Changes in holding and ion-channel currents during activation of an ascidian egg under voltage clamp

Calmodulin and immunophilin are required as functional partners of a ryanodine receptor in ascidian oocytes at fertilization

Fertilization of oocytes incites numerous changes relying on Ca(2+) signaling. In inseminated ascidian eggs, an increase in the egg surface membrane, monitored by a change in electrical capacitance, is recorded at the onset of meiosis resumption. This membrane addition to the cell surface is controlled by calcium release through a ryanodine receptor (RyR), sensitive to cyclic ADP-ribose. Using confocal microscopy analysis of ascidian oocytes immunostained with anti-RyR antibody, we show here that this calcium channel is asymmetrically located in the vegetal cortical zone. Interestingly, the increase in cell capacitance occurring at fertilization is correlated with a fluorescent signal, imaged by the marker of vesicle trafficking FM 1-43, located close to the RyR region. Two putative partners of RyR, namely an FKBP-like protein and a calmodulin, are identified in these oocyte extracts by detection of enzyme activity and PCR amplification. Both are necessary to sustain ryanodine receptor activity in these oocytes since the membrane insertion triggered by fertilization is inhibited by the FKBP ligand rapamycin and by a calmodulin antagonist peptide. These findings suggest that exocytosis in ascidian eggs is triggered at fertilization by a functional Ca(2+) release unit operating as a complex of several proteins, including a calmodulin and an immunophilin, around the intracellular calcium channel itself.

Ion channels and early development of neural cells

In this review we underscore the merits of using voltage-dependent ion channels as markers for neuronal differentiation from the early stages of uncommitted embryonic blastomeres. Furthermore, a fairly large part of the review is devoted to the descriptions of the establishment of a simple model system for neural induction derived from the cleavage-arrested eight-cell ascidian embryo by pairing a single ectodermal with a single vegetal blastomere as a competent and an inducer cell, respectively. The descriptions are focused particularly on the early developmental processes of various ion channels in neuronal and other excitable membranes observed in this extraordinarily simple system, and we compare these results with those in other significant and definable systems for neural differentiation. It is stressed that this simple system, for which most of the electronic and optical methods and various injection experiments are applicable, may be useful for future molecular physiological studies on the intracellular process of differentiation of the early embryonic cells. We have also highlighted the importance of suppressive mechanisms for cellular differentiation from the experimental results, such as epidermal commitment of the cleavage-arrested one-cell Halocynthia embryos or suppression of epidermal-specific transcription of inward rectifier channels by neural induction signals. It was suggested that reciprocal suppressive mechanisms at the transcriptional level may be one of the key processes for cellular differentiation, by which exclusivity of cell types is maintained.

The two intracellular Ca2+ release channels, ryanodine receptor and inositol 1,4,5-trisphosphate receptor, play different roles during fertilization in ascidians

Fertilization in the ascidians triggers an activation wave of calcium release followed by intracellular calcium oscillations synchronous with periodic membrane potential excursions during the completion of the meiotic cell cycle. Fertilization also causes a fast decrease in the egg plasma membrane depolarization-activated calcium current and a large increase in capacitance thought to represent membrane addition to the egg surface. We have analyzed the temporal and causal relationships between these changes in the eggs of Phallusia mammillata using whole-cell patch-clamp recording while simultaneously imaging calcium with fura-2 dextran. We have defined the role of ryanodine receptor (RyR) and InsP3 receptor (InsP3R) during fertilization and meiosis by looking at the effects of InsP3, cyclic ADP ribose (cADPR), and ryanodine in perfused oocytes. We show that InsP3 (10 microM perfused through the patch pipette) is able to trigger sustained oscillations in intracellular calcium concentration in unfertilized oocytes, resembling those recorded in fertilized egg completing meiosis. In addition the sustained oscillations resulting from InsP3 perfusion in unfertilized oocytes are sufficient to cause the emission of both polar bodies. In contrast, ryanodine or cADPR never trigger detectable calcium signal in perfused oocytes. Instead, nanomolar concentrations of ryanodine or cADPR cause a capacitance change, implying a net insertion of membrane to the oocyte surface, and trigger a fast decrease in the depolarization-activated calcium current. Both changes are similar to the changes in conductance and capacitance naturally observed following fertilization. These effects, although not associated with measurable calcium signals, are abolished by coperfusion of the calcium chelator BAPTA. In contrast to ryanodine or cADPR, sustained perfusion of the oocyte with nanomolar concentrations of InsP3 causes no capacitance change and a slow and moderate decrease in calcium current. Our observations on inseminated patch-clamped eggs further indicate that membrane insertion, which starts 15-20 sec after the onset of the membrane conductance change at fertilization, can be altered by interfering with the RyR. Our results imply that, in ascidians, as in some mammals, RyR and InsP3R play distinct roles during fertilization.

