108 research outputs found

    Structure and Anticipatory Movements of the S6 Gate in K v Channels

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    Palmitoylation Affects the Interaction of Animal Toxins with Sodium Channels

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    PRISMS 2009 Flow Diagram. Flow chart of data extraction process. (DOC 64 kb

    Stabilizing the Closed S6 Gate in the Shaker K v Channel Through Modification of a Hydrophobic Seal

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    The primary activation gate in K+ channels is thought to reside near the intracellular entrance to the ion conduction pore. In a previous study of the S6 activation gate in Shaker (Hackos et al., 2002), we found that mutation of V478 to W results in a channel that cannot conduct ions even though the voltage sensors are competent to translocate gating charge in response to membrane depolarization. In the present study we explore the mechanism underlying the nonconducting phenotype in V478W and compare it to that of W434F, a mutation located in an extracellular region of the pore that is nonconducting because the channel is predominantly found in an inactivated state. We began by examining whether the intracellular gate moves using probes that interact with the intracellular pore and by studying the inactivation properties of heterodimeric channels that are competent to conduct ions. The results of these experiments support distinct mechanisms underlying nonconduction in W434F and V478W, suggesting that the gate in V478W either remains closed, or that the mutation has created a large barrier to ion permeation in the open state. Single channel recordings for heterodimeric and double mutant constructs in which ion conduction is rescued suggest that the V478W mutation does not dramatically alter unitary conductance. Taken together, our results suggest that the V478W mutation causes a profound shift of the closed to open equilibrium toward the closed state. This mechanism is discussed in the context of the structure of this critical region in K+ channels

    Defining the Conductance of the Closed State in a Voltage-Gated K+ Channel

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    AbstractThe opening and closing of the ion conduction pathway in ion channels underlies the generation and propagation of electrical signals in biological systems. Although electrophysiological approaches to measuring the flow of ions in the open state have contributed profoundly to our understanding of ion permeation and gating, it remains unclear how much the ion-throughput rate decreases upon closure of the ion conduction pore. To address this fundamental question, we expressed the Shaker Kv channel at high levels and then measured macroscopic K+ currents at negative membrane voltages and counted the number of channels by quantifying the translocation of gating charge. Our results show that the conductance of the closed state is between 0 and 0.16 fS, or at least 100,000 times lower than for the open state of the channel, indicating that the flow of ions is very tightly regulated in this class of K+ channels

    Constitutive Activation of the Shaker Kv Channel

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    In different types of K+ channels the primary activation gate is thought to reside near the intracellular entrance to the ion conduction pore. In the Shaker Kv channel the gate is closed at negative membrane voltages, but can be opened with membrane depolarization. In a previous study of the S6 activation gate in Shaker (Hackos, D.H., T.H. Chang, and K.J. Swartz. 2002. J. Gen. Physiol. 119:521–532.), we found that mutation of Pro 475 to Asp results in a channel that displays a large macroscopic conductance at negative membrane voltages, with only small increases in conductance with membrane depolarization. In the present study we explore the mechanism underlying this constitutively conducting phenotype using both macroscopic and single-channel recordings, and probes that interact with the voltage sensors or the intracellular entrance to the ion conduction pore. Our results suggest that constitutive conduction results from a dramatic perturbation of the closed-open equilibrium, enabling opening of the activation gate without voltage-sensor activation. This mechanism is discussed in the context of allosteric models for activation of Kv channels and what is known about the structure of this critical region in K+ channels

    Secondary Structure and Gating Rearrangements of Transmembrane Segments in Rat P2X4 Receptor Channels

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    P2X receptors are cation selective channels that are activated by extracellular nucleotides. These channels are likely formed by three identical or related subunits, each having two transmembrane segments (TM1 and TM2). To identify regions that undergo rearrangement during gating and to probe their secondary structure, we performed tryptophan scanning mutagenesis on the two putative TMs of the rat P2X4 receptor channel. Mutant channels were expressed in Xenopus oocytes, concentration–response relationships constructed for ATP, and the EC50 estimated by fitting the Hill equation to the data. Of the 22 mutations in TM1 and 24 in TM2, all but one in TM1 and seven in TM2 result in functional channels. Interestingly, the majority of the functional mutants display an increased sensitivity to ATP, and in general these perturbations are more pronounced for TM2 when compared with TM1. For TM1 and for the outer half of TM2, the perturbations are consistent with these regions adopting α-helical secondary structures. In addition, the greatest perturbations in the gating equilibrium occur for mutations near the outer ends of both TM1 and TM2. Surface biotinylation experiments reveal that all the nonfunctional mutants traffic to the surface membrane at levels comparable to the WT channel, suggesting that these mutations likely disrupt ion conduction or gating. Taken together, these results suggest that the outer parts of TM1 and TM2 are helical and that they move during activation. The observation that the majority of nonconducting mutations are clustered toward the inner end of TM2 suggests a critical functional role for this region

    Scanning the Intracellular S6 Activation Gate in the Shaker K+ Channel

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    In Kv channels, an activation gate is thought to be located near the intracellular entrance to the ion conduction pore. Although the COOH terminus of the S6 segment has been implicated in forming the gate structure, the residues positioned at the occluding part of the gate remain undetermined. We use a mutagenic scanning approach in the Shaker Kv channel, mutating each residue in the S6 gate region (T469-Y485) to alanine, tryptophan, and aspartate to identify positions that are insensitive to mutation and to find mutants that disrupt the gate. Most mutants open in a steeply voltage-dependent manner and close effectively at negative voltages, indicating that the gate structure can both support ion flux when open and prevent it when closed. We find several mutant channels where macroscopic ionic currents are either very small or undetectable, and one mutant that displays constitutive currents at negative voltages. Collective examination of the three types of substitutions support the notion that the intracellular portion of S6 forms an activation gate and identifies V478 and F481 as candidates for occlusion of the pore in the closed state
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