Connexin32 gap junction channels in stably transfected cells: unitary conductance.

Pairs of SKHep1 cells, which are derived from a highly metastatic human hepatoma, were studied using the whole cell voltage clamp technique with patch-type electrodes containing CsCl as the major ionic species. In 12 of 81 cell pairs, current flow through junctional membranes was detectable; in the remaining 69 cell pairs, junctional conductance was less than the noise limit of our recording apparatus (worst case: 10 pS). Macroscopic junctional conductance (gj) in the small percentage of pairs where it was detectable ranged from 100 to 600 pS. Unitary junctional conductance (gamma j) determined in the lowest conductance pairs or after reducing conductance with a short exposure to the uncoupling agent halothane was 25-35 pS. To study properties of gap junction channels formed of connexin32, the parental SKHep1 cell line was stably transfected with a plasmid containing cDNA that encodes connexin32, the major gap junction protein of rat liver cells. In 85 of 98 pairs of voltage clamped connexin32-transfected SKHep1 cells, macroscopic gj was greater than 1 nS; gj increased with time after dissociation (from 1.8 +/- 0.6 [mean +/- SE; n = 7] nS at 2 h after plating to 9.3 +/- 2.2 [n = 9] nS, the maximal value, at 24 h). Unitary conductance of gap junction channels between pairs of transfected SKHep1 cells was measured in low conductance pairs and after reducing gj by exposure to halothane or heptanol. Histograms of gamma j values in transfected cells, in 10 experiments where greater than 100 transitions were measurable, displayed two peaks; 120-130 pS and 25-35 pS. The smaller size corresponded to channels that were occasionally detected in the parental cells. We therefore conclude that connexin32 forms gap junctions channels of the 120-130 pS size class.     

Gating characteristics of a steeply voltage-dependent gap junction channel in rat Schwann cells

The gating properties of macroscopic and microscopic gap junctional currents were compared by applying the dual whole cell patch clamp technique to pairs of neonatal rat Schwann cells. In response to transjunctional voltage pulses (Vj), macroscopic gap junctional currents decayed exponentially with time constants ranging from < 1 to < 10 s before reaching steady-state levels. The relationship between normalized steady-state junctional conductance (Gss) and (Vj) was well described by a Boltzmann relationship with e-fold decay per 10.4 mV, representing an equivalent gating charge of 2.4. At Vj > 60 mV, Gss was virtually zero, a property that is unique among the gap junctions characterized to date. Determination of opening and closing rate constants for this process indicated that the voltage dependence of macroscopic conductance was governed predominantly by the closing rate constant. In 78% of the experiments, a single population of unitary junctional currents was detected corresponding to an unitary channel conductance of approximately 40 pS. The presence of only a limited number of junctional channels with identical unitary conductances made it possible to analyze their kinetics at the single channel level. Gating at the single channel level was further studied using a stochastic model to determine the open probability (Po) of individual channels in a multiple channel preparation. Po decreased with increasing Vj following a Boltzmann relationship similar to that describing the macroscopic Gss voltage dependence. These results indicate that, for Vj of a single polarity, the gating of the 40 pS gap junction channels expressed by Schwann cells can be described by a first order kinetic model of channel transitions between open and closed states.     

Electrophysiological properties of gap junctions between dissociated pairs of rat hepatocytes

Physiological properties of isolated pairs of rat hepatocytes were examined within 5 h after dissociation. These cells become round when separated, but cell pairs still display membrane specializations. Most notably, canaliculi are often present at appositional membranes which are flanked by abundant gap and tight junctions. These cell pairs are strongly dye-coupled; Lucifer Yellow CH injected into one cell rapidly diffuses to the other. Pairs of hepatocytes are closely coupled electrically. Conductance of the junctional membrane is not voltage sensitive: voltage clamp studies demonstrate that gj is constant in response to long (5 s) transjunctional voltage steps of either polarity (to greater than +/- 40 mV from rest). Junctional conductance (gj) between hepatocyte pairs is reduced by exposure to octanol (0.1 mM) and by intracellular acidification. Normal intracellular pH (pHi), measured with a liquid ion exchange microelectrode, was generally 7.1-7.4, and superfusion with saline equilibrated with 100% CO2 reduced pHi to 6.0-6.5. In the pHi range 7.5-6.6, gj was constant. Below pH 6.6, gj steeply decreased and at 6.1 coupling was undetectable. pHi recovered when cells were rinsed with normal saline; in most cases gj recovered in parallel so that gj values were similar for pHs obtained during acidification or recovery. The low apparent pK and very steep pHi-gj relation of the liver gap junction contrast with higher pKs and more gradually rising curves in other tissues. If H+ ions act directly on the junctional molecules, the channels that are presumably homologous in different tissues must differ with respect to reactive sites or their environment.     

