Pore-lining residues identified by single channel SCAM studies in Cx46 hemichannels.

The substituted cysteine accessibility method was applied to single Cx46 hemichannels to identify residues that participate in lining the aqueous pore of channels formed of connexins. Criteria for assignment to the pore included reactivity to sulfydryl-specific methanethiosulfonate (MTS) reagents from both sides of an open hemichannel and observable effects on open channel properties. We demonstrate reactivity to MTS reagents over a stretch of seventeen amino acids, D51 through L35, that constitute segments of E1 and TM1. Qualitatively, the nature of the effects caused by the Cys substitutions alone and their modification with MTS reagents of either charge indicate side chain valence is most influential in determining single channel properties with D51 and L35 defining the extracellular and intracellular limits, respectively, of the identified pore-lining region. A number of Cys substitutions beyond L35 in TM1 caused severe alterations in hemichannel function and precluded assignment to the pore. Although all six subunits can be modified by smaller MTS reagents, modifications appear limited to fewer subunits with larger reagents.

Single-channel SCAM identifies pore-lining residues in the first extracellular loop and first transmembrane domains of Cx46 hemichannels.

Gap junction (GJ) channels provide an important pathway for direct intercellular transmission of signaling molecules. Previously we showed that fixed negative charges in the first extracellular loop domain (E1) strongly influence charge selectivity, conductance, and rectification of channels and hemichannels formed of Cx46. Here, using excised patches containing Cx46 hemichannels, we applied the substituted cysteine accessibility method (SCAM) at the single channel level to residues in E1 to determine if they are pore-lining. We demonstrate residues D51, G46, and E43 at the amino end of E1 are accessible to modification in open hemichannels to positively and negatively charged methanethiosulfonate (MTS) reagents added to cytoplasmic or extracellular sides. Positional effects of modification along the length of the pore and opposing effects of oppositely charged modifying reagents on hemichannel conductance and rectification are consistent with placement in the channel pore and indicate a dominant electrostatic influence of the side chains of accessible residues on ion fluxes. Hemichannels modified by MTS-EA+, MTS-ET+, or MTS-ES- were refractory to further modification and effects of substitutions with positively charged residues that electrostatically mimicked those caused by modification with the positively charged MTS reagents were similar, indicating all six subunits were likely modified. The large reductions in conductance caused by MTS-ET+ were visible as stepwise reductions in single-channel current, indicative of reactions occurring at individual subunits. Extension of single-channel SCAM using MTS-ET+ into the first transmembrane domain, TM1, revealed continued accessibility at the extracellular end at A39 and L35. The topologically complementary region in TM3 showed no evidence of reactivity. Structural models show GJ channels in the extracellular gap to have continuous inner and outer walls of protein. If representative of open channels and hemichannels, these data indicate E1 as constituting a significant portion of this inner, pore-forming wall, and TM1 contributing as pore-lining in the extracellular portion of transmembrane span.

Gap junction hemichannels in astrocytes of the CNS.

Connexins are protein subunits that oligomerize into hexamers called connexons, gap junction hemichannels or just hemichannels. Because some gap junction channels are permeable to negatively and/or positively charged molecules up to approximately 1kDa in size, it was thought that hemichannels should not open to the extracellular space. A growing amount of evidence indicates that opening of hemichannels does occur under both physiological and pathological conditions in astrocytes and other cell types. Electrophysiological studies indicate that hemichannels have a low open probability under physiological conditions but may have a much higher open probability under certain pathological conditions. Some of the physiological behaviours of astrocytes that have been attributed to gap junctions may, in fact, be mediated by hemichannels. Hemichannels constituted of Cx43, the main connexin expressed by astrocytes, are permeable to small physiologically significant molecules, such as ATP, NAD+ and glutamate, and may mediate paracrine as well as autocrine signalling. Hemichannels tend to be closed by negative membrane potentials, high concentrations of extracellular Ca2+ and intracellular H+ ions, gap junction blockers and protein phosphorylation. Hemichannels tend to be opened by positive membrane potentials and low extracellular Ca2+, and possibly by as yet unidentified cytoplasmic signalling molecules. Exacerbated hemichannel opening occurs in metabolically inhibited cells, including cortical astrocytes, which contributes to the loss of chemical gradients across the plasma membrane and speeds cell death.

