The effects of external Ca++ and Mg++ on the voltage sensitivity of desensitization in Electrophorus electroplaques

Desensitization onset was studied in voltage-clamped Electrophorus electroplaques during prolonged exposure to bath-applied carbamylcholine. The time-course of desensitization was described by a first-order rate constant kappa obs, which increased exponentially with membrane hyperpolarization from -20 to -90 mV. When Ca++ was increased from 2 to 10 mM, the voltage sensitivity of kappa obs decreased; kappa obs decreased for voltages more negative than -40 mV, and increased slightly at voltages more positive than -40 mV. 10 mM Mg++ had a less pronounced effect and the voltage sensitivity of kappa obs was unchanged. The equilibrium level of desensitization, estimated from the carbamylcholine-dependent conductance which remained after desensitization was apparently complete, also increased with hyperpolarization.     

Calcium channel currents in isolated smooth muscle cells from human bronchus

An electrophysiological study was carried out on smooth muscle cells that were enzymatically dissociated from bundles of muscle fibers dissected out of human bronchi obtained at thoracotomy. These cells that retain the contractile properties of intact bundles were voltage-clamped by means of the whole-cell patch-clamp technique. Upon voltage steps from a holding potential of -60 mV to more positive levels, the initial inward current was followed by large outward currents that inactivated slowly. These were subsequently reduced by substituting Cs+ for K+ in the internal solution and by using Ba2+ instead of Ca2+ as a charge carrier in the external solution. Under these conditions, the inward current did not completely inactivate in the course of 300-ms voltage steps. Inward current measured after leak subtraction was activated at a membrane potential of -25.8 +/- 5 mV, was maximum at +18 +/- 4 mV, and had an apparent reversal potential of +52.5 +/- 5.5 mV (n = 5). The potential at which steady-state inactivation was half-maximum was -28 mV (n = 5). This inward current was identified as a calcium current on the following basis: 1) it was not altered by 10 microM tetrodotoxin (TTX) or by lowering to 10 mM external Na+ concentration; 2) it was blocked by 2.5 mM Co2+ or 1 microM PN 200-110; 3) it was enhanced by 1 microM BAY K 8644, which in addition suppressed the PN 200-110 blockade.(ABSTRACT TRUNCATED AT 250 WORDS)     

Kinetic properties of cholinergic desensitization in Aplysia neurons

The kinetic properties of desensitization onset of excitatory cholinergic responses were studied in isolated, voltage-clamped Aplysia neurons. Desensitization of the acetylcholine (ACh)-induced current in response to microperfused acetylcholine occurred in two phases, and was best modelled as the sum of two exponential components plus a constant. Both exponential components were accelerated by increasing ACh dose. At the higher ACh doses the current decline was dominated by the fast exponential component, and the ratio of the plateau-peak current was reduced. Over the range of membrane potentials -50 to -110 mV, no change in the kinetics of desensitization onset was observed. The mean time constants of both exponential components were doubled by cooling from 20 degrees C to 5 degrees C. These results demonstrate that, as at the vertebrate neuromuscular junction, the onset of desensitization of this ACh response involves at least two processes which are dose- and temperature-sensitive. The lack of voltage dependence contrasts with results from vertebrate preparations, and indicates a fundamental difference between the properties of the excitatory ACh response in Aplysia neurons and the vertebrate neuromuscular junction.     

A quantitative comparison of the time-course of sensitivity changes produced by calcium injection and light adaptation in Limulus ventral photoreceptors

The time-course of light and dark adaptation was quantitatively compared with the time-course of the onset of and recovery from desensitization produced by intracellular calcium injection in Limulus ventral photoreceptors. The onset of light adaptation tended to be faster (by 60-90 s) than the onset of desensitization produced by intracellular Ca++ injection. The initial portion of the time-course of dark adaptation was faster (about 10-20 s) than the time-course of recovery from desensitization produced by intracellular Ca++ injection. The final portion of recovery from Ca++ injection had the same time-course as a comparable dark adaptation.     

