42 research outputs found

    I8Q mutation has distinct effects on AKv1 Inactivation.

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    <p>A) Inactivation of AKv1(I8Q) is much less complete that AKv1, similar to the IB region mutant AKv1(E2D). B) Inactivation midpoint for AKv1(I8Q) is predicted by the activation midpoint for AKv1(Ξ”2-5, I8Q) further showing that the regulation of activation by the IP region is retained during N-type inactivation of AKv1(E2x) channels. C) Despite less efficient inactivation block, the kinetics for inactivation of AKv1(I8Q) and AKv1(E2D) are not significantly different from AKv1. D) Despite similar inactivation levels and inactivation and recovery time courses, tail currents for AKv1(I8Q) show 2-exponential decay whereas AKv1(E2D) tail currents are single exponential.</p

    Identification the Inactivation Proximal (IP) Domain.

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    <p>A) Representative currents for N-terminal deletions. Removal of the initial 5 residues eliminates N-type inactivation. B) Activation midpoint for AKv1(Ξ”2-5) is shifted to a more negative midpoint compared to larger N-terminal Deletions AKv1(Ξ”2-14) and AKv1(Ξ”2-57). C) Deletion effects on activation midpoint identify the IP region between residues 5-14. D) Despite the shift in activation midpoint, AKv1(Ξ”2-5) closing kinetics and voltage dependence are similar to AKv1(Ξ”2-57). D) Using AKv1(Ξ”2-5) activation midpoint and slope from AKv1 inactivation accurately predicts inactivation midpoints for AKv1(E2x) mutant series (Model Prediction line).</p

    Slowed Closing produced by N-type Inactivation matches the voltage-dependence for normal channel closing.

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    <p>A) Time course for AKv1 tail currents matches the Inactivation recovery time course. B) Kinetics for normal closing measured in AKv1(Ξ”2-57) and recovery tails measured in AKv1 are voltage dependent. C) Comparing tail current closing rates from single exponential fits. Voltage-dependence for AKv1(Ξ”2-57) closing matches the voltage-dependence for AKv1 tail currents despite the dramatically different rates. D) Ratio of tail closing rates predicts a consistent value for K<sub>I</sub>. For wild type AKv1 this value is similar to K<sub>I</sub><sup>1</sup> measured from the fraction of current that is not inactivated at the end of a pulse.</p

    Identification of Conserved Motif in IP Domain.

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    <p>A) IP Domain retained in AKv1(Ξ”2-5) and deleted in AKv1(Ξ”2-14) contains a highly conserved [(A/V)-(G/S/C)-(H<sub>5</sub>)] Motif. Mutations to residue Leu7 from <i>Drosophila</i> ShB channel, highlighted in red, that make this residue more polar disrupt ShB N-type inactivation. B) AKv1(Ξ”2-5, I8Q) mutant shows expected non-inactivating currents. C) Activation Curve for AKv1(Ξ”2-5, I8Q) is shifted back to more positive potentials and matches AKv1(Ξ”2-57). D) Summary data showing deletions and mutations identifying the IP Domain and the disruption of IP Domain effects on activation by the I8Q mutation.</p

    <i>Drosophila Shaker</i> based Model Poorly Predicts AKv1 Steady State Inactivation.

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    <p>Best fit to AKv1(E2x) channel data is shown in black. While there is a trend in the data matching the prediction of the model, error bars for most data points do not contact the best fit line. The y-intercept of the best fit is significantly different from the activation midpoint for AKv1(Ξ”2-57).</p

    Slowed Closing predicts steady state inactivation midpoints for AKv1(E2x) series mutants.

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    <p>A) Best fit to AKv1(E2x) channel data is shown in black. Prediction for the steady state inactivation midpoints based on AKv1(Ξ”2-57) activation gating shown in orange. AKv1(E2x) data are well fit with a linear model (rβ€Š=β€Šβˆ’0.99); however, the y-intercept is more negative than expected and the slope is flatter than predicted from AKv1(Ξ”2-57) activation. B) Predicted value for k<sub>s</sub> from the fit is smaller than the activation curve k<sub>s</sub>, and similar to k<sub>s</sub> values measured from the inactivation curves, as expected from the more complex multi-step activation of the real channel.</p

    Modeling the Pre-Block Interaction.

