were used for comparison. 2. When a myocyte was held at -100 mV, depolarizing clamp steps produced a rapid outward current transient, which was followed by an inward current transient upon repolarization. This current was identified as the movement of charged particles in the cell membrane, rather than ionic movement across the membrane, for the following reasons: (1) the current saturated at membrane potentials positive to +20 mV; (2) the current was capacitative in nature, having no reversal potential; (3) in general, the charge moved during depolarization (Qon) approximated the charge moved during repolarization (Qoff). 3. Qoff was significantly less than Qon for a depolarization from -100 mV to 0 mV. However, the Qoff/Qon ratio approached unity if the cell was instead repolarized to -140 mV. This was interpreted as being due to the immobilization of a fraction of the charge during the depolarization, which recovered rapidly enough to be measured at -140 mV, but recovered too slowly at -100 mV. 4. Charge movement in these cells had a sigmoidal dependence on the membrane potential, which could be empirically described by the two-state Boltzmann equation Q = Qmax/(1 + exp[-(V-V*)/kappa]), where Q is the charge movement at potential V, Qmax is the maximum charge, V* is the membrane potential at Q = Qmax/2, and kappa is a slope factor. Qmax was 11.7 nC/microF, V* was -18 mV and kappa was 16 mV in guinea-pig myocytes held at -100 mV, while the values in rat myocytes were 10.9 nC/microF, -32 mV and 13 mV. 5. The charge movement could be partially immobilized by a prior depolarization. This effect developed over a broad voltage range, from -120 to +20 mV. The fraction of charge that could be immobilized by a 10 s pre-pulse to +20 mV was 59%. 6. The time course of decay of both Qon and Qoff could basically be described as a single-exponential process. The time constant was largest at -40 mV and decreased at both more positive and negative test potentials. A second, slower Qoff time constant, possibly representing remobilization of immobilized charge, could be seen under some conditions. 7. The temperature dependence of charge movement was studied between 11 and 35 degrees C.(ABSTRACT TRUNCATED AT 400 WORDS)

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.

Perchlorate and the relationship between charge movement and contractile activation in frog skeletal muscle fibres

1. The effects of perchlorate ions (1-8 mM) on intramembrane charge movement, myoplasmic Antipyrylazo III Ca2+ transients and contractile activation were examined in voltage-clamped cut skeletal muscle fibres of the frog. 2. Perchlorate shifted both the voltage dependence of charge movement and the rheobase of the strength-duration relation for contraction threshold towards more negative membrane potentials. 3. Both charge movements and myoplasmic Ca2+ transients were much slower at the new rheobase in the presence of perchlorate than in the control solution but there was no change in the threshold amount of charge or in the calculated peak binding of Ca2+ to troponin C. 4. The peak release rate had a steeper voltage dependence than the non-linear charge, but a lower concentration (2 mM) of perchlorate shifted both voltage dependences equally without altering the maxima in the amount of charge and in the rate of Ca2+ release. 5. The voltage dependence of the difference between total charge and charge at the threshold of Ca2+ transients agreed well with the voltage dependence of the rate of Ca2+ release in both the presence and absence of perchlorate. 6. It is concluded that the effect of perchlorate on contractile activation can be accounted for by its action on the intramembrane charge movement responsible for contraction, without significant effects on subsequent Ca2+ release from the sarcoplasmic reticulum or on Ca2+ binding to regulatory sites of troponin C.

Suppression of charge movement in frog skeletal muscle by D600

Charge movements in intact frog twitch fibres were studied using a three-microelectrode voltage-clamp technique. When high potassium solution was applied transiently to the muscle fibres at low temperature in the presence of D600, the fibres became paralysed and, concomitantly, charge movement disappeared. The amount of charge suppressed by the paralysis treatment was about 70-100% of that in control experiments. This paralysing action of D600 is not shared by its derivative D890. The requirement of conditioning potassium contracture is, most likely, related to prolonged membrane depolarization, as voltage-clamped depolarization to 0 mV lasting tens of seconds also suppressed charge movement. When paralysed fibres were warmed, the main charge component (Q beta) was reprimed. By contrast, the hump charge component (Q gamma) was only reprimed in some of the fibres. Other than by warming, as paralysed fibre could be revived by stimulating it with large suprathreshold pulses but not by voltage-clamped hyperpolarization to -160 mV for tens of seconds. The paralysing action of D600 described here appears to be unrelated to its ability in blocking Ca2+ channels.

Intramembrane charge movement in frog skeletal muscle fibres. Properties of charge 2

