Gating of Connexin Channels by transjunctional-voltage: Conformations and models of open and closed states.

Voltage is an important physiologic regulator of channels formed by the connexin gene family. Connexins are unique among ion channels in that both plasma membrane inserted hemichannels (undocked hemichannels) and intercellular channels (aggregates of which form gap junctions) have important physiological roles. The hemichannel is the fundamental unit of gap junction voltage-gating. Each hemichannel displays two distinct voltage-gating mechanisms that are primarily sensitive to a voltage gradient formed along the length of the channel pore (the transjunctional voltage) rather than sensitivity to the absolute membrane potential (Vm or Vi-o). These transjunctional voltage dependent processes have been termed Vj- or fast-gating and loop- or slow-gating. Understanding the mechanism of voltage-gating, defined as the sequence of voltage-driven transitions that connect open and closed states, first and foremost requires atomic resolution models of the end states. Although ion channels formed by connexins were among the first to be characterized structurally by electron microscopy and x-ray diffraction in the early 1980's, subsequent progress has been slow. Much of the current understanding of the structure-function relations of connexin channels is based on two crystal structures of Cx26 gap junction channels. Refinement of crystal structure by all-atom molecular dynamics and incorporation of charge changing protein modifications has resulted in an atomic model of the open state that arguably corresponds to the physiologic open state. Obtaining validated atomic models of voltage-dependent closed states is more challenging, as there are currently no methods to solve protein structure while a stable voltage gradient is applied across the length of an oriented channel. It is widely believed that the best approach to solve the atomic structure of a voltage-gated closed ion channel is to apply different but complementary experimental and computational methods and to use the resulting information to derive a consensus atomic structure that is then subjected to rigorous validation. In this paper, we summarize our efforts to obtain and validate atomic models of the open and voltage-driven closed states of undocked connexin hemichannels. This article is part of a Special Issue entitled: Gap Junction Proteins edited by Jean Claude Herve.

Voltage-dependent gating of the Cx32*43E1 hemichannel: conformational changes at the channel entrances.

Voltage is an important parameter that regulates the open probability of both intercellular channels (gap junctions) and undocked hemichannels formed by members of the connexin gene family. All connexin channels display two distinct voltage-gating processes, termed loop- or slow-gating and V(j)- or fast-gating, which are intrinsic hemichannel properties. Previous studies have established that the loop-gate permeability barrier is formed by a large conformational change that reduces pore diameter in a region of the channel pore located at the border of the first transmembrane domain and first extracellular loop (TM1/E1), the parahelix (residues 42-51). Here, we use cadmium metal bridge formation to measure conformational changes reported by substituted cysteines at loci demarcating the intracellular (E109 and L108) and extracellular (Q56) entrance of hemichannels formed by the Cx32 chimera (Cx32*43E1). The results indicate that the intracellular pore entrance narrows from ∼15 Što ∼10 Šwith loop-gate but not apparently with V(j)-gate closure. The extracellular entrance does not appear to undergo large conformational changes with either voltage-gating process. The results presented here combined with previous studies suggest that the loop-gate permeability is essentially focal, in that conformational changes in the parahelix but not the intracellular entrance are sufficient to prevent ion flux.

Voltage-dependent conformational changes in connexin channels.

Channels formed by connexins display two distinct types of voltage-dependent gating, termed V(j)- or fast-gating and loop- or slow-gating. Recent studies, using metal bridge formation and chemical cross-linking have identified a region within the channel pore that contributes to the formation of the loop-gate permeability barrier. The conformational changes are remarkably large, reducing the channel pore diameter from 15 to 20Å to less than 4Å. Surprisingly, the largest conformational change occurs in the most stable region of the channel pore, the 3(10) or parahelix formed by amino acids in the 42-51 segment. The data provide a set of positional constraints that can be used to model the structure of the loop-gate closed state. Less is known about the conformation of the V(j)-gate closed state. There appear to be two different mechanisms; one in which conformational changes in channel structure are linked to a voltage sensor contained in the N-terminus of Cx26 and Cx32 and a second in which the C-terminus of Cx43 and Cx40 may act either as a gating particle to block the channel pore or alternatively to stabilize the closed state. The later mechanism utilizes the same domains as implicated in effecting pH gating of Cx43 channels. It is unclear if the two V(j)-gating mechanisms are related or if they represent different gating mechanisms that operate separately in different subsets of connexin channels. A model of the V(j)-closed state of Cx26 hemichannel that is based on the X-ray structure of Cx26 and electron crystallographic structures of a Cx26 mutation suggests that the permeability barrier for V(j)-gating is formed exclusively by the N-terminus, but recent information suggests that this conformation may not represent a voltage-closed state. Closed state models are considered from a thermodynamic perspective based on information from the 3.5Å Cx26 crystal structure and molecular dynamics (MD) simulations. The applications of computational and experimental methods to define the path of allosteric molecular transitions that link the open and closed states are discussed. This article is part of a Special Issue entitled: The Communicating junctions, composition, structure and characteristics.

Precise, facile initial rate measurements.