Differential developmental fates of the two calcium currents in early embryos of the ascidian Ciona intestinalis

Two voltage-dependent calcium currents have been described in unfertilized eggs of the ascidian Ciona intestinalis: a low threshold, slowly activating current, and a high threshold fast one. According to the classical criteria for classification of calcium currents, they both share some of the features of L-like and T-like currents. We have studied these two calcium currents further by measuring their sensitivity to permeant ions, temperature and inhibitors. Both currents were sensitive to relatively high concentrations of nitrendipine, which was a selective blocker of the low threshold channel. The lanthanide ion gadolinium was a potent blocker of the low threshold current, and cadmium preferentially inhibited the high threshold current. The two calcium currents were regulated in a different manner after fertilization. The density of the high threshold current remained relatively constant, while the low threshold current was lost by the time of first cleavage. This loss following fertilization is similar to the loss of a low threshold sodium current in fertilized eggs of the ascidian Boltenia villosa. Block of the cell cycle with various compounds did not prevent loss of the low threshold calcium current. This observation adds weight to the hypothesis that a loss of excitability is a general property of early development. We conclude that fertilization can differentially modulate channel populations before first cleavage. The mechanism by which this occurs in the ascidian embryo has yet to be discovered.

Neural induction suppresses early expression of the inward-rectifier K+ channel in the ascidian blastomere

1. Early expression of ion channels following neural induction was examined in isolated, cleavage-arrested blastomeres from the ascidian embryo using a two-electrode voltage clamp. Currents were recorded from the isolated, cleavage-arrested blastomere, a4-2, after treatment with serine protease, subtilisin, which induces neural differentiation as consistently as cell contact. 2. The inward-rectifier K+ current increased at the late gastrula stage shortly after the sensitive period for neural induction both in the induced (protease-treated) and uninduced cells. Ca2+ channels, characteristic of epidermal-type differentiation, and delayed-rectifier K+ channels and differentiated-type Na+ channels, characteristic of neural-type differentiation appeared much later than the inward-rectifier K+ channels, at a time corresponding to the tail bud stage of the intact embryo. 3. When cells were treated with subtilisin during the critical period for neural induction, the increase in the inward-rectifier K+ current from the late gastrula stage to the neurula stage was about three times smaller (3.67 +/- 1.74 nA, mean +/- S.D., n = 14) than in untreated cells (11.25 +/- 3.10 nA, n = 26). The same changes in the inward-rectifier K+ channel were also observed in a4 2 blastomeres which were induced by cell contact with an A4-1 blastomere. However, when cells were treated with subtilisin after the critical period for neural induction, the amplitude of the inward-rectifier K+ current was the same as in untreated cells. Thus the expressed level of the inward-rectifier K+ channel was linked to the determination of neural or epidermal cell types. 4. There was no significant difference in the input capacitance of induced and uninduced cells, indicating that the difference in the amplitude of the inward-rectifier K+ currents derived from a difference in the channel density rather than a difference in cell surface area. 5. The expression of the inward-rectifier K+ channel at the late gastrula stage was sensitive to alpha-amanitin, a highly specific transcription inhibitor. In both induced and uninduced cells, injection of alpha-amanitin at the 32-cell stage reduced the current density of the inward-rectifier K+ channel to about 2 nA/nF, corresponding to 13% of that recorded from uninjected cells. By contrast, the expression of the fast-inactivating-type Na+ current, which transiently increased along with the inward-rectifier K+ channel, was resistant to alpha-amanitin injection. 6. The dose of alpha-amanitin injected was controlled by monitoring co-injected fluorescent dye, fura-2.(ABSTRACT TRUNCATED AT 400 WORDS)

Changes in voltage-dependent ion currents during meiosis and first mitosis in eggs of an ascidian