Voltage dependence of desensitization. Influence of calcium and activation kinetics

The voltage dependence of carbachol-induced desensitization has been analyzed in potassium-depolarized frog sartorius muscle preparations with voltage clamp techniques over a wide voltage range (-120 to +40 mV). Desensitization developed exponentially at all voltages with tau, the time constant of desensitization onset, varying as a logarithmic function of membrane voltage. The voltage dependence of tau remained in calcium-deficient solutions and was not altered by elevating either the level of extracellular or intracellular calcium. We have analyzed our results according to a simple sequential kinetic scheme in which the rate-limiting step in the development of desensitization is a transition of the receptor channel complex from the activated conducting state to a desensitized, nonconducting state. We conclude (a) that the observed voltage sensitivity of desensitization primarily resides in the voltage dependence of this transition, and (b) the kinetics of activation appear to have a greater influence on the observed rate of desensitization than on its voltage dependence. The magnitude of the voltage dependence suggests that a greater change in free energy is required for the transition to the desensitized state than for the transition between the open and closed states of the receptor channel complex.     

Kinetics of intramembrane charge movement and sodium current in frog node of Ranvier

Intramembrane charge movement (Q) and sodium current (INa) were monitored in isolated voltage-clamped frog nodes of Ranvier, ON charge movements (QON) for pulses from the holding potential (-100 mV) to potentials V less than or equal to 0 mV followed single exponential time courses, whereas two exponentials were found for pulses to V greater than or equal to 20 mV. The voltage dependence of both QON and its time constant tauON indicated that the two ON components resolved at V greater than or equal to 20 mV were also present, though not resolvable, for pulses to V less than or equal to 0 mV. OFF charge movements (QOFF) monitored at various potentials were well described by single exponentials. When QOFF was monitored at -30 or -40 mV after a 200-microsecond pulse to +20 mV and QON was monitored at the same potential using pulses directly from -100 mV, tauON/tauOFF = 2.5 +/- 0.3. At a set OFF potential (-90 to -70 mV), tauOFF first increased with increasing duration tON of the preceding pulse to a given potential (0 to +30 mV) and then decreased with further increases in tON. The declining phase of tauOFF followed a time course similar to that of the decline in QOFF with tON. For the same pulse protocol, the OFF time constant tauNa for INA also first increased with tON but then remained constant over the tON interval during which tauOFF and QOFF were declining. After 200- or 300-microsecond pulses to +20, +20, or +50 mV, tauOFF/tauNa at -70 to -90 mV was 1.2 +/- 0.1. Similar tauOFF/tauNa ratios were predicted by channel models having three identical charged gating particles that can rapidly and reversibly form an immobile dimer or trimer after independently crossing the membrane from their OFF to their ON locations.     

Voltage-dependent block of charge movement components by nifedipine in frog skeletal muscle

Potential-dependent inhibition of charge movement components by nifedipine was studied in intact, voltage-clamped, frog skeletal muscle fibers. Available charge was reduced by small shifts in holding potential (from -100 mV to -70 mV) in 2 microM nifedipine, without changes in the capacitance deduced from control (-120 mV to -100 mV) voltage steps made at a fully polarized (-100 mV) holding potential. These voltage-dependent effects did not occur in lower (0-0.5 microM) nifedipine concentrations. The voltage dependence of membrane capacitance at higher (10 microM) nifedipine concentrations was reduced even in fully polarized fibers, but shifting the holding voltage produced no further block. Voltage-dependent inhibition by nifedipine was associated with a fall in available charge, and a reduction in the charge and capacitance-voltage relationships and of late (q gamma) charging transients. It thus separated a membrane-capacitance with a distinct and steep steady-state voltage dependence. Tetracaine (2 mM) reduced voltage-dependent membrane capacitance and nonlinear charge more than did nifedipine. However, nifedipine did not exert voltage-dependent effects on charging currents, membrane capacitance, or inactivation of tetracaine-resistant (q beta) charge. This excludes participation of q beta, or the membrane charge as a whole, from the voltage-dependent effects of nifedipine. Rather, the findings suggest that the charge susceptible to potential-dependent block by nifedipine falls within the tetracaine-sensitive (q gamma) category of intramembrane charge.     

