Effect of postsynaptic blockade of neuromuscualar transmission on properties of the frog fast muscle fiber membrane

Sensitivity of the postsynpatic membrane to acetylcholine, the resting membrane potential, input resistance, and membrane time constant of fast muscle fibers were measured in experiments on frogs. Complete immobilization of the animals with D-tubocurarine or local immobilization of a muscle with α-bungarotoxin was found not to affect these parameters of the muscle membrane, whereas denervation of the muscle widens the zone of postsynaptic sensitivity to acetylcholine, lowers the resting membrane potential, and increases the input resistance and time constant of the muscle membrane. These results are evidence that neurotrophic control of the frog fast muscle fiber membrane is achieved mainly by substances reaching the muscle via axoplasmic transport and not by the character of the neuronal discharge and motor activity or by synaptic acetylcholine.     

Graded and All-or-None Electrogenesis in Arthropod Muscle : I. The effects of alkali-earth cations on the neuromuscular system of Romalea microptera

Graded electrically excited responsiveness of Romalea muscle fibers is converted to all-or-none activity by Ba⁺⁺, Sr⁺⁺, or Ca⁺⁺, the two former being much the more effective in this action. The change occurs with as little as 7 to 10 per cent of Na⁺ substituted by Ba⁺⁺. The spikes now produced have overshoots and may be extremely prolonged, lasting many seconds. During the spike the membrane resistance is lower than in the resting fiber, but the resting resistance and time constant are considerably increased by the alkali-earth ions. The excitability is also increased, spikes arising neurogenically from spontaneous repetitive discharges in the axon as well as myogenically from spontaneous activity in the muscle fibers. Repetitive responses frequently occur on intracellular stimulation with a brief pulse. The data indicate that the alkali-earth ions exert a complex of effects on the different action components of electrically excitable membrane. They may be described in terms of the ionic theory as follows: The resting K⁺ conductance is diminished. The sodium inactivation process is also diminished, and sodium activation may be increased. Together these changes can act to convert graded responsiveness to the all-or-none variety. The alkali-earth ions can also to some degree carry inward positive charge during activity, since spikes are produced when Na⁺ is fully replaced with the divalent ions.     

Length-dependent electromechanical coupling in single muscle fibers

In single muscle fibers from the giant barnacle, a small decrease in muscle length decreases both the calcium activation and the peak isometric tension produced by a constant current stimulus. The effect is most pronounced if the length change immediately precedes the stimulation. In some cases, the decrease in tension with shortening can be accounted for almost entirely by a decrease in calcium release rather than changes in mechanical factors such as filament geometry. During the constant current stimulation the muscle membrane becomes more depolarized at longer muscle lengths than at the shorter muscle lengths. Under voltage clamp conditions, when the membrane potential is kept constant during stimulation, there is little length dependence of calcium release. Thus, the effect of length on calcium release is mediated through a change in membrane properties, rather than an effect on a subsequent step in excitation-contraction coupling. Stretch causes the unstimulated fiber membrane to depolarize by about l mV while release causes the fiber membrane to hyperpolarize by about the same amount. The process causing this change in potential has an equilibrium potential nearly 10 mV hyperpolarized from the resting level. This change in resting membrane potential with length may account for the length dependence of calcium release.     

Effect of motor function disorder on the properties of the muscle fiber membrane

Experiments on frogs with the use of the microelectrode techniques were made to study the effect of tenotomy and immobilization of a limb with a metal cast in the extension position on the properties of the membrane of muscle fibers. Two weeks after tenotomy there were no changes in the magnitude of the membrane rest potential, input resistance and time constant of the membrane of muscle fibers or in the pattern of its sensitivity to acetylcholine. Two and three weeks after the limb immobilization no changes in the membrane rest potential and passive electrical properties of the muscle membrane were recorded either. However, if the time elapsed after immobilization was 2 and 3 weeks, the zone of the sensitivity of muscle fibers to acetylcholine was slightly greater than in the control. It is suggested that the motor activity in the frog per se is not the determinant of the muscle fiber differentiation preset by the nervous system.     