Gap junction formation and functional interaction between neonatal rat cardiocytes in culture: A correlative physiological and ultrastructural study

Summary The time course of gap junction formation and growth, following contraction synchronization of cardiac myocytes in culture, has been studied in a combined (electro)physiological and ultrastructural study. In cultures of collagenase-dissociated neonatal rat cardiocytes, pairs of spontaneously beating myocytes synchronized their contractions within one beat interval within 2–20 min after they apparently had grown into contact, 45 sec after the first synchronized beat an appreciable junctional region containing several small gap junctions was already present. In the following 30 min, neither the area of individual gap junctions nor their total area increased, 75 min after synchronization both the area of individual gap junctions and their total area had increased by a factor of 10–15 with respect to what was found in the first half hour. In the period between 75 and 300 min again no further increase in gap junctional area was found. In double voltage-clamp experiments, gap junctions between well-coupled cells behaved like ohmic conductors. In poorly coupled cells, in which the number of functional gap-junctional channels was greatly reduced, the remaining channels showed voltage-dependent gating. Their single-channel conductance was 40–50 pS. The electrophysiologically measured junctional conductance agreed well with the conductance calculated from the morphometrically determined gap-junctional area. It is concluded that a rapid initial gap junction formation occurs during the 2–20 min period prior to synchronization by assembly of functional channels from existing channel precursors already present in the cell membranes. It then takes at least another 30 min before the gap-junctional area increases possibly byde novo synthesis or by recruitment from intracellular stores or from nonjunctional membranes, a process completed in the next 45 min.     

Gap junctions in cultured astrocytes: single-channel currents and characterization of channel-forming protein.

Currents from gap junction channels were recorded from pairs of astrocytes in primary culture using the double whole-cell recording technique. In weakly coupled pairs, single-channel events could be resolved without pharmacological uncoupling treatment. Under these conditions, unitary conductance was 56 +/- 7 pS, and except for multiples of this value, no other level of conductance was observed consistently. To characterize the type of junctional protein constituting astrocyte gap junction channels, immunological and biochemical experiments were carried out on the same material. Specific cDNA probes for three connexins identified in mammals (Cx26, Cx32, and Cx43) showed that only Cx43 mRNA was expressed in cultured astrocytes. The presence of Cx43 protein in cultured astrocytes was demonstrated by immunoblotting, immunofluorescence, and immunogold labeling using anti-peptide antibodies specific to Cx43. These results strongly suggest that gap junctions in astrocytes have a 50-60 pS unitary conductance associated with channels composed of Cx43 protein.     

Single channel behavior of recombinant beta 2 gap junction connexons reconstituted into planar lipid bilayers.

The beta 2 gap junction protein (Cx26) was expressed in an insect cell line by infection with a baculovirus vector containing the rat beta 2 cDNA. Isolated beta 2 gap junction connexons were reconstituted into planar lipid bilayers. Single channel activity was observed with a unitary conductance of 35-45 pS in 200 mM KCl. Channels with conductance values of 60 pS and 90-110 pS also coexisted with the lower conducting channel suggesting that there are channels with different conductance properties within a population of connexons. Channel activity was observed at voltages of up to 150 mV. Furthermore, the characterization of these channel properties from the beta 2 connexons that were generated by this heterologous expression system has provided the basis for identifying an endogenous beta 2 connexon channel in material reconstituted from native rat liver gap junctions.     

Gating of gap junction channels.