Inactivation of excitation-contraction coupling in rat extensor digitorum longus and soleus muscles

K contractures and two-microelectrode voltage-clamp techniques were used to measure inactivation of excitation-contraction coupling in small bundles of fibers from rat extensor digitorum longus (e.d.l.) and soleus muscles at 21 degrees C. The rate of spontaneous relaxation was faster in e.d.l. fibers: the time for 120 mM K contractures to decay to 50% of maximum tension was 9.8 +/- 0.5 s (mean +/- SEM) in e.d.l. and 16.8 +/- 1.7 s in soleus. The rate of decay depended on membrane potential: in e.d.l., the 50% decay time was 14.3 +/- 0.7 s for contractures in 80 mM K (Vm = 25 mV) and 4.9 +/- 0.4 s in 160 mM K (Vm = -3 mV). In contrast to activation, which occurred with less depolarization in soleus fibers, steady state inactivation required more depolarization: after 3 min at -40 mV in 40 mM K, the 200 mM K contracture amplitude in e.d.l. fell to 28 +/- 10% (n = 5) of control, but remained at 85 +/- 2% (n = 6) of control in soleus. These different inactivation properties in e.d.l. and soleus fibers were not influenced by the fact that the 200 mM K solution used to test for steady state inactivation produced contractures that were maximal in soleus fibers but submaximal in e.d.l.: a relatively similar depression was recorded in maximal (200 mM K) and submaximal (60 and 80 mM K) contracture tension. A steady state "pedestal" of tension was observed with maintained depolarization after K contracture relaxation and was larger in soleus than in e.d.l. fibers. The pedestal tension was attributed to the overlap between the activation and inactivation curves for tension vs. membrane potential, which was greater in soleus than in e.d.l. fibers. The K contracture results were confirmed with the two-microelectrode voltage clamp: the contraction threshold increased to more positive potentials at holding potentials of -50 mV in e.d.l. or -40 mV in soleus. At holding potentials of -30 mV in e.d.l. or 0 mV in soleus, contraction could not be evoked by 15-ms pulses to +20 mV. Both K contracture and voltage-clamp experiments revealed that activation in soleus fibers occurred with a smaller transient depolarization and was maintained with greater steady state depolarization than in e.d.l. fibers. The K contracture and voltage-clamp results are described by a model in which contraction depends on the formation of a threshold concentration of activator from a voltage-sensitive molecule that can exist in the precursor, activator, or inactive states.     

Developmental differences in Ca2+-activated K+ channel activity in ovine basilar artery

A primary determinant of vascular smooth muscle (VSM) tone and contractility is the resting membrane potential, which, in turn, is influenced heavily by K+ channel activity. Previous studies from our laboratory and others have demonstrated differences in the contractility of cerebral arteries from near-term fetal and adult animals. To test the hypothesis that these contractility differences result from maturational changes in voltage-gated K+ channel function, we compared this function in VSM myocytes from adult and fetal sheep cerebral arteries. The primary current-carrying, voltage-gated K+ channels in VSM myocytes are the large conductance Ca2+-activated K+ channels (BKCa) and voltage-activated K+ (KV) channels. We observed that at voltage-clamped membrane potentials of +60 mV in perforated whole cell studies, the normalized outward current densities in fetal myocytes were >30% higher than in those of the adult (P < 0.05) and that these were predominantly due to iberiotoxin-sensitive currents from BKCa channels. Excised, insideout membrane patches revealed nearly identical unitary conductances and Hill coefficients for BKCa channels. The plot of log intracellular [Ca2+] ([Ca2+]i) versus voltage for half-maximal activation (V(1/2)) yielded linear and parallel relationships, and the change in V(1/2) for a 10-fold change in [Ca2+] was also similar. Channel activity increased e-fold for a 19 +/- 2-mV depolarization for adult myocytes and for an 18 +/- 1-mV depolarization for fetal myocytes (P > 0.05). However, the relationship between BKCa open probability and membrane potential had a relative leftward shift for the fetal compared with adult myocytes at different [Ca2+]i. The [Ca2+] for half-maximal activation (i.e., the calcium set points) at 0 mV were 8.8 and 4.7 microM for adult and fetal myocytes, respectively. Thus the increased BKCa current density in fetal myocytes appears to result from a lower calcium set point.     

Sodium channel inactivation in the crayfish giant axon. Must channels open before inactivating?

Experiments on sodium channel inactivation kinetics were performed on voltage-clamped crayfish giant axons. The primary goal was to investigate whether channels must open before inactivating. Voltage-clamp artifacts were minimized by the use of low-sodium solutions and full series resistance compensation, and the spatial uniformity of the currents was checked with a closely spaced pair of electrodes used to measure local current densities. For membrane potentials between -40 and +40 mV, sodium currents decay to zero with a single exponential time-course. The time constant for decay is a steep function of membrane potential. The time-course of inactivation measured with the double-pulse method is very similar to the decay of current at the same potential. Steady-state inactivation curves measured with different test pulses are identical. The time-course of double pulse inactivation shows a lag that roughly correlates with the opening of sodium channels, but detailed comparisons with the time course of the prepulse current suggest that it is not strictly necessary for channels to open before inactivating. Measurements of the potential dependence of the integral of sodium conductance area also inconsistent with the simplest cases of models in which channels must open before inactivating.     

