Biomedical subjects
R Nuccitelli
Publications and source records attributed to R Nuccitelli.
Calcium ion levels in resting and depolarized goldfish retinal ganglion cell somata and growth cones.
1. We have estimated free, intracellular calcium ion concentrations ([Ca]i) in isolated retinal ganglion cells of adult goldfish by ratio-imaging fura-2 emission intensity at two excitation wavelengths. Here we describe [Ca]i in these cells, both at rest and during depolarization by elevated levels of extracellular potassium ions ([K]o). 2. [K]o was varied between 5 and 60 mM in sodium-free, tetrodotoxin-containing salines. Ganglion cell membrane potential, measured with patch electrodes, fell with each increment of [K]o used, from approximately -70 mV in 5 mM K+ to approximately -20 mV in 60 mM K+. 3. In control saline, [Ca]i was roughly 120 nM in cell somata and at least twofold higher in their growth cones. [Ca]i increased in both somata and growth cones to as high as 1.5 microM in salines containing 60 mM K+. [Ca]i exceeded 1.5 microM in some cells in high-K+ salines, although these levels could not be quantified accurately with fura-2. 4. Increases in [Ca]i elicited by elevated [K]o persisted for the duration of the exposure to high-K+ saline and were blocked by replacement of most of the bath Ca2+ by Co2+. These increases in [Ca]i were also sensitive to dihydropyridine calcium-channel ligands, viz., enhanced by BAY K 8644 (3 microM) and antagonized by nifedipine (10 microM). 5. Partial recovery of control [Ca]i occurred when [K]o was reduced to 5 mM after exposure to high-K+ saline and in high-K+ saline when nifedipine was included. These results show that goldfish retinal ganglion cells can partially buffer intracellular Ca2+ in the absence of extracellular Na+ ions. 6. These results provide measurements of the changes in [Ca]i brought about by depolarization of goldfish retinal ganglion cells in Na(+)-free salines. In these salines, at least part of the increase in [Ca]i appears to result from Ca2+ influx through a voltage-activated, noninactivating calcium conductance in the somata and growth cones of these cells. These measurements complement whole-cell patch-clamp and vibrating microprobe recordings from the somata and neurites of these cells and also immunocytochemical studies and patch-clamp measurements in amphibian, reptilian, and mammalian retinal ganglion cells.
The effect of myo-inositol 1,4,5-trisphosphorothioate on Cl- current pattern and intracellular Ca2+ in the Xenopus laevis oocyte.
Microinjection of myo-inositol 1,4,5-trisphosphate into voltage-clamped Xenopus laevis oocytes or the stimulation of the phosphatidylinositol cycle elicits a complex Ca2(+)-dependent Cl- current pattern. Microinjection of myo-inositol 1,3,4,5-tetrakisphosphate causes an immediate release of Ca2+, but elicits a different Cl- current pattern than myo-inositol 1,4,5-trisphosphate. We have studied the effects of myo-inositol 1,4,5-trisphosphorothioate, which can not be converted to myo-inositol 1,3,4,5-tetrakisphosphate. Myo-inositol 1,4,5-trisphosphorothioate caused an immediate release of intracellular Ca2+, as measured by fura-2 imaging. Myo-inositol 1,4,5-trisphosphorothioate generated a Cl- current pattern similar to myo-inositol 1,3,4,5-tetrakisphosphate, not myo-inositol 1,4,5-trisphosphate.
Activation of protein kinase C triggers premature compaction in the four-cell stage mouse embryo.
