Voltage-dependent gating and single-channel conductance of adult mammalian atrial gap junctions

A microstructural model of reentry arising from focal breakthrough at sites of source-load mismatch in a central region of slow conduction

Regions of cardiac tissue that have a combination of focal activity and poor, heterogeneous gap junction coupling are often considered to be arrhythmogenic; however, the relationship between the properties of the cardiac microstructure and patterns of abnormal propagation is not well understood. The objective of this study was to investigate the effect of microstructure on the initiation of reentry from focal stimulation inside a poorly coupled region embedded in more well-coupled tissue. Two-dimensional discrete computer models of ventricular monolayers (1 × 1 cm) were randomly generated to represent heterogeneity in the cardiac microstructure. A small, central poorly coupled patch (0.40 × 0.40 cm) was introduced to represent the site of focal activity. Simulated unipolar electrogram recordings were computed at various points in the tissue. As the gap conductance of the patch decreased, conduction slowed and became increasingly complex, marked by fractionated electrograms with reduced amplitude. Near the limit of conduction block, isolated breakthrough sites occurred at single cells along the patch boundary and were marked by long cell-to-cell delays and negative deflections on electrogram recordings. The strongest determinant of the site of wavefront breakthrough was the connectivity of the brick wall architecture, which enabled current flow through small regions of overlapping cells to drive propagation into the well-coupled zone. In conclusion, breakthroughs at the size scale of a single cell can occur at the boundary of source-load mismatch allowing focal activations from slow conducting regions to produce reentry. These breakthrough regions, identifiable by distinct asymmetric, reduced amplitude electrograms, are sensitive to tissue architecture and may be targets for ablation.

Multidimensional atomic force microscopy: a versatile novel technology for nanopharmacology research

Nanotechnology is giving us a glimpse into a nascent field of nanopharmacology that deals with pharmacological phenomena at molecular scale. This review presents our perspective on the use of scanning probe microscopy techniques with special emphasis to multidimensional atomic force microscopy (m-AFM) to explore this new field with a particular emphasis to define targets, design therapeutics, and track outcomes of molecular-scale pharmacological interactions. The approach will be to first discuss operating principles of m-AFM and provide representative examples of studies to understand human health and disease at the molecular level and then to address different strategies in defining target macromolecules, screening potential drug candidates, developing and characterizing of drug delivery systems, and monitoring target–drug interactions. Finally, we will discuss some future directions including AFM tip-based parallel sensors integrated with other high-throughput technologies which could be a powerful platform for drug discovery.

Calcium-dependent Open/Closed Conformations and Interfacial Energy Maps of Reconstituted Hemichannels

Using an atomic force microscope, we have studied three-dimensional molecular topography and calcium-sensitive conformational changes of individual hemichannels. Full-length (non-truncated) Cx43 hemichannels (connexons), when reconstituted in lipid bilayer, appear as randomly distributed individual particles and clusters. They show a lack of preferential orientation of insertion into lipid membrane; in a single bilayer, connexons with protrusion of either the extracellular face or the large non-truncated cytoplasmic face are observed. Extracellular domains of these undocked hemichannels are structurally different from hemichannels in the docked gap junctional plaques examined after their exposure by force dissection or chemical dissection. Calcium induced a reversible change in the extracellular pore diameter. Hemichannels imaged in a physiological buffer with 1.8 mm Ca(+2) had the pore diameter of approximately 1.8 nm, consistent with the closed channel conformation. Reducing Ca(+2) concentration to approximately 1.4, 1, and 0 mm, which changes hemichannels from the closed to open conformation, increased the pore diameter to approximately 2.5 nm for approximately 27, 74, and 100% of hemichannels, respectively. Thus, open/close probability of the hemichannel appears to be [Ca(2+)]-dependent. Computational analysis of the atomic force microscopy phase mode imaging reveals a significantly higher interfacial energy for open hemichannels that results from the interactions between the atomic force microscope probe and the hydrophobic domains. Thus, hydrophobic extracellular domains of connexins regulate calcium-dependent conformational changes.