Different patterns of voltage-dependent ion currents are present in mature eggs and in early embryos of the ascidian Boltenia villosa, as if each ion current is regulated in a different manner between fertilization and the early cleavages of embryogenesis. The ion currents appear and/or disappear with precise timing suggesting that they play important roles at specific times during early development. We investigated changes in three voltage-dependent ion currents (an inwardly rectifying chloride current, a calcium current, and a sodium current) and membrane surface area over time between the resumption of meiosis (with fertilization or activation) and the first mitotic cleavage. Using time-lapse video recordings made during whole-cell patch-clamp experiments, we were able to correlate electrophysiological changes with morphological changes and cell cycle related events. Between fertilization and first cleavage, INa was lost exponentially, the density of ICa remained relatively constant, and the amplitudes of both ICl and membrane surface area fluctuated in time with the cell cycle. ICl and surface area increased whenever the cell began dividing--with the polar body extrusions and the formation of the first cleavage furrow. This suggested that the values of ICl and surface area were largest during interphase and smallest during M-phase of each cell cycle. This hypothesis was supported by an experiment in which entry into M-phase was blocked in fertilized eggs by inhibiting protein synthesis. This prevented the decreases of ICl and surface area but allowed the increases to occur normally. Patterns of change in ion currents are current specific and, as is the case with ICl, are tightly correlated with developmental events.

The fertilization potential and associated membrane potential oscillations during the resumption of meiosis in the egg of the ascidian Phallusia mammillata

The fertilization potential in Phallusia mammillata consisted of an initial rapid depolarization. This initial sperm-triggered depolarization was followed by a phase of membrane depolarization which was of either long or short duration, depending on the eggs. When of long duration, the phase of membrane depolarization was divided into two periods: the first one began with a plateau (Em = +20.2 +/- 1.1 mV; duration = 1.7 +/- 0.14 min) which was followed by a series of membrane potential oscillations (n = 3.1 +/- 0.25) lasting 2.4 +/- 0.2 min. The second period also began as a plateau (Em = approximately 0 mV; duration = 3.40 +/- 0.20 min) which was followed by a series of oscillations (n = 11.5 +/- 0.5) lasting 11.8 +/- 0.6 min, followed by a membrane repolarization. The second series of oscillations often continued rising from the resting potential value. In the eggs displaying a short duration of membrane depolarization, the second period of depolarization was shortened (lasting only 3.5 +/- 0.5 min) since it lacked the second plateau. In addition it displayed a smaller number of oscillations (n = 4.7 +/- 0.6). As a consequence of this shortening, the membrane repolarized sooner. After repolarization, the membrane displayed several potential oscillations that started from the repolarization level. Regardless of the length of the depolarized plateau phases, the total number of membrane oscillations and the time period during which they occurred were constant. Eggs displaying a long depolarization phase had 15.9 +/- 0.6 oscillations in a 19.5 +/- 0.6 min interval, while eggs having a short depolarization phase had 16.0 +/- 0.8 oscillations in a 18.1 +/- 0.3 min interval. The time period during which the potential oscillations occurred corresponded remarkably well with the time of the meiotic divisions: the formation of the first polar body was detected about 80 sec after the end of the first series of oscillations; the second polar body was extruded about 85 sec after the last membrane oscillation occurred.

A localized zone of increased conductance progresses over the surface of the sea urchin egg during fertilization

Although activation of a sea urchin egg by sperm leads to three phases of membrane conductance increase in the egg, the mechanism by which the sperm causes these conductance changes is not known. We used the loose patch clamp technique to localize the conductance changes in voltage clamped eggs. A patch of the egg's membrane was isolated from the bath by pressing the loose patch clamp pipette against the egg surface. Sperm added to the bath attached to the surface of the egg in a region other than at the isolated membrane patch. During phase 1 of the activation current, no changes of the membrane conductance were detected. At the time of, and subsequent to the onset of phase 2, large currents recorded between the interior of the patch pipette and the bath were attributed to changes of the seal resistance between the surface of the egg and the pipette. A local change of membrane conductance was observed during phase 2 despite the changes of seal resistance. During phase 2, the large amplitude and short duration of the local membrane conductance increase relative to the membrane, conductance increase for the whole egg during phase 2 indicated that the conductance increase occurred over the entire surface of the egg, but not simultaneously. The time when the peak conductance for the membrane patch occurred, relative to the time of onset for phase 2 in the whole egg, depended on the distance, measured in a straight line, between the site of sperm attachment and the tip of the pipette. These data indicate that the localized conductance increase progressed over the surface of the egg from the site of sperm attachment to the opposite pole of the egg. It is proposed that the local conductance increase, the cortical reaction, and the change of seal resistance are all evoked by a common cytoplasmic message that progresses throughout the cytoplasm of the egg from the site of sperm attachment to the opposite pole of the egg.

