Charge movement in a fast twitch skeletal muscle from rat

Voltage-dependent charge movement in the rat omohyoid muscle was investigated using the three microelectrode voltage clamp technique. The charge that moved during a depolarization from the holding potential (-90 mV) to the test potential, V, increased with increasing V, saturating around 0 mV. The charge vs. voltage relationship was well fitted by Q = Q_max/{1 + exp[-(V - V)/k]}, with Q_max = 28.5 nC/μF, V = -34.2 mV, and k = 8.7 mV. Repolarization of the fiber from the test potential back to the holding potential caused an equal but opposite amount of charge to move. The kinetics of ON charge movement could be well described by a model developed for frog muscle by Horowicz and Schneider (1981b), which suggests that rat and frog charge movements are similar. This model failed to describe the kinetics of OFF charge movement for steps in potential from 0 mV to test potentials of -10 to -90 mV. OFF-charge movement rose to a peak more slowly and decayed more slowly than predicted by the theory.     

The effects of modified ringer's solutions on the membrane potentials of innervated and denervated frog sartorius muscle fibers

Comparison has been made between innervated and chronically denervated frog sartorius muscle fibers for resting potentials and a number of features of the action potential. Muscles were obtained from force-fed frogs maintained at room temperature for periods up to one year, and were studied with intracellular microelectrodes. Denervated muscles increased in sensitivity to acetylcholine by 100–400-fold. Studies were made in normal Ringer's solution, and in media in which concentrations of K⁺, Na⁺, Ca⁺⁺, and Cl? were altered. The only significant differences noted between the denervated and the innervated fibers were a reduction in the maximum rate of fall of the action potential (ca. 20%) and an increase in the fall time of the active membrane potential (ca. 25%). These differences were present in normal Ringer's solution and remained when the bathing medium was modified. The resting membrane potential of denervated and innervated muscles varied with log [K⁺]_o in exactly the same manner, and followed the theoretical relation proposed by Hodgkin (Proc. Roy. Soc., B, 148: 1–37, ′58), with the term representing the ratio of the sodium to potassium permeabilities assigned a value of 0.01. The results suggest that (a) the resting sodium and potassium permeabilities are reduced proportionately after denervation, since it is known that denervated frog muscle has a smaller potassium permeability, and (b) the mechanism controlling the increase in potassium conductance during the action potential is less available after denervation. Data indicate that the system controlling the sodium permeability is capable of activation to the same extent as in innervated muscles. Muslces which had been allowed to reinnervate did not show the differences presented by the denervated muscles. Innervated and denervated muscles did not show any significant changes in maximum rates of rise or fall of the action potential, nor of the active membrane potential amplitude over a 30 mV range of resting membrane potentials, indicating that the sodium and potassium permeability systems are fully available in frog muscle at membrane potentials larger than ?80 mV.     

Voltage-clamp of cut-end skeletal muscle fibre: a diffusion experiment

Membrane potential and current were studied in cut end fibres of frog skeletal muscle under current and voltage clamp conditions, by the double sucrose gap technique. Similar action potentials were recorded under current clamp conditions with either the microelectrode or the double sucrose gap techniques. Under voltage clamp conditions, the control of the membrane potential was maintained adequately. The early current was sensitive to both TTX and external Na concentration suggesting that the current was carried by Na ions. Sodium current (INa) was subsequently analysed using the Hodgkin-Huxley formulae. INa half-activation and inactivation occurred at -34 mV and -60 mV, respectively. Na-rich solution applied internally by diffusion through cut ends produced a reduction of INa associated with a shift of the sodium current reversal potential (VNa) towards more negative membrane potentials. This suggested that the sodium electromotive force was reduced by the increase in internal Na content of the fibre. Iodate applied externally changed neither the activation nor the inactivation time courses of INa, but reduced the peak current. Conversely, internally applied by diffusion from the cut end of skeletal muscle fibre, iodate slowed down the time course of INa inactivation and decreased the current peak. In conclusion, the double sucrose gap technique adapted to cut end frog skeletal muscle fibre allows a satisfactory analysis of INa.     