The electrical behaviour of rat connexin46 gap junction channels expressed in transfected HeLa cells

Pairs of human HeLa cells expressing rat connexin46 were used to study the electrical properties of gap junction channels with the dual voltage-clamp method. The steady-state conductance ( g(j,ss)) had a bell-shaped dependence on transjunctional voltage ( V(j)). The parameters of the Boltzmann fit were: V(j,0)=42 mV, g(j,min)=0.12, z=2.5 (pipette solution: K(+) aspartate(-); 27 degrees C). The Boltzmann parameters were sensitive to the ionic composition of the pipette solution (KCl, K(+) aspartate(-), TEA(+) Cl(-), TEA(+) aspartate(-)). The V(j)-dependent inactivation of the junctional current I(j) was approximated by single exponentials (exceptions: two exponentials with KCl at V(j)>or=75 mV and K(+) aspartate(-) at V(j)=125 mV). The time constant of inactivation (tau(i)) decreased with increasing V(j) and was sensitive to the pipette solution. The larger the ions, the slower the inactivation. Recovery from inactivation followed a single exponential. The time constant of recovery (tau(r)) increased with increasing V(j). Single-channel currents showed a main state, several substates and a residual state. The corresponding conductances gamma(j,main) and gamma(j,residual) decreased slightly with increasing V(j); extrapolation to V(j)=0 mV yielded values of 152 and 28 pS, respectively (K(+) aspartate(-); 37 degrees C). The values of gamma(j,main) and gamma(j,residual) were dependent on pipette solution. The ratio gamma(j,main)/gamma(j,residual) increased with increasing ionic size, suggesting that the residual state impairs ion permeation more severely than the main state. The gamma(j,main) data suggest that the ionic selectivity of Cx46 channels may be controlled primarily by ionic size. Compared with hemichannel results, docking of connexons may modify the channel structure and thereby affect the ionic selectivity of gap junction channels. The open channel probability at steady state ( P(o)) decreased with increasing V(j). The parameters of the Boltzmann fit were: V(j,0)=41 mV, z=2.2 (K(+) aspartate(-); 27 degrees C).

Osmotic forces and gap junctions in spreading depression: a computational model

In a computational model of spreading depression (SD), ionic movement through a neuronal syncytium of cells connected by gap junctions is described electrodiffusively. Simulations predict that SD will not occur unless cells are allowed to expand in response to osmotic pressure gradients and K+ is allowed to move through gap junctions. SD waves of [K+]out approximately 25 to approximately 60 mM moving at approximately 2 to approximately 18 mm/min are predicted over the range of parametric values reported in gray matter, with extracellular space decreasing up to approximately 50%. Predicted waveform shape is qualitatively similar to laboratory reports. The delayed-rectifier, NMDA, BK, and Na+ currents are predicted to facilitate SD, while SK and A-type K+ currents and glial activity impede SD. These predictions are consonant with recent findings that gap junction poisons block SD and support the theories that cytosolic diffusion via gap junctions and osmotic forces are important mechanisms underlying SD.

Molecular dissection of transjunctional voltage dependence in the connexin-32 and connexin-43 junctions

Most gap junction channels are sensitive to the voltage difference between the two cellular interiors, termed the transjunctional voltage (V(j)). In several junctions, the conductance transitions induced by V(j) show more than one kinetic component. To elucidate the structural basis of the fast and slow components that characterize the V(j )dependence of connexin-32 (Cx32) and connexin-43 (Cx43) junctions, we created deletions of both connexins, where most of the carboxy-terminal (CT) domain was removed. The wild-type and "tailless" mutants were expressed in paired Xenopus oocytes, and the macroscopic gating properties were analyzed using the dual voltage clamp technique. Truncation of the CT domain of Cx32 and Cx43 abolished the fast mechanism of conductance transitions and induced novel gating properties largely attributable to the slow mechanism of gating. The formation of hybrid junctions comprising wild-type and truncated hemichannels allowed us to infer that the fast and slow components of gating reside in each hemichannel and that both gates close at a negative V(j) on the cytoplasmic side. Thus we conclude that the two kinetic components of V(j)-sensitive conductance are a result of the action of two different gating mechanisms. They constitute separate structures in the Cx32 and Cx43 molecules, the CT domain being an integral part of fast V(j) gating.

Cardiac ionic currents and acute ischemia: from channels to arrhythmias

The aim of this review is to provide basic information on the electrophysiological changes during acute ischemia and reperfusion from the level of ion channels up to the level of multicellular preparations. After an introduction, section II provides a general description of the ion channels and electrogenic transporters present in the heart, more specifically in the plasma membrane, in intracellular organelles of the sarcoplasmic reticulum and mitochondria, and in the gap junctions. The description is restricted to activation and permeation characterisitics, while modulation is incorporated in section III. This section (ischemic syndromes) describes the biochemical (lipids, radicals, hormones, neurotransmitters, metabolites) and ion concentration changes, the mechanisms involved, and the effect on channels and cells. Section IV (electrical changes and arrhythmias) is subdivided in two parts, with first a description of the electrical changes at the cellular and multicellular level, followed by an analysis of arrhythmias during ischemia and reperfusion. The last short section suggests possible developments in the study of ischemia-related phenomena.

