scholarly journals Interference Between Two Modulators of N-Type (CaV2.2) Calcium Channel Gating Charge Movement

2010 ◽  
Vol 98 (3) ◽  
pp. 15a
Author(s):  
Viktor Yarotskyy ◽  
Keith S. Elmslie
Keyword(s):  
Calcium Channel ◽  
Channel Gating ◽  
Charge Movement ◽  
Gating Charge

scholarly journals Nonlinear charge movement in mammalian cardiac ventricular cells. Components from Na and Ca channel gating.

1989 ◽  
Vol 94 (1) ◽  
pp. 65-93 ◽  
Author(s):  
B P Bean ◽  
E Rios
Keyword(s):  
Channel Gating ◽  
Cell Voltage ◽  
Na Channel ◽  
Charge Movement ◽  
Ca Channel ◽  
Gating Current ◽  
Channel Inactivation ◽  
Gating Charge ◽  
Ventricular Cells ◽  
Extra Charge

Intramembrane charge movement was recorded in rat and rabbit ventricular cells using the whole-cell voltage clamp technique. Na and K currents were eliminated by using tetraethylammonium as the main cation internally and externally, and Ca channel current was blocked by Cd and La. With steps in the range of -110 to -150 used to define linear capacitance, extra charge moves during steps positive to approximately -70 mV. With holding potentials near -100 mV, the extra charge moving outward on depolarization (ON charge) is roughly equal to the extra charge moving inward on repolarization (OFF charge) after 50-100 ms. Both ON and OFF charge saturate above approximately +20 mV; saturating charge movement is approximately 1,100 fC (approximately 11 nC/muF of linear capacitance). When the holding potential is depolarized to -50 mV, ON charge is reduced by approximately 40%, with little change in OFF charge. The reduction of ON charge by holding potential in this range matches inactivation of Na current measured in the same cells, suggesting that this component might arise from Na channel gating. The ON charge remaining at a holding potential of -50 mV has properties expected of Ca channel gating current: it is greatly reduced by application of 10 muM D600 when accompanied by long depolarizations and it is reduced at more positive holding potentials with a voltage dependence similar to that of Ca channel inactivation. However, the D600-sensitive charge movement is much larger than the Ca channel gating current that would be expected if the movement of channel gating charge were always accompanied by complete opening of the channel.

scholarly journals Molecular Action of Lidocaine on the Voltage Sensors of Sodium Channels

2003 ◽  
Vol 121 (2) ◽  
pp. 163-175 ◽  
Author(s):  
Michael F. Sheets ◽  
Dorothy A. Hanck
Keyword(s):  
Channel Gating ◽  
Ionic Current ◽  
Na Channel ◽  
Relative Reduction ◽  
Charge Movement ◽  
Charge Voltage ◽  
Voltage Sensors ◽  
Gating Charge ◽  
Voltage Dependent ◽  
Domain Iii

Block of sodium ionic current by lidocaine is associated with alteration of the gating charge-voltage (Q-V) relationship characterized by a 38% reduction in maximal gating charge (Qmax) and by the appearance of additional gating charge at negative test potentials. We investigated the molecular basis of the lidocaine-induced reduction in cardiac Na channel–gating charge by sequentially neutralizing basic residues in each of the voltage sensors (S4 segments) in the four domains of the human heart Na channel (hH1a). By determining the relative reduction in the Qmax of each mutant channel modified by lidocaine we identified those S4 segments that contributed to a reduction in gating charge. No interaction of lidocaine was found with the voltage sensors in domains I or II. The largest inhibition of charge movement was found for the S4 of domain III consistent with lidocaine completely inhibiting its movement. Protection experiments with intracellular MTSET (a charged sulfhydryl reagent) in a Na channel with the fourth outermost arginine in the S4 of domain III mutated to a cysteine demonstrated that lidocaine stabilized the S4 in domain III in a depolarized configuration. Lidocaine also partially inhibited movement of the S4 in domain IV, but lidocaine's most dramatic effect was to alter the voltage-dependent charge movement of the S4 in domain IV such that it accounted for the appearance of additional gating charge at potentials near −100 mV. These findings suggest that lidocaine's actions on Na channel gating charge result from allosteric coupling of the binding site(s) of lidocaine to the voltage sensors formed by the S4 segments in domains III and IV.

Comparison of the effects of BAY K 8644 on cardiac Ca2+ current and Ca2+ channel gating current

1992 ◽  
Vol 262 (2) ◽  
pp. H472-H477 ◽  
Author(s):  
R. W. Hadley ◽  
W. J. Lederer
Keyword(s):  
Ventricular Myocytes ◽  
Channel Gating ◽  
Bay K 8644 ◽  
Charge Movement ◽  
Gating Current ◽  
Inhibitory Effects ◽  
Open Probability ◽  
Charge Voltage ◽  
Gating Charge ◽  
Voltage Dependent

Effects of (-)-BAY K 8644 on Ca2+ channel function were studied in guinea pig ventricular myocytes. It was found that the compound has both voltage-dependent stimulatory and inhibitory effects on the Ca2+ current (ICa), in agreement with prior studies. The basis for these effects was studied by evaluating the effects of (-)-BAY K 8644 on the Ca2+ channel gating current. It was found that the voltage-dependent inhibitory effects of the drug on ICa could be well explained by similar reductions in the amount of gating charge moved. However, the stimulatory effect of (-)-BAY K 8644 on ICa could not be simply correlated with changes in the amount of gating charge moved. Although the drug produced a shift of the charge-voltage relationship to more negative potentials, the drug actually reduced the total amount of movable gating charge. Thus it could be demonstrated that there are membrane potentials where (-)-BAY K 8644 reduced the Ca2+ channel gating current while enhancing ICa. In addition, the drug was found to slow the decay of the gating current during repolarization. It seems likely that (-)-BAY K 8644 has a dual effect on Ca2+ channels: affecting both the voltage dependence of gating charge and the relationship between open probability and charge movement.

scholarly journals A Dipeptidyl Aminopeptidase–like Protein Remodels Gating Charge Dynamics in Kv4.2 Channels

2006 ◽  
Vol 128 (6) ◽  
pp. 745-753 ◽  
Author(s):  
Kevin Dougherty ◽  
Manuel Covarrubias
Keyword(s):  
Membrane Potentials ◽  
Charge Movement ◽  
Transmembrane Segment ◽  
Gating Currents ◽  
Voltage Sensing ◽  
Charge Voltage ◽  
Charge Dynamics ◽  
Gating Charge ◽  
Kv4 Channels ◽  
Dipeptidyl Aminopeptidase

Dipeptidyl aminopeptidase–like proteins (DPLPs) interact with Kv4 channels and thereby induce a profound remodeling of activation and inactivation gating. DPLPs are constitutive components of the neuronal Kv4 channel complex, and recent observations have suggested the critical functional role of the single transmembrane segment of these proteins (Zagha, E., A. Ozaita, S.