Kinetic properties of intramembrane charge movement under depolarized conditions in frog skeletal muscle fibers

Intramembrane charge movement was measured on skeletal muscle fibers of the frog in a single Vaseline-gap voltage clamp. Charge movements determined both under polarized conditions (holding potential, VH = -100 mV; Qmax = 30.4 +/- 4.7 nC/micro(F), V = -44.4 mV, k = 14.1 mV; charge 1) and in depolarized states (VH = 0 mV; Qmax = 50.0 +/- 6.7 nC/micro(F), V = -109.1 mV, k = 26.6 mV; charge 2) had properties as reported earlier. Linear capacitance (LC) of the polarized fibers was increased by 8.8 +/- 4.0% compared with that of the depolarized fibers. Using control pulses measured under depolarized conditions to calculate charge 1, a minor change in the voltage dependence (to V = -44.6 mV and k = 14.5 mV) and a small increase in the maximal charge (to Qmax = 31.4 +/- 5.5 nC/micro(F] were observed. While in most cases charge 1 transients seemed to decay with a single exponential time course, charge 2 currents showed a characteristic biexponential behavior at membrane potentials between -90 and -180 mV. The voltage dependence of the rate constant of the slower component was fitted with a simple constant field diffusion model (alpha m = 28.7 s-1, V = -124.0 mV, and k = 15.6 mV). The midpoint voltage (V) was similar to that obtained from the Q-V fit of charge 2, while the steepness factor (k) resembled that of charge 1. This slow component could also be isolated using a stepped OFF protocol; that is, by hyperpolarizing the membrane to -190 mV for 200 ms and then coming back to 0 mV in two steps. The faster component was identified as an ionic current insensitive to 20 mM Co2+ but blocked by large hyperpolarizing pulses. These findings are consistent with the model implying that charge 1 and the slower component of charge 2 interconvert when the holding potential is changed. They also explain the difference previously found when comparing the steepness factors of the voltage dependence of charge 1 and charge 2.     

Fast inactivation causes rectification of the IKr channel

The mechanism of rectification of HERG, the human cardiac delayed rectifier K+ channel, was studied after heterologous expression in Xenopus oocytes. Currents were measured using two-microelectrode and macropatch voltage clamp techniques. The fully activated current- voltage (I-V) relationship for HERG inwardly rectified. Rectification was not altered by exposing the cytoplasmic side of a macropatch to a divalent-free solution, indicating this property was not caused by voltage-dependent block of outward current by Mg2+ or other soluble cytosolic molecules. The instantaneous I-V relationship for HERG was linear after removal of fast inactivation by a brief hyperpolarization. The time constants for the onset of and recovery from inactivation were a bell-shaped function of membrane potential. The time constants of inactivation varied from 1.8 ms at +50 mV to 16 ms at -20 mV; recovery from inactivation varied from 4.7 ms at -120 mV to 15 ms at -50 mV. Truncation of the NH2-terminal region of HERG shifted the voltage dependence of activation and inactivation by +20 to +30 mV. In addition, the rate of deactivation of the truncated channel was much faster than wild-type HERG. The mechanism of HERG rectification is voltage-gated fast inactivation. Inactivation of channels proceeds at a much faster rate than activation, such that no outward current is observed upon depolarization to very high membrane potentials. Fast inactivation of HERG and the resulting rectification are partly responsible for the prolonged plateau phase typical of ventricular action potentials.     

Voltage-activated Ca2+ currents in insulin-secreting cells

Membrane voltage and voltage-clamped membrane currents have been investigated with the whole-cell patch clamp method in the insulin-secreting cell line RINm5F. The mean resting membrane potential of RINm5F cells was found to be -52 mV. Overshooting spike potentials could be evoked by depolarising voltage steps in the absence of a secretagogue. Inward membrane currents evoked by depolarising voltage steps were dependent upon extracellular Ca2+ and blocked by Co2+, nifedipine and verapamil. Outward membrane currents which were evoked by depolarising voltage steps to positive membrane potentials were reduced when Ca2+ entry was prevented. It is concluded that the voltage-activated Ca2+ currents underlie the voltage-activated spike potentials recorded from insulin-secreting cells.     