L-type Ca2+ currents in ascidian eggs

We have studied Ca2+ currents in ascidian eggs using the whole-cell clamp technique. T and L components, as observed in somatic cells, are present and the L-type current predominates. Since the IV relationship for these inward currents overlap at -30 mV, separation of the two components using different voltage regimes is not feasible. Increasing external Ca2+ results in larger currents. The L-type current decreases in a dose-dependent fashion in the presence of Mn2+ and Nifedipine, while the T-type current is inhibited in Ni2+. When Ba2+ was used as the carrier ion, channel kinetics and conductance were completely altered. Considering the density and kinetics of L-type channels in unfertilized eggs it is probable they play an important role in regulating cytosolic Ca2+ during early developmental processes.

Changes in sodium channels during neural differentiation in the isolated blastomere of the ascidian embryo

1. The current density and the kinetics of voltage-sensitive sodium channels during neural differentiation were examined in the isolated, cleavage-arrested blastomere of ascidian embryos which contains presumptive neural regions. The macroscopic sodium current were measured with the two-microelectrode voltage-clamp technique and the single sodium channel currents were recorded with the patch-clamp technique under the cell-attached configuration. 2. The entire time course of sodium channel development could be divided into three phases from the current density and channel gating properties. 3. In the first phase, from fertilization to about 40 h, the density of the sodium channel current was from 8 to 50 microA cm-2. The channel gating properties were similar to those of the sodium channel in the egg cell except for a negative shift in the voltage dependence of the peak inward current, the steady-state inactivation, and the decay time constant. The sodium channels in this phase were classified as 'type-I' channels. 4. In the second phase (40-60 h after fertilization), the density of the sodium channel current increased from 20 to 800 microA cm-2. The curves of the I-V relationship and of the steady-state inactivation shifted in the positive direction by 5-10 mV. 5. At 45-55 h, when the rate of increase in the sodium current was greatest, as much as 40 microA cm-2 h-1, the decay time course of the sodium current became slowest. The time for the current to decline from the peak to the one-tenth of the peak (t 1/10) increased to about five times that in the first phase. After 55 h t 1/10 gradually decreased. 6. In this phase, steady-state inactivation curves showed two inflexion points at different levels of membrane potential and were fitted with a sum of two Boltzmann distribution curves with distinct parameters. The relative contribution of the component with its voltage dependence shifted in the positive direction tended to decrease with development. 7. On examining single-channel recordings, two types of sodium channel were identified in this phase. One type (type-II) showed frequent repetitions of open-to-shut states throughout a voltage step. The ensemble current of the type-II channel showed a slow decay, suggesting that this type of channel may underlie the markedly slow decay of the macroscopic current in this phase. The second type (type-III) had more late openings than the type-I channel but fewer than the type-II channel.(ABSTRACT TRUNCATED AT 400 WORDS)

Voltage clamp studies of fertilization in sea urchin eggs. II. Current patterns in relation to sperm entry, nonentry, and activation