Gating properties of gap junction channels assembled from connexin43 and connexin43 fused with green fluorescent protein.

We used cell lines expressing wild-type connexin43 (Cx43) and Cx43 fused with enhanced green fluorescent protein (Cx43-EGFP) to examine mechanisms of gap junction channel gating. Previously it was suggested that each hemichannel in a cell-cell channel possesses two gates, a fast gate that closes channels to a nonzero conductance or residual state via fast (< approximately 2 ms) transitions and a slow gate that fully closes channels via slow transitions (> approximately 10 ms). Here we demonstrate that transjunctional voltage (V(j)) regulates both gates and that they are operating in series and in a contingent manner in which the state of one gate affects gating of the other. Cx43-EGFP channels lack fast V(j) gating to a residual state but show slow V(j) gating. Both Cx43 and Cx43-EGFP channels exhibit slow gating by chemical uncouplers such as CO(2) and alkanols. Chemical uncouplers do not induce obvious changes in Cx43-EGFP junctional plaques, indicating that uncoupling is not caused by dispersion or internalization of junctional plaques. Similarity of gating transitions during chemical gating and slow V(j) gating suggests that both gating mechanisms share common structural elements. Cx43/Cx43-EGFP heterotypic channels showed asymmetrical V(j) gating with fast transitions between open and residual states only when the Cx43 side was relatively negative. This result indicates that the fast V(j) gate of Cx43 hemichannels closes for relative negativity at its cytoplasmic end.

The first extracellular loop domain is a major determinant of charge selectivity in connexin46 channels.

Intercellular channels formed of members of the gene family of connexins (Cxs) vary from being substantially cation selective to being anion selective. We took advantage of the ability of Cx46 to function as an unopposed hemichannel to examine the basis of Cx charge selectivity. Previously we showed Cx46 hemichannels to be large pores that predominantly conduct cations and inwardly rectify in symmetric salts, properties suggesting selectivity is influenced by fixed negative charges located toward the extracellular end of the pore. Here we demonstrate that high ionic strength solutions applied to the extracellular, but not the intracellular, side of Cx46 hemichannels substantially reduce the ratio of cation to anion permeability. Substitution of the first extracellular loop (E1) domain of Cx32, an anion-preferring Cx, reduces conductance, converts Cx46 from cation to anion preferring, and changes the I-V relation form inwardly to outwardly rectifying. These data suggest that fixed negative charges influencing selectivity in Cx46 are located in E1 and are substantially reduced and/or are replaced with positive charges from the Cx32 E1 sequence. Extending studies to Cx46 cell-cell channels, we show that they maintain a strong preference for cations, have a conductance nearly that expected by the series addition of hemichannels, but lack rectification in symmetric salts. These properties are consistent with preservation of the fixed charge region in E1 of hemichannels, which upon docking, become symmetrically placed near the center of the cell-cell channel pore. Furthermore, heterotypic cell-cell channels formed by pairing Cx46 with Cx32 or Cx43 rectify in symmetric salts in accordance with the differences in the charges we ascribed to E1. These data are consistent with charged residues in E1 facing the channel lumen and playing an important role in determining Cx channel conductance and selectivity.

Functional expression of the murine connexin 36 gene coding for a neuron-specific gap junctional protein.

The mouse connexin 36 (Cx36) gene was mapped on chromosome 2 and an identical transcriptional start site was determined in brain and retina on exon I. Rabbit polyclonal antibodies to the presumptive cytoplasmic loop of the Cx36 protein recognized in immunohistochemical analyses Cx36 expression in the retina, olfactory bulb, hippocampus, inferior olive and cerebellum. In olivary neurons strong punctate labeling at dendritic cell contacts and weaker labeling in the cytoplasm of dendrites were shown by immuno electron microscopy. After expression of mouse Cx36 cDNA in human HeLa cells, neurobiotin transfer was increased 1.8-fold and electrical conductance at least 15-fold compared to untransfected HeLa cells. No Lucifer Yellow transfer was detected in either untransfected or Cx36 transfected HeLa cells. Single Cx36 channels in transfected HeLa cells showed a unitary conductance of 14.3 + or - 0. 8 pS. The sensitivity of Cx36 channels to transjunctional voltage was low in both HeLa-Cx36 cells and Xenopus oocytes expressing mouse Cx36. No increased transfer of neurobiotin was detected in heterotypic gap junctions formed by Cx36 and 9 other connexins expressed in HeLa cells. Our results suggest that Cx36 channels function as electrical synapses for transmission of electrical and metabolic signals between neurons in the central nervous system.

