Electrical Properties of Structural Components of the Crystalline Lens

The electrical properties of the crystalline lens of the frog eye are measured with stochastic currents applied with a microelectrode near the center of the preparation and potential recorded just under the surface. The stochastic signals are decomposed by Fourier analysis into sinusoidal components, and the impedance is determined from the ratio of mean cross power to input power. The data are fit by an electrical model that includes two paths for current flow: one through the cytoplasm, gap junctions, and outer membrane; the other through inner membranes and the extracellular space between lens fibers. The electrical properties of the structures of the lens which appear as circuit components in the model are determined by the fit to the data. The resistivity of the extracellular space within the lens is comparable to the resistivity of Ringer. The outer membrane has a normal resistance of 5 kohm · cm² but large capacitance of 10 μF/cm², probably because it represents the properties of several layers of fibers. The inner membranes have properties reminiscent of artificial lipid bilayers: they have high membrane resistance, 2.2 megohm · cm², and low specific capacitance, 0.8 μF/cm². There is so much membrane within the lens, however, that the sum of the current flow across all the inner membranes is comparable to that across the outer surface.     

The route of passive ion movement through the epithelium ofNecturus gallbladder

Summary Electrophysiological experiments were performed onNecturus gallbladder to determine whether the main route of passive ion flow was via the cells or via a paracellular shunt path. In the first approach the following values were determined: the transepithelial resistance, the ratio of the voltage deflections across the luminal and basal cell membrane during transepithelial current flow, and the voltage spread within the epithelial cell layer during intracellular application of current pulses. From these data the luminal and basal cell membrane resistances were calculated to be 4,500 and 2,900 cm², respectively, whereas the transepithelial resistance was only 310 cm², indicating that approximately 96% of the transepithelial current bypassed the cells. This result was confirmed in a second approach, in which the intracellular voltage deflections were found to remain approximately constant, when the current pulses were passed from a cell into the interstitial compartment with the luminal compartment being empty or when they were passed from the cell into both external compartments simultaneously. In the third approach current was passed through the epithelium and a voltage-scanning microelectrode was moved across the surface of the epithelium to explore the induced electrical field. Significant distortions of the field were observed in the immediate vicinity of the cell borders. This result indicated that the paracellular shunt, which carries the main part of the transepithelial current, leads through the terminal bars and that the terminal bars or tight junctions arenot tight for transepithelial movement of small ions in gallbladder epithelium.     

Junctions in the central nervous system of the cat

Summary The leptomeningeal tissue of the choroid plexuses and of the brain surfaces have been studied by means of the freeze-etching technique. The pia-arachnoid membrane and the subdural neurothel represent the morphological barrier between the extracerebral tissue and the cerebrospinal compartment. The freeze-etch findings indicate that the arachnoid and neurothelial cells are coupled by extensive zonulae occludentes which seem to represent the structural basis of the barrier mechanism provided by these cell layers. Furthermore, it became evident that gap junctions of considerable structural heterogeneity occur on the pial and arachnoid cells of the interstitial choroidal compartment and of the free brain surfaces. The structural heterogeneity of the nexuses is taken as an indication of the plasticity of the leptomeningeal tissue. The different morphological characteristics of the nexal formations are discussed with respect to their probable functional meaning.This investigation was supported by the Deutsche Forschungsgemeinschaft SFB 114 (Bionach).     

Propagation of Action Potentials and the Structure of the Nexus in Cardiac Muscle

The hypothesis that the nexus is a specialized structure allowing current flow between cell interiors is corroborated by concomitant structural changes of the nexus and changes of electrical coupling between cells due to soaking in solutions of abnormal tonicity. Fusiform frog atrial fibers are interconnected by nexuses. The nexuses, desmosomes, and regions of myofibrillar attachment of this muscle are not associated in a manner similar to intercalated discs of guinea pig cardiac muscle. Indeed, nexuses occur wherever cell membranes are closely apposed. Action potentials of frog atrial bundles detected extracellularly across a sucrose gap change from monophasic to diphasic when the gap is shunted by a resistor. This indicates that action potentials are transmitted across the gap when sufficient excitatory current is allowed to flow across the gap. When the sucrose solution in the gap is made hypertonic, propagation past the gap is blocked and the resistance between the cells in the gap increases. Electron micrographs demonstrate that the nexuses of frog atrium and guinea pig ventricle are ruptured by hypertonic solutions.     