A study of properties of batrachotoxin modified sodium channels

A further analysis of the effects of the steroidal alkaloid batrachotoxin (BTX) on sodium channels in frog node of Ranvier has been carried out under voltage-clamp conditions. The main properties of modified channels as compared with those of normal ones are as follows: The rate of channel closing is drastically decreased, whereas that of opening is changed slightly if at all; The steady-state voltage dependence of channel activation is shifted towards more negative potentials by 60-70 mV; Currents through modified channels do not show a decay during maintained depolarization as it is typical for normal channels. However modified channels retain the ability to partial inactivation as shown by experiments with depolarizing prepulses; Sodium against potassium selectivity beyond--20 mV suggesting either nonhomogeneity of the modified channels as for their kinetic and selectivity properties or potential-dependence of ionic selectivity for each channel; The selectivity sequence determined from peak current reversal potential measurements is as follows: H: Na :NH4:K = 528:1:0.47: :0.19; The effective pK value of proton block is decreased by about 0.4; 7) The sensitivity of the channels to tetrodotoxin (TTX) block is practically unchanged.     

Measurement of Intracellular pH of Bullfrog Skeletal Muscle and Renal Tubular Cells with Double-Barreled Antimony Microelectrodes

A pencil-type antimony microelectrode of double-barreled design with a tip of less than 1 to 2 μm in outside diameter was constructed and used to measure intracellular pH(pHi) on frog sartorius muscle and renal tubular cells. Simultaneous observations of membrane potential difference (EM) were made. The results obtained were as follows: (1) The in vivo pHi of frog sartorius muscle was 7.12 ± 0.07 (SD) (n = 144); the simultaneously measured E_M was -51.1 ± 7.9 mV. The in vivo pHi of frog proximal tubule was 7.49 ± 0.07 (n = 221) and the E_M peri across the peritubular membrane was -50.2 ± 9.0 mV. (2) In proximal tubule in vivo, there was a negative correlation between pHi and E_M (r = -.62, p <. 05). On the other hand, in sartorius muscle in vivo, a positive correlation between the two was found (r =. 85, p <. 001). (3) In in vitro sartorius muscle, the pHi was 7.03 ± 0.14 (n = 9) and E_M was -62.4 ± 4.4 mV within one hour after isolation. (4) Increasing the external potassium concentration in the preparations to 75 mM caused a progressive depolarization by 43.3 ± 15.9 (m = 4) mV, while pHi changed in the alkaline direction by 0.22 ± 0.03 pH unit. (5) These results indicate that the pHi in both tissues does not obey the Donnan rule.     

The electrical block to polyspermy induced by an intracellular Ca2+ increase at fertilization of the clawed frogs,Xenopus laevis and Xenopus tropicalis

Polyspermy blocking, to ensure monospermic fertilization, is necessary for normal diploid development in most animals. We have demonstrated here that monospermy in the clawed frog, Xenopus tropicalis, as well as in X. laevis, is ensured by a fast, electrical block to polyspermy on the egg plasma membrane after the entry of the first sperm, which is mediated by the positive‐going fertilization potential. An intracellular Ca²⁺ concentration ([Ca²⁺]_i) at the sperm entry site was propagated as a Ca²⁺ wave over the whole egg cytoplasm. In the X. tropicalis eggs fertilized in 10% Steinberg's solution, the positive‐going fertilization potential of +27 mV was generated by opening of Ca²⁺‐activated Cl^?‐channels (CaCCs). The fertilization was completely inhibited when the egg's membrane potential was clamped at +10 mV and 0 mV in X. tropicalis and X. laevis, respectively. In X. tropicalis, a small number of eggs were fertilized at 0 mV. In the eggs whose membrane potential was clamped below ?10 mV, a large increase in inward current, the fertilization current, was recorded and allowed polyspermy to occur. A small initial step‐like current (IS current) was observed at the beginning of the increase in the fertilization current. As the IS current was elicited soon after a small increase in [Ca²⁺]_i, this is probably mediated by the opening of CaCCs. This study not only characterized the fast and electrical polyspermy in X. tropicalis, but also explained that the initial phase of [Ca²⁺]_i increase causes IS current during the early phase of egg activation of Xenopus fertilization.     