During mouse preimplantation development, the cells of the mouse embryo undergo a progressive subcellular reorganization at compaction, which eventually results in the formation of two distinct cell types. We have investigated the effect that activators of the Ca2(+)-phospholipid-dependent protein kinase (PKC) have on mouse compaction. Phorbol ester activation of PKC caused premature compaction of four-cell embryos within a few minutes of addition followed by a prolonged decompaction phase after 1 hr. This response was dose-dependent to concentrations as low as 250 pg/ml. Diacylglycerides also caused compaction; however, it was more sustained than with phorbol esters and was not followed by a phase of decompaction. Inhibition of PKC with sphingosine blocks induced compaction in a dose-dependent manner and also blocks normal compaction of eight-cell embryos. A monoclonal antibody to the cell adhesion molecule, E-cadherin, which mediates mouse embryo compaction, completely blocks compaction induced by these activators of PKC. Indirect immunofluorescence with a monoclonal antibody to E-cadherin indicates that PKC activation causes a rapid shift in the localization of this cell adhesion molecule, which coincides with the observed compaction. These results suggest that PKC plays a role in the initiation of compaction through its effect either directly or indirectly on E-cadherin.
Inositol 1,4,5-trisphosphate-induced calcium release in the organelle layers of the stratified, intact egg of Xenopus laevis.
Using double-barreled, Ca2(+)-sensitive microelectrodes, we have examined the characteristics of the Ca2+ release by inositol 1,4,5-trisphosphate (Ins(1,4,5)P3) in the various layers of Xenopus laevis eggs in which the organelles had been stratified by centrifugation. Centrifugation of living eggs stratifies the organelles yet retains them in the normal cytoplasmic milieu. The local increase in intracellular free Ca2+ in each layer was directly measured under physiological conditions using theta-tubing, double-barreled, Ca2(+)-sensitive microelectrodes in which one barrel was filled with the Ca2+ sensor and the other was filled with Ins(1,4,5)P3 for microinjection. The two tips of these electrodes were very close to each other (3 microns apart) enabling us to measure the kinetics of both the highly localized intracellular Ca2+ release and its subsequent removal in response to Ins(1,4,5)P3 injection. Upon Ins(1,4,5)P3 injection, the ER-enriched layer exhibited the largest release of Ca2+ in a dosage-dependent manner, whereas the other layers, mitochondria, lipid, and yolk, released 10-fold less Ca2+ in a dosage-independent manner. The removal of released Ca2+ took place within approximately 1 min. The sensitivity to Ins(1,4,5)P3 and the time course of intracellular Ca2+ release in the unstratified (unactivated) egg is nearly identical to that observed in the ER layer of the stratified egg. Our data suggest that the ER is the major organelle of the Ins(1,4,5)P3-sensitive Ca2+ store in the egg of Xenopus laevis.
Octaploid mouse embryos produced by electrofusion polarize and cavitate at the same time as normal embryos.
We created enlarged octaploid mouse blastomeres by subjecting four-cell embryos to a large (greater than 2,000 V/cm) dc field of brief duration (10 microseconds). This electrofusion pulse caused three to four of the blastomeres to fuse in 60% of the embryos tested. Modifications of fusion chamber and medium enabled fusion of up to 20 embryos per pulse, greatly increasing the yield for this fusion method. The effectiveness of the electrofusion pulse depended upon such parameters as embryonic cell cycle time and the pH and temperature of the electrofusion medium. There was no discernable lag in the onset of the third cleavage division or the time of cavitation in fused blastomeres. These fused blastomeres also underwent polarization of their apical surfaces at the same time as controls in spite of their increased cell size. These results suggest that octaploid mouse blastomeres created via electrofusion divide normally through the blastocyst stage and polarize at the same time and in the same sequence as smaller control blastomeres. This suggests that the mechanisms underlying cell division, cavitation, and cortical polarization are not affected by changes in cellular size or ploidy.
Ionic currents in morphogenesis.