Hippocampal connexin 43 expression in human complex partial seizure disorder

An increase in the cellular production of gap junction proteins and increased numbers of gap junctions in the neuronoglial syncytium of an epileptic focus have been proposed as a possible mechanism underlying synchronization of discharge. To study this issue, both Northern and Western blot analyses of the gap junction protein connexin 43 mRNA and protein abundance were performed on hippocampal tissue resected from patients presenting with a complex partial seizure disorder arising from the medial temporal area and the hippocampus in particular. Samples from 15 patients with medically intractable seizures were compared to those from 5 nonepileptic patients requiring temporal lobectomy in life-threatening situations. Six of the 15 epileptic patients underwent noninvasive electrographic recording, whereas the remaining 9 patients required intracerebral electrodes for extraoperative recording and therefore showed a more discrete focality than the noninvasive recordings. A decline in the mean levels of connexin 43 mRNA expressed predominantly in astrocytes was noted in the epileptic patient groups, particularly for those cases requiring intracranial electrode placement where ictal onset was more clearly established to be intrahippocampal. Quantitation of connexin 43 protein in both epileptogenic and nonepileptogenic hippocampal tissues showed no significant differences in expression. Although mean values for mRNA showed a decline, clinical outcomes postoperatively showed no correlation with either mRNA or protein expression individually in our epileptic population. The findings indicate that there is effectively no upregulation of mRNA and no increased production of connexin 43 protein in response to the development of epileptogenicity. Rather it appears the influence of gap junctions as a substrate of epileptogenicity in any mechanism(s) underlying synchrony or electrical propagation may be a function of the dynamic state (open versus closed) of the membrane-bound gap junction.

Gap junction channel gating at bass retinal electrical synapses

To further characterize the properties of retinal horizontal cell electrical synapses, we have studied the gating characteristics of gap junctions between cone-driven horizontal cells from the hybrid striped bass retina using double whole-cell voltage-clamp techniques. In a total of 105 cell pairs, the macroscopic conductance ranged from 0.4-100 nS with most cell pairs exhibiting junctional conductances between 10 and 30 nS. The junctional current-voltage relationship showed that peak or instantaneous currents (Iinst) were linear within the Vj range of +/- 100 mV and that steady-state junctional currents (Iss) exhibited rectification with increasing voltage beginning around +/- 30-40 mV Vj. The normalized junctional current-voltage relationship was well fit by a two-state Boltzmann distribution, with an effective gating charge of 1.9 charges/channel, a half-maximal voltage of approximately +/- 55 mV, and a normalized residual conductance of 0.28. The decay of junctional current followed a single exponential time course with the time constant decreasing with increasing Vj. Recovery of junctional current from voltage-dependent inactivation takes about 1 s following a pulse of 80 mV, and is about five times slower than the inactivation time course at the same Vj. Single-channel analysis showed that the unitary conductance of junctional channels is 50-70 pS. The overall open probability decreased in a voltage-dependent manner. Both the mean channel open time and the frequency of channel opening decreased, while the channel closure time increased. The ratio of closed time/total recording time significantly increased as Vj increased. Increased Vj reduced the number of events at all levels and shifted the unitary conductance to a lower level. Kinetic analysis of channel open duration showed that the distribution of channel open times was best fit by two exponentials and increased Vj significantly reduced the slower time constant. These results indicate that bass retina horizontal cells exhibit voltage-dependent inactivation of macroscopic junctional current. The inactivation occurs at the single-channel level mainly by increasing the rate of closure of voltage-sensitive channels.

Connexin43 gap junctions exhibit asymmetrical gating properties

A communication-deficient cell line (RIN cells, derived from a rat islet tumour), stably transfected with cDNA coding for rat connexin43 (Cx43), was chosen to further assess the mechanism of voltage gating of Cx43 gap junction channels. The experiments were carried out on preformed cell pairs using a dual whole-cell, voltage-clamp method. The junctional current, Ij, revealed a time- and voltage-dependent inactivation at transjunctional voltages Vj>+/-40 mV. When an asymmetrical pulse protocol was used (in cell 1 the holding potential was maintained, in cell 2 it was altered to establish a variable Vj), the channels exhibited an asymmetrical gating behaviour: Vj,0=-73.7 mV and 65.1 mV for negative and positive Vj, respectively (Vj at which Ij is half-maximally inactivated); gj(min)=0.34 and 0.29 (normalized minimal conductance); tau = 350 ms and 80 ms at Vj=100 mV (time constant of Ij inactivation). Hence, these parameters were more sensitive to positive Vj values. When a symmetrical pulse protocol was used (the holding potentials in cell 1 and cell 2 were altered simultaneously in steps of equal amplitude but of opposite polarity), the Vj -dependent asymmetries were absent: Vj,0=-60.5 and 59.5; gj (min)=0.27 and 0.29; tau =64 ms and 47 ms at 100mV. Putative explanations for these observations are discussed. A possibility is that the number of channels alters with the polarity of Vj.