Potential-dependent changes in ionic selectivity of batrachotoxin-modified sodium channels of frog nerve fiber

Ionic currents through sodium channels modified by batrachotoxin were measured by the voltage clamp method on a myelinated frog nerve fiber membrane. The reversal potential (E_rev) of steady-state currents was shown to be on the average 5 mV less positive than E_rev corresponding to the initial (peak) values of the currents. The results of control experiments using procaine and tetrodotoxin showed that the change in E_rev observed during a depolarizing pulse is not connected with the presence of unmodified sodium channels or unblocked potassium channels, with nonlinearity of leakage, or with a change in transmembrane gradients of current-carrving cations. In experiments with measurement of "instant" currents it was shown that E_rev becomes less positive as the amplitude and duration of preliminary depolarization increase. The results support the view that sodium-potassium selectivity of batrachotoxin-modified sodium channels depends on potential.     

Potassium channels in Eremosphaera viridis

The dependence of the membrane potential of Eremosphaera viridis on different external concentrations of potassium, sodium, calcium, and protons was compared with the diffusion potential measured in the dark and in the presence of NaN₃. In contrast to some other algae, the membrane potential in the light as well as in the dark seemed to be predominantly determined by the calculated diffusion potential and less by an electrogenic pump which, however, seemed to be involved at potassium concentrations >1 mol·m^-3 and at higher pH_os (>pH 6). Furthermore, some characteristics of an action-potential-like response (CAP) triggered by light-off, and independent of the membrane-potential threshold value, were determined. The CAP had a delay period of 5.4 s and needed 4.5 s for polarization to a plateau. On average, the plateau held for 8.8 s and the CAP lasted 37.7 s. The peak amplitudes of CAP (P _AP) exactly followed the Nernst potential of potassium. Other cations like sodium, calcium and protons did not appreciably affect the peak amplitudes of CAP. From these and other results it can be assumed that the CAP is caused by a temporary opening of potassium channels in the plasma membrane of Eremosphaera (Köhler et al., 1983, Planta 159, 165–171). The release of a CAP by light-off has been partly explained by the participation of a transient increase of proton concentration in the cytoplasm. It was possible to trigger a CAP by external pH changes and by the addition of sodium acetate, thus supporting the hypothesis that a pH decrease in the cytoplasm may be one element of the signal transfer from the photosynthetic system to the potassium channels in the plasmalemma. Calcium also seemed to have an influence on triggering the CAP.Abbreviations and symbols CAP chemical-induced action-potential-like response - E _D calculated diffusion potential (mV) - E _D ^* measured diffusion potential (mV) - E _K potassium equilibrium potential (mV) - E _m membrane potential (mV) - P _AP peak of action potential (mV) Part II will appear in Planta, Vol. 167, No. 1, 1986     

Contractile activity is required for Z‐disc sarcomere maturation in vivo

Sarcomere structure underpins structural integrity, signaling, and force transmission in the muscle. In embryos of the frog Xenopus tropicalis, muscle contraction begins even while sarcomerogenesis is ongoing. To determine whether contractile activity plays a role in sarcomere formation in vivo, chemical tools were used to block acto‐myosin contraction in embryos of the frog X. tropicalis, and Z‐disc assembly was characterized in the paralyzed dicky ticker mutant. Confocal and ultrastructure analysis of paralyzed embryos showed delayed Z‐disc formation and defects in thick filament organization. These results suggest a previously undescribed role for contractility in sarcomere maturation in vivo. genesis 53:299–307, 2015. © 2015 The Authors. Genesis Published by Wiley Periodicals, Inc.     

