An electrophysiological study of the membrane properties of the immature and mature oocyte of the Batstar,Patiria miniata

Immature oocyte membrane properties of a starfish, Patiria miniata, were investigated by microelectrode techniques. The resting membrane potential in artificial seawater (ASW) was ?78.5 ± 6.7 mV (n = 61, inside negative). This was mainly accounted for by a selective permeability to potassium ions. Potassium ion-selective microelectrodes were used to measure intracellular K⁺ ion activity, which was 350 mM. The sodium to potassium permeability ratio was 0.02 ± 0.01 (n = 4). The current-voltage relation was nonlinear. The I–V curve included both areas of inward and outward rectification. The dependence of inward rectification upon the K⁺ ion electrochemical gradient was demonstrated. The membrane was capable of a regenerative action potential due to permeability changes for Ca²⁺ and Na⁺ ions. The Ca and Na components of the action potential were identified. The Ca component was reversibly suppressed by cobalt and irreversibly blocked by D-600. The Na component was tetrodotoxin (TTX) insensitive. The excitable response of P. miniata oocytes is similar to that described by Miyazaki et al. (1975a) for those of the starfish Asterina pectinifera.Immature oocytes were stimulated to mature with 10^?5M 1-methyladenine (1-MA) during continuous monitoring of the membrane potential. The resting potential in ASW became more inside negative during maturation. This change of the passive membrane property of the oocyte may be accounted for by the increased selectivity to K⁺ ions. The specific membrane resistance near the resting potential increased from 4.2 ± 1.4 to 21 ± 8.7 kΩ·cm² (n = 15) during maturation, while the specific membrane capacitance decreased slightly from 2 ± 0.5 to 1.7 ± 0.6 μF/cm² (n = 5). Maturation had little effect upon the active membrane properties.     

Membrane potential of the unfertilized sea urchin egg

The membrane potential, specific resistance, and potassium selectivity of the unfertilized Strongylocentrotus purpuratus egg were determined by two independent methods: tracer flux and microelectrode. The potassium influx was 0.50 ± 0.2 pmole/cm²· sec, which was greater than the sodium, chloride, and calcium influxes by factors of 4, 7, and 75, respectively. By means of the constant-field equations, the flux data were used to calculate membrane potential (?70 mV) and specific resistance (420 kΩ · cm²). The effect of the external potassium concentration on the sodium influx was determined and the results closely fit the result expected if the membrane behaved as a potassium electrode. Microelectrode measurements of the potential and resistance were ?75 ± 3 mV and 380 ± kΩ · cm².     

Maturation and fertilization of the sea urchin oocyte: An electrophysiological study

Some electrical properties of the sea urchin oocyte during germinal vesicle breakdown (GVBD) and fertilization have been studied using two intracellular electrodes. Oocytes with distinct germinal vesicles have resting potentials of ?70 to ?90 mV and the specific membrane resistance may range from 3 to 10 kΩ·cm². Around rest the I–V relationship is concave toward the axis origin and the membrane is K⁺ selective. A second electrical state, of lower potential and higher resistance, preexists in the membrane. Following GVBD, the K⁺-selective system is lost and the oocyte attains the characteristics of the second state with a resting potential of ?10 to ?50 mV and specific membrane resistance of 10–50 kΩ·cm². At rest the I–V relationship tends to be convex toward the axis origin. The majority of sea urchin eggs (which have undergone GVBD and completed meiosis) have a resting state of ?10 to ?30 mV; 10–50 kΩ·cm². The I–V relationship around rest is convex toward the axis origin and the resting potential is sensitive to changes of Na⁺, Cl^?, and K⁺ in the external medium. There is probably no major change in the electrical properties of the oocyte during the completion of meiosis. A small percentage of eggs from suboptimal animals have high resting potentials of ?70 to ?90 mV and specific membrane resistance of 5–50 kΩ·cm². Such eggs have predominantly K⁺-selective membranes and we suggest that they are either underripe or aged. The first electrical event across the egg plasma membrane during fertilization is a step-like depolarization which occurs about 2 sec after the attachment of the fertilizing spermatozoon to the vitelline layer. There is no change—at the level of the light microscope—either in the egg surface or in the behavior of the spermatozoon until the second event, the fertilization potential (FP), is initiated 11 sec later. The cortical reaction occurs simultaneously with the FP and during the rising phase of the FP the spermatozoon stops gyrating around its point of attachment. Oocytes, which do not have cortical granules, upon insemination exhibit step events but no FP; in contrast artificially activated eggs, either spontaneous or induced by the ionophore A23187, give rise to only the FP. We suggest that the FP is the electrical result of the modification of the egg plasma membrane during cortical exocytosis.     