Characterization of gap junctions between pairs of Leydig cells from mouse testis

Leydig cells are coupled in vivo by numerous gap junctions. In vivo and in vitro cells were immunolabeled by connexin 43 (Cx43) but not by Cx26 or Cx32 antibodies; immunoblotting confirmed specificity of Cx43 labeling. Pairs of Leydig cells dissociated from mouse testis were studied by dual whole cell voltage clamp, and a high incidence of dye (n = 20) and electrical coupling (n = 60; > 90%) was found. Coupling coefficients were near 1 and junctional conductance (gj) averaged 7.2 +/- 1.2 nS (SE, n = 40). Large transjunctional voltage (Vj) decreased gj; currents decayed exponentially with time constants of seconds that decreased at greater Vj. The residual conductance at large Vj was at least approximately 40% of the initial conductance. Exposure of cell pairs to saline solutions saturated with CO2 (n = 15) or containing 2 mM halothane (n = 15) or 3.5 mM heptanol (n = 15) rapidly and reversibly reduced gj. In eight cell pairs, gating of single junctional channels was observed during halothane-induced reduction in gj. Most gating events at Vj < 40 mV were fit by a Gaussian distribution with a mean of approximately 100 pS. With Vj > 40 mV, smaller transitions of approximately 30 pS were also recorded, and the frequency and duration of the approximately 100-pS transitions decreased. Also, approximately 70-pS transitions between 30- and 100-pS conductances were observed in the absence of 70-pS transitions to or from the baseline, indicating that the 30-pS conductance was a substate induced by large Vj.

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.

Gap junction gating sensitivity to physiological internal calcium regardless of pH in Novikoff hepatoma cells

Gap junction conductance (Gj) and channel gating sensitivity to voltage, Ca2+, H+, and heptanol were studied by double whole-cell clamp in Novikoff hepatoma cell pairs. Channel gating was observed at transjunctional voltages (Vj) > +/- 50 mV. The cells readily uncoupled with 1 mM 1-heptanol. With heptanol, single (gap junctional) channel events with unitary conductances (gamma j) of 46 and 97 pS were detected. Both Ca(2+)-loading (EGTA.Ca) and acidifying (100% CO2) solutions caused uncoupling. However, CO2 was effective when Ca2+i was buffered with EGTA (a H(+)-sensitive Ca-buffer) but not with BAPTA (1,2-bis(2-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid) (a H(+)-insensitive Ca-buffer), suggesting a Ca(2+)-mediated H+ effect on gap junctions. This was tested by monitoring the Gj decay at different pCai values (9, 6.9, 6.3, 6, and 5.5; 1 mM BAPTA) and pHi values (7.2 or 6.1, 10 mM 4-(2-hydroxyethyl)-1-piperazineethanesulfonic acid and 2-(N-morpholino)ethansulphonic acid, respectively). With pCai > or = 6.9 (pH 7.2 or 6.1), Gj decreased to 10-70% of initial values in approximately 40 min, following single exponential decays (tau = approximately 28 min). With pCai 6-6.3 (pH 7.2 or 6.1), Gj decreased to 10-25% of initial values in 15 min (tau = approximately 5 min); the Student t gave a P = 0.0178. With pCa 5.5 the cells uncoupled in less than 1 min (tau = approximately 20 s). Low pHi affected neither time course nor shape of Gj decay at any pCai tested. The data indicate that these gap junctions are sensitive to [Ca2+]i in the physiological range (< or = 500 nM) and that low pHi, without an increase in [Ca2+]i, neither decreases Gj nor increases channel sensitivity to Ca2+.

Connexin40, a component of gap junctions in vascular endothelium, is restricted in its ability to interact with other connexins

The cellular distribution of connexin40 (Cx40), a newly cloned gap junction structural protein, was examined by immunofluorescence microscopy using two different specific anti-peptide antibodies. Cx40 was detected in the endothelium of muscular as well as elastic arteries in a punctate pattern consistent with the known distribution of gap junctions. However, it was not detected in other cells of the vascular wall. By contrast, Cx43, another connexin present in the cardiovascular system, was not detected in endothelial cells of muscular arteries but was abundant in the myocardium and aortic smooth muscle. We have tested the ability of these connexins to interact functionally. Cx40 was functionally expressed in pairs of Xenopus oocytes and induced the formation of intercellular channels with unique voltage dependence. Unexpectedly, communication did not occur when oocytes expressing Cx40 were paired with those expressing Cx43, although each could interact with a different connexin, Cx37, to form gap junction channels in paired oocytes. These findings indicate that establishment of intercellular communication can be spatially regulated by the selective expression of different connexins and suggest a mechanism that may operate to control the extent of communication between cells.