Gap junctional conductance ( gj ) in various species is gated by voltage and intracellular pH (pHi). In amphibian embryos, gj is reduced to half by a 14 mV transjunctional voltage ( Vj ), a change that in fish embryo requires approximately 28 mV. Crayfish septate axon and pairs of dissociated rat myocytes show no voltage dependence of gj over a range of Vj greater than +/- 50 mV. In fish and amphibian blastomeres , gj is steeply decreased by decrease in pHi (n, Hill coefficient: 4.5) and the apparent pKH (7.3) is in the physiological range. In crayfish septate axon the pKH is lower (6.7) and the curve is less steep (n = 2.7). Rises in cytoplasmic Ca can also decrease gj but much higher concentrations are required (greater than 0.1 mM in fish blastomeres). Voltage and pH gates on gap junctions in amphibian embryos appear independent. In squid blastomeres pH gates exhibit some sensitivity to potential, both transjunctional and between inside and outside. A pharmacology of gap junctions is being developed: certain agents block gj directly (aldehydes, alcohols, NEM in crayfish); others block by decreasing pHi (esters that are hydrolyzed by intrinsic esterases, NEM in vertebrates, and, as in the experiments demonstrating the effect of pHi, weak acids). Certain agents block pH sensitivity without affecting voltage dependence (retinoic acid, glutaraldehyde, EEDQ), further indicating separateness of pH and voltage gates. These studies demonstrate a dynamics of gap junctional conductance and variability in gating in a series of possibly homologous membrane channels.     

Gating of mammalian cardiac gap junction channels by transjunctional voltage.

Numerous two-cell voltage-clamp studies have concluded that the electrical conductance of mammalian cardiac gap junctions is not modulated by the transjunctional voltage (Vj) profile, although gap junction channels between low conductance pairs of neonatal rat ventricular myocytes are reported to exhibit Vj-dependent behavior. In this study, the dependence of macroscopic gap junctional conductance (gj) on transjunctional voltage was quantitatively examined in paired 3-d neonatal hamster ventricular myocytes using the double whole-cell patch-clamp technique. Immunolocalization with a site-specific antiserum directed against amino acids 252-271 of rat connexin43, a 43-kD gap junction protein as predicted from its cDNA sequence, specifically stained zones of contact between cultured myocytes. Instantaneous current-voltage (Ij-Vj) relationships of neonatal hamster myocyte pairs were linear over the entire voltage range examined (0 less than or equal to Vj less than or equal to +/- 100 mV). However, the steady-state Ij-Vj relationship was nonlinear for Vj greater than +/- 50 mV. Both inactivation and recovery processes followed single exponential time courses (tau inactivation = 100-1,000 ms, tau recovery approximately equal to 300 ms). However, Ij recovered rapidly upon polarity reversal. The normalized steady-state junctional conductance-voltage relationship (Gss-Vj) was a bell-shaped curve that could be adequately described by a two-state Boltzmann equation with a minimum Gj of 0.32-0.34, a half-inactivation voltage of -69 and +61 mV and an effective valence of 2.4-2.8. Recordings of gap junction channel currents (ij) yielded linear ij-Vj relationships with slope conductances of approximately 20-30 and 45-50 pS. A kinetic model, based on the Boltzmann relationship and the polarity reversal data, suggests that the opening (alpha) and closing (beta) rate constants have nearly identical voltage sensitivities with a Vo of +/- 62 mV. The data presented in this study are not consistent with the contingent gating scheme (for two identical gates in series) proposed for other more Vj-dependent gap junctions and alternatively suggest that each gate responds to the applied Vj independently of the state (open or closed) of the other gate.     

Voltage-clamp studies of gap junctions between uterine muscle cells during term and preterm labor.

Gap junctions between myometrial cells increase dramatically during the final stages of pregnancy. To study the functional consequences, we have applied the double-whole-cell voltage-clamp technique to freshly isolated pairs of cells from rat circular and longitudinal myometrium. Junctional conductance was greater between circular muscle-cell pairs from rats delivering either at term (32 +/- 16 nS, mean +/- SD, n = 128) or preterm (26 +/- 17 nS, n = 33) compared with normal preterm (4.7 +/- 7.6 nS, n = 114) and postpartum (6.5 +/- 10 nS, n = 16); cell pairs from the longitudinal layer showed similar differences. The macroscopic gap junction currents decayed slowly from an instantaneous, constant-conductance level to a steady-state level described by quasisymmetrical Boltzmann functions of transjunctional voltage. In half of circular-layer cell pairs, the voltage dependence of myometrial gap junction conductance is more apparent at smaller transjunctional voltages (< 30 mV) than for other tissues expressing mainly connexin-43. This unusual degree of voltage dependence, although slow, operates over time intervals that are physiologically relevant for uterine muscle. Using weakly coupled pairs, we observed two unitary conductance states: 85 pS (85-90% of events) and 25 pS. These measurements of junctional conductance support the hypothesis that heightened electrical coupling between the smooth muscle cells of the uterine wall emerges late in pregnancy, in preparation for the massive, coordinate contractions of labor.     