Electrogenic Na?K pump current in rat skeletal myoballs

Catecholamines and insulin have been reported to hyperpolarize skeletal muscle fibers via stimulation of the electrogenic Na-K pump (Flatman and Clausen, 1979, Nature, 281:580–581). Therefore, the electrogenic Na-K pump current was investigated in cultured colcemid-treated rat skeletal myoballs using whole-cell voltage clamp. Skeletal muscles were taken from newborn rat hindlegs, trypsin digested, and cultured. By day 7, all myoblast cells fused into myotubes. After treatment with the microtubule disrupter colcemid (10^?7 M) for 2 days, some of the myotubes became transformed into spherical myoballs, having an average diameter of 41.2 ± 1.5 μm (n = 21). The resting membrane potential averaged -56.8 ± 1.7 mV (n = 40). Ouabain (1 mM) quickly depolarized the myoballs to -51.1 ± 1.1 mV (n = 27), showing the existence of an electrogenic Na-K pump in the skeletal myoball preparation. The values for the specific membrane resistance and capacitance were 5.5 ± 1.0 KΩ-cm² (n = 21) and 3.7 ± 0.3 μF/cm² (n = 21), respectively. The pump current averaged 0.28 ± 0.03 pA/pF (n = 10), with the membrane potential at -60 mV and 10 mM intrapipette Na⁺. The Na-K pump contribution to resting membrane potential was calculated to be 5.7 mV, matching the ouabain-induced rapid depolarization. When the Na-K pump was stimulated with 50 mM intrapipette Na⁺, the pump current was about doubled (0.52 ± 0.08 pA/pF; n = 10). Isoproterenol (1 μM) and 8-Br-cAMP (1 mM) also significantly increased pump current by 50% (0.42 ± 0.04 pA/pF; n = 9) and 64% (0.46 ± 0.09 pA/pF; n = 7), respectively. In contrast, although insulin and phorbol ester also increased pump current, this increase was not statistically significant. The ineffectiveness of insulin and phorbol ester may be due to colcemid interfering with Na-K pump translocation from internal vesicles to the sarcolemma. © 1994 wiley-Liss, Inc.     

The electrical changes accompanying fertilization and cortical vesicle secretion in the medaka egg

The electrical properties of the egg of the medaka, Oryzias latipes, were studied before, during, and after fertilization. The resting potential of the unfertilized egg averaged ?39 ± 9 mV in Yamamoto's Ringers (Y. Ringers), but 20% of the values were between ?50 and ?60 mV. Fertilization triggers a small depolarization of 4 ± 3 mV in 10% Y. Ringers with an average duration of 20 ± 10 sec. The amplitude of this depolarization is independent of [Na⁺]_o, [Ca²⁺]_o, and [Cl^?]_o, so it appears to be due to a nonspecific leak triggered by sperm-egg fusion. The depolarization is followed by a longer hyperpolarizing phase with an average amplitude of 31 ± 12 mV. Recovery from this hyperpolarization has a fast phase lasting 155 ± 18 sec, followed by a slower phase which reaches a steady average membrane potential of ?19 ± 1 mV by 9 min after fertilization. The membrane resistance falls 10-fold during the first 2 min after fertilization, from 40 (1520 kΩ-cm²) to 3 MΩ. This is largely due to an increase in the K⁺ conductance. At the peak of the hyperpolarization, the membrane potential exhibits a 28 mV/decade [K⁺]_o dependence and a 6 mV/decade [Na⁺]_o dependence. The membrane resistance slowly recovers over the next 8 min to a value about 30% larger than before fertilization. The relation of current vs voltage was linear before, during, and after fertilization and indicated a reversal potential of ?98 ± 20 mV for the hyperpolarization peak. The egg's capacitance averaged 0.04 ± 0.01 μF (0.9 μF/cm²) before fertilization and approximately doubles within 90 sec after fertilization. It then decreases over a 9-min period, reaching a value 25% smaller than before fertilization.     