Tonic activity of parasympathetic efferent nerve fibers hyperpolarizes the resting membrane potential of frog taste cells

We investigated the relationship between the membrane potential of frog taste cells in the fungiform papillae and the tonic discharge of parasympathetic efferent fibers in the glossopharyngeal (GP) nerve. When the parasympathetic preganglionic fibers in the GP nerve were kept intact, the mean membrane potential of Ringer-adapted taste cells was -40 mV but decreased to -31 mV after transecting the preganglionic fibers in the GP nerve and crushing the postganglionic fibers in the papillary nerve. The same result occurred after blocking the nicotinic acetylcholine receptors on parasympathetic ganglion cells in the tongue and blocking the substance P neurokinin-1 (NK-1) receptors in the gustatory efferent synapses. This indicates that the parasympathetic nerve (PSN) hyperpolarizes the membrane potential of frog taste cells by -9 mV. Repetitive stimulation of a transected GP nerve revealed that a -9-mV hyperpolarization of taste cells maintained under the intact GP nerve derives from an approximately 10-Hz discharge of the PSN efferent fibers. The mean frequency of tonic discharges extracellularly recorded from PSN efferent fibers of the taste disks was 9.1 impulses/s. We conclude that the resting membrane potential of frog taste cells is continuously hyperpolarized by on average -9 mV by an approximately 10-Hz tonic discharge from the parasympathetic preganglionic neurons in the medulla oblongata.     

Activation of contraction by voltage-clamped stimulation in crayfish muscle fibers (author's transl)

It is known that the properties of the excitation-contraction coupling of crayfish skeletal muscle are different in some respects from those of frog muscle. In the present study, activation of contraction of the crayfish muscle induced by short depolarizing pulses was investigated and it was compared with the results of frog muscle obtained by Adrian, Chandler and Hodgkin (1969). Two glass microelectrodes were inserted into the thoracal muscle of the crayfish. The muscle was stimulated by the voltage-clamped pulses of different durations and the resulting contractions were observed under the binocular microscope with the magnification of 60 X at 20 approximately 23 degrees C. The rheobasic membrane potential was -55mV. The mechanical threshold potential was -42 mV for 10 msec, -15 mV for 2.5 msec, +18 mV for 1 msec and around +90 mV for 0.5 msec pulses. For short pulses where the threshold potential was more positive than -20 mV, the area of the depolarization above -30 mV was 51 mV-msec. Subthreshold pulses produced contraction if applied repetitively. The effect of a just suprathreshold short pulse on the activation of contraction was cancelled by the hyperpolarizing pulse.     

Electrogenic responses elicited by transmembrane depolarizing current in aerated body wall muscles ofDrosophila melanogaster larvae

Summary Electrical excitability of the longitudinal ventrolateral body wall muscle of the third instar larva ofDrosophila melanogaster was demonstrated. This is in contrast to previous papers which have reported that this muscle is electrically inexcitable. It was found that an air supply to the muscle through the tracheoles is essential for maintaining its excitability. In an aerated preparation, the muscle maintained a resting potential of around –80 mV for more than 1.5 h, while a nonaerated muscle depolarized to about –30 mV within 30 min. Muscles with resting potentials larger than –70 mV showed graded regenerative potentials with a double-peaked configuration in response to transmembrane depolarizing current. A tetrodotoxin- (TTX-)sensitive, voltage-dependent inward sodium current, and a tetraethylammonium-(TEA-)sensitive, voltage-dependent outward potassium current were found to be responsible for the first peak of the electrogenic response of this muscle. The rising phase of the second peak was caused by a cobalt/manganese-sensitive, voltage-dependent inward calcium current that had a threshold level near –40 mV. Elimination by TEA or barium of the delayed rectification following the first peak caused the second peak to be triggered at a lower threshold. The second peak was profoundly elongated by barium, and this effect was antagonized by external calcium. Thus, the falling phase of the second peak was most likely driven by a calcium-dependent, outward potassium current.     

Determination of the electromotive force of active sodium transport in frog skin epithelium (Rana temporaria) from presteady-state flux ratio experiments

Summary The presteady-state influxes and effluxes of sodium across frog skin epithelium have been determined as a function of time while all electrophysiological parameters were maintained constant. The fluxes measured were resolved in the fractions which have passed a pathway through the cells and those that have used a paracellular pathway. The procedure is based on the theory that all presteady-state flux ratios have to be equal to the steady-state flux ratio if only one pathway is involved. The flux ratios for the transcellular route were used to calculate the electromotive force of the sodium pump. The calculation hinges on the assumptions (a) that both influx and efflux have to pass through the sodium pump and (b) that single file diffusion of sodium is not taking place anywhere along the path. The validity of both assumptions is discussed. Our calculated values for the electromotive force of the sodium pumpE _Na ^a vary between 146 and 200 mV, which is in agreement with the energy of the ATP/ADP system. There is a distinct indication that, as the electrochemical gradient for sodium opposing the transport is being increased, the emf increases towards an asymptotic value around 200 mV. The relation between the value ofE _Na ^a and the cellular phosphorylation potential for ATP is discussed.     

