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Bezanilla, F.

Publications and source records attributed to Bezanilla, F..

9 recordsLinked to original sources

Mechanistical and structural basis of Kv channel inhibition by 4 aminopyridine

Inhibition of Kv channels by 4-aminopyridine (4AP) improves motor function in multiple sclerosis by enhancing neuronal excitability. The mechanism of inhibition and the structural basis of 4AP binding to Kv channels remain unclear. Here, we determined the structure of the Shaker V369I-I372L-S376T (ILT) mutant bound to 4AP at 3.3 [A], demonstrating that 4AP binds to the closed state of the channel. This structure is inconsistent with an open channel block mechanism. Electrophysiology experiments show that 4AP binds even when intracellular pore access is constitutively blocked, suggesting that 4AP enters the pore through membrane-facing fenestrations. MD simulations and mutational analysis agree with the proposed fenestration pathway and suggest that 4AP binds in its neutral form. These results support a mechanism where 4AP binds to a partially activated closed state that prevents complete activation of Kv channels, explaining its pharmacological activity.

biophysics↗

Molecular Basis of Sodium Channel Inactivation

Voltage-gated sodium channels initiate action potentials and control electrical signaling throughout the animal kingdom. Fast inactivation is an essential auto-inhibitory mechanism and requisite component of sodium channel physiology. Recent structural and electrophysiological results are inconsistent with the canonical "ball and chain" model of fast inactivation thus necessitating an updated theoretical framework. Here, we use encoded fluorescence spectroscopy and high-resolution electrophysiology to capture key steps in the fast inactivation mechanism, from voltage-sensor activation to pore occlusion, an ultra-fast process which occurs in less than 2 milliseconds. Upon depolarization, activation of the domain IV voltage sensor initiates cytoplasmic DIII_DIV linker movement and quickly repositions the IFM motif into a hydrophobic pocket adjacent to the pore. This triggers a structural rearrangement of the pocket. The phenylalanine of the IFM motif contacts the pore-forming helices via a hydrophobic interaction with S6 of DIV and an aromatic/hydrophobic interaction with S6 of DIIII. These two interactions occur only after both S6 segments rotate, thus exposing the hydrophobic gate into the pore producing the fast inactivation. Based on the current results, we propose an alternative "lock and key" model to explain the molecular mechanism of fast inactivation.

biophysics↗

Closed State Structure of the Pore Revealed by Uncoupled Shaker K+ Channel

Voltage gated potassium (Kv) channels play key roles in numerous physiological processes from cellular excitability to immune response and are among the most important pharmaceutical targets. Despite recent advances in the structural determination of Kv channels, the closed state structure of strictly coupled Kv1 family remains elusive. Here, we captured the closed state structure of the pore in the Shaker potassium by uncoupling the voltage sensor domains from the pore domains. Ionic current, gating current and fluorescence measurements show that a conserved isoleucine residue in the S4-S5 linker region, plays a key role controlling the strength of the electromechanical coupling and the channel activation-deactivation equilibrium. Structural determination of completely uncoupled I384R mutant by single particle cryoEM revealed a fully closed pore in the presence of fully activated but non-relaxed voltage sensors. The putative conformational transitions from a fully open pore domain indicates a "roll and turn" movement along the whole length of the pore-forming S6 helices in sharp contrast to canonical gating models based on limited movements of S6. The rotational and translational movement posits two hydrophobic residues, one at inner cavity and the other at the bundle crossing region, directly at the permeation pathway, limiting the pore radius to less than 0.7[A]. Voltage clamp fluorimetry of wild type channel incorporating a fluorescent unnatural amino acid strongly supports the cryoEM structural model. Surprisingly, the selectivity filter was captured in a noncanonical state, unlike the previously described dilated or pinched filter conformations. With the present experiment results, we propose a new gating model for strictly coupled Kv1 channels and the molecular mechanism of interactions among different functional states.

biophysics↗

Turning a Kv channel into hot and cold receptor by perturbing its electromechanical coupling.