Extracting cancer cell line electrochemical parameters at the single cell level using a microfabricated device

Cancer cells have distinctive electrochemical properties. This work sheds light on the system design aspects and key challenges that should be considered when experimentally analyzing and extracting the electrical characteristics of a tumor cell line. In this study, we developed a cellularbased functional microfabricated device using lithography technology. This device was used to investigate the electrochemical parameters of cultured cancer cells at the single-cell level. Using impedance spectroscopy analyses, we determined the average specific capacitance and resistance of the membrane of the cancer cell line B16-F10 to be 1.154 ± 0.29 μF/cm², and 3.9 ± 1.15 KΩ.cm² (mean ± SEM, n =14 cells), respectively. The consistency of our findings via different trails manifests the legitimacy of our experimental procedure. Furthermore, the data were compared with a proposed constructed analytical-circuit model. The results of this work may greatly assist researchers in defining an optimal procedure while extracting electrical properties of cancer cells. Detecting electrical signals at the single cell level could lead to the development of novel approaches for analysis of malignant cells in human tissues and biopsies.     

Ionic currents during the action potential in the molluscan neurone with the self-clamp technique

The ionic currents during the action potential in the F1 neurone of Helix aspersa were investigated, using the Self-Clamp Technique. A spontaneous action potential was recorded and then replayed, both in its direct and in its inverted form, to the same cell in voltage clamp and in control conditions. Under various experimental conditions such as treatment with the specific ionic channels blockers tetrodotoxin, lanthanum, 4-aminopyridine or tetraethylammonium, as well as low sodium and low calcium external media, the single ionic currents were detected by stimulating the membrane with the direct pulse only. The Self-Clamp Technique allowed the measuring of the following parameters, in their real time course during the action potential: a) the total action currents; b) the pharmacologically blocked ionic components; c) the ionic components which remained insensitive to the agents used (residual currents). These data were compared with those obtained by applying conventional rectangular pulses in voltage clamp. The membrane capacity was measured with the Self-Clamp Technique and the recorded currents were normalized assuming a specific capacity of 4 μF/cm². The isolated ionic components were directly compared with the total action currents to evaluate the degree to which blockage was complete. The electric charge transported by each ionic specimen was evaluated as well as the individual ionic amounts. The sodium influx was 3.18 ± 0.55 pM/cm² per impulse (9 cells), calcium influx 1.03 ± 0.37 pM/cm² per impulse (10 cells). A value of 6.37 ± 1.03 pM/cm² per impulse was found for the potassium outflux, with a probable overestimation of about 1 pM/cm² per impulse (9 cells).     