Biophysical properties of human astrocytic brain tumor cells in cell culture

For malignant cells cultured from a human astrocytoma, electrophysiological characteristics of the plasma membrane included specific resistivity of 446.82 ± 279.5 ohm·cm², specific capacitance of 0.758 ± 0.52 microfarads/cm², time constant 0.318± 0.10 msec. The resting membrane potential averaged-14.07 ± 7.4 mV; the mean input resistance 8.1 ± 4.0 megohms. The average cell area was 1638 ± 585 ±² for contactual and 1919 ± 989 ±² for noncontactual cells. Changes in input resistance and resting membrane potential were observed with increasing time in culture, possibly reflecting cell cycling. There did not appear to be electrical coupling in this cell line.     

Aldosterone regulates paracellular pathway resistance in rabbit distal colon

Summary Regulation of the paracellular pathway in rabbit distal colon by the hormone aldosterone was investigated in vitro in Ussing chambers by means of transepithelial and microelectrode techniques. To evaluate the cellular and paracellular resistances an equivalent circuit analysis was used. For the analysis the apical membrane resistance was altered using the antibiotic nystatin. Under control conditions two groups of epithelia were found, each clearly dependent on the light: dark regime. Low-transporting epithelia (LT) were observed in the morning and high-transporting epithelia (HT) in the afternoon. Na⁺ transport was about 3-fold higher in HT than in LT epithelia. Incubating epithelia of both groups with 0.1 mol·1^-1 aldosterone on the serosal side nearly doubled in LT epithelia the short circuit current and transepithelial voltage but the transepithelial resistance was not influenced. Maximal values were reached after 4–5 h of aldosterone treatment. In HT epithelia due to the effect of aldosterone all three transepithelial parameters remained constant over time. Evaluation of the paracellular resistance revealed a significant increase after aldosterone stimulation in both epithelial groups. This increase suggests that tight junctions might have been regulated by aldosterone. The hormonal effect on electrolyte transport was also dependent on the physiological state of the rabbit colon. Since net Na⁺ absorption in distal colon is, in addition to transcellular absorption capacity, also dependent on the permeability of the paracellular pathway, the regulation of tight junctions by aldosterone may be a potent mechanism for improving Na⁺ absorption during hormone-stimulated ion transport.Abbreviations V _t transepithelial potential difference (mV) - R _t transepithelial resistance (·cm²) - G _t transepithelial conductance (mS·cm^-2) - I_sc calculated short circuit current (A·cm^-2) - V _a apical membrane potential difference (mV) - V _bl basolateral membrane potential difference (mV) - voltage divider ratio - R _a apical membrane resistance (·cm²) - R _bl basolateral membrane resistance (·cm²) - R _c cellular resistance ( of apical and basolateral resistance) (·cm²) - R _p resistance of the paracellular pathway (·cm²) - G _a apical membrane conductance (mS·cm^-2) - G _bl basolateral membrane conductance (mS·cm^-2) - G _p paracellular conductance (mS·cm^-2) - G _t transepithelial conductance (mS·cm^-2) - HT _contr high transporting control epithelia - LT _contr low transporting control epithelia - HT _aldo aldosterone incubated high transporting epithelia - LT _aldo aldosterone incubated low transporting epithelia     

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.     

Mitochondria-rich Cells and Voltage-activated Chloride Current in Toad Skin Epithelium: Analysis with the Scanning Vibrating Electrode Technique