Following attachment of a sperm to the surface of a sea urchin egg clamped at a membrane potential (Vm) more positive than +17 mV, no changes in membrane conductance can be detected, the sperm does not enter egg, and no morphological changes can be detected. At Vm from +17 to -100 mV three characteristically different types of current profiles are observed: Type I are activation currents in eggs penetrated by a sperm. These have three phases, which occur in all eggs clamped at Vm from +17 to -20 mV and in decreasing percentages at clamped Vm more negative than -20 mV (to -75 mV). Complete fertilization envelopes are elevated, relatively large mound-shaped fertilization cones form, and the eggs develop to normal embryos. Type II are sperm transient currents in eggs not penetrated by a sperm, the eggs otherwise remaining in the unfertilized state. These transients are simpler and shorter than type I currents, and are observed only at clamped Vm more negative than -20 mV. Type III are modified activation currents in eggs not penetrated by a sperm. These have three phases, are observed only at clamped Vm more negative than -20 mV, and are the only type of activation current seen at clamped Vm more negative than -75 mV. Complete fertilization envelopes are elevated, the fertilization cones are small and filament-like, and the eggs fail to cleave. We conclude that (a) the sperm transient currents (type II) and phase 1 of the activation currents (type I and III) are similar events generated by a sperm-initiated localized conductance increase, (b) the abrupt decrease of current which terminates the sperm transients and phase 1 of type III currents results from a turnoff of the sperm-induced conductance increase and signals that the sperm will not enter the egg, and (c) the occurrence of phase 2 during an electrophysiological response induced by a sperm indicates that the egg is activating.

Fertilization alters the spatial distribution and the density of voltage-dependent sodium current in the egg of the ascidian Boltenia villosa

The spatial distribution of voltage-dependent ionic currents was characterized in Boltenia villosa eggs before and after fertilization using two-microelectrode voltage clamp of paired animal-vegetal halves of eggs (merogones) made surgically. Major voltage-dependent conductances in the Boltenia egg are a transient inward Na current, a transient inward Ca current, and an inwardly rectifying K current. These currents were randomly distributed along the animal-vegetal axis in the unfertilized egg. When paired merogones (surgically prepared egg fragments) were made at the vegetal cap stage, 15-30 min after fertilization, Ca and K currents remained randomly distributed along the animal-vegetal axis. In contrast, the relative Na current density was found to be twofold lower in the vegetal vs the animal merogones made at the vegetal cap stage. By making pairs of merogones from unfertilized eggs and subsequently fertilizing one merogone of a pair, we showed that this change in current density ratio was due to a loss of absolute Na current density in the vegetal hemisphere shortly after fertilization. These results also show that this loss was intrinsic to the vegetal hemisphere, rather than being determined solely by the point of sperm entry. A second decrease in Na current was observed during the hour before first cleavage, 60-120 min after fertilization (M.L. Block and W.J. Moody, 1987, J. Physiol. 393, 619-634), both in fertilized eggs and in animal merogones fertilized after isolation. This second loss of Na current was not observed in vegetal merogones fertilized after isolation or in either animal or vegetal merogones made from fertilized eggs at the vegetal cap stage. Possible mechanisms for te rapid (complete by 40 min after fertilization) and the late (occurring from ca. 60 to 120 minutes after fertilization) Na current losses are discussed.

Development of ionic channels and cell-surface antigens in the cleavage-arrested one-cell embryo of an ascidian

1. The developmental time course of the appearance of ionic channels was studied with the voltage-clamp technique at 8 degrees C in ascidian embryos in which cleavage was arrested with cytochalasin B immediately after fertilization. The ontogeny of cell-surface antigens was also studied using monoclonal antibodies in both normal and cleavage-arrested embryos. The cleavage-arrested 1-cell embryo differentiates into a cell of epidermal type expressing Ca2+, anomalous rectifier and Ca2+-induced K+ channels, and cell-surface antigens against tunic. 2. The size of the Sr2+ current through egg-type Ca2+ channels decreased during the initial 15 h and disappeared. At about 45 h a Sr2+ current reappeared; the properties of these new channels were different from those of the egg type and were considered to be those of differentiated epidermal Ca2+ channels. 3. Na+ currents also decreased during the first 15 h, and then tended to increase, reaching a peak at about 35 h before decreasing again and finally disappearing. 4. The K+ current through anomalous rectifier channels gradually increased in amplitude, reached a peak at about 35 h and then slightly decreased to a minimum at 45 h. It then increased with further development. 5. The K+ current through the Ca+-induced K+ channels appeared at 50 h and then increased. 6. Input capacity started to increase at 15 h, attained a peak value of three times that of the egg at about 35 h, and then decreased. 7. Two anti-tunic monoclonal antibodies, C1 and 2C5, were obtained. C1 bound only to the tunic; 2C5 bound to the tunic and to the cytoplasm of epidermal cells. 8. C1 antigens first appeared on the surface of the epidermis of the normal embryos and on the surface of the cleavage-arrested 1-cell embryo at about 45 h, and then increased in amount. 9. In the normal embryo 2C5 antigen was first detected at about 40 h inside epidermal cells. It started to accumulate on the epidermal surface at about 45 h and then appeared also in the tunic. In the cleavage-arrested embryo the antigen was first detected at about 50 h, and became more intensely stained as development proceeded.(ABSTRACT TRUNCATED AT 400 WORDS)