Connexin hemichannels and cell-cell channels: comparison of properties.

Connexin46 (Cx46) forms functional hemichannels in the absence of contact by an apposed hemichannel and we have used these hemichannels to study gating and permeation at the single channel level with high time resolution. Using both cell-attached and -excised patch configurations, we find that single Cx46 hemichannels exhibit some properties expected of half of a gap junction channel, as well as novel properties. Cx46 hemichannels have a large unitary conductance (approximately 300 pS) and a relatively large pore as inferred from permeability to TEA. Both monovalent cations and anions can permeate, but cations are substantially more permeable. The open channel conductance shows marked inward rectification in symmetric salts. We find that the conductance and permeability properties of Cx46 cell-cell channels can be explained by the series addition of two hemichannels. These data suggest that the pore structures of unapposed hemichannels and cell-cell channels are conserved. Also like cell-cell channels, unapposed Cx46 hemichannels are closed by elevated levels of H+ or Ca2+ ions on the cytoplasmic face. Closure occurs in excised patches indicating that the actions of these agents do not require a soluble cytoplasmic factor. Fast (<0.5 ms) application of H+ to either side of the open hemichannel causes an immediate small reduction in unitary conductance followed by complete closure with latencies that are dependent on H+ concentration and side of application; sensitivity is much greater to H+ on the cytoplasmic side. Closure by cytoplasmic H+ does not require that the hemichannel be open. Thus, H+ ions readily permeate Cx46 hemichannels, but at high enough concentration close them by acting at a cytoplasmic site(s) that causes a conformational change resulting in complete closure. Extracellular H+ may permeate to act on the cytoplasmic site or act on a lower affinity extracellular site. Thus, the unapposed hemichannel is a valuable tool in addressing fundamental questions concerning the operation of gap junction channels that are difficult to answer by existing methods. The ability of Cx46, and perhaps other connexins, to form functional unapposed hemichannels that are opened by moderate depolarization may represent an unexplored role of connexins as mediators of transport across the plasma membrane.

Clustering of connexin 43-enhanced green fluorescent protein gap junction channels and functional coupling in living cells.

Communication-incompetent cell lines were transfected with connexin (Cx) 43 fused with enhanced green fluorescent protein (EGFP) to examine the relation between Cx distribution determined by fluorescence microscopy and electrical coupling measured at single-channel resolution in living cell pairs. Cx43-EGFP channel properties were like those of wild-type Cx43 except for reduced sensitivity to transjunctional voltage. Cx43-EGFP clustered into plaques at locations of cell-cell contact. Coupling was always absent in the absence of plaques and even in the presence of small plaques. Plaques exceeding several hundred channels always conferred coupling, but only a small fraction of channels were functional. These data indicate that clustering may be a requirement for opening of gap junction channels.

Rapid and direct effects of pH on connexins revealed by the connexin46 hemichannel preparation.