The pathway for the voltage-activated chloride current across isolated toad skin was analyzed using a scanning 2D-vibrating voltage probe technique, which permits discrimination of local current peaks if their origins are more than 50 μm apart. The epithelium was separated from the corial connective tissue after enzymatic digestion with collagenase. Cl⁻ current was activated by voltage clamping the transepithelial potential to 60–100 mV, serosa positive. Activated inward current was between 85 and 450 μA/cm². In more than 25 tissue areas of 150 × 100 μm from 10 animals, which were automatically scanned with the vibrating probe, between 0 and 4 peaks of elevated local current (up to 800 μA/cm²) could be identified in individual fields. The density of current peaks, which were generally located at sites of mitochondria-rich (MR) cells, was less than 10% of the density of microscopically identified MR cells. The total current across individual sites of elevated conductance was 3.9 ± 0.6 nA. Considering the density of peaks, they account for 17 ± 2.5% of the applied transepithelial clamping current. The time course of current activation over previously identified conductive sites was in most cases unrelated to that of the total transepithelial current. Moreover, initially active sites could spontaneously inactivate. The results indicate that detection of elevated current above some MR cells is not sufficient to verify these cells as the pathway for transepithelial voltage-activated Cl⁻ current. Since the major fraction of activated current is apparently not associated with a route through MR cells, channel-like structures in the tight junctions of the paracellular pathway must be considered as an alternative possibility. Current peaks over MR cells could be due to high density of such sites in tight junctions between MR and surrounding principal cells. Improvement of the spatial resolution of the vibrating probe is required to verify this view. Received: 29 May 1997/Revised: 29 September 1997     

Electrical Transmission at the Nexus between Smooth Muscle Cells

The hypothesis that nexuses between cells are responsible for the core conductor properties of tissues was tested using smooth muscle preparations from the taenia coli of guinea pigs. Action potentials recorded from small diameter preparations across a sucrose gap change from monophasic to diphasic when a shunt resistor is connected across the gap. This indicates that transmission between smooth muscle cells is electrical, because the resistor only allows current to flow. Nexal fusion of cell membranes occurs especially where one cell sends a large bulbous projection into a neighbor. Hypertonic solutions rupture the nexuses between smooth muscle cells. Hypertonicity also increases the resistance of a bundle across the sucrose gap and blocks propagation of action potentials. Thus the structural and functional changes in smooth muscle due to hypertonicity correlate with the hypothesis.     

Differentiated structure and function of primary cultures of monkey oviductal epithelium

Summary We have established well-differentiated, polarized cultures of monkey oviductal epithelium. Oviductal epithelial cells were isolated by protease digestion and plated on collagen-coated, porous cell culture inserts. About 5 d after plating, cells developed detectable transepithelial electrical resistance of up to 2000 Ω.cm² (an index of tight junction formation) and transepithelial voltages of up to 20 mV (an index of vectorial transepithelial ion transport). Measurements of short-circuit current in Ussing chambers indicated that active secretion of Cl was the major transepithelial active ion transport process, and that this was stimulated by elevation of either cAMP or Ca. Furthermore, estimates of the volume of mucosal liquid were consistent with Cl secretion mediating fluid secretion. Various microscopical methods showed that the cultures were densely ciliated and contained mature secretory cells. Transport across the oviductal epithelium determines the composition of the oviductal fluid, and the study of the relevant transport processes will be greatly enhanced by well-differentiated cultures of oviductal epithelium of the kind established here.     

Electrotonic spread of current in monolayer cultures of neonatal rat heart cells

Summary The passive electrical properties of neonatal rat heart cells grown in monolayer cultures were determined. Hyperpolarizing current pulses were injected through one microelectrode via an active bridge circuit. Membrane voltage displacements caused by the injected current pulses were measured at various distances from the first with a second microelectrode. Using a modified least-squares method the experimental results were fitted to a Bessel function, which is the steady-state solution of the differential equation describing the relation between membrane voltage caused by current injection and interelectrode distance in a very large and very thin plane cell. Best fit was obtained with a space constant of 360 m and an internal resistivity of 500 cm. From these figures, specific membrane resistance was calculated to be 1,300 cm², assuming all current to leave through the upper surface of the monolayer.The time constant of the membrane was measured from the time course of the current-induced membrane voltage displacements. From its value of 1.7 msec a membrane capacity of 1.3 F/cm² was calculated.From these results and some literature data on nexus distribution (A. W. Spira,J. Ultrastruct. Res. 34:409, 1971) specific nexus resistance was calculated to range between 0.25 and 1.25 cm², depending on the amount of folding of the intercalated discs. The results suggest that spread of activation in monolayer cultures of heart cells by means of local circuit currents is very likely.     