Some electrophysiological and permeability properties of the mouse egg

Certain electrophysiological and ionic properties of the mouse egg (CF-1 and BDF 12–18 hr post ovulation) have been investigated. Membrane potential (?14 ± 0.4 mV, ± SE, inside negative), membrane resistance (2610 ± 38 ohm·cm²), and membrane capacitance (1.6 ± 0.03 μF cm^?2) have been determined by means of intracellular microelectrode recording techniques. Membrane potential and related parameters are stable for extended periods of time upon impalement and the magnitude of the cell membrane potential has been demonstrated to be sensitive to alteration in external sodium. The electrophysiological studies in conjunction with measurements of unidirectional potassium fluxes using isotope tracer-techniques have allowed determination of membrane permeability to potassium (8 × 10^?8 cm sec^?1) and membrane potassium conductance (25 μmho cm^?2). Furthermore, the use of tracer flux techniques has indicated that the exchangeable fraction of intracellular potassium is 204 ± 14 mM. This represents the bulk of egg potassium (222 ± 19 mM as determined from flame photometry). Studies of unidirectional potassium efflux have indicated that its movement out of the egg is made up of at least two components; an external potassium-independent potassium efflux and external potassium-dependent efflux, the latter possibly representing a potassium exchange mechanism. The combined electrophysiological and tracer-flux data indicate that only a small portion of the total membrane conductance is composed of potassium conductance at this stage of development. This and the fact that the membrane potential is far from the potassium equilibrium potential are similar to observations made on mature eggs of several other species.     

Rotation of a single swollen thylakoid vesicle in a rotating electric field. Electrical properties of the photosynthetic membrane and their modification by ionophores,lipophilic ions and pH

Rotation of single swollen thylakoid vesicles (‘blebs’) was induced by means of a rotating electric field of strength 104 V · cm⁻¹, inducing a membrane voltage of 72 mV peak. Within the range of medium conductives described (40–300 μS · cm⁻¹), measurement of the field frequency (2–100 kHz) giving maximum rotation rate is equivalent to measuring the electrical time constant of the bleb membrane. Hence the membrane capacity (specific capacitance) was determined, and the value found at pH 8.1 (0.93 ± 0.07 μF · cm⁻²) is in agreement with values deduced from measurements using other techniques. However, the capacity was also found to decreased with pH: a minimum value of 0.77 ± 0.01 μF · cm⁻² was measured at pH 4.4. The present study was extended to measurements of the effects of the lipid-soluble anion of dipicrylamine on the membrane capacity. At pH 7.2 and dipicrylamine concentration of 1.0 μM, a minimum estimate of the apparent membrane capacity was found to be 2.0 ± 0.2 μF · cm⁻², with 2.6 ± 0.2 μF · cm⁻² being observed at 5.0 μM concentration. In addition, it was found possible to measure the membrane resistivity (specific resistance) in the presence of either gramicidin (1.0 to 10 nM) or valinomycin (1.0 to 10 μM). In the case of gramicidin, it was possible to derive a maximum estimate of the mean channel conductance, and this agrees very well with the values for individual, single channels that may be deduced from artificial bilayer work. Unless the gramicidin channels in blebs are in fact substantially more conductive than in artificial bilayers, this indicates that a high percentage of the added gramicidin forms channels which are open for most of the time. In the case of valinomycin, a much greater amount had to be added to produce the same reduction of membrane resistivity as seen with a given concentration of gramicidin. However, calculations indicate that the majority of this effect is due to the difference in partioning behaviour of the two ionophores.     

The Action Potentials and Currents on the I-V Plane in the Molluscan Neuron

The action potentials and the corresponding transmembrane currents, directly recorded in the F1 neuron of Helix aspersa by the Self-clamp Technique, were plotted on the I-V plane to represent the real electrical cycle of the cell membrane during activity. The membrane electrical cycle, experimentally obtained, agreed in several aspects with a similar cycle obtained from calculated data on the giant axon of Loligo, but not for the sign, with the consequence of a different localization, as far as voltage and time are concerned, of the negative impedance period. The negative impedance proved to be −614 ± 181 Ω cm² and corresponded to the late phase of the repolarization after the action potential peak. A constant positive impedance was found of 522 ± 131 Ω cm² during the ascending tract of the action potential. These two results are in contrast with previous analyses. The simultaneous availability of the conjugate voltage and current directly measured signals led to the immediate representation of the membrane total conductance in its real time course during activity, in agreement with the Hodgkin and Huxley predictive model. The peak conductance was 1.9 ± 0.7 mmho/cm² in this preparation. The electrical work spent to sustain a single active event proved to be 70 ± 19 nJ/cm². A vectorial representation of the membrane electrical activity is proposed to describe analytically the characteristic behaviour of excitable cells, as well as a new method that utilizes the only action potential to measure the threshold potential in spontaneously discharging cells. The proposed new experimental protocol, based on the use of the Self-clamp Technique, proved to be faster, easier, more productive when compared with the conventional methods; it could be used advantageously in the electrophysiological studies on excitable cells both to define the basic conditions of the investigated preparation and to directly evaluate the effects of subsequent pharmacological stimulations.     