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    <p>A) Minimal AKv1 N-type Inactivation gating scheme. AKv1 gating model is only slightly more complicated than the Single Step <i>Drosophila</i> Model (red states) because in addition to the <b>C</b>, <b>O</b> and <b>I</b> labels to indicate the pore state, a subscript is needed to indicate : <b>P</b>- the <b>P</b> site bound states (black states) that shift activation and enhances inactivation and, <b>W</b>- a separate <b>W</b>ithheld state (blue state), from which the IB region cannot directly access the pore block state. Rate constants k<sub>c</sub>(v) β€Š=β€Š40(βˆ’0.015) and k<sub>o</sub>(v) β€Š=β€Š1500(0.32) as described previously. Equilibrium constants and cooperativity factor Ξ± determined as described in the text. The model produces a reasonable fit for the steady state properties for AKv1, AKv1(I8Q), and AKv1(E2D) (with K<sub>I</sub> changed to 0.1). Accurate activation and inactivation kinetics at strong depolarizations requires additional steps along the red pathway to rate limit the kinetics. If direct closing from O<sub>P</sub> and O<sub>W</sub> open states is included using the same k<sub>c</sub>(v) value then closing and recovery kinetics for AKv1, AKv1(I8Q), and AKv1(E2D) channels at strong negative potentials can be reproduced with this model if the K<sub>I</sub> equilibrium is made rapid. B) Structural model of key regions involved in N-type inactivation based on the 3LUT structure of Kv1.2 <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0079891#pone.0079891-Chen1" target="_blank">[23]</a>. A tilted perspective (see inset upper right) of the channel showing the inner aqueous volume of the channel in gray. Residue Tyr417 is shown in red and the S4-S5 linker in green. Selectivity filter is marked by the locations of the potassium ions in purple. C) Internal aqueous volume of the channel seen from a side perspective divided into the pore inner vestibule (white) and the side window vestibule (green). Volumes of these regions are given in the matching color. A single subunit P region backbone trace from the S4-S5 linker to the end of the determined S6 structure is shown along with its residue Tyr417 (red) and S4-S5 linker (brown) highlighted. The S4-S5 linker from the adjacent subunit is close to Tyr417 and therefore is also shown. D) Same picture only rotated 90<sup>o</sup> to show the locations of Tyr417 and the S4-S5 linkers from 2 subunits relative to the pore inner vestibule and the side window vestibule. Both Tyr417 and the S4-S5 linkers are side window vestibule lining residues, not pore inner vestibule lining residues.</p

    <i>Drosophila Shaker</i> based Single-Step Model for N-type Inactivation.

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    <p>Model has 3 basic states: Closed (C), Open (O) and Inactivated (I). Relative occupancy of these three states at equilibrium is given by the Equilibrium constants: Voltage-Dependent Activation- K<sub>O</sub>(v), and Inactivation- K<sub>I</sub>. The rate limiting step for inactivation at strong positive potentials is the binding of the N-terminus into the pore, the k<sub>on</sub> rate, highlighted in red. The rate limiting step for recovery at strong negative potentials is the unbinding of the N-terminus from the pore block site, the k<sub>off</sub> rate, highlighted in orange. These same rate limiting steps are proposed to control Ball Peptide inactivation (Dashed), or for that matter pore block by long chain quaternary ammonium derivatives like C9. Note that the rate limiting steps are not inherently voltage dependent; however, some voltage dependence to the recovery rate could be due to electric field effects mediated in the pore by K<sup>+</sup> ions or charges on the ball peptide that accelerate unblocking, or re-blocking before closing that becomes less likely as k<sub>c</sub>(v) becomes faster.</p

    Conserved N-Terminal Negative Charges Support Optimally Efficient N-type Inactivation of Kv1 Channels

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    <div><p></p><p>N-type inactivation is produced by the binding of a potassium channel's N-terminus within the open pore, blocking conductance. Previous studies have found that introduction of negative charges into N-terminal inactivation domains disrupts inactivation; however, the Aplysia AKv1 N-type inactivation domain contains two negatively charged residues, E2 and E9. Rather than being unusual, sequence analysis shows that this N-terminal motif is highly conserved among Kv1 sequences across many phyla. Conservation analysis shows some tolerance at position 9 for other charged residues, like D9 and K9, whereas position 2 is highly conserved as E2. To examine the functional importance of these residues, site directed mutagenesis was performed and effects on inactivation were recorded by two electrode voltage clamp in Xenopus oocytes. We find that inclusion of charged residues at positions 2 and 9 prevents interactions with non-polar sites along the inactivation pathway increasing the efficiency of pore block. In addition, E2 appears to have additional specific electrostatic interactions that stabilize the inactivated state likely explaining its high level of conservation. One possible explanation for E2's unique importance, consistent with our data, is that E2 interacts electrostatically with a positive charge on the N-terminal amino group to stabilize the inactivation domain at the block site deep within the pore. Simple electrostatic modeling suggests that due to the non-polar environment in the pore in the blocked state, even a 1 Γ… larger separation between these charges, produced by the E2D substitution, would be sufficient to explain the 65Γ— reduced affinity of the E2D N-terminus for the pore. Finally, our studies support a multi-step, multi-site N-type inactivation model where the N-terminus interacts deep within the pore in an extended like structure placing the most N-terminal residues 35% of the way across the electric field in the pore blocked state.</p></div

    Model of Important Sites and Reaction Steps during N-type Inactivation.

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    <p>Structural model of the AKv1 channel showing the approximate locations of Sites 1, 2, and 3 along the internal aqueous pathway leading to the selectivity filter. Channel profile is taken from a slab cut from an AKv1 structural model showing a side window opening and the internal vestibule of the transmembrane pore. The 1.4 Γ… accessible surface map is colored according to electrostatic potential with red negative, white neutral, and blue positive. Schematic to the right lists the hypothesized locations of residues E2, E9 and D19 during different phases of the N-type inactivation cycle. The intensity of red indicates the approximate level of negative charge along the pathway relative to residues 161–3. Dashed vertical line indicates approximate location of the pore entry beyond which chain occupancy produces pore block. This picture provides an approximate explanation for the electrostatic coupling seen between these residues and 161–3 during the inactivation cycle. Precisely how this electrostatic field is actually experienced by any residue along the path will depend on the microenvironment of the N-terminal residue and the direction the residue is pointing relative to residues 161–3.</p
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