Gap junctional communication of primary human keratinocytes: characterization by dual voltage clamp and dye transfer.

We have compared dye coupling in pairs of small (less than 10 microns in diameter) and large (greater than 20 microns in diameter) keratinocytes isolated from normal human epidermis, using Lucifer yellow microinjection. Under control conditions, dye coupling was found in only 1 out of the 25 small pairs tested, whereas it was evident in 75% of the large pairs (n = 52). After a 30-min incubation of the latter pairs in the presence of 10(-6) and 10(-4) M all-transretinoic acid (RA), the percentage of coupling was 53% (n = 15; NS) and 7% (n = 14; P less than 0.001), respectively. The almost complete uncoupling observed after 10(-4) M RA was not reversible even 30 min after return to control medium (n = 8). Dual whole-cell patch-clamp recordings from large keratinocyte pairs showed a macroscopic junctional conductance (gj) of 9 +/- 2 nS (n = 43), which was abolished by heptanol (3.5 mM) in a fully reversible way. Compared to heptanol, 10(-4) M RA abolished keratinocyte gj more slowly and irreversibly (n = 10). By contrast, 10(-6) M RA had no significant effect on gj (n = 8). Single-gap junctional channels were also identified between large keratinocytes. Events histograms of 152 transitions from three experiments revealed three main unitary conductances (gamma j) of 45 +/- 4, 78 +/- 4, and 106 +/- 7 pS. The dye coupling results indicate that junctional communication is markedly different in pairs of small and large cells, which showed the phenotype and keratin markers of basal and suprabasal keratinocytes, respectively. In the latter cell type, coupling is ensured by channels of three sizes and is blocked irreversibly by pharmacologic concentrations of RA.     

Gap junction channels: distinct voltage-sensitive and -insensitive conductance states.

All mammalian gap junction channels are sensitive to the voltage difference imposed across the junctional membrane, and parameters of voltage sensitivity have been shown to vary according to the gap junction protein that is expressed. For connexin43, the major gap junction protein in the cardiovascular system, in the uterus, and between glial cells in brain, voltage clamp studies have shown that transjunctional voltages (Vj) exceeding +/- 50 mV reduce junctional conductance (gj). However, substantial gj remains at even very large Vj values; this residual voltage-insensitive conductance has been termed gmin. We have explored the mechanism underlying gmin using several cell types in which connexin43 is endogenously expressed as well as in communication-deficient hepatoma cells transfected with cDNA encoding human connexin43. For pairs of transfectants exhibiting series resistance-corrected maximal gj (gmax) values ranging from < 2 to > 90 nS, the ratio gmin/gmax was found to be relatively constant (about 0.4-0.5), indicating that the channels responsible for the voltage-sensitive and -insensitive components of gj are not independent. Single channel studies further revealed that different channel sizes comprise the voltage-sensitive and -insensitive components, and that the open times of the larger, more voltage-sensitive conductance events declined to values near zero at large voltages, despite the high gmin. We conclude that the voltage-insensitive component of gj is ascribable to a voltage-insensitive substate of connexin43 channels rather than to the presence of multiple types of channels in the junctional membrane. These studies thus demonstrate that for certain gap junction channels, closure in response to specific stimuli may be graded, rather than all-or-none.     