pH is a potent modulator of gap junction (GJ) mediated cell-cell communication. Mechanisms proposed for closure of GJ channels by acidification include direct actions of H+ on GJ proteins and indirect actions mediated by soluble intermediates. Here we report on the effects of acidification on connexin (Cx)46 cell-cell channels expressed in Neuro-2a cells and Cx46 hemichannels expressed in Xenopus oocytes. Effects of acidification on hemichannels were examined macroscopically and in excised patches that permitted rapid (<1 ms) and uniform pH changes at the exposed hemichannel face. Both types of Cx46 channel were found to be sensitive to cytoplasmic pH, and two effects were evident. A rapid and reversible closure was reproducibly elicited with short exposures to low pH, and a poorly reversible or irreversible loss occurred with longer exposures. We attribute the former to pH gating and the latter to pH inactivation. Half-maximal reduction of open probability for pH gating in hemichannels occurs at pH 6.4. Hemichannels remained sensitive to cytoplasmic pH when excised and when cytoplasmic [Ca2+] was maintained near resting ( approximately 10(-7) M) levels. Thus, Cx46 hemichannel pH gating does not depend on cytoplasmic intermediates or a rise in [Ca2+]. Rapid application of low pH to the cytoplasmic face of open hemichannels resulted in a minimum latency to closure near zero, indicating that Cx46 hemichannels directly sense pH. Application to closed hemichannels extended their closed time, suggesting that the pH sensor is accessible from the cytoplasmic side of a closed hemichannel. Rapid closure with significantly reduced sensitivity was observed with low pH application to the extracellular face, but could be explained by H+ permeation through the pore to reach an internal site. Closure by pH is voltage dependent and has the same polarity with low pH applied to either side. These data suggest that the pH sensor is located directly on Cx46 near the pore entrance on the cytoplasmic side.

Long-chain n-alkanols and arachidonic acid interfere with the Vm-sensitive gating mechanism of gap junction channels.

Experiments were carried out on preformed cell pairs and induced cell pairs of an insect cell line (mosquito Aedes albopictus, clone C6/36). The coupling conductance, gj, was determined with the dual voltage-clamp method. Exposure of preformed cell pairs to lipophilic agents, such as long-chain n-alkanols (n-hexanol, n-heptanol, n-octanol, n-nonanol, n-decanol) or arachidonic acid, provoked a decrease in gj. Hyperpolarization of both cells led to a recovery of gj. Systematic studies revealed that this phenomenon is caused by a shift of the sigmoidal relationship gj(ss) = f(Vm) towards more negative values of Vm (where gj(ss) = conductance at steady-state; Vm = membrane potential). The shift was dose dependent, it developed with time and was reversible. The longer the hydrocarbon chain of n-alkanols, the lower was the concentration required to produce a given shift. Besides shifting the function gj(ss) = f(Vm), arachidonic acid decreased the maximal conductance, gj(max). Single-channel records gained from induced cell pairs revealed that the lipophilic agents interfere with the Vm-sensitive slow channel gating mechanism. Application provoked slow current transitions (transition time: 5-40 ms) between an open state of the channel (i.e. main state or residual state) and the closed state; subsequently, fast channel transitions (transition time: < 2 ms) involving the main state and the residual state ceased completely. Hyperpolarization of Vm or washout of the lipophilic agents gave rise to the inverse sequence of events. The single-channel conductances gammaj(main state) and gammaj(residual state) were not affected by n-heptanol. We conclude that long-chain n-alkanols and arachidonic acid interact with the Vm-sensitive gating mechanism.

Conductances and selective permeability of connexin43 gap junction channels examined in neonatal rat heart cells.

Myocytes from neonatal rat hearts were used to assess the conductive properties of gap junction channels by means of the dual voltage-clamp method. The experiments were carried out on three types (groups) of preparations: (1) induced cell pairs, (2) preformed cell pairs with few gap junction channels (1 to 3 channels), and (3) preformed cell pairs with many channels (100 to 200 channels) after treatment with uncoupling agents such as SKF-525A (75 micromol/L), heptanol (3 mmol/L), and arachidonic acid (100 micromol/L). In group 1, the first opening of a newly formed channel was slow (20 to 65 ms) and occurred 7 to 25 minutes after physical cell contact. The rate of channel insertion was 1.3 channels/min. Associated with a junctional voltage gradient (Vj), the channels revealed multiple conductances, a main open state [gamma(j)(main state)], several substates [gamma(j)(substates)], and a residual state [gamma(j)(residual state)]. On rare occasions, the channels closed completely. The same phenomena were observed in groups 2 and 3. The existence of gamma(j)(residual state) provides an explanation for the incomplete inactivation of the junctional current (Ij) at large values of Vj in cell pairs with many gap junction channels. The values of gamma(j)(main state) and gamma(j)(residual state) gained from groups 1, 2, and 3 turned out to be comparable and hence were pooled. The fit of the data to a Gaussian distribution revealed a narrow single peak for both conductances. The values of gamma(j) were dependent on the composition of the pipette solution. Solutions were as follows: (1) KCl solution, gamma(j)(main state)=96 pS and gamma(j)(residual state)=23 pS; (2) Cs+ aspartate solution, gamma(j)(main state)=61 pS and gamma(j)(residual state)=12 pS; and (3) tetraethylammonium+ aspartate solution, gamma(j)(main state)=19 pS and gamma(j)(residual state)=3 pS. The respective gamma(j)(main state)-to-gamma(j)(residual state) ratios were 4.2, 5.1, and 6.3. This indicates that the residual state restricts ion permeation more efficiently than does the main state. Transitions of Ij between open states (main open state, substates, and residual state) were fast (<2 ms), and transitions involving the closed state and an open state were slow (15 to 65 ms). This implies the existence of two gating mechanisms. The residual state may be regarded as the ground state of electrical gating controlled by Vj; the closed state, as the ground state of chemical gating.