Investigation of electrophysiological responses of Neurospora crassa to blue light

The influence of light in a spectrum range of 350–500 nm 20 W m^-2 (20,000 erg · cm^-2 · s^-1) has been studied in the mycelial cells of Neurospora crassa. Light-induced input resistance and membrane potential changes can be measured by means of intracellular microelectrodes. The value of the input resistance reached maximum after a 2–5 min illumination. The maximum hyperpolarization of the cell membrane reaching 30–40 mV was observed after 20–25 min illumination, when the input resistance values did not differ significantly in the illuminated and non-illuminated cells.     

Chloride conductance of denervated gastrocnemius fibers from normal goats

Membrane potentials, cable parameters, and component resting ionic conductances of gastrocnemius fibers from normal goats were measured in vitro at six to 32 days following denervation by section of the tibial nerve. Denervated fibers were depolarized an average of 11.6 ± 1.5 mV (six preparations) from the control mean of 62.1 ± 1.0 mV (124 fibers) over the period studied. Fibrillation, tetrodotoxin-resistant action potentials, and anodebreak excitation were present in the denervated preparations after 13 days. The control cable parameters from 124 fibers (13 preparations) were membrane resistance, 1052 ± 70 ω·cm² and membrane capacitance, 6.2 μF/cm². In denervated fibers membrane resistance increased two to three times in the 13 to 32 day period; membrane capacitance increased about 50% in normal solution at eight to nine, 27–28, and 32 days. Myoplasmic resistivity was assumed to be 112 Ωcm. Measurements were made at 38°C. Component resting conductances were determined from the cable parameters in normal and chloride-free solution. Mean chloride conductance G_Cl and mean potassium conductance G_K of control fibers were 776 ± 49 μmhos/cm² and 175 ± 15 μmhos/cm² (92 fibers), respectively. Following denervation G_Cl increased slightly at six to nine days then fell to low values at 16 to 32 days that were close to or indistinguishable from zero. G_K increased significantly to 372 ± 40 μmhos/cm² and 499 ± 90 μmhos/cm² at 16 to 20 and 32 days, respectively. It was concluded from these findings that G_Cl and G_K of mammalian skeletal muscle are controlled by factors from the nerve and/or muscle action potentials. Goat muscle is different from frog muscle in which G_Cl does not change and G_K decreases during denervation.     

Membrane Potential Measurements in Cultured Intestinal Villi

Fragmented epithelia of newborn rat small intestine were successfully cultured for periods of up to 4 weeks. Stable intracellular recordings of membrane potential were obtained from these cultured cells. Membrane resting potential varied according to cell location along a villus. The potentials ranged from -70 to -15 mV, being highest at the tip of the villus. The mean resting potential and membrane resistance were -72.4 mV and 8.6 M Ω, respectively. The membrane potential was markedly dependent on the extracellular K⁺ concentration ([K]₀], but not significantly on [Na]₀ and [Cl]₀-Deprivation of Ca²⁺ from the surrounding medium depolarized the membrane by 20 mV. When the cells were cooled down to 6°C, membrane potential was reduced by 40 mV. Based on these data, basic mechanisms underlying the resting potential are discussed in connection with cell differentiation or maturation.     