Slow potential changes in mammalian muscle fibers during prolonged hyperpolarization: Transport number effects and chloride depletion

Summary Mammalian skeletal muscle fibers exhibit large slow changes in membrane potential when hyperpolarized in standard chloride solutions. These large slow potential changes are radically reduced in low chloride solutions, where the faster and smaller potential change (creep), usually observed in amphibian fibers, becomes apparent. The slow potential change during a hyperpolarizing current pulse leads to an increase in apparent resistance of up to nine times the instantaneous value and takes minutes to reach a steady value. It then takes a similar time to decay very slowly back to the resting membrane potential after the current pulse. The halftime for the slow potential change was found to be inversely proportional to the current magnitude. From measurements of immediate postpulse membrane potentials, assuming constant ionic permeabilities, the internal chloride concentration was calculated to decrease exponentially towards a steady value (e.g., for one fiber from 12.3 to 6.6mm after a 330-sec pulse). The time course and magnitude of the concentration change were predicted from chloride transport number differences, and the known and measured properties of the fibers, and were found to agree very well with the values obtained from experimental measurements. In addition, the shapes of theV ₂-V ₁ responses, measured in the three-electrode current clamp set-up with either potassium chloride or potassium citrate current electrodes, were as predicted by transport number chloride depletion effects and were at variance with the predictions of a permeability change mechanism.     

Effects of morphine and meperidine on action potential production in frog's skeletal muscle fibers.

Morphine (3.3 times 10-minus 4 M) and meperidine (8.8 times 10-minus 5 M) inhibited action potential production in frog's skeletal muscle fibers. Over these concentration ranges, neither the resting membrane potentials nor the resting membrane electric properties of the fibers appeared to be modified. Both drugs depressed excitability and the rising phase of the action potential by inhibiting the specific increase in sodium conductance which normally follows an adequate stimulus. Both drugs also seemed to inhibit the secondary rise in potassium conductance which normally occurs during an action potential, causing a prolongation of the action potential duration.     

Innervation and acetylcholine sensitivity of muscle fibers of the tail of the tadpole Rana temporaria

Changes in the distribution of Ach-sensitivity in two types of muscle fibers in the tail of the tadpoles as well as the innervation pattern of these fibers have been investigated during metamorphosis. It was shown by iontophoretic application of acetylcholine that the entire muscle membrane exhibits Ach-sensitivity only during premetamorphosis. Ultrastructural studies revealed mature nerve-muscle junctions at this stage of development of the tadpoles. At later stages (prometamorphosis), Ach-sensitivity decreased and finally (climax) became restricted by the innervation region. It is suggested that special neurotrophic regulation of extra-junctional Ach-sensitivity takes place in myotomal muscles of the tadpoles.     

Effects of phlorizin and phloretin on passive and dynamic electrical properties in muscle membrane

The effects of phlorizin and phloretin on the cable properties were investigated in frog sartorius muscle by conventional cable analysis. Actions of phloretin on voltage-dependent ionic conductances were also studied by analysis of the phase plane trajectories. Both drugs evoked a significant decrease in specific membrane resistance (Rm) in chloride-containing Ringer's solution. The linear membrane capacitance increased by about 30%. On the contrary, in the presence of the non-penetrating anion, glutamate, a slight increase in Rm was induced by phlorizin. It is suggested that these drugs may increase the chloride conductance in the muscle membrane. Under the effect of phloretin the resting membrane potential remained unchanged but the amplitude of the action potential was lowered and the rate of repolarization was significantly reduced. The rate of depolarization during the "foot" of the action potential and the conduction velocity calculated from the rate constant of depolarization decreased. The maximum Na conductance was not altered by phloretin but K conductance was reduced. The time constant (tau K) reflecting the kinetic properties of K conductance was increased about seven-fold. It is suggested that great importance may be attributed to the dipole properties of these drugs in the actions presented above.     

Effects of β-endorphin on the development of denervation changes in rat muscle fiber membrane

Recordings were made of post-denervation changes in resting potential and input resistance in muscle fiber membrane, as well as anode break, tetrodotoxin resistant action potentials, and asynaptic sensitivity to acetylcholine during experiments on cultured diaphragm muscle fiber isolated from rats. Addition of -endorphin to the culture medium prevented increase in the input resistance of muscle fibers and reduced development of asynaptic transmitter sensitivity in the membrane, but failed to change the ability of the denervated muscle membrane to generate anode break and tetrodotoxin-resistant action potentials. The effects of -endorphin were not abolished by naloxone, which itself had endorphin-like powers as measured by the indices used in this research. It is therefore suggested that -endorphin or like substances could be claimed as the neurotrophic factors responsible for controlling passive electrical properties of the muscle fiber membrane and contribute to regulating its acetylcholine sensitivity.S. V. Kurashov Medical Institute, Ministry of Public Health of the RSFSR, Kazan'. Translated from Neirofiziologiya, Vol. 19, No. 6, pp. 759–766, November–December, 1987.     