Two distinct gating mechanisms in gap junction channels: CO2-sensitive and voltage-sensitive.

The chemical gating of single-gap junction channels was studied by the dual whole-cell voltage-clamp method in HeLa cells transfected with connexin43 (HeLa43) and in fibroblasts from sciatic nerves. Junctional current (Ij), single-channel conductance, and Ij kinetics were studied in cell pairs during CO2 uncoupling and recoupling at small transjunctional voltages (Vj < 35 mV: Vj gating absent) and at high Vj (Vj > 40 mV: Vj gating strongly activated). In the absence of Vj gating, CO2 exclusively caused Ij slow transitions from open to closed channel states (mean transition time: approximately 10 ms), corresponding to a single-channel conductance of approximately 120 pS. At Vj > 40 mV, Vj gating induced fast Ij flickering between open, gamma j(main state), and residual, gamma j(residual), states (transition time: approximately 2 ms). The ratio gamma j(main state)/gamma j(residual) was approximately 4-5. No obvious correlation between Ij fast flickering and CO2 treatment was noticed. At high Vj, in addition to slow Ij transitions between open and closed states, CO2 induced slow transitions between residual and closed states. During recoupling, each channel reopened by a slow transition (mean transition time: approximately 10 ms) from closed to open state (rarely from closed to residual state). Fast Ij flickering between open and residual states followed. The data are in agreement with the hypothesis that gap junction channels possess two gating mechanisms, and indicate that CO2 induces channel gating exclusively by the slow gating mechanism.

Biophysical properties of heterotypic gap junctions newly formed between two types of insect cells.

1. Cell pairs of the insect cell line Sf9 (Spodoptera frugiperda) were chosen to examine the electrical properties of gap junction channels. The dual voltage-clamp method was used to control the membrane potential of each cell (Vm,1 and Vm,2) and hence the junctional voltage gradient (Vj), and to measure intercellular current. 2. Studies with preformed pairs revealed that the gap junction conductance (gj) is controlled by a Vj- and a Vm-sensitive gate. At steady state, gj = f(Vj) was bell shaped and symmetrical (Boltzmann: Vj.0 = -54 and 55 mV, the normalized minimum conductance at large Vj values (gj,min) = 0.24 and 0.23, z = 5.5 and 6.1 for negative and positive Vj, respectively) and gj = f(Vm) was S shaped (Vm.0 = 13 mV, gj,min = 0, z = 1.5). 3. Single channels exhibited two conductances, a main state (gamma j,main) of 224 pS and a residual state (gamma j,residual) of 42 pS. 4. We conclude that gap junctions in Sf9 cells behave similarly to those in the insect cell line C6/36 (Aedes albopictus). 5. An induced cell pair approach was used to examine heterotypic gap junction channels between Sf9 cells and C3/36 cells. 6. Heterotypic channels showed a gamma j,main of 303 pS and a gamma j,residual of 45 and 64 pS, depending on whether the Sf9 cell or C6/36 cell was positive inside. 7. In heterotypic gap junctions, gj = f(Vj) was bell shaped and asymmetrical (gj was more sensitive to Vj when the C6/36 cell was positive inside) and gj = f(Vm) was S shaped (Vm,0 = 2 mV, gj,min = 0, z = 2.9). 8. We conclude that heterotypic channels possess a Vj- and Vm-sensitive gating mechanism. Vj gating involves two gates, one located in each hemi-channel. Vj gates are operated independently and close when the cytoplasmic aspect is made positive. 9. A comparison of homo- and heterotypic channel data suggests that docking of hemi-channels may affect channel gating, but not channel conductance.