1. Membrane currents were measured in cut skeletal muscle fibres voltage-clamped in a double Vaseline gap in solutions that had impermeant ions substituted for Na+, K+ and Cl-. The fibres were maintained at a holding potential of 0 mV. Pulses to positive voltages elicited outward currents that were proportional to voltage at all times; these were used to estimate linear capacitive currents, which in turn were used in the construction of non-linear current transients. 2. Large negative-going pulses elicited proportionally larger inward currents that decayed during the pulse with voltage-dependent kinetics. A portion of the non-linear current could be eliminated by solutions containing EGTA, as well as by large negative conditioning pulses of 200 ms or more. This portion was probably an inward Ca2+ current. 3. The non-linear current remaining in EGTA-containing solutions had characteristics of intramembrane charge movement ('charge 2'). This charge depended on voltage according to a two-state Boltzmann function of average parameters Qmax = 47.7 nC/microF, V = -115 mV, K = 21.5 mV (seven fibres). 4. The charge movement current transients were single-exponential decays (after a short rising phase) with time constants (tau) that depended on voltage (V). A single-barrier Eyring rate model described well the dependence of time constant on voltage. This fit permitted an independent estimate of a transition voltage, V, and a slope parameter K related to apparent valence of the mobile particle. The values of V and K that best fitted the kinetic data were close to the corresponding values estimated from the charge vs. voltage distribution. 5. Effective capacitance was measured by the transfer of capacitive charge by a small pulse superimposed on a variable pre-pulse. The capacitance was found to depend on pre-pulse voltage. The voltage dependence of the capacitance was as expected from the properties of charge 2 measured independently in the same fibres. 6. The presence of charge 2, defined as charge that moves in a very negative voltage range, was compared on the same fibres in a depolarized and a normally polarized (holding potential = -100 mV) situation. All fibres had less charge 2 at a holding potential of -100 mV (14 nC/microF average reduction). In these fibres charge 1, explored with pulses from -70 mV to 0 mV, was greater at a holding potential of -100 mV (18 nC/microF average increase).(ABSTRACT TRUNCATED AT 400 WORDS)

Suppression of charge movement by calcium antagonists is not related to calcium channel block

The calcium channel-inhibiting drugs nitrendipine and diltiazem represent two important classes of organic calcium antagonists. In the present study, the effect of these drugs on calcium currents and charge displacement currents in bullfrog semitendinosus muscle fibers was examined using a vaseline gap voltage clamp. Nitrendipine (10 microM) reduced the quantity of charge that moved both during the ON phase (QON) and the OFF phase (QOFF) of charge movement. This action appeared to be most selective for QON. However, at this same concentration, nitrendipine had no blocking action on inward calcium currents. In contrast to these findings, diltiazem blocked calcium currents in a concentration-dependent manner, while slightly increasing the quantity of charge moved during QON and QOFF. The enhancement of charge movement by diltiazem resulted from two actions. First, diltiazem shifted the voltage-dependence of charge movement to more negative potentials. Second, diltiazem increased the maximum amount of charge moved.

'Off' tails of intramembrane charge movements in frog skeletal muscle in perchlorate-containing solutions

1. Charge movements in response to hyperpolarizing ('off') voltage-clamp steps were examined in frog skeletal muscle fibres in the presence of 8 mM-perchlorate. 2. The appearance of prolonged 'off' decays, of duration 50-100 ms coincided with those of slow 'q gamma' charge transfers in preceding 'on' transients. 3. Charge was conserved in the presence of perchlorate whether testing or pre-pulse voltages were varied. Additionally, steady-state charge as a function of voltage was independent of the direction from which the voltage was reached. 4. 'Off' recoveries were most prolonged at voltages around -90 to -100 mV and became less marked with depolarization. 5. Charging currents in response to hyperpolarizing steps that intercepted prolonged ('q gamma') 'on' decays showed reduced slow 'off' tails but intact 'off' decays at early times. 6. Transients elicited by depolarizing steps that intercepted 'off' tail currents showed decreased slow 'on' components. By varying the time at which 'off' responses were so intercepted, it was shown that 'off' tails can require well over 100 ms to attain a steady state in perchlorate. 7. Prolonged depolarization to a holding potential of -30 mV inactivated delayed ('q gamma') components in both 'on' and 'off' responses but left the more rapid ('q beta') decays intact. 8. These observations are easier to reconcile with parallel systems responsible for independent early ('q beta') and delayed ('q gamma') transients in both 'on' and 'off' steps than with the existence of 'q beta' and 'q gamma' transitions in a causal sequence.

Contractile inactivation in frog skeletal muscle fibers. The effects of low calcium, tetracaine, dantrolene, D-600, and nifedipine

Short muscle fibers (approximately 1.5 mm) of Rana pipiens were voltage-clamped with a two-microelectrode technique at a holding potential of -100 mV. Using conditioning depolarizing ramps, with slopes greater than 0.2 mV/s, partially inactivated responses are obtained at threshold values between -55 and -35 mV. With slopes equal to or slower than 0.1 mV/s, one inactivates contraction without ever activating it. When the membrane potential is brought slowly to values more positive than about -40 mV, test pulses, applied on top of the ramps, bringing the membrane potential to values up to +100 mV, are ineffective in eliciting contractile responses, which indicates complete inactivation. After inactivation, contractile threshold is shifted by perhaps 10 mV, to about -40 mV. The sensitivity of fibers to depolarizing ramps is increased by D-600 (50 microM), dantrolene (50 microM), tetracaine (100 microM), and low calcium (10(-8) M). In the presence of these agents, complete inactivation was obtained using ramp slopes of 1, 0.8, 0.4, and 0.2 mV/s, respectively. Nifedipine was less effective. With D-600, once inactivation had been induced, no repriming occurred after repolarization to -100 mV, and partial recovery occurred after washing out the drug. With low calcium, tetracaine, and nifedipine, the tension-voltage relationship was not affected, whereas the steady state inactivation curve (obtained in repriming experiments) was shifted by 10-25 mV toward more negative potentials. With D-600, the activation curve was not modified, whereas the inactivation curve could not be obtained, because of repriming failure. With dantrolene, the inactivation curve was not affected, whereas the activation curve was shifted toward less negative potentials and peak tension diminished, depending on the pulse duration. The results indicate that it is possible to induce complete inactivation without activation, and to differentiate activation and inactivation parameters pharmacologically, which suggests that the two are separate processes.