Electrical responses of eggs to acrosomal protein similar to those induced by sperm

The earliest known response of eggs to sperm in many species is a change in egg membrane potential. However, for no species is it known what components of the sperm cause the opening of the egg plasma membrane channels. Protein isolated from sperm acrosomal granules of the marine worm Urechis caused electrical responses in oocytes with the same form, amplitude, and ion dependence as the fertilization potentials induced by living sperm. Sperm initiated fertilization potentials in oocytes when sperm-oocyte fusion, but not binding, was inhibited by clamping oocyte membrane potentials to positive values. Acrosomal protein also initiated electrical responses in clamped oocytes. These results support the hypothesis that it is the sperm acrosomal protein that opens ion channels in the oocyte membrane.

Sperm-activated currents in ascidian oocytes

Using patch electrodes and the whole-cell recording technique to study fertilization currents in ascidian oocytes under voltage clamp, this paper shows that between -85 and 0 mV the currents are inward with an initial peak ranging from 50 to 600 pA. Voltages more positive than 0 mV inhibit initiation of the fertilization current, but by allowing the oocyte to return briefly to its resting potential fertilization occurs and fertilization currents are outward at positive potentials. By comparison with previous single-channel work, a fertilizing spermatozoon opens about 300 large-conductance channels with zero reversal potential.

A calcium-activated sodium conductance contributes to the fertilization potential in the egg of the nemertean worm Cerebratulus lacteus

The fertilization potential of the egg of the nemertean worm Cerebratulus lacteus consisted of a rapid shift from a resting potential of about -65 mV to a peak of about +44 mV; the peak was followed by a positive plateau at about +24 mV, lasting an average of 80 min. Reduction of extracellular calcium reduced the peak of the fertilization potential, indicating that the peak resulted from a calcium conductance, while reduction of extracellular sodium reduced the plateau potential, indicating that the plateau resulted from a sodium conductance. Microinjection of ethylene glycol bis(beta-aminoethyl ether)-N,N'-tetraacetic acid (EGTA) or 1,2-bis(o-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid (BAPTA)/CaBAPTA buffers, having a free calcium concentration of less than or equal to about 0.1 microM lowered the fertilization potential plateau. Injection of a BAPTA/CaBAPTA mixture with a free calcium concentration of about 1 microM resulted in a prolonged positive potential at the level of the fertilization potential plateau. These observations indicated that the fertilization potential of the Cerebratulus egg depended on a calcium-activated sodium conductance. The plateau potential was reduced little, if any, when calcium-free seawater was perfused through the bath during the fertilization potential; nor was it reduced in seawater containing cadmium. These observations suggested the possibility that intracellular calcium stores could be important in producing the fertilization potential.

Electrical characteristics of ascidian egg fragments

Fragments of ascidian eggs, but at random in any plane and ranging in size from 10 to 90% of the total egg volume, displayed the electrical characteristics of the intact egg, having a resting potential of -86 mV and giving rise to an action potential upon stimulation by electrical current injection. Following insemination, the fragments generated fertilization potentials, comparable to those of intact eggs, although the repolarization phase was shorter. Our data show that there are sufficient ion channels throughout the egg surface to generate action potentials and fertilization potentials in excised egg fragments, irrespective of their global origin. Furthermore, the fertilizing spermatozoon is capable of activating fertilization channels in areas of the egg plasma membrane not destined for sperm entry.