Membrane properties of identified embryonic nerve and glial cells of the leech central nervous system

Summary The membrane potential of identified nerve (Retzius) cells and neuropil glial cells from 11 (±1) day-old embryos of the leechHirudo medicinalis was recorded using conventional intracellular microelectrodes. At this stage all ganglia of the segmental nervous system are formed. The membrane potential of Retzius cells was –68±4 mV (±SD,n=8), and showed a slope of 42 mV between 10 mM and 100 mM external K concentration. Retzius cells were able to fire action potentials which had a fast Na-dependent component, and, under appropriate conditions, also generated slow Ca (Ba) action potentials. The mean membrane potential of the neuropil glial cell at physiological K concentration (4 mM) was –83±5 mV (±SD,n=10), and showed a dependence of 56 mV for a tenfold change in the external K concentration (> 4mM). Neuropil glial cells showed no signs of voltage-activated excitability, but they repeatedly depolarized in the presence of 0.1 mM 5-HT.     

Development of transgenic Xenopus laevis with a high C-src gene expression

Xenopus laevis larvae with an elevated expression of c-src were generated by mating a transgenic X. laevis male frog carrying proviral Rous sarcoma virus (RSV) long terminal repeat (LTR) and most of the pol gene sequences in its sperm DNA and a normal X. laevis female frog. Offspring (15–20%) with a higher dosage of c-Src, detected in disorganized myotomal musculature and in cerebral and spinal neuronal cells by immunohistochemical analysis, developed abnormally, with edemas (in most cases), head deformities, and eye and axial system defects. In the remaining embryos, a small increase in c-src expression seemed to be compatible with normal embryogenesis. The dosage of c-Src correlated with the dosage of RSV LTR integrated in frog DNA as revealed by Southern and polymerase chain reaction (PCR) analyses. Authenticity of the integrated RSV LTR including enhancer sequence was proved by sequencing. Probing of total RNA from aberrant larvae demonstrated several times higher dosage of c-src mRNA in their tissues than in control tadpoles. We hypothesize that the integrated RSV regulatory sequences can stimulate the expression of c-src proto-oncogene of X. laevis above a treshold that interferes with the early developmental program of frog embryos. Mol. Reprod. Dev. 50:410–419, 1998. © 1998 Wiley-Liss, Inc.     

Hyperpolarizing photoreceptors in the eyes of the giant clamTridacna: physiological evidence for both spiking and nonspiking cell types

Summary Intracellular studies on photoreceptors in the eyes of the giant clamTridacna give evidence for two types of light-sensitive cells, both of which are hyperpolarized by light. These cells are distinguished by the presence or absence of spikes and corresponding characteristics of the receptor potential. In non-spiking (NS) receptors, the average resting potential in the dark is low (-15 mV) and peak receptor potentials are large (to 100 mV) and adapt rapidly to light. Spiking (S) receptors have higher average resting potentials (-45 mV), but receptor potentials do not exceed 20 mV and also do not adapt to light. The spikes in S-receptors are small (3–8 mV), occur spontaneously at low levels of illumination and are inhibited by light. Bursts of spikes arise on the repolarizing off-component of the receptor potential. Light adaptation increases the excitability of S-receptors in terms of a higher frequency and shorter latency of the off response burst. The receptor potential in both cells is due to a light-activated increase in membrane conductance to potassium ions. Membrane conductance decreases in NS-receptors in relation to light adaptation. Unlike the scallop eye, no depolarizing photoreceptors are present.Abbreviations NS non-spiking photoreceptors - S spiking photoreceptors - SW seawater     