Cellular ions in intact and denervated muscles of the rat

Summary Tissue composition, membrane potentials and cellular activity of potassium, sodium and chloride have been measured in innervated and denervated rat skeletal muscles incubatedin vitro. After denervation for 3 days, tissue water, sodium and chloride were increased but cellular potassium content and measured activity were little affected, despite a decrease of 16 mV in resting membrane potential which would have necessitated a decrease in cellular potassium activity of almost 50% were potassium distributed at electrochemical equilibrium. These findings, therefore, preclude a decreased electrochemical potential gradient for potassium as the cause of the membrane depolarization characteristic of denervated muscle fibers. Analysis of the data excludes an important contribution of rheogenic sodium transport to the resting potential of innervated muscles. These results strongly support the hypothesis that the decreased membrane potential in denervated fibers reflects a relative increase in the membrane permeability to sodium.     

Ultrastructural and physiological studies on the longitudinal body wall muscle of Dolabella auricularia. II. Localization of intracellular calcium and its translocation during mechanical activity

The localization of Ca-accumulating structures in the longitudinal body wall muscle (LBWM) of the opisthobranch mollusc Dolabella auricularia and their role in the contraction-relaxation cycle were studied by fixing the LBWM fibers at rest and during mechanical response to 400 mM K or to 10(-4)--10(-3) M acetylcholine in a 1% OsO4 solution containing 2% K pyroantimonate. In the resting fibers, electron-opaque pyroantimonate precipitate was mostly localized at the peripheral structures, i.e., along the inner surface of the plasma membrane, at the membrane of the surface tubules, and at the sarcoplasmic reticulum. In the fibers fixed during mechanical activity, the precipitate was diffusely distributed in the myoplasm in the form of numerous particles with corresponding decrease in the amount of the precipitate at the peripheral structures. Electron-probe X-ray microanalysis showed the presence of Ca in the precipitate, indicating that the precipitate may serve as a measure of Ca localization. These results are in accord with the view that, in the LBWM, the Ca stored in the peripheral structures is released into the myoplasm to activate the contractile mechanism.     

An analysis of the relationships between subthreshold electrical properties and excitability in skeletal muscle

Skeletal muscle activation requires action potential (AP) initiation followed by its sarcolemmal propagation and tubular excitation to trigger Ca(2+) release and contraction. Recent studies demonstrate that ion channels underlying the resting membrane conductance (G(M)) of fast-twitch mammalian muscle fibers are highly regulated during muscle activity. Thus, onset of activity reduces G(M), whereas prolonged activity can markedly elevate G(M). Although these observations implicate G(M) regulation in control of muscle excitability, classical theoretical studies in un-myelinated axons predict little influence of G(M) on membrane excitability. However, surface membrane morphologies differ markedly between un-myelinated axons and muscle fibers, predominantly because of the tubular (t)-system of muscle fibers. This study develops a linear circuit model of mammalian muscle fiber and uses this to assess the role of subthreshold electrical properties, including G(M) changes during muscle activity, for AP initiation, AP propagation, and t-system excitation. Experimental observations of frequency-dependent length constant and membrane-phase properties in fast-twitch rat fibers could only be replicated by models that included t-system luminal resistances. Having quantified these resistances, the resulting models showed enhanced conduction velocity of passive current flow also implicating elevated AP propagation velocity. Furthermore, the resistances filter passive currents such that higher frequency current components would determine sarcolemma AP conduction velocity, whereas lower frequency components excite t-system APs. Because G(M) modulation affects only the low-frequency membrane impedance, the G(M) changes in active muscle would predominantly affect neuromuscular transmission and low-frequency t-system excitation while exerting little influence on the high-frequency process of sarcolemmal AP propagation. This physiological role of G(M) regulation was increased by high Cl(-) permeability, as in muscle endplate regions, and by increased extracellular [K(+)], as observed in working muscle. Thus, reduced G(M) at the onset of exercise would enhance t-system excitation and neuromuscular transmission, whereas elevated G(M) after sustained activity would inhibit these processes and thereby accentuate muscle fatigue.     