Exchange of gating properties between rat cx46 and chicken cx45.6

Cx46 and Cx50 are coexpressed in lens fiber cells where they form fiber-fiber gap junctions. Recent studies have shown that both proteins play a critical role in maintaining lens transparency. Although both Cx46 and Cx50 (or its chicken ortholog, Cx45.6) show a high degree of sequence homology, they exhibit marked differences in gap junctional channel gating, unitary gap junctional channel conductance, and hemichannel gating. To better understand which regions of the protein are responsible for these functional differences, we have constructed a series of chimeric Cx46-Cx45.6 gap junctional proteins in which a single transmembrane or intracellular domain of Cx45.6 was replaced with the corresponding domain of Cx46, expressed them in Xenopus oocyte pairs or N2A cells, and examined the resulting gap junctional conductances. Our results showed that four out of six of the chimeras induced high levels of gap junctional coupling. Of these chimeras, only Cx45.6-46NT showed significant changes in voltage-dependent gating properties. Exchanging the N-terminus had multiple effects. It slowed the inactivation kinetics of the macroscopic junctional currents so that they resembled those of Cx46, reduced the voltage sensitivity of the steady-state junctional conductance, and decreased the conductance of single gap junctional channels. Additional point mutations identified a uniquely occurring arginine in the N-terminus of Cx46 as the main determinant for the change in voltage-dependent gating.     

The influence of surface charges on the conductance of the human connexin37 gap junction channel

The single-channel conductance of the hCx37 homotypic gap junction channel does not saturate with transjunctional voltages up to +/-75 mV, nor does it depend linearly on the intracellular electrolyte concentration. The average maximum unitary conductances measured in KCl were 175 pS (30 mM), 236 pS (55 mM), 343 pS (110 mM), and 588 pS (270 mM) in the presence of 0.1 mM MgCl(2). The unexpectedly high unitary conductance at low salt concentrations can be explained by fixed charge groups within or near the channel orifice. Fixed cytoplasmic surface charges (3.4 e) positioned adjacent (15 A) to the channel pore adequately model the data (surface charge density of 0.24 e/(nm)(2)). In other experiments, high Mg(2+) reduced the unitary conductance of hCx37 homotypic gap junction channels more than predicted by screening alone, consistent with specific effects of Mg(2+) on the channel.     

Single-membrane and cell-to-cell permeability properties of dissociated embryonic chick lens cells

Ion channels are believed to play an important role in the maintenance of lens transparency. In order to ascribe junctional and nonjunctional permeability properties to specific lens cell types, embryonic chick lenses were enzymatically dissociated into cell clusters, cell pairs and single cells, and both cell-to-cell and single-membrane permeability properties were characterized with the patch-clamp technique. Double patch-clamp experiments and single patch-clamp experiments with Lucifer yellow in the pipette demonstrated that the cells in the dissociated preparation were well coupled, the average conductance between pairs being 42 +/- 27 nS. Double patch-clamp experiments also revealed single cell-to-cell channel events with a predominant unitary conductance of 286 +/- 38 pS. Whole-cell measurements of surface membrane conductance indicate heterogeneity within the population of dissociated embryonic chick lens cells: 63% of the cells have a voltage-independent leak current, 14% of the cells have a potassium-selective inward-rectifier current, and 23% of the cells have a current which turns off with positive voltage on a time scale on the order of seconds. The time constant for this turnoff is voltage dependent.     

Nontransformed cells can normalize gap junctional communication with transformed cells

We demonstrate that the Src kinase can augment gap junctional communication between cells derived from homozygous null Cx43 knockout mice. The total conductance between Src transformed cells was nearly twice that of nontransformed cells. In addition, the unitary conductance of the majority of single channel events between transformed cells was about 35% greater than that of nontransformed cells. Analysis showed that both nontransformed and transformed cells expressed at least two populations of channels, suggesting that Src increased junctional conductance by up-regulating one population and/or by increasing the unitary conductance of another population of channels. Interestingly, the conductance displayed by heterologous pairs of transformed and nontransformed cells resembled that of nontransformed cells. The majority of single channel events between heterologous pairs shifted back to lower conductances that were exhibited by nontransformed cells. Thus, nontransformed cells can effectively "normalize" the conductance of gap junction channels expressed by adjacent tumor cells.     

Patch clamp recordings from membranes which contain gap junction channels.