Cytoplasm Resistivity of Mammalian Atrial Myocardium Determined by Dielectrophoresis and Impedance Methods

Many cardiac arrhythmias are caused by slowed conduction of action potentials, which in turn can be due to an abnormal increase of intracellular myocardial resistance. Intracellular resistivity is a linear sum of that offered by gap junctions between contiguous cells and the cytoplasm of the myocytes themselves. However, the relative contribution of the two components is unclear, especially in atrial myocardium, as there are no precise measurements of cytoplasmic resistivity, R_c. In this study, R_c was measured in atrial tissue using several methods: a dielectrophoresis technique with isolated cells and impedance measurements with both isolated cells and multicellular preparations. All methods yielded similar values for R_c, with a mean of 138 ± 5 Ω·cm at 23°C, and a Q₁₀ value of 1.20. This value is about half that of total intracellular resistivity and thus will be a significant determinant of the actual value of action potential conduction velocity. The dielectrophoresis experiments demonstrated the importance of including divalent cations (Ca²⁺ and Mg²⁺) in the suspension medium, as their omission reduced cell integrity by lowering membrane resistivity and increasing cytoplasm resistivity. Accurate measurement of R_c is essential to develop quantitative computational models that determine the key factors contributing to the development of cardiac arrhythmias.     

The Chloride Conductance of Tight Junctions of Rat Ileum Can Be Increased by cAMP But Not by Carbachol

It is well known, that in mammalian small intestine, cAMP increases Cl⁻ permeability of the apical membrane of enterocytes as part of its secretory action. Paradoxically, this is usually accompanied by an increase of the transepithelial resistance. In the present study we report that in the presence of bumetanide (to block basolateral Cl⁻ uptake) cAMP always decreased the transepithelial resistance. We examined whether this decrease in resistance was due to a cAMP-dependent increase of the paracellular electrolyte permeability in addition to the increase of the Cl⁻ permeability of the apical cell membrane. We used diffusion potentials induced by serosal replacement of NaCl, and transepithelial current passage to evoke transport number effects. The results revealed that cAMP (but not carbachol) could increase the Cl⁻ permeability of the tight junctions in rat ileum. Moreover, we observed a variation in transepithelial resistance of individual tissue preparations, inversely related to the cation selectivity of the tissue, suggesting that Na⁺ permeability of the tight junctions can vary between preparations. Received: 7 September 1996/Revised: 5 November 1996     

Freeze-fracture studies of the sinoatrial and atrioventricular nodes of the caprine heart,with special reference to the nexus

Summary The caprine sinoatrial node (SAN) and atrioventricular node (AVN) were studied by freeze-fracture techniques, and their nexus or gap junction structure were compared with that of ordinary atrial and ventricular muscle cells. The general features of the nexus in both the SAN and AVN were essentially identical. Approximately two-thirds of the nexuses observed in the nodal cells consisted of typical macular arrangements of nexal particles, and the remaining third, of atypical configurations of either circular arrangements or linear arrays of particles in continuity with the macular nexuses. Such atypical nexuses were never observed in the ordinary adult myocardial cells. Quantitative analysis revealed that all of the nexuses in the nodal cells measured, were less than 0.1 m², whereas the majority of the nexuses in ordinary myocardial cells (64% in the atrium and 76% in the ventricle) were larger than 0.1 m². No significant differences in diameter and center-to-center distance of nexal particle were found between the nodal cells and ordinary myocardial cells.     

The resistance of the septum of the medium giant axon of the earthworm

It is generally thought that nexuses constitute low-resistance pathways between cell interiors in epithelial, neural, muscular, and even connective tissues. However, there are no reliable estimates of the specific resistance of a nexus. The reason for this is that in most cases the surfaces of nexuses between cells are geometrically complex and therefore it has been very hard to accurately estimate nexal areas. However, the septa of the median giant axon have a relatively simple shape. Moreover, in this preparation, it is possible to make a measuring current flow parallel to the axon axis so that from the voltage difference appearing between intracellular electrodes during current flow, the specific septal membrane resistance could be calculated. The average specific nexal resistance obtained was 5.9 ω cm(2) if one assumes that 100 percent of the septum is nexus. The steady state I-V curve for the septum is linear (+/- 10 mV). Placement of electrodes was validated by septa even though the septa were found to be permeable to fluorescein and TEA. Exposure of the axon to hypertonic saline impedes the movement of fluorescein across the septa. By analogy with other tissues it is concluded that hypertonic solutions disrupt nexuses.

