Correlation analysis of gap junction lattice images.

Fourier averages of connexon images computed from low-irradiation electron micrographs of isolated negatively stained gap junction domains exhibited differences in stain distribution and connexon orientation. To analyze these polymorphic structures, correlation averaging methods were applied to images from negatively stained and frozen-hydrated specimens. For the negatively stained specimens, separate averages over two subsets of connexons with differing degrees of stain accumulation in the axial channel were obtained. Two populations of connexons with opposite skew orientations were distinguishable within a single junctional domain of a frozen-hydrated specimen. Correlation maps calculated using the left- and right-skewed references showed that the selected connexons tend to locally cluster. Using correlation methods to analyze packing disorder in a typical connexon lattice, we estimated the root-mean-square variation in the nearest neighbor pair separation to be approximately 11% of the lattice constant. Displacements of the connexons relative to each other increased with increasing pair separation in the lattice, rather like a liquid, although long-range orientation order was conserved as in a crystal. These results support the hypothesis that the hexagonal ordering of the connexons results from short-range repulsive forces.     

Two forms of isolated gap junctions

Gap junctions, containing regular hexagonal arrays of connexons, have been isolated from rat liver. The projected structures of these gap junctions have been studied to a resolution of 18 Å by electron microscopy of negatively stained samples. Two closely related forms of junction were produced that have different structures for the connexon, but the same hexagonal lattice constant. In one form the connexon is seen as a weakly contrasted annulus, which is broadest at the locations where other connexons come closest; in the other, the connexon is seen as a strongly contrasted annulus, which is broadest midway between the locations where other connexons come closest. The forms appear to reflect two configurations of the connexon subunits.     

Gap junction structures. VII. Analysis of connexon images obtained with cationic and anionic negative stains

Micrographs of isolated gap junction specimens, negatively stained with one molybdate, three tungstate and three uranyl stains, were recorded at low and high irradiation. Fourier-averaged images of the negatively stained gap junctions have been self-consistently scaled to identify conserved and variable features. Intrinsic features in the hexagonally averaged images have been distinguished from residual noise by statistical comparisons among similarly prepared specimens. The cationic uranyl stains can penetrate the axial connexon channel, whereas the anionic stains are largely excluded; these observations indicate that the channel is negatively charged. Variability in the extent of the axial stain penetration, and enhancement of this staining by radiation damage and heating may be accounted for by a leaky, labile channel gate. The peripheral stain concentrations marking the perimeter of the skewed, six-lobed connexon image and the stain-excluding region at the 3-fold axis of the lattice, which are seen only under conditions of low irradiation with both anionic and cationic stains, are identified as intrinsic features of the isolated gap junction structure. The stain concentrations located approximately 30 A from the connexon center appear to be symmetrically related on opposite sides of the junction by non-crystallographic 2-fold axes oriented approximately 8 degrees to the lattice axes at the plane of the gap. The radiation-sensitive hexagonal features seen in the negatively stained images may correspond to substructure on the cytoplasmic surfaces of the paired gap junction membranes.     

Gap junction structures. VIII. Membrane cross-sections.

Profiles of negatively stained gap junctions have been measured by grid sectioning. After normal levels of electron irradiation, the membrane thickness shrinks to about half that of unirradiated controls, but no shrinkage occurs in the hexagonal lattice plane. Even under low irradiation conditions, there is significant thinning of the membranes. Edge views, in which rows of connexons are aligned parallel to the beam, were obtained from grid sections, folds in normal negatively stained specimens, and sections of a positively stained specimen. Averaging these micrographs with the translational and mirror symmetry of the projected lattice image displays conserved and variable features in the stain distribution of different specimens. Variations in the relative amount of negative stain in the gap at the surfaces and in the channel are uncorrelated with the irradiation but appear to depend on the local staining conditions and the integrity of the connexons. The dimensions measured from previously unirradiated grid sections, folds, and positively stained sections are in accord with x-ray diffraction measurements. Radiation-induced shrinkage can be accounted for by mass loss principally from the membrane bilayer. Disordering of the surface structure appears to be correlated with the radiation sensitivity of the bilayer; in contrast, the gap structure is well preserved under a variety of conditions.     

On gap junction structure

We have studied the stain distribution within rat liver gap junctions for specimens prepared by thin sectioning and negative staining. Pools of stain molecules exist in two specific locations with respect to the distinctive morphological units (connexons) of the junction. One pool of stain surrounds the connexons and is restricted to the extracellular space in the gap between the adjacent plasma membranes. The other pool of stain is located along in the central axis of each connexon, measures 1-2 nm in diameter and 4-5 nm in length, and is restricted to the gap region. On rare occasions, barely discernible linear densities seem to extend from this latter pool of stain and traverse the entire width of the junction. The data indicate the existence of a hydrophilic cavity along the central axis of te connexon which, in most instances, is restricted to the gap region. However, the precise depth to which this cavity may further extend along the connexon axis is still uncertain.     