The effects of the antibiotics gramicidina,amphotericin B,and nystatin on the electrical properties of frog skeletal muscle

The antibiotics gramicidin A, amphotericin B, and nystatin drastically decrease the membrane resistance of frog skeletal muscle fibers without changing the total capacitance. The resting potential of muscle fibers treated with these antibiotics is essentially normal if the Ringer solution does not contain Na⁺.     

Functional properties of locust locomotor muscles

The ultrastructure of the muscle fibers and the electrical constants and responses of the membrane to microapplication of L-glutamate and acetylcholine were investigated in the longitudinal flight muscle and the flexor tibiae ofLocusta migratoria migratorioides. The twitch flight muscle differs from the slower leg muscle in the smaller size of its sarcomeres and the lower values of the space attenuation factor of the electrotonic potential, time constant, and resistance of the membrane. Microapplication of sodium L-glutamate at strictly definite points of the fibers of both muscles evoked depolarization responses of the membrane. In experiments on normal and denervated muscle, during microapplication of acetylcholine, changes in the level of the membrane potential were never observed. It is concluded that L-glutamic acid is the excitatory mediator of the twitch and slow muscle systems of insects.I. M. Sechenov Institute of Evolutionary Physiology and Biochemistry, Academy of Sciences of the USSR, Leningrad. Translated from Neirofiziologiya, Vol. 9, No. 5, pp. 532–538, September–October, 1977.     

The neural control of contraction in a fast insect muscle.

The wing muscles used in singing by the katydid, Neoconocephalus robustus, are extraordinarily fast. At 35 degrees C, the animal's thoracic temperature during singing, an isometric twitch lasts only five to eight msec (onset to 50% relaxation) and the fusion frequency of these muscles is greater than 400 Hz. Stimulating the motornerve to a singing muscle initiates a short (2.5 msec at 35 degrees C), sometimes overshooting depolarization of the muscle fibers. Despite their spike-like appearance, the electrical responses are largely synaptic potentials. The muscle membrane appears to be capable of only weak, electrically-excitable, depolarizing electrogenesis. The short synaptic potentials result in part from rapidly-developing delayed rectification, in part from a low resting membrane resistance (Rm = 162 omega cm2) and a concomitantly short membrane time constant (about 1.5 msec).     

Electrical Properties of Structural Components of the Crystalline Lens

The electrical properties of the crystalline lens of the frog eye are measured with stochastic currents applied with a microelectrode near the center of the preparation and potential recorded just under the surface. The stochastic signals are decomposed by Fourier analysis into sinusoidal components, and the impedance is determined from the ratio of mean cross power to input power. The data are fit by an electrical model that includes two paths for current flow: one through the cytoplasm, gap junctions, and outer membrane; the other through inner membranes and the extracellular space between lens fibers. The electrical properties of the structures of the lens which appear as circuit components in the model are determined by the fit to the data. The resistivity of the extracellular space within the lens is comparable to the resistivity of Ringer. The outer membrane has a normal resistance of 5 kohm · cm² but large capacitance of 10 μF/cm², probably because it represents the properties of several layers of fibers. The inner membranes have properties reminiscent of artificial lipid bilayers: they have high membrane resistance, 2.2 megohm · cm², and low specific capacitance, 0.8 μF/cm². There is so much membrane within the lens, however, that the sum of the current flow across all the inner membranes is comparable to that across the outer surface.     

Electrical properties and transmitter output associated with growth and transformation in shrimp muscle fibers

Summary Comparisons were made of the passive electrical properties of closer muscle fibers in the dimorphic claws of snapping shrimp,Alpheus armillatus. During claw transformation the small fibers of pincer claws grow to become much larger snapper claw fibers. As muscle fibers grow, the relationship of fiber input resistance (R ₀) to fiber diameter (d) is predicted by the proportionality,R ₀d ^–3/2. Muscle fiber membrane resistance,R _m, is independent of fiber diameter, but membrane capacitance,C _m, grows with diameter. This results in a 40 to 50 fold reduction in fiber input impedance as fiber diameter enlarges during transformation. Reductions of muscle fiber impedance are partially compensated by 2–5 fold increases in quantal content at excitatory synapses on snapper muscle fibers. However, changes in quantal content during transformation apparently are independent of fiber diameter per se. Excitatory junction potentials in both pincer and snapper muscle fibers have equal amplitude. Because fiber input impedance decreases precipitously during transformation, and in view of the relatively small compensatory changes in quantal content at excitatory synapses, additional pre- or post-synaptic modifications must supplement increased quantal content to maintain synaptic efficacy in transformed muscle fibers.Abbreviations ejp excitatory junctional potential - epp endplate potential - mepp miniature endplate potential     