Voltage-dependent potassium channels (Kv) are extremely sensitive to membrane voltage and play a crucial role in membrane repolarization during action potentials. Kv channels undergo voltage-dependent transitions between closed states before opening. Despite all we have learned using electrophysiological methods and structural studies, we still lack a detailed picture of the energetics of the activation process. We show here that even a single mutation can drastically modify the temperature response of the Shaker Kv channel. Using rapid cell membrane temperature steps (Tsteps), we explored the effects of temperature on the ILT mutant (V369I, I372L, and S376T) and the I384N mutant. The ILT mutant produces a significant separation between the transitions of the voltage sensor domain (VSD) activation and the I384N uncouples its movement from the opening of the domain (PD). ILT and I384N respond to temperature in drastically different ways. In ILT, temperature facilitates the opening of the channel akin to a "hot" receptor, reflecting the temperature dependence of the voltage sensors last transition and facilitating VSD to PD coupling (electromechanical coupling). In I384N, temperature stabilizes the channel closed configuration analogous to a "cold" receptor. Since I384N drastically uncouples the VSD from the pore opening, we reveal the intrinsic temperature dependence of the PD itself. Here, we propose that the electromechanical coupling has either a "loose" or "tight" conformation. In the loose conformation, the movement of the VSD is necessary but not sufficient to efficiently propagate the electromechanical energy to the S6 gate. In the tight conformation the VSD activation is more effectively translated into the opening of the PD. This conformational switch can be tuned by temperature and modifications of the S4 and S4-S5 linker. Our results show that we can modulate the temperature dependence of Kv channels by affecting its electromechanical coupling.

biophysics↗

Photolipid excitation triggers depolarizing optocapacitive currents and action potentials

Optically-induced changes in membrane capacitance may regulate neuronal activity without requiring genetic modifications. Previously, they mainly relied on sudden temperature jumps due to light absorption by membrane-associated nanomaterials or water. Yet, nanomaterial targeting or the required high infrared light intensities obstruct broad applicability. Now, we propose a very versatile approach: photolipids (azobenzene-containing diacylglycerols) mediate light-triggered cellular de- or hyperpolarization. As planar bilayer experiments show, the respective currents emerge from millisecond-timescale changes in bilayer capacitance. UV light changes photolipid conformation, which awards embedding plasma membranes with increased capacitance and evokes depolarizing currents. They open voltage-gated sodium channels in cells, generating action potentials. Blue light reduces the area per photolipid, decreasing membrane capacitance and eliciting hyperpolarization. If present, mechanosensitive channels respond to the increased mechanical membrane tension, generating large depolarizing currents that elicit action potentials. Membrane self-insertion of administered photolipids and focused illumination allows cell excitation with high spatiotemporal control. HighlightsO_LIRapid photolipid photoisomerization generates optocapacitive currents in planar lipid bilayers and HEK293 cells. C_LIO_LIThese currents originate from photo-induced changes in membrane capacitance C_LIO_LIUV light-triggered membrane depolarization opens NaV1.3, evoking action potentials. C_LIO_LIBlue light-induced mechanosensitive channel opening gives rise to depolarizing currents, which may evoke NaV1.3-mediated action potentials. C_LI

biophysics↗

A Mechanistic Reinterpretation of Fast Inactivation in Voltage-Gated Na+ Channels

Fast Inactivation in voltage-gated Na+ channels plays essential roles in numerous physiological functions. The canonical hinged-lid model has long predicted that a hydrophobic motif in the DIII-DIV linker (IFM) acts as the gating particle that occludes the permeation pathway during fast inactivation. However, the fact that the IFM motif is located far from the pore in recent high-resolution structures of Nav+ channels contradicts this status quo model. The precise molecular determinants of fast inactivation gate once again, become an open question. Here, we provide a mechanistic reinterpretation of fast inactivation based on ionic and gating current data. In Nav1.4 the actual inactivation gate is comprised of two hydrophobic rings at the bottom of S6. These function in series and closing once the IFM motif binds. Reducing the volume of the sidechain in both rings led to a partially conductive inactivated state. Our experiments also point to a previously overlooked coupling pathway between the bottom of S6 and the selectivity filter.