A mathematical model was derived which predicts the steady- state transmembrane potential vs. distance from a point source of intracellular current. When the specific nexal membrane resistance is 5.9 ω cm(2), the prediction closely approximates the fall of transmembrane potential vs. distance in an ordinary infinite cable. This is commensurate with the electrophysiological behavior of this multicellular “axon.”

     

Structural changes in the zonulae occludentes of the chloride cells of young adult lampreys following acclimation to seawater

Summary Thin sections and freeze-fracture replicas have been used to study the structure of the zonulae occludentes of the branchial chloride cells in young adults of the anadromous lamprey Geotria australis, caught during their downstream migration to the sea and after acclimation to full-strength seawater (35). The chloride cells in the epithelium of the gill filaments of both freshwater- and seawater-acclimated animals form extensive multicellular complexes. In freshwater animals, the majority of chloride cells (64%) are covered by pavement cells and are thus not exposed to the external environment. Most of the other chloride cells are separated from each other by pavement cells or their processes. The zonulae occludentes between chloride cells and pavement cells and between adjacent chloride cells are extensive and characterised by a network of 4 (range 3–7) superimposed strands. In seawater-acclimated animals, the pavement cells cover only 30% of the chloride cells and their processes no longer occur between chloride cells. Whereas the zonulae occludentes between chloride cells and pavement cells are still extensive, those between chloride cells are shallow and comprise only a single strand or two parallel strands. The zonulae occludentes between the chloride cells of lampreys acclimated to seawater are similar to those in the gills of teleosts in seawater, and are thus considered to be leaky and to provide a low-resistance paracellular pathway for the passive transepithelial movement of Na⁺.     

Stimulation of dome formation in MDCK kidney epithelial cultures by inducers of differentiation: Dissociation from effects on transepithelial resistance and cyclic AMP levels

Changes in transepithelial electrical resistance and cyclic nucleotide levels were monitored accompanying chemical induction of domes in a clonal subline of MDCK kidney epithelial cells. Confluent cell monolayers grown on nitrocellulose filters exhibited a relatively high mean transepithelial resistance (387 ohms · cm²). Hexamethylene bisacetamide, a potent inducer of dome formation (Lever, 1979b), stimulated significantly increased transmonolayer resistance as well as elevated levels of intracellular cyclic AMP. By contrast, dimethylformamide, an equally potent inducer of dome formation in MDCK cells, did not appreciably alter either resistance values or cyclic nucleotide levels. These results suggest that induction of dome formation in epithelial cell cultures by compounds generally known as inducers of differentiation may involve multiple and separate mechanisms.     

Further evidence for the regulation of the tight junction ion selectivity by cAMP in goldfish intestinal mucosa

Summary It has been reported that cAMP controls the transepithelial Cl^– conductance in fish intestine (Bakker, R., Groot, J.A., 1984,Am. J. Physiol. 246:G213–G217; Krasny, E.J., Madara, J.L., DiBona, D.L., Frizzell, R.A., 1983,Fed. Proc. 42:1100). In both studies, the cAMP effect was interpreted as an increase in tight junction Cl^– conductance, because cAMP did not change the membrane potential or membrane resistance ratio. However, the activation of a Cl^– conductance in the membranes of a subset of the epithelial cells might be difficult to discern from an increase in tight junction Cl^– conductance. Here we report experiments that were designed to distinguish a tight junction Cl^– conductance from a membrane Cl^– conductance in a subpopulation of the epithelial cells. The effect of hypotonicity on the cAMP-induced increase in transepithelial conductance showed that cAMP-induced conductance is located in series with the lateral intercellular spaces. Transepithelial serosa to mucosa direct current caused an increase in resistance due to so-called transport number effects. Forskolin abolished the transport number effects, indicating that cAMP increases the Cl^– conductance of the tight junctions. Increasing cAMP did not change mannitol fluxes, whereas Cl^– fluxes more than doubled. Changes in dilution potential and transepithelial resistance demonstrated that the cAMP-induced conductance is specific for Cl^– and Br^– as opposed to I^–, NO ₃ ^– , SO ₄ ^2– and gluconate^–. In contranst, cytochalasin D also decreased the transepithelial resistance and dilution potential in Nagluconate Ringer's. This demonstrates that cAMP acts on the tight junctions in a more specific manner than cytochalasin D.     