Electrical properties and excitation-contraction coupling in skeletal muscle treated with ethylene glycol

The contractility of the frog sartorius muscle was suppressed after treatment with a Ringer solution added with ethylene glycol (EGR). No contraction was elicited by nerve stimulation when the muscle was brought back to normal Ringer solution after having been soaked in 876 mM EGR for 4 hr or in 1095 mM EGR for 2 hr. However, the action potential of normal amplitude was generated and followed by a depolarizing afterpotential. The resting membrane potential was slightly decreased from the mean normal value of –91.1 mv to –78.8 mv when 1095 mM EGR was used, and to –82.3 mv when 876 mM EGR was used, but remained almost constant for as long as 2 hr. The afterpotential that follows a train of impulses and a slow change in membrane potential produced by a step hyperpolarizing current (so-called "creep") were suppressed after treatment with ethylene glycol. The specific membrane capacity decreased to about 50% of the control values while the specific membrane resistance increased to about twice the control values Therefore, the membrane time constant remained essentially unchanged. The water content of the muscle decreased by about 30% during a 2 hr immersion in 1095 mM EGR, and increased by about 30% beyond the original control level after bringing the muscle back to normal Ringer. The intracellular potassium content did not change significantly during these procedures. Some differences between the present results and those obtained with glycerol are discussed.     

Influence of intercellular clefts on potential and current distribution in a multifiber preparation.

A theoretical model is presented for current and voltage clamp of multifiber bundles in a double sucrose gap. Attention is focused on methodological errors introduced by the intercellular cleft resistance. The bundle is approximated by a continuous geometry. Voltage distribution, as a function of radial distance and time, is defined by a parabolic partial differential equation which is specified for different membrane characteristics. Assuming a linear membrane, analytical solutions are given for current step and voltage step conditions. The theoretical relations (based on Bessel functions) may be used to calculate membrane conductance and capacity from experimental clamp data. The case of a nonlinear membrane with standard Hodgkin-Huxley kinetics for excitatory Na current is treated assuming maximum Na conductances (gNa) of 120, 10, and 1 mmho/cm2. Numerical simulations are presented for potential and current distribution in a bundle of 60 microns diameter during depolarizing voltage steps. Adequate voltage control is restricted to the peripheral fibers of the bundle whereas the membrane potential of the inner fibers deviates from the command level during early inward current, tending to the Na equilibrium potential. In the peak current-voltage diagram the loss of voltage control is reflected by an increased steepness of the negative region and a decreased slope conductance of the positive region. With gNa = 120 mmho/cm2, the positive slope conductance is approximately 25% of the slope expected from ideal space clamping. With the lower values of gNa, the slope conductance ratio is in the order of 50%. Implications of the results for an experimental voltage clamp analysis of early inward current on multifiber preparations are discussed.     

An analysis of the relationship between the current and potential generated by a quantum of acetylcholine in muscle fibers without transverse tubules

Summary Miniature end plate potentials (MEPPs) were recorded in glyceroltreated muscle fibers with four microelectrodes which were used to determine the passive electrical characteristics of the same fibers. Voltage responses which were computed from miniature end plate currents (MEPCs) and the passive cable properties of a fiber, agreed very closely with experimentally recorded MEPPs confirming the hypothesis that MEPPs spread passively along a muscle fiber. The model was used to analyze the effect of variations in synaptic current and the properties of a muscle fiber on the postsynaptic response. The decrement of MEPPs was exponential for distances up to 1 to 2 mm from an origin but then deviated from the initial exponential. Variations in the growth time of the input current up to 1 msec had little effect on computed MEPPs whereas an increase in the decay time constant caused a significant increase in MEPP amplitude and effective space constant. An increase in the internal resistivity of a muscle fiber increased MEPP amplitude at the origin but decreased the effective space constant. The amplitude of MEPPs was inversely proportional to the 1.5 power of the diameter of a muscle fiber, and the MEPP space constant increased as the square root of the diameter. The amplitude of MEPPs is not necessarily determined by the input resistance of the muscle fiber. Changes in input resistance caused by changes in membrane resistance would have little effect on te amplitude or decrement of MEPPs.