Resting potential of the mouse neuroblastoma cells: II. Significant contribution of the surface potential to the resting potential of the cells under physiological conditions

In the previous paper, we showed that the K⁺ channels of the mouse neuroblastoma cell (clone N-18) are closed at low concentration of external K⁺ ([K⁺]₀) including the physiological concentration for the cells. In the present study, the origin of the resting membrane potential of N-18 cells has been examined. (1) The resting membrane potential of N-18 cells was depolarized by increasing concentration of the polyvalent cations (La³⁺, Fe³⁺, Co²⁺, Ca²⁺, Sr²⁺, Mg²⁺) and by decreasing the pH of the medium. The input membrane resistance was slightly increased during the depolarization. The depolarization was not explained in terms of the diffusion of the cations across the membrane, since the trivalent cations of greater ionic size were effective at much lower concentrations than the divalent cations. The results obtained from the measurements of ⁸⁶Rb efflux suggested that the depolarization cannot be explained in terms of blocking of the K⁺ channels by the cations. (2) An increase in Ca²⁺ concentration from 0.3 to 1.8 mM induced depolarization of about 10 mV at low [K⁺]₀ where the K⁺ channels are closed, but did not induce any depolarization at high [K⁺]₀ where the channels are open. (3) In order to estimate the changes in the zeta-potential, the electrophoretic mobility of N-18 cells was measured under various conditions. There was a close correlation between the changes in the zeta-potential and those in the membrane potential in response to the polyvalent cations and proton. On the other hand, an increase in K⁺-concentration in the medium, which induced a large depolarization in the cells, did not affect the zeta-potential. (4) The results obtained were explained by an electrical circuit model for the membranes of N-18 cells. In this model, an electrical circuit for the membrane part carrying no selective ionic channels, in which changes in the surface potential directly affect the transmembrane potential, is connected in parallel to the usual circuit model representing selective ionic channel systems. It was concluded that the surface potential contributes significantly to the resting membrane potential of N-18 cells at low [K⁺]₀ where the K⁺ channels are closed.     

ELECTRICAL COUPLING BETWEEN EMBRYONIC CELLS BY WAY OF EXTRACELLULAR SPACE AND SPECIALIZED JUNCTIONS

The meroblastic egg of the teleost, Fundulus heteroclitus, was studied electrophysiologically from cleavage to mid-gastrula stages. The yolk is an intracellular inclusion surrounded by a membrane of high resistivity (50 kΩcm²). This membrane generates a cytoplasm-negative resting potential in later stages. Cells of all stages studied are coupled electrically. In gastrulae, coupling is both by way of specialized junctions between cells and by way of intra-embryonic extracellular space, the segmentation cavity. The latter mode is present because the segmentation cavity is sealed off from the exterior by a high resistance barrier, and the outer membrane of surface cells is of high resistance (50–100 kΩcm²) compared to the inner membrane. It can be inferred that clefts between surface cells are occluded by circumferential junctions. Isolated cells from late cleavage stages develop coupling in vitro, confirming the existence of coupling by way of intercellular junctions. Both modes of coupling could mediate communication between cells that is important in embryonic development.     

Electrical characteristics of sensory neurons of Hirudo medicinalis

During intracellular polarization of identified sensory neurons of the leech by square pulses of hyperpolarizing current electrical parameters of the cell membranes were determined: input resistance of the neuron R_n, time constant of the membrane , the ratio between conductance of the cell processes and conductance of the soma , the resistance of the soma membrane r_s, the input resistance of the axon r _a , capacitance of the membrane C_s, and resistivity of the soma membrane R_s. The results obtained by the study of various types of neurons were subjected to statistical analysis and compared with each other. Significant differences for neurons of N- and T-types were found only between the values of , C_s, and R_s (P<0.01). These parameters also had the lowest coefficients of variation. The surface area of the soma of the neurons, calculated from the capacitance of the membrane (the specific capacitance of the membrane was taken as 1 µF/cm²) was 7–10 times (N-neurons) or 4–6 times (T-neurons) greater than the surface area of a sphere of the same diameter. The resistivity of the soma membrane R_s was 35.00 k·cm² for cells of the N-type and 19.50 k·cm² for T-neurons. The reasons for the relative stability of this parameter compared with the input resistance of the cell (coefficient of variation 22–7 and 53–31% respectively) are discussed. The possible effects of electrical characteristics on the properties of repeated discharges in neurons of different types also are discussed.A. A. Zhdanov Leningrad State University. Translated from Neirofiziologiya, Vol.7, No.3, pp.295–301, May–June, 1975.     