Biophysical properties of gap junction channels formed by mouse connexin40 in induced pairs of transfected human HeLa cells.

A clone of human HeLa cells stably transfected with mouse connexin40 DNA was used to examine gap junctions. Two separate cells were brought into physical contact with each other ("induced cell pair") to allow insertion of gap junction channels and, hence, formation of a gap junction. The intercellular current flow was measured with a dual voltage-clamp method. This approach enabled us to study the electrical properties of gap junction channels (cell pairs with a single channel) and gap junctions (cell pairs with many channels). We found that single channels exhibited multiple conductances, a main state (gamma j(main state)), several substates (gamma j(substates)), a residual state (gamma j (residual state)), and a closed state (gamma j(closed state)). The gamma j(main state) was 198 pS, and gamma j(residual state) was 36 pS (temperature, 36-37 degrees C; pipette solution, potassium aspartate). Both properties were insensitive to transjunctional voltage, Vj. The transitions between the closed state and an open state (i.e., residual state, substate, or main state) were slow (15-45 ms); those between the residual state and a substate or the main state were fast (1-2 ms). Under steady-state conditions, the open channel probability, Po, decreased in a sigmoidal manner from 1 to 0 (Boltzmann fit: Vj,o = -44 mV; z = 6). The temperature coefficient, Q10, for gamma j(main state) and gamma j(residual state) was 1.2 and 1.3, respectively (p < 0.001; range 15-40 degrees C). This difference suggests interactions between ions and channel structure in case of gamma j(residual state). In cell pairs with many channels, the gap junction conductance at steady state, gj, exhibited a bell-shaped dependency from Vj (Boltzmann fit, negative Vj, Vj,o = -45 mV, gj(min) = 0.24; positive Vj, Vj,o = 49 mV, gj(min) = 0.26; z = 6). We conclude that each channel is controlled by two types of gates, a fast one responsible for Vj gating and involving transitions between open states (i.e., residual state, substates, main state), and a slow one involving transitions between the closed state and an open state.

Heterotypic gap junction channels (connexin26-connexin32) violate the paradigm of unitary conductance.

Human HeLa cells transfected with mouse DNA coding for connexin26 (Cx26) or connexin32 (Cx32) were used to examine the properties of heterotypic Cx26-Cx32 gap junction channels. Intercellular current flow was examined in induced cell pairs by means of the dual voltage-clamp method. We found that Cx26-Cx32 channels exhibit voltage-dependent conductances, gamma j: gamma j(main state) increases with increasing positivity at the cytoplasmic aspect of the Cx26 connexon and decreases with increasing negativity (slope: 32 pS/100 mV; gamma j(main state) reaches 48 pS as Vj approaches 0 mV); gamma j(residual state) with a similar Vj-dependence is present when the cytoplasmic end of Cx26 connexon is positive, but absent when it is negative. The single channel data provide an explanation for the asymmetric relationships between the gap junction conductance, gj, and Vj. The results are consistent with the notion that docking of two connexons co-determines the biophysical properties of a gap junction channel.

Voltage-dependent gating of single gap junction channels in an insect cell line.