Morphogenetic fields must be generated by mechanisms based on known physical forces which include gravitational forces, mechanical forces, electrical forces, or some combination of these. While it is unrealistic to expect a single force, such as a voltage gradient, to be the sole cause of a morphogenetic event, spatial and temporal information about the electrical fields and ion concentration gradients in and around a cell or embryo undergoing morphogenesis can take us one step further toward understanding the entire morphogenetic mechanism. This is especially true because one of the handful of identified morphogens is Ca2+, an ion that will not only generate a current as it moves, but which is known to directly influence the plasma membrane's permeability to other ions, leading to other transcellular currents. It would be expected that movements of this morphogen across the plasma membrane might generate ionic currents and gradients of both electrical potential and intracellular concentration. Such ionic currents have been found to be integral components of the morphogenetic mechanism in some cases and only secondary components in other cases. My goal in this review is to discuss examples of both of these levels of involvement that have resulted from investigations conducted during the past several years, and to point to areas that are ripe for future investigation. This will include the history and theory of ionic current measurements, and a discussion of examples in both plant and animal systems in which ionic currents and intracellular concentration gradients are integral components of morphogenesis as well as cases in which they play only a secondary role. By far the strongest cases for a direct role of ionic currents in morphogenesis is the polarizing fucoid egg where the current is carried in part by Ca2+ and generates an intracellular concentration gradient of this ion that orients the outgrowth, and the insect follicle in which an intracellular voltage gradient is responsible for the polarized transport from nurse cell to oocyte. However, in most of the systems studied, the experiments to determine if the observed ionic currents are directly involved in the morphogenetic mechanism are yet to be done. Our experience with the fucoid egg and the fungal hypha of Achlya suggest that it is the change in the intracellular ion concentration resulting from the ionic current that is critical for morphogenesis.
The cortical reaction in the egg of Discoglossus pictus: a study of the changes in the endoplasmic reticulum at activation.
In Discoglossus pictus previous ultrastructural observations have shown that at the animal dimple, where sperm fuse with the egg, cortical granules (CG), vacuoles, and tightly packed clusters of small cisternae are present. At fertilization the clusters open (i.e., become loose) and give rise to longer cisternae arranged in whorls and chains which migrate toward the plasma membrane. The vacuoles fuse to form cisternae and exocytose along with the CG. In the rest of the egg periphery, while exocytosis occurs, the clusters do not open as a result of activation (C. Campanella, R. Talevi, U. Atripaldi, and L. Quaglia (1986). In "Molecular and Cellular Biology of Fertilization" (J.L. Hedrick, Ed.). Plenum, New York). We have recently conducted electrophysiological studies which have detected inward currents at the dimple center, outward current at the rest of the egg surface, and an eightfold increase in [Ca2+]i which propagates from the site of activation throughout the egg (R. Nuccitelli, D. Kline, W. Busa, R. Talevi, and C. Campanella (1988). Dev. Biol. 130, 120-132). In this paper we have asked whether the anionic current and the Ca2+ increase could be causally related to the changes of the smooth endoplasmic reticulum (SER) at activation. The results obtained by activating the eggs in ion-substituted Ringers indicate that (1) the migration of cisternae is not dependent on the polarity of the activation current crossing the dimple, but is strongly impaired, together with CG exocytosis, by 5 x Cl- Ringer; (2) TMB-8, a drug which partially blocks calcium release (C. Y. Choiu and M. J. Malagodi (1975). Brit. J. Pharmacol. 53, 279-288), partially inhibits opening of cisternae clusters and the formation of an SER network in the dimple. This suggests a causal relationship between the Ca2+ rise and the cluster transformation at activation.
A highly localized activation current yet widespread intracellular calcium increase in the egg of the frog, Discoglossus pictus.