Gap junction structures. I. Correlated electron microscopy and x-ray diffraction

X-ray crystallographic methods and electron microscope image analysis have been used to correlate the structure and the chemical composition of gap junction plaques isolated intact from mouse liver. The requirement that the interpretations of X-ray, electron microscope, and chemical measurements be consistent reduces the uncertainties inherent in the separate observations and leads to a unified picture of the gap junction structures. Gap junctions are built up of units called connexons that are hexagonally arrayed in the pair of connected cell membranes. X-ray diffraction and electron microscope measurements show that the lattice constant of this array varies from about 80 to 90 A. Analysis of electron micrographs of negatively stained gap junctions shows that there is significant short range disorder in the junction lattice. even though the long range order of the array is remarkably regular. Analysis of the disorder provides information about the nature of the intermolecular forces that hold the array together.     

Reversible structure transition in gap junction under Ca++ control seen by high-resolution electron microscopy.

Deoxycholate-extracted rat liver gap junction was studied by high-resolution low-dose electron microscopy. Communicating channels between two adjoining cells supposedly form along the common axis of two apposed hexameric trans-membrane protein assemblies. These double hexamers are often arranged in large plaques on an ordered hexagonal net (8-9 nm lattice constant) and seem able to undergo structural alteration as a possible permeability control mechanism. Calcium is widely reported to uncouple gap junction, and we observed this alteration on exposure to Ca++ down to 10(-4) M concentration. When EGTA was added at matching concentrations, the alteration was reversible several times over one hour, but with considerable variability. It was imaged in the absence of any negative stain to avoid ionic and other complications. The resulting lack of contrast plus low-dose "shot" noise required digital Fourier filtering and reconstruction, but no detail was recovered below 1.8 nm. In other experiments with negative stain at neutral pH, gap junction connexons were apparently locked in the "closed" configuration and no transition could be induced. However, recovery of repeating detail to nearly 1.0 nm was possible, reproducibly showing a fine connective matrix between connexons . Whether this was formed by unfolded portions of the 28,000-dalton gap junction protein is not known, but its existence could explain the observed lattice invariance during the connexon structural transition.     

Organization of connexons in isolated rat liver gap junctions.

Gap junction plaques from rat liver plasma membranes have been subjected to a range of detergent treatments in order to evaluate systematically the influence of different isolation procedures on their structure. The separation of the connexons was found to vary depending on the conditions used. In the absence of detergent the center-to-center separation of the connexons is, on average, approximately 90 A, and they are arranged on a hexagonal lattice so that the symmetry of the double-layered structure approximates to p6m in projection (or p622 in three-dimensions). Exposure to increasing concentration of detergent reduces the connexon separation to values below 80 A. More severe detergent treatment leads to disintegration of the gap junction plaques. Specimens with center-to-center separations smaller than 86 A show progressively larger deviation from p6m symmetry, seen as apparent rotations of the connexon assemblies within the crystal lattice. This reorganization occurs with both ice-embedded and negatively-stained specimens, using ionic or nonionic detergents, and therefore is probably a packing readjustment caused by depletion of intervening lipid molecules.     

In vitro assembly of gap junctions.

Gap junction structures were assembled in vitro from octyl-beta-D-glucopyranoside-solubilized components of lens fiber cell membranes. Individual pore structures (connexons), short double-membrane structures, and other amorphous material were evident in the solubilized mixture. Following the removal of the detergent by dialysis, these connexons associated to form single- and double-layered, two-dimensional hexagonal arrays (unit cell size a = b = 8.5 nm). The formation of larger arrays was dependent on the lipid-to-protein ratio and the presence of Mg2+ ions. Crystallographic analysis of electron micrographs revealed that lens junctional connexons consisted of six subunits surrounding a stain-filled channel. Upon further detergent treatment, in vitro assembled gap junctions were insoluble and formed three-dimensional stacks while other components were solubilized. SDS-PAGE and mass data from scanning transmission electron microscopy strongly suggest that a 38-kDa polypeptide, which is a processed form of the lens specific gap junction protein MP70, is a major component of the arrays. The in vitro assembly of gap junctions opens new avenues for the structural analysis of gap junctions and for the study of the intermolecular interactions of connexons during junctional assembly.     