Altered E-C coupling in rat ventricular myocytes from failing hearts 6 wk after MI

Excitation-contraction (E-C) coupling was investigated in rat hearts 6 wk after induction of myocardial infarction (MI) by ligation of the left coronary artery. Heart weight was increased by 74% and left ventricular end-diastolic pressure was 23 +/- 2 mmHg in MI compared with 8 +/- 2 mmHg in sham-operated controls (Sham, P < 0.001). Cell shortening was measured in voltage-clamped myocytes at 36 degrees C. In solutions where Cs(+) had been replaced by K(+), the voltage dependence of contraction was sigmoidal between -20 and +100 mV in Sham and MI cells. Verapamil (20 microM) blocked L-type Ca(2+) current and reduced contraction in Sham cells by approximately 50% (P < 0.01) but did not decrease contraction significantly in MI cells at test potentials above +10 mV. Verapamil-insensitive contractions were blocked by Ni(2+) (5 mM). Na(+)/Ca(2+) exchange current was doubled in MI compared with Sham cells at test potentials between -20 and +80 mV (P < 0.05), whereas mRNA and protein expression increased by 30-40%. Finally, voltage dependence of contraction was bell shaped in Na(+)-free solutions, but contraction was significantly increased in MI cells over a wider voltage range (P < 0.05). The insensitivity to Ca(2+) channel block in MI cells may result from an increased contribution of the Na(+)/Ca(+) exchanger to triggering of E-C coupling. These results suggest significant changes in E-C coupling in the hypertrophy and failure that develop in response to extensive MI.     

Intramembrane charge movement and L-type calcium current in skeletal muscle fibers isolated from control and mdx mice

Dystrophin-deficient muscle fibers from mdx mice are believed to suffer from increased calcium entry and elevated submembranous calcium level, the actual source and functional consequences of which remain obscure. Here we compare the properties of the dihydropyridine receptor as voltage sensor and calcium channel in control and mdx muscle fibers, using the silicone-voltage clamp technique. In control fibers charge movement followed a two-state Boltzmann distribution with values for maximal charge, midpoint voltage, and steepness of 23 +/- 2 nC/ micro F, -37 +/- 3 mV, and 13 +/- 1 mV (n = 7). Essentially identical values were obtained in mdx fibers and the time course of charge recovery from inactivation was also similar in the two populations (tau approximately 6 s). In control fibers the voltage dependence of the slow calcium current elicited by 100-ms-long pulses gave values for maximal conductance, apparent reversal potential, half-activation potential, and steepness factor of 156 +/- 15 S/F, 65.5 +/- 2.9 mV, -0.76 +/- 1.2 mV, and 6.2 +/- 0.5 mV (n = 17). In mdx fibers, the half-activation potential of the calcium current was slightly more negative (-6.2 +/- 1.2 mV, n = 16). Also, when using longer pulses, the time constant of calcium current decay was found to be significantly larger (by a factor of 1.5-2) in mdx than in control fibers. These changes in calcium current properties are unlikely to be primarily responsible for a dramatic alteration of intracellular calcium homeostasis. They may be speculated to result, at least in part, from remodeling of the submembranous cytoskeleton network due to the absence of dystrophin.     

Membrane depolarization facilitates sperm entry, large fertilization cone formation, and prolonged current responses in sea urchin oocytes

Depolarization of the sea urchin egg's membrane is required for two processes during fertilization: the entry of the fertilizing sperm and the block to polyspermy which prevents the entry of supernumerary sperm. In an immature sea urchin oocyte, the depolarization is very small in response to the attachment of a sperm. The purpose of this study was to determine whether the depolarization evoked by sperm attaching to an oocyte can facilitate sperm entry or induce the block to polyspermy. Individual oocytes of the sea urchin with diameters which ranged from 86 to 102% that of the average diameter for mature eggs from the same female were examined. The oocytes have a membrane potential of -73 +/- 6 mV (SD, n = 80) and a very low input resistance compared to that of mature eggs. Single sperm, following attachment to an oocyte, elicit a brief, small depolarization with a maximum amplitude of 8 +/- 1.4 mV (SE, n = 15), frequently followed by the formation of tiny filament-like fertilization cones, but the sperm fail to enter. If oocytes are voltage-clamped at membrane potentials more negative than -20 mV, following attachment of the sperm small transient inward currents occur, similar filament-like cones form, and the sperm do not enter. When many sperm attach to an oocyte which is not voltage clamped, the depolarizations sum to create a large depolarization with an amplitude of 60 to 80 mV, which shifts the oocyte's membrane potential to a value between -10 and +5 mV; more positive values are not attained. At such membrane potentials, whether the potential is maintained by the summed depolarizations of many attached sperm or by voltage clamp, large fertilization cones form, the sperm enter, and the oocytes can become highly polyspermic. In oocytes voltage clamped at +20 mV, however, both sperm entry and fertilization cone formation are suppressed. Therefore, both types of voltage-dependence for sperm entry are present in oocytes, although the depolarization caused by a single sperm is not large enough to permit its entry, nor is the depolarization caused by many sperm sufficient to prevent the entry of supernumerary sperm.     