Progress curve analysis has been used sparingly in studies of enzyme-catalyzed reactions due largely to the complexity of the integrated rate expressions used in data analysis. Using an experimental design that simplifies the analysis, the advantages and limitations of progress curve experiments are explored in a study of four different enzyme-catalyzed reactions. The approach involves relatively simple protocols, requires 20-25% of the materials, and provides 10- to 20-fold signal enhancements compared to analogous initial rate studies. Product inhibition, which complicates integrated rate analysis, was circumvented using cloned, purified enzymes that remove the products and draw the reaction forward. The resulting progress curves can be transformed into the equivalent of thousands of initial rate and [S] measurements and, due to the absence of product inhibition, are plotted in the familiar, linear double-reciprocal format. Allowing product to accumulate during a reaction produces a continuously changing substrate/product ratio that can be used as the basis for obtaining product inhibition constants and to distinguish among the three classical inhibition mechanisms. Algebraic models describing the double-reciprocal patterns obtained from such inhibition studies are presented. The virtual continuum of substrate concentrations that occurs during a progress curve experiment provides a nearly errorless set of relative concentrations that results in remarkably precise data; kinetic constant standard deviations are on the order of 0.5%.

Conformational changes in a pore-forming region underlie voltage-dependent "loop gating" of an unapposed connexin hemichannel.

The structure of the pore is critical to understanding the molecular mechanisms underlying selective permeation and voltage-dependent gating of channels formed by the connexin gene family. Here, we describe a portion of the pore structure of unapposed hemichannels formed by a Cx32 chimera, Cx32*Cx43E1, in which the first extracellular loop (E1) of Cx32 is replaced with the E1 of Cx43. Cysteine substitutions of two residues, V38 and G45, located in the vicinity of the border of the first transmembrane (TM) domain (TM1) and E1 are shown to react with the thiol modification reagent, MTSEA-biotin-X, when the channel resides in the open state. Cysteine substitutions of flanking residues A40 and A43 do not react with MTSEA-biotin-X when the channel resides in the open state, but they react with dibromobimane when the unapposed hemichannels are closed by the voltage-dependent "loop-gating" mechanism. Cysteine substitutions of residues V37 and A39 do not appear to be modified in either state. Furthermore, we demonstrate that A43C channels form a high affinity Cd2+ site that locks the channel in the loop-gated closed state. Biochemical assays demonstrate that A43C can also form disulfide bonds when oocytes are cultured under conditions that favor channel closure. A40C channels are also sensitive to micromolar Cd2+ concentrations when closed by loop gating, but with substantially lower affinity than A43C. We propose that the voltage-dependent loop-gating mechanism for Cx32*Cx43E1 unapposed hemichannels involves a conformational change in the TM1/E1 region that involves a rotation of TM1 and an inward tilt of either each of the six connexin subunits or TM1 domains.

Determinants of gating polarity of a connexin 32 hemichannel.

There is good evidence supporting the view that the transjunctional voltage sensor (V(j)-sensor) of Cx32 and other Group 1 connexins is contained within a segment of the N-terminus that contributes to the formation of the channel pore. We have shown that the addition of negatively charged amino acid residues at several positions within the first 10 amino acid residues reverses the polarity of V(j)-gating and proposed that channel closure is initiated by the inward movement of this region. Here, we report that positive charge substitutions of the 2nd, 5th, and 8th residues maintain the negative polarity of V(j)-gating. These data are consistent with the original gating model. Surprisingly, some channels containing combinations of positive and/or negative charges at the 2nd and 5th positions display bipolar V(j)-gating. The appearance of bipolar gating does not correlate with relative orientation of charges at this position. However, the voltage sensitivity of bipolar channels correlates with the sign of the charge at the 2nd residue, suggesting that charges at this position may have a larger role in determining gating polarity. Taken together with previous findings, the results suggest that the polarity V(j)-gating is not determined by the sign of the charge lying closest to the cytoplasmic entry of the channel, nor is it likely to result from the reorientation of an electrical dipole contained in the N-terminus. We further explore the mechanism of polarity determination by utilizing the one-dimensional Poisson-Nernst-Plank model to determine the voltage profile of simple model channels containing regions of permanent charge within the channel pore. These considerations demonstrate how local variations in the electric field may influence the polarity and sensitivity of V(j)-gating but are unlikely to account for the appearance of bipolar V(j)-gating.

Cysteine biosynthetic enzymes are the pieces of a metabolic energy pump.

Understanding the mechanisms of free energy transfer in metabolism is fundamental to understanding how the chemical forces that sustain the molecular organization of the cell are distributed. Recent studies of molecular motors (1-3) and ATP-driven proton transport (4-6) describe how chemical potential is transferred at the molecular level. These systems catalyze energy transfer through structural change and appear to be dedicated exclusively to their coupling tasks (7, 8). Here we report the discovery of a new class of energy-transfer system. It is a biosynthetic pump composed of cysteine biosynthesis enzymes, ATP sulfurylase and O-acetylserine sulfhydrylase, each with its own catalytic function and from whose interactions emerge new function: the hydrolysis of ATP. The hydrolysis is kinetically and energetically linked to the chemistry catalyzed by ATP sulfurylase, the first enzyme in the cysteine biosynthetic pathway, in such a way that each molecule of ATP hydrolyzed, each stroke of the pump, produces 1 equivalent of that enzyme's product. These findings integrate cysteine metabolism and broaden our understanding of the ways in which higher order allostery is used to effect free energy transfer.