Three-dimensional structure of an invertebrate intercellular communicating junction

Gap junctions containing extensive, highly ordered crystalline arrays of hexagonally packed connexons have been isolated from the hepatopancreas of the arthropod, Homarus americanus (American lobster). The structure of such junctions has been studied to a resolution of approximately 25 A in three dimensions by electron microscopy of negatively stained specimens. The structure, which has the crystallographic symmetry of the two-sided plane group p6, reveals the connexon as an annular oligomer which projects approximately 30-45 A from the cytoplasmic surface. The stain-filled channel structure appears to be approximately 40-45 A wide in the extracellular region. Projection images of glucose-embedded specimens extend to a resolution of 10 A, and show a strong contrast from the connexon subunits. Overall the structure is quite similar to that of rat liver junctions, except that less stain is seen in the aqueous region of the gap and more surrounding the protrusions of the protein into the cytoplasm.     

Gap junction ultrastructure in rat liver parenchymal cells after in vivo ischemia

The ultrastructure of gap junctions between rat liver parenchymal cells has been studied after in vivo ischemia, with and without subsequent blood reflow. Freeze fracture replicas were analysed by electron microscopic observation, optical diffraction and morphometric analysis. In control specimens gap junction connexons were widely dispersed and arranged in nearly random fashion over nearly the whole junctional area, with only minute spots of hexagonal connexon arrangement. An ischemic period of 30 min, from which the vast majority of cells are capable of recovery after restoration of the blood supply, usually entails only a slight enlargement of the areas of hexagonally arranged connexons. After 120 min of ischemia without reflow, which results in necrosis of most parenchymal cells, all gap junctions showed a completely hexagonal arrangement of connexons. The numerical density of connexons after 30 and 120 min of ischemia without reflow was significantly higher than in controls, whereas after 30 min of ischemia followed by 2 h of reflow the numerical density had returned to control levels. A fully hexagonal arrangement of gap junction connexons, as occurs after longer periods of ischemia, seems to be related to irreversible cell damage and presumably to metabolic uncoupling of cells. This was preceded by an increase in the numerical density of connexons, which is probably a reversible phenomenon.     

Preparation,characterization, and structure of half gap junctional layers split with urea and EGTA

Gap junctions, collections of membrane channels responsible for intercellular communication, contain two paired hemichannels (also called connexons). We have investigated conditions for splitting the membrane pair using urea. We have developed a protocol which consistently splits the gap junction samples with 60–90% efficiency. Our results indicate that hydrophobic forces are important in holding the two connexons together but that Ca²⁺ ions are also important in the assembly of the membrane pair. Greater yields and better structural integrity of split junctions were obtained with a starting preparation of gap junctions which had been detergent treated. Image analysis of edge views of single connexon layers reveal an asymmetry in the appearance of the cytoplasmic and extracellular surface. Cryo-electron microscopy and image analysis of split junctions show that the packing and structural detail of membranes containing arrays of single connexons are the same as for intact junctions, and that the urea treatment causes no gross structural changes in the connexon assembly.The antibodies used to analyze the protein composition in our samples were the generous gift of Dr. David Paul. We thank Dr. Camillo Peracchia for sending us a preprint of his chapter on molecular mechanisms of connexon gating and docking which helped guide our thinking about interconnexon forces and John Badger for information on divalent cation sites in protein structure. We thank Amani Thomas-Yusuf for technical assistance. The photographic expertise of Marie Craig is gratefully acknowledged. This work was funded by National Institutes of Health GM43217 to G.E.S. and GM18974 to D.A.G.     

In vitro assembly of gap junctions

Gap junction structures were assembled in vitro from octyl-β- -glucopyranoside-solubilized components of lens fiber cell membranes. Individual pore structures (connexons), short double-membrane structures, and other amorphous material were evident in the solubilized mixture. Following the removal of the detergent by dialysis, these connexons associated to form single- and double-layered, two-dimensional hexagonal arrays (unit cell size a = B = 8.5 nm). The formation of larger arrays was dependent on the lipid-to-protein ratio and the presence of Mg²⁺ ions. Crystallographic analysis of electron micrographs revealed that lens junctional connexons consisted of six subunits surrounding a stain-filled channel. Upon further detergent treatment, in vitro assembled gap junctions were insoluble and formed three-dimensional stacks while other components were solubilized. SDS-PAGE and mass data from scanning transmission electron microscopy strongly suggest that a 38-kDa polypeptide, which is a processed form of the lens specific gap junction protein MP70, is a major component of the arrays. The in vitro assembly of gap junctions opens new avenues for the structural analysis of gap junctions and for the study of the intermolecular interactions of connexons during junctional assembly.     