Electrophysiological and Theoretical Analysis of Depolarization-Dependent Outward Currents in the Dendritic Membrane of an Identified Nonspiking Interneuron in Crayfish

Depolarization-dependent outward currents were analyzed using the single-electrode voltage clamp technique in the dendritic membrane of an identified nonspiking interneuron (LDS interneuron) in situ in the terminal abdominal ganglion of crayfish. When the membrane was depolarized by more than 20 mV from the resting potential (65.0 ± 5.7 mV), a transient outward current was observed to be followed by a sustained outward current. Pharmacological experiments revealed that these outward currents were composed of 3 distinct components. A sustained component (I _s) was activated slowly (half rise time > 5 msec) and blocked by 20 mM TEA. A transient component (I _t1) that was activated and inactivated very rapidly (peak time < 2.5 msec, half decay time < 1.2 msec) was also blocked by 20 mM TEA. Another transient component (I _t2) was blocked by 100 M 4AP, activated rapidly (peak time < 10.0 msec) and inactivated slowly (half decay time > 131.8 msec). Two-step pulse experiments have revealed that both sustained and transient components are not inactivated at the resting potential: the half-maximal inactivation was attained at –21.0 mV in I _t1, and –38.0 mV in I _t2. I _s showed no noticeable inactivation. When the membrane was initially held at the resting potential level and clamped to varying potential levels, the half-maximal activation was attained at –36.0 mV in I _s, –31.0 mV in I _t1 and –40.0 mV in I _t2. The activation and inactivation time constants were both voltage dependent. A mathematical model of the LDS interneuron was constructed based on the present electrophysiological records to simulate the dynamic interaction of outward currents during membrane depolarization. The results suggest that those membrane conductances found in this study underlie the outward rectification of the interneuron membrane as well as depolarization-dependent shaping of the excitatory synaptic potential observed in current-clamp experiments.     

Activation of the frog sartorius acetylcholine receptor by a covalently attached group

Summary The frog sartorius motor endplate was treated with the specific disulfide bond reducing agent dithiothreitol and subsequently exposed to a covalently reacting compound (the nitrophenyl ester ofp-carboxyphenyltrimethylammonium iodide, NPTMB) known to activate the dithiothreitol-reduced acetylcholine receptor inElectrophorus electroplax. NPTMB causes a maximum depolarization of about 35 mV when applied to the dithiothreitol-treated sartorius motor endplate. It is ineffective on postjunctional membrane prior to disulfide bond reduction and on extrajunctional regions, reduced or unreduced. High concentrations of a competitive antagonist such as (+)-tubocurarine prevent reaction between NPTMB and the reduced receptor and cause a repolarization of the membrane when applied to the already-depolarized preparation. We conclude that in frog muscle, as in electroplax, the attached activator bridges the acetylcholine binding site of the reduced receptor between a sulfhydryl group, to which it is covalently bound, and a negative subsite, with which it forms a reversible ionic bond.     

Potential dependence of unidirectional chloride fluxes across isolated frog skin

Isolated frog skins were voltage clamped at transepithelial potentials (Vt) ranging from -60 mV to 60 mV to measure transepithelial 36Cl- fluxes from the apical to the basolateral bathing solution (J13) and in the opposite direction (J31). The potential dependence of fluxes obtained in Na+-free choline Ringer's indicates the presence of conductive and nonconductive components that probably correspond to fluxes through paracellular and cellular pathways, respectively. Rectification of fluxes with reversal of the potential reflects a structural asymmetry, presumably in surface charge density. The data are consistent with a charge density of one negative charge per 280 A2 on the apical side. A new model for passive Cl- transport was developed that includes surface charge asymmetry and specifically accounts for the observed variation of conductance with potential. In normal frog Ringer's, J13 was larger than J31 at zero potential (active Cl- transport), J13 rose exponentially with increasing positive potential to reach a maximum at 40 mV (approximately open-circuit), and the predicted partial Cl- conductance exceeded the measured conductance leading to the conclusion that when J13 is largely driven by Na+ transport, much of the coupling occurs via nonconductive pathways. Theophylline stimulates Cl- transport that also occurs via nonconductive pathways as Vt becomes more positive.