Membrane dielectric responses of bufalin-induced apoptosis in HL-60 cells detected by an electrorotation chip

A non-invasive electrorotation (ROT) technique was used to monitor the apoptosis-induced changes in HL-60 cells. The specific membrane capacitance of the cells fell from 15.6 ± 0.9 mF/cm² to 6.4 ± 0.6 mF/cm² after 48 h treatment with 10 nM bufalin, a component of bufadienolides in traditional Chinese medicine, Chan Su. However, the average membrane conductance remained almost constant during the first 24 h of treatment and then increased afterwards. Apoptosis was verified by a DNA fragmentation assay and scanning electron microscopy. The results demonstrate that the ROT technique gives a quantitative analysis of the toxic damage by chemicals to cells and can be exploited in the testing and development of new pharmaceuticals and active cell agents. Chengjun Huang and Ailiang Chen contributed equally to this work.     

TEA-Sensitive Currents Contribute to Membrane Potential of Organ Surface Primo-node Cells in Rats

The primo-vascular (Bonghan) tissue has been identified in most tissues in the body, but its structure and functions are not yet well understood. We characterized electrophysiological properties of the cells of the primo-nodes (PN) on the surface of abdominal organs using a slice patch clamp technique. The most abundant were small round cells (~10 μm) without processes. These PN cells exhibited low resting membrane potential (−36 mV) and did not fire action potentials. On the basis of the current–voltage (I–V) relationships and kinetics of outward currents, the PN cells can be grouped into four types. Among these, type I cells were the majority (69%); they showed strong outward rectification in I–V relations. The outward current was activated rapidly and sustained without decay. Tetraethylammonium (TEA) dose-dependently blocked both outward and inward current (IC₅₀, 4.3 mM at ±60 mV). In current clamp conditions, TEA dose-dependently depolarized the membrane potential (18.5 mV at 30 mM) with increase in input resistance. The tail current following a depolarizing voltage step was reversed at −27 mV, and transient outward current like A-type K⁺ current was not expressed at holding potential of −80 mV. Taken together, the results demonstrate for the first time that the small round PN cells are heterogenous, and that, in type I cells, TEA-sensitive current with limited selectivity to K⁺ contributed to resting membrane potential of these cells.     

Electrical properties of the Drosophila egg membrane

Electrical properties of the egg membrane of Drosophila melanogaster were examined using intracellular microelectrodes. Unfertilized eggs and fertilized eggs for the period up to the syncytial blastoderm stage were used. Among Na, K, and Cl, K was most permeant to the membrane. The K permeability, however, did not completely determine the membrane potential. The resting potential in standard solution was ?63.5 ± 8.0 mV (mean ± SD) in unfertilized eggs collected within 2–3 days after virgin flies started to lay eggs. The resting potential in fertilized eggs was ?27.0 ± 8.4 mV within 20 min after egg deposition, while it was ?55.1 ± 6.5 mV at the syncytial blastoderm stage. These changes at different developmental stages were associated with changes in the K-dependence of the membrane. The larger amplitude of the resting potential was suggested to be due to increased K permeability but not to decreased nonspecific leakage. The current-voltage relation was linear throughout the stages examined. Action potentials, such as those in eggs of other animals, were not observed. High Ca media significantly increased the amplitude of the resting potential associated with increase in the membrane resistance. A remarkable nonlineality in the I–V relation appeared in high Ca media, which caused continuously increasing hyperpolarization during sustained inward current. Eggs of temperature-sensitive mutants, shi^ts1 and para^ts1 showed properties similar to those in wild-type eggs with transient temperature changes.