The septal membranes of the median and lateral giant axons of earthworm, which contain gap junctions, were exposed by cutting one segment of the cord. Patch recordings were obtained from the exposed cytoplasmic side of the septum. Seal resistances ranged from 2 to 15 G omega. The patch could be excised (detached) or left attached to the whole cell. Two types of channels were observed. One type was blocked by tetraethylammonium (TEA) or Cs+ and had a unitary conductance of 30-40 pS. It appears to be a K+ channel. The other channel type had a unitary conductance of 90-110 pS and was unaffected by TEA+ or Cs+. In the detached configuration the channel was shown to conduct Cs+, K+, Na+, TMA+, Cl- and TEA+ even in the presence of 2 mM Zn2+, 1 mM Ni2+, 1 mM Co2+, and 4 mM 4-aminopyridine. The conductance ratios relative to K+ were 1.0 for Cs+, 0.84 for Na+, 0.64 for TMA+, 0.52 for Cl- and 0.2 for TEA+. The channel appears to be voltage insensitive whether monitored in detached or attached recording mode. Both H+ and Ca2+ reduce the probability of opening. Thus, the 100 pS channel has many of the properties expected of a gap junction channel.     

Voltage-dependent blockade of connexin40 gap junctions by spermine

The effects of spermine and spermidine, endogenous polyamines that block many forms of ion channels, were investigated in homotypic connexin (Cx)-40 gap junctions expressed in N2A cells. Spermine blocked up to 95% of I(j) through homotypic Cx40 gap junctions in a concentration- and transjunctional voltage (V(j))-dependent manner. V(j) was varied from 5 to 50 mV in 5-mV steps and the dissociation constants (K(m)) were determined from spermine concentrations ranging from 10 micro M to 2 mM. The K(m) values ranged from 4.9 mM to 107 micro M for 8.6 < or = V(j) < or = 37.7 mV, within the physiological range of intracellular spermine for V(j) > or = 20 mV. The K(m) values for spermidine were > or = 5 mM. Estimates of the electrical distance (delta) for spermine (z = +4) and spermidine (z = +3) were 0.96 and 0.76 respectively. Cx40 single channel conductance was 129 pS in the presence of 2-mM spermine and channel open probability was significantly reduced in a V(j)-dependent manner. Similar concentrations of spermine did not block I(j) through homotypic Cx43 gap junctions, indicating that spermine selectively blocks Cx40 gap junctions. This is contrary to our previous findings that large tetraalkylammonium ions, also known to block several forms of ion channels, block junctional currents (I(j)) through homotypic connexin Cx40 and Cx43 gap junctions.     

Size selectivity between gap junction channels composed of different connexins

Gap junction channels are traditionally viewed as large, nonspecific pores connecting cells. Recently the diversity in the connexin family has drawn more attention to their permeability characteristics. Several studies have shown that both size and charge contribute to the permeability of gap junctional channels. We have used a graded series of neutral polyethylene glycol probes (PEGs), which eliminate charge contribution completely, to specifically assess the physical exclusion limits of gap junction channels formed by different connexins. Cx 26, 32 and 37 were expressed in paired Xenopus oocytes to form homotypic gap junctional channels. PEG probes were perfused intracellularly into one side of the oocyte pair. A reversible drop in conductance of the gap juctional channels indicated that the probe was small enough to enter the pore and hinder ion flux. Our data suggest that Cx32 channels have a size cut-off between PEG 400 (11.2 A) and PEG 300 (9.6 A) despite their relatively small single channel conductance (approximately 55 pS). Cx26 channels (approximately 130 pS single channel conductance) have a size exclusion limit around PEG 200 (8.0 A), while Cx37 channels show the most restricted size cut-off between PEG 200 (8.0 A) and TriEG (6.8 A), despite having the largest unitary conductance (approximately 300 pS).     

Heterogeneity of calcium channels from a purified dihydropyridine receptor preparation.

Dihydropyridine receptors were purified from rabbit skeletal muscle transverse tubule membranes and incorporated into planar lipid bilayers. Calcium channels from both the purified dihydropyridine receptor preparation and the intact transverse tubule membranes exhibited two sizes of unitary currents, corresponding to conductances of 7 +/- 1 pS and 16 +/- 3 pS in 80 mM BaCl2. Both conductance levels were selective for divalent cations over monovalent cations and anions. Cadmium, an inorganic calcium channel blocker, reduced the single channel conductance of calcium channels from the purified preparation. The organic calcium channel antagonist nifedipine reduced the probability of a single channel being open with little effect on the single channel conductance. The presence of two conductance levels in both the intact transverse tubule membranes and the purified dihydropyridine receptor preparation suggests that the calcium channel may have multiple conductance levels or that multiple types of calcium channels with closely related structures are present in transverse tubule membranes.