Fertilization potential and polyspermy prevention in the egg of the nemertean, Cerebratulus lacteus

We investigated the electrical properties of the egg of the nemertean worm Cerebratulus, and found evidence that an electrically-mediated polyspermy block operates for a period of about 1 hr after fertilization. At fertilization, in natural or artificial sea water, the membrane potential shifts from its resting level of about -66 mV to a peak of about +43 mV, and in most cases remains greater than 0 mV for more than 1 hr. The average potential during the first 30 min is +22 +/- 8 mV (SD, n = 12). When the external Na+ concentration is reduced from 486 to 51 mM (choline substituted) the fertilization potential amplitude is reduced; the average potential during the first 30 min is -27 +/- 21 mV (SD, n = 5). Eggs inseminated in 51 mM Na+ sea water become polyspermic, indicating that polyspermy prevention depends on an electrically-mediated mechanism. The electrical block is required for about 60 min, since transfer to 51 mM Na+ sea water during this period results in polyspermy. During the first hour following fertilization, the egg is also developing a permanent, nonelectrical block; the degree of polyspermy which results upon transfer to low Na+ sea water decreases progressively with time. The permanent block appears to be at the level of the egg plasma membrane or glycocalyx, since the egg envelope is not a barrier to sperm penetration, nor does its removal induce polyspermy. Electron micrographs show no obvious changes in the morphology of the extracellular layers, plasma membrane or cortex of the egg after fertilization.

Fertilization-induced ionic conductances in eggs of the frog, Rana pipiens

Fertilization of the frog egg (Rana pipiens) elicits a positive-going shift in membrane potential (fertilization potential) that lasts 10-20 min and functions as a fast block to polyspermy. We examined the ion conductances underlying the fertilization potential, using the voltage-clamp technique. We measured the membrane capacitance during the fertilization potential by applying an alternating current. We also determined the intracellular K and Cl concentrations in the egg, using ion-selective micro-electrodes. The conductance is largest in the first 2 min after fertilization. Regardless of whether the stimulus is provided by one or by more than one sperm or by artificial activation, the size of the conductance increase is the same, reaching a maximum of about 40 microseconds. Two separate conductances are involved at fertilization: Cl and K. [K]i = 121 mM and [Cl]i = 44 mM. The natural external medium is pond water (approximated in our experiments by 10% Ringer solution); therefore, an increase in K and Cl conductances leads to an efflux of both ions. The equilibrium potential of the fertilization current is between the Cl and K equilibrium potentials (ECl and EK), closer to ECl. 10 mM-external tetraethylammonium (TEA) brings the equilibrium potential close to ECl and reduces the maximum conductance by about half. The Cl conductance is not blocked by 4-acetamido-4'-isothiocyanostilbene-2,2'-disulphonic acid (SITS). The time courses of the K and Cl conductances are similar. The TEA-resistant conductance (primarily Cl conductance) activated at fertilization increases as the membrane potential becomes more positive. A voltage-sensitive Na conductance present in the unfertilized egg disappears after fertilization. During fertilization this conductance is too small to contribute significantly to the fertilization potential. The membrane capacitance increases by an average of 1.9 times in the first 2 min following the rise of the fertilization potential, during the period of cortical vesicle exocytosis. Capacitance then gradually decreases; at 1 h after fertilization, capacitance is 82% of the value in the unfertilized egg. The conductance increase precedes the capacitance increase by several seconds. Therefore the initial appearance of Cl and K channels cannot be accounted for by addition of membrane by cortical vesicle exocytosis. The conductance subsequently decreases, suggesting that the disappearance of the Cl and K channels is not caused by membrane removal.

Determination of excitability types in blastomeres of the cleavage-arrested but differentiated embryos of an ascidian

Cleavage of the embryo of Halocynthia roretzi was arrested with cytochalasin B at 1- to 32-cell stages and the embryo was cultured in sea water containing cytochalsin B until a developmental time equivalent to the hatching of the control larva. Membrane properties of the blastomeres were studied with constant-current and voltage-clamp techniques. Four types of membrane response - neural, epidermal, muscular and non-excitable - were identified on the basis of the shapes and ionic dependence of action potentials in the blastomeres of 8- to 32-cell embryos. Only the epidermal type of response was found in the blastomeres of 1- to 4-cell embryos. The blastomeres with responses of neural type had Na, Ca, delayed K rectifier, anomalous K rectifier and Ca-induced K channels. Those of epidermal type had Ca, anomalous K rectifier and Ca-induced K channels. Those of muscular type had Ca, delayed K rectifier, anomalous K rectifier and possibly Ca-induced K channels. Those of non-excitable type had almost none or small amounts of outward- and inward-going rectifier channels. The characteristic responses of neural type were found in small blastomeres in the animal hemisphere, which included some presumptive neural regions. The responses of muscular type were found in large blastomeres of the vegetal hemisphere, which included some presumptive regions for muscle. Those of epidermal type were found in the blastomeres of the animal hemisphere which did not differentiate into the neural type. Those of non-excitable type were found in some blastomeres of the vegetal hemisphere. Blasomeres of 1- to 32-cell cleavage-arrested embryos, which were presumed to possess more than one possible developmental fate, did not develop mosaic membrane properties but differentiated into one of the four types, with a probability dependent upon a gradient of ooplasmic segregation at the time of arrest.