Use of AC Impedance Analysis to Study Membrane Changes Related to Acid Secretion in Amphibian Gastric Mucosa

We have applied transepithelial AC impedance techniques to gastric mucosa to reconcile ultrastructural and electrophysiological findings about gastric acid secretion and the mucosal barrier. By fitting impedance data measured at different HCl secretion rates to equivalent circuit models, we extracted capacitances and resistances (as measures of membrane area and ionic conductance, respectively) for the apical and basolateral membranes. The impedance measurements were found to be incompatible with earlier equivalent circuit models that modeled membrane electrical properties as lumped circuits based on one or two cell types. A distributed circuit model was developed that assumed only one dominant electrical pathway (i.e., one cell type), but that incorporated electrical effects arising from long and narrow membrane-lined structures present in the epithelium (e.g., gastric crypts, tubulovesicles, lateral intercellular spaces). This morphologically based model was found to represent the measured data accurately, and to yield values for membrane capacitances consistent with morphometric measurements of membrane areas. The main physiological conclusions from this analysis were as follows: (a) The dominant transepithelial current pathway may reside in the oxyntic cells. (b) The transepithelial conductance increase associated with the onset of acid secretion is entirely due to increased conductance of the apical membrane. This is in turn due entirely to increased area of this membrane, resulting from incorporation of tubulovesicular membrane. (c) When membrane conductances are normalized to actual membrane area by use of membrane capacitances, it turns out that acid secretion is not associated with a change in specific ionic conductance (change in conductance per unit area) at either the apical or basolateral membrane. (d) The puzzlingly low value of transepithelial resistance (≤400 Ω-cm²) arises because there are hundreds or thousands of square centimeters of actual membrane area per square centimeter chamber area. Apical membrane resistance is 25 kΩ-cm² (actual membrane area), implying a tight barrier to back-diffusion of protons.     

Evaluation of electric field changes in the cleft between excitable cells

Two contiguous myocardial cells with a narrow junctional cleft between them (intercalated disk) and bathed in a large volume conductor were modelled by an electrical analog circuit. Both a circuit analysis and a computer simulation were done. Each cell was divided into four lumped regions (units): (1) junctional membrane (JM) at left end of cell, (2) surface membrane (SM) at left half of cell, (3) SM at right half, and (4) JM at right end. Each region (unit) was represented by two parallel legs: (1) a K⁺ resistance in series with a K⁺ battery, and (2) a Na⁺ resistance in series with a Na⁺ battery. The JMs were given the same resistivity as the SM. The radial resistance of the cleft was varied to represent different cleft widths. Firing an action potential in one JM bordering the cleft (cell 1), by lowering its Na⁺ resistance, caused the potential in the cleft to swing negative with respect to ground (fluid bathing the cells). Although the inner surface of the JM of cell 2 remained at nearly constant potential with respect to ground, the membrane was depolarized by the same degree as the negativity at its outer surface. The depolarization for a 200 Å cleft was beyond the hypothetical threshold potential. The narrower the cleft, the greater the electric field effect. The activated JM, in turn, activated the remainder of cell 2. Thus, virtually no local-circuit current flowed through cell 2, and it fired without low-resistance connections between the cells. However, because simultaneous firing of the right half SM of cell 1 (unit 3) causes complete cancellation of the cleft potential, for the present model to give a workable basis for the transfer of excitation from cell to cell, it is required that unit 4 fire a fraction of a millisecond before unit 3. (Unit 2 causes partial cancellation.) This is possible for several reasons: (a) the depolarization of unit 4 (when unit 1 is fired) is slightly larger than that of unit 3, (b) K⁺ accumulation in the cleft and (c) the threshold of the JM may be slightly lower. Thus, intercellular communication can occur electrically without low-resistance connections.