De novo formation of cell pairs was used to examine the gating properties of single gap junction channels. Two separate cells of an insect cell line (clone C6/36, derived from the mosquito Aedes albopictus) were pushed against each other to provoke formation of gap junction channels. A dual voltage-clamp method was used to control the voltage gradient between the cells (Vj) and measure the intercellular current (Ij). The first sign of channel activity was apparent 4.7 min after cell contact. Steady-state coupling reached after 30 min revealed a conductance of 8.7 nS. Channel formation involved no leak between the intra- and extracellular space. The first opening of a newly formed channel was slow (25-28 ms). Each preparation passed through a phase with only one operational gap junction channel. This period was exploited to examine the single channel properties. We found that single channels exhibit several conductance states with different conductances gamma j; a fully open state (gamma j(main state)), several substates (gamma j(substates)), a residual state (gamma j(residual)) and a closed state (gamma j(closed)). The gamma j(main state) was 375 pS, and gamma j(residual) ranged from 30 to 90 pS. The transitions between adjacent substates were 1/7-1/4 of gamma j(main state). Vj had no effect on gamma j(main state), but slightly affected gamma j (residual). The lj transitions involving gamma j(closed) were slow (15-60 ms), whereas those not involving gamma j(closed) were fast (< 2 ms). An increase in Vj led to a decrease in open channel probability. Depolarization of the membrane potential (Vm) increased the incidence of slow transitions leading to gamma j(closed). We conclude that insect gap junctions possess two gates, a fast gate controlled by Vj and giving rise to gamma j(substates) and gamma j(residual), and a slow gate sensitive to Vm and able to close the channel completely.

Gap junction channels of insects exhibit a residual conductance.

Formation of gap junction coupled cell pairs was used to assess the basic properties of single gap junction channels. For this purpose, two single cells (clone C6/36, derived from larvae of an insect, Aedes albopictus) were maneuvered against each other to provoke gap junction channel insertion. Intercellular current flow was measured with a dual voltage-clamp method. Utilizing this approach, we were able to demonstrate that gap junction channels, after formation, do not close completely upon application of a transjunctional voltage gradient, Vj. Instead, they exhibit a residual conductance, gamma j(residual). On average, gamma j(residual) was 64 +/- 4 pS (n = 40). This corresponds to about 1/6 of the conductance of a fully open channel. The existence of gamma j(residual) explains the observation that the conductance of the entire gap junction, gj, decreases only partially at large Vj.

Temperature dependence of gap junction properties in neonatal rat heart cells.

Cell pairs of neonatal rat hearts were used to study the influence of temperature on the electrical properties of gap junctions. A dual voltage-clamp method was adopted, which allowed the voltage gradient between the cells to be controlled and the intercellular current flow to be measured. Cell pairs with normal coupling revealed a positive correlation between the conductance of the junctional membranes, gj, and temperature. Cooling from 37 degrees C to 14 degrees C led to a steeper decrease in gj, cooling from 14 degrees C to -2 degrees C to a shallower decrease (37 degrees C: gj = 48.3 nS; 14 degrees C: gj = 21.4 nS; -2 degrees C: gj = 17.5 nS), corresponding to a temperature coefficient, Q10, of 1.43 and 1.14 respectively. The existence of two Q10 values implies that gj may be controlled by enzymatic reactions. When gj was low, i.e. below 5 nS (conditions: low temperature; treatment with 3 mM heptanol), it showed voltage-dependent gating. This property was not visible when gj was large, i.e. 20-70 nS (conditions: high temperature; normal saline), presumably because of series resistances (pipette resistance). Cell pairs with weak intrinsic coupling and normally coupled cell pairs treated with 3 mM heptanol revealed a positive correlation between the conductance of single gap-junction channels, gamma j, and temperature (37 degrees C: 75.6 pS; -2 degrees C: 19.6 pS), corresponding to a Q10 of 1.41.

Multiple conductance states of newly formed single gap junction channels between insect cells.

Two cells of an insect cell line (Aedes albopictus, clone C6/36) were pushed together to form a cell pair while the intercellular current flow was monitored. This approach enabled us to study the formation of gap junction channels and explore their electrical properties. We found that the single channels exhibit multiple conductance states. The conductance of a fully open channel was 365 pS; the subconductance steps were 1/7 to 1/5 of the maximal conductance. The voltage gradient across the junction did not influence the conductance of fully open channels, but affected the dwell time at particular conductance states. The latter provides an explanation for the voltage-dependent conductance of gap junction membranes seen in these cells. The very first channel opening always was slow (15-50 ms), suggesting the involvement of a mechanism different from conventional channel gating.