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.     

Acetylcholine contracture of the fast muscle fibers in the lamprey, Lampetra fluviatilis]

Fast fibers of m. longitudinalis linguae respond to Ach by a transient contracture with a half-decay period of 3-5 sec. The threshold concentration of Ach is approximately 10(-7) g/ml. Ach contracture is based on even depolarization of the whole muscle membrane. Threshold level of the MP for the onset of contracture lies between --50 and --40 mV. In the presence of Ach depolarization decreases twofold within 40-70 sec. Relaxation is not due to the decrease of depolarization. Contraction--Ach concentration curve has a small slope; it reaches maximum at a concentration 10(-4) g/ml, which corresponds to the MP ca. -10mV. Equilibrium Ach potential is significantly shifted to depolarization as compared to that in frog muscles, being equal to +1+/-1.8 mV.     

Simultaneous measurements of Ca2+ currents and intracellular Ca2+ concentrations in single skeletal muscle fibers of the frog

The relationship between Ca2+ current amplitudes and myoplasmic Ca2+ transients was studied in single muscle fibers. Segments of muscle fibers were voltage-clamped in a double Vaseline gap chamber. Ca2+ transients were measured as an optical signal derived from the interaction between Ca2+ and the dye antipyrylazo III. The cells were maintained at -90 mV. Ca2+ currents were detected at pulse potentials to -50 mV, reached a maximum value at 0 mV, were reduced in size for larger depolarizations, and reversed at about 40 mV. Ca2+ transients were also detected at -50 Mv and progressively increased in size with larger pulse potentials up to 10 mV. Depolarizations to voltages greater than 10 mV did not further increase the size of the transient. The magnitude and time course of transients from 10 to 70 mV were almost identical Ca2+ fluxes into the myoplasm (Ca2+ input fluxes) were calculated from the Ca2+ transients applying a removal model. The size of the input fluxes increased with depolarization up to 0 mV. Between 0 and 70 mV the peak input flux slightly increased, while the flux measured at 200 ms remained unchanged. In conclusion, Ca2+ transients and input fluxes were not reduced during pulses to large positive potentials, even though a drastic reduction of Ca2+ current occurred at these potentials. These observations make it very unlikely that a voltage-dependent Ca2+ entry is the triggering signal for contraction.     

The sodium current underlying action potentials in guinea pig hippocampal CA1 neurons

Neurons were acutely dissociated from the CA1 region of hippocampal slices from guinea pigs. Whole-cell recording techniques were used to record and control membrane potential. When the electrode contained KF, the average resting potential was about -40 mV and action potentials in cells at -80 mV (current-clamped) had an amplitude greater than 100 mV. Cells were voltage-clamped at 22-24 degrees C with electrodes containing CsF. Inward currents generated with depolarizing voltage pulses reversed close to the sodium equilibrium potential and could be completely blocked with tetrodotoxin (1 microM). The amplitude of these sodium currents was maximal at about -20 mV and the amplitude of the tail currents was linear with potential, which indicates that the channels were ohmic. The sodium conductance increased with depolarization in a range from -60 to 0 mV with an average half-maximum at about -40 mV. The decay of the currents was not exponential at potentials more positive than -20 mV. The time to peak and half-decay time of the currents varied with potential and temperature. Half of the channels were inactivated at a potential of -75 mV and inactivation was essentially complete at -40 to -30 mV. Recovery from inactivation was not exponential and the rate varied with potential. At lower temperatures, the amplitude of sodium currents decreased, their time course became longer, and half-maximal inactivation shifted to more negative potentials. In a small fraction of cells studied, sodium currents were much more rapid but the voltage dependence of activation and inactivation was very similar.