Sperm-activated channels in ascidian oocytes

Ionic channels activated during fertilization in the ascidian oocyte membrane have been studied using the single-channel recording technique. These channels, which we have called "fertilization channels," have a single-channel conductance of about 400 pS, a reversal potential of about O mV, and an open time of 2-30 msec. The open channel probability is about 0.2 at +20 mV and increases as the membrane is depolarized. The unitary conductance is among the largest hitherto observed in biological membranes.

An electrophysiological study of parthenogenetic activation in mammalian oocytes

Using conventional electrophysiological techniques, we have investigated the electrical responses of mouse and hamster oocytes in metaphase of the second meiotic division to agents which induce parthenogenetic activation. Oocytes from MF1 mice responded to 8.7% ethanol and to 0.3% benzyl alcohol by a depolarization (sometimes preceded by a brief hyperpolarization). The response to ethanol did not "desensitize," and the membrane potential recovered completely when the exposure to ethanol was interrupted. The response was accompanied by a decrease in membrane input resistance (Rin) and had an equilibrium potential of about +5 mV in standard medium and of -10mV in Na-free medium. The oocytes responded to A23187 and to La3+ by an increased Rin, and usually lysed during or after treatment. Multiphasic responses were elicited by ethanol and by Ca-ionophore in metaphase II hamster oocytes; an early hyperpolarization accompanied by a decreased Rin was a common feature of the response to both activating agents. The early hyperpolarization was no longer elicited when the cells were exposed for a second time to ethanol or A23187. K+ and Cl- were the ions mainly involved in the hyperpolarizing potential elicited by A23187, and K+ (but not Cl-) was the ionic species mainly involved in ethanol response. The above responses were peculiar to metaphase II oocytes since mouse and hamster ovarian oocytes (in prophase I) and fertilized eggs either failed to respond to the activating agents, or responded by increasing Rin. The variety of electrical responses to parthenogenetic agents indicates that in mammalian oocytes parthenogenetic activation is not triggered by a "classical" activation potential.

Enhancement of ionic currents through voltage-gated channels in the mouse oocyte after fertilization

1. The changes of voltage-gated ion channels in the mouse oocyte after fertilization were investigated under voltage clamp.2. About 60 min after introduction of sperm suspension into the fertilization medium, the amplitude of inward current through Ca(2+)-channels increased, which occurred at anaphase during the second meiotic division. The peak amplitude of the maximum inward current per unit membrane capacity of the oocytes at metaphase was 20+/-3 muA/muF in 50 mM-Sr medium. It was 28+/-8 muA/muF at anaphase, and 32+/-5 muA/muF at telophase. The kinetic properties as well as selectivity among Ca, Sr and Mn ions were not altered after fertilization.3. The outward surge current which was found at the higher membrane potential over +50 mV also increased in amplitude after fertilization, simultaneously with the increase in amplitude of inward current through Ca(2+)-channels. The means and the standard deviations of the surge current per unit membrane capacity at 120 mV were 31+/-8 muA/muF at metaphase, and 48+/-7 muA/muF at telophase. The kinetic properties of the outward surge current were not altered after fertilization.4. Application of colcemid (10(-7) mole/l.) or cytochalasin B (2 x 10(-5) mole/l.) did not prevent the increase in amplitude of both inward current through Ca channels and the outward surge current.5. The membrane currents in N-18 mouse neuroblastoma cells in logarithmic growth phase were examined under voltage clamp. The N-18 neuroblastoma cells possessed the Ca inward current and the delayed outward current. The kinetic properties and the steady-state inactivation of Ca(2+)-channels in N-18 neuroblastoma cells were compared with those in mouse oocytes. It was concluded that they could be regarded as identical between the mouse oocyte and the N-18 neuroblastoma cell.