Sperm entry in the egg of the painted frog, Discoglossus pictus, occurs only at a specialized region of the animal hemisphere called the animal dimple, a structure not found in other species of frog. An extracellular vibrating electrode was used to measure the activation current to determine if the ion channels that open to generate the fertilization potential are localized in this region. Eggs that were activated by microinjecting inositol-1,4,5-trisphosphate (Ins(1,4,5)P3) exhibited activation potentials very similar to those of fertilized eggs. There was a delay between the time of Ins(1,4,5)P3 injection and the initiation of the activation potential that was proportional to the distance between the site of the activating stimulus and the animal dimple, similar to the delay previously observed in prick-activated eggs (R. Talevi, B. Dale, and C. Campanella (1985). Dev. Biol. 111, 316-323). The delay lasted 30 sec when the stimulus site was 20 degrees (300 micron) from the animal dimple and 14 min when it was 150 degrees C from the dimple. Once the activation potential was initiated, there was an excellent temporal correlation between the time of depolarization and the time of the first detectable current entering the dimple region. This inward current was typically 60 microA/cm2 in amplitude and was found only in the central 200 micron of the dimple region. The outward current was distributed over the remainder of the egg surface and was much smaller in amplitude. The activation current was carried by Cl- efflux in the animal dimple region, and was reduced by DIDS and reversed by high external Cl- or I-. The occurrence of inward current only at the dimple region indicates that Cl- channels which open to produce the activation potential are localized there. Using Ca2+-specific microelectrodes, we found that [Ca2+]i increased from 0.25 to 2 microM following both fertilization and activation and returned to the unactivated level after about 37 min. Immature oocytes of D. pictus were also studied with the vibrating probe and the inward current in these cells was much less localized than that in the activating egg. A steady transcellular current of up to 4 microA/cm2 entered the entire animal hemisphere of the oocyte and exited the vegetal hemisphere.
Cortical activity in vertebrate eggs. I: The activation waves.
We present a physical model for the propagation of chemical and mechanical waves on the surface of vertebrate eggs. As a first step we analyzed the propagation of the calcium wave observed to sweep over the surface of the Medaka egg (Gilkey et al., 1978). It has been assumed that this wave is driven by a mechanism of calcium-stimulated-calcium-release. By formulating this hypothesis mathematically we can use the observed wavefront data to obtain a map of cortical reactivity. This map indicates a gradient of reactivity along the egg: highest in the animal hemisphere and tapering off towards the vegetal hemisphere. The cortex of Xenopus eggs is also capable of propagating a calcium wave (Busa & Nuccitelli, 1985). At about the same time a wave of expansion followed by a wave of contraction sweeps across the egg surface (Takeichi et al., 1984). We have proposed a mechanism for this wave pair based on the physical chemistry of actomyosin gels. The calcium wave activates solation factors which sever some of the actin chains which leads to an osmotic swelling of the gel. Calcium also activates the contractile machinery of the actomyosin system which causes the gel to contract. The contraction lags the swelling because of the nature of the kinetics: solation and swelling is a more rapid process than contraction. By writing the equations for gel expansion and contraction we can mimic the mechanical and chemical wave propagation by a computer simulation. If the model is correct this provides a method for using the waves as a diagnostic of the mechanochemical properties of the egg cortex.
The wave of activation current in the egg of the medaka fish.
An extracellular vibrating electrode was used to measure the ring-shaped wave of inward current, the activation current, that propagates at 10 micron/sec across the egg of the medaka fish, Oryzias latipes, from the site of sperm-egg fusion at the animal pole to the vegetal pole. This activation wave is due to a localized increase in the conductance to Na+, K+, and Ca2+ and reflects the propagated opening of these ion channels. The earliest detectable current begins to enter the animal pole 20 sec after the initiation of the fertilization potential, so the first ion movements responsible for the fertilization potential are below the resolution of the vibrating probe system. These channels are present in both the animal and vegetal hemispheres, but the magnitude of the activation current is about seven times greater in the animal hemisphere. An outward current of smaller magnitude and spread out over a larger area precedes and follows the inward current except at the point of fertilization where the current is first inward. The current direction is dependent on the external Na+ concentration, and in the more physiological solution of 10% NaCl-Yamamoto's Ringer's, its direction reverses to become outward, apparently carried by K+ efflux. Raising the external Ca2+ in this same low-Na+ medium reverses the current so that it becomes inward again and increases the propagation velocity of the wave, suggesting a Ca2+ component to the inward current. Current enters a given region on the egg's surface about 16 sec before any vesicle fusion occurs in that region. Iontophoresis of inositol-1,4,5,-trisphosphate immediately triggers egg activation with a minimum activating charge of 0.6 nC.