On the structure of isolated junctions between communicating cells

Summary Gap junctions are specialized regions of contact between apposed plasma membranes of communicating cells. They are composed of hexagonally arranged units (connexons) embedded in plasma membranes and linked together in the extracellular space. The three-dimensional structure of the connexon, was obtained by Fourier analysis on specimens of isolated rat liver gap junctions. The connexon is an annular oligomer, composed of six subunits, that protrudes from both sides of the plasma membrane. The subunits are tangentially displaced about the connexon axis. A narrow channel is located along the connexon, axis spanning the thickness of the junction, but it is greatly reduced in the hydrophobic zones of the membranes. Two closely related forms of isolated gap junctions which have different connexon subunit structures but the same hexagonal lattice, were obtained. The transition between the two forms of communicating junctions seen in isolation is produced by radial inward motion of the connexon subunits near their cytoplasmic surfaces and a reduction of their inclination tangential to the 6-fold axis. Similar rearrangement of essentially rigid subunits embedded in the membrane could provide a mechanism for modulation of the junction permeability. Presented in the symposium on Molecular and Morphological Aspects of Cell-Cell Communication at the 31st Annual Meeting of the Tissue Culture Association, St. Louis, Missouri, June 1–5, 1980. This symposium was supported in part by Contract 263-MD-025754 from the National Cancer Institute and the Fogarty International Center. This work was supported by NH Grants 5P1GM23911-07 and 5T32-6M07403-04.     

In vitro formation of gap junction vesicles

A method is described that uses trypsin digestion combined with collagenase-hyaluronidase which produces a population of gap junction vesicles. The hexagonal lattice of subunits ("connexons") comprising the gapjunctions appears unaltered by various structural criteria and by buoyant density measurements. The gap junction vesciles are closed by either a single or a double profile of nonjunctional "membrane," which presents a smooth, particle-free fracture face. Horseradish peroxidase and cytochrome c studies have revealed that about 20% of the gap junction vesicles are impermeable to proteins 12,000 daltons or larger. The increased purity of the trypsinized junction preparation suggests that one of the disulfide reduction products of the gap-junction principal protein may be a nonjunctional contaminating peptide. The gap junction appears to be composed of a single 18,000-dalton protein, connexin, which may be reduced to a single 9,000-dalton peak. The number of peptides in this reduced peak are still unknown.     

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.     

Molecular modeling and mutagenesis of gap junction channels

Gap junction channels connect the cytoplasms of adjacent cells through the end-to-end docking of hexameric hemichannels called connexons. Each connexon is formed by a ring of 24 alpha-helices that are staggered by 30 degrees with respect to those in the apposed connexon. Current evidence suggests that the two connexons are docked by interdigitated, anti-parallel beta strands across the extracellular gap. The second extracellular loop, E2, guides selectivity in docking between connexons formed by different isoforms. There is considerably more sequence variability of the N-terminal portion of E2, suggesting that this region dictates connexon coupling. Mutagenesis, biochemical, dye-transfer and electrophysiological data, combined with computational studies, have suggested possible assignments for the four transmembrane alpha-helices within each subunit. Most current models assign M3 as the major pore-lining helix. Mapping of human mutations onto a C(alpha) model suggested that native helix packing is important for the formation of fully functional channels. Nevertheless, a mutant in which the M4 helix has been replaced with polyalanine is functional, suggesting that M4 is located on the perimeter of the channel. In spite of this substantial progress in understanding the structural biology of gap junction channels, an experimentally determined structure at atomic resolution will be essential to confirm these concepts.     

Connexon rearrangement in cardiac gap junctions: Evidence for cytoskeletal control?

Summary Using ultrarapid-freezing techniques and freezefracture electron microscopy, we report here a close association between cardiac gap junctions and specialized membrane domains containing regularly-spaced furrows. These specialized furrowed domains are observed only during periods of gap junction re-organisation (i.e., connexon redistribution) and may reflect the presence of underlying cytoskeletal elements controlling the position of connexons in the membrane.     

Gap junction connexon configuration in rapidly frozen myocardium and isolated intercalated disks

By using two ultrarapid freezing techniques, we have captured the structure of rat and rabbit cardiac gap junctions in a condition closer to that existing in vivo than to that previously achieved. Our results, which include those from fully functional hearts frozen in situ in the living animal, show that the junctions characteristically consist of multiple small hexagonal arrays of connexons. In tissue frozen 10 min after animal death, however, unordered arrays are common. Examination of junction structure at intervals up to 40 min after death reveals a variety of configurations including dispersed and close-packed unordered arrays, and hexagonal arrays. By use of an isolated intercalated disk preparation, we show that the configuration of cardiac gap junctions in vitro cannot be altered by factors normally considered to induce functional uncoupling. These experiments demonstrate that, contrary to the conclusions of some earlier studies (Baldwin, K. M., 1979, J. Cell Biol., 82:66-75; Peracchia, C., and L. L. Peracchia, 1980, J. Cell Biol., 87:708-718), the arrangement of gap junction connexons, in cardiac tissue at least, cannot be used as a reliable guide to the functional state of the junctions.