biophysics↗

ION CHANNEL THERMODYNAMICS STUDIED WITH TEMPERATURE JUMPS MEASURED AT THE MEMBRANE

Perturbing the temperature of a system modifies its energy landscape thus providing a ubiquitous tool to understand biological processes. Here, we developed a framework to generate sudden temperature jumps (Tjumps) and sustained temperature steps (Tsteps) to study the temperature dependence of membrane proteins under voltage-clamp, while measuring the membrane temperature. Utilizing the melanin under the Xenopus laevis oocytes membrane as a photothermal transducer, we achieved short Tjumps up to 10 {o}C in less than 1.5 ms and constant Tsteps for durations up to 150 ms. We followed the temperature at the membrane with submillisecond time resolution by measuring the time-course of membrane capacitance, which is linearly related to temperature. We applied Tjumps in Kir 1.1b, which reveals a highly temperature-sensitive blockage relief and characterized the effects of Tsteps on the temperature-sensitive channels TRPM8 and TRPV1. These newly developed approaches provide a general tool to study membrane proteins thermodynamics.

biophysics↗

The trajectory of discrete gating charges in a voltage-gated potassium channel

Positively-charged amino acids respond to membrane potential changes to drive voltage sensor movement in voltage-gated ion channels, but determining the trajectory of voltage sensor gating charges has proven difficult. We optically tracked the movement of the two most extracellular charged residues (R1, R2) in the Shaker potassium channel voltage sensor using a fluorescent positively-charged bimane derivative (qBBr) that is strongly quenched by tryptophan. By individually mutating residues to tryptophan within the putative trajectory of gating charges, we observed that the charge pathway during activation is a rotation and a tilted translation that differs between R1 and R2 and is distinct from their deactivation pathway. Tryptophan-induced quenching of qBBr also indicates that a crucial residue of the hydrophobic plug is linked to the Cole-Moore shift through its interaction with R1. Finally, we show that this approach extends to additional voltage-sensing membrane proteins using the Ciona intestinalis voltage sensitive phosphatase (CiVSP).

biophysics↗

Metal bridge in S4 segment supports helix transition in Shaker channel

Voltage-gated ion channels play important roles in physiological processes, especially in excitable cells, where they shape the action potential. In S4-based voltage sensors voltage-gated channels, a common feature is shared: the transmembrane segment 4 (S4) contains positively charged residues intercalated by hydrophobic residues. Although several advances have been made in understating how S4 moves through a hydrophobic plug upon voltage changes, possible helix transition from -to 310-helix in S4 during activation process is still unresolved. Here, we have mutated several hydrophobic residues from I360 to F370 in the S4 segment into histidine, in i, i+3 and i, i+6 or i, i+4 and i, i+7 pairs, to favor 310- or -helical conformations, respectively. We have taken advantage that His can be coordinated by Zn+2 to promote metal ion bridges and we have found that the histidine introduced at position 366 (L366H) can interact with the introduced histidine at position 370 (stabilizing that portion of the S4 segment in -helical conformation). In presence of 20 M of Zn+2, the activation currents of L366H:F370H channels were slowed down by a factor of 3.5, the voltage-dependence is shifted by 10 mV towards depolarized potentials with no change on the deactivation time constant. Our data supports that by stabilizing a region of the S4 segment in -helical conformation a closed (resting or intermediate) state is stabilized rather than destabilizing the open (active) state. Taken together, our data indicates that the S4 undergoes -helical conformation to a short-lived different secondary structure transiently before reaching the active state in the activation process.\n\nSTATEMENT OF SIGNIFICANCEConformational transitions between -helix and 310-helix in the S4 segment of Shaker potassium channel during gating has been under debate. The present study shows the coordination by Zn2+ of a pair of engineered histidine residues (L366H:F370H) in the intermediate region of S4 in Shaker, favoring -helical conformation. In presence of 20M of Zn+2 the activation currents of L366H:F370H channels become slower, with 10 mV positive shift in the voltage-dependence and no effects on deactivation time constants suggesting a stabilization of a closed state rather than destabilization the open (active) state. Collectively, our data indicate that S4 undergoes secondary structure changes, including a short-lived secondary structure transition, when S4 moves from the resting to the active state during activation.

biophysics↗