On electrical currents in development.
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A two-dimensional vibrating probe with a computerized graphics display.
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Detection of transcellular currents and effect of an imposed electric field on mouse blastomeres.
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Role of electric fields in fibroblast motility.
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New insights into galvanotaxis and other directed cell movements: an analysis of the translocation distribution function.
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Fertilization potential and electrical properties of the Xenopus laevis egg.
The membrane potential of Xenopus eggs was monitored continuously from prior to fertilization until early cleavage. A rapid decay of the initial potential of -33.1 +/- 8.1 (SD) mV (N = 14) upon impalement to a value of -19.3 +/- 4.2 (SD) mV (N = 68) suggested that insertion of the first electrode caused depolarization. Outward and inward rectification were observed when the resting potential was made more positive than about 5 mV or more negative than about -30 mV. Eggs were not activated by this level of current injection. Fertilization and activation evoked a membrane depolarization which was influenced by the external Cl- concentration, the nature of the halide species, and 4,4-diisothiocyanostilbene-2,2-disulfonic acid. Smaller transient depolarizations were associated with the initial stages of the fertilization potential but not with activation. Only when the fertilization potential was significantly diminished, as in high external Cl- or in the presence of Br- or I- solutions did polyspermy ensue. The input resistance of the unfertilized egg was 13.2 +/- 9.8 M omega (N = 26) and decreased about 200-fold at the peak of the fertilization potential to 0.077 +/- 0.020 M omega (N = 9). Ninety minutes after the onset of the fertilization potential and about 6 min after the start of furrow formation the membrane began a series of cleavage cycle-associated hyperpolarizations. These were unaffected by either the external Cl- concentration or other halide species. Reduction in amplitude of the fertilization potential had no apparent effect upon the normal elevation of the fertilization envelope or upon cleavage and later development. The fast electrical block to polyspermy appears to have a lower threshold in Xenopus compared with other species and is also effective at negative membrane potentials.
Polarity of isolated blastomeres from mouse morulae: detection of transcellular ion currents.
Eight- to sixteen-cell stage mouse morulae were dissociated with Ca2+-free medium into blastomeres that were labeled with fluoresceinated-succinylated Con A (FS-Con A) to mark their apical-basal axes. The vibrating probe was then used to map their extracellular current patterns. The average current density around normal blastomeres approached the resolution of the probe system (0.2 microA/cm2) and was undetectable in the majority of blastomeres. Since the current density at the measuring point outside the cell is known to increase with cell size in other systems, enlarged blastomeres were created by fusing together blastomeres of 4-cell stage embryos in 45% polyethylene glycol. Enlarged blastomeres were then aggregated with normal blastomeres using phytohemagglutinin and cultured to the 8- to 16-cell stage to allow them to become polarized. Such aggregates were then dissociated with Ca2+-free medium to recover polarized, enlarged blastomeres. The enlarged blastomeres were 30-65 microns in diameter and 70% of them generated a detectable current; currents were detected around 83% of those blastomeres larger than 40 micron in diameter. The current pattern in these most reliable cases was predominantly inward apical (11/16 or 69%) and outward basal (15/16 or 94%), with lateral currents about three-fold smaller in amplitude than these apical-basal currents. Lateral currents were undetectable in 53% of the cases. Preliminary data suggest that the inward current is carried in part by Na+ influx and is independent of the Na+,K+-ATPase over the short term. Transcellular ion currents were detectable as long as 4 hr after dissociation, and the apical-basal current pattern was usually stable during that time. In contrast, the fluorescent cap of FS-Con A faded within 7-30 min at 35 degrees C but remained stable in 0.1% azide or 1.5 micrograms/ml cytochalasin D. The electrical polarity therefore persisted after the apical cap of Con A fluorescence was no longer visible. We propose that these transcellular ion currents may be involved in the establishment of blastomere polarity and describe a mechanism of action in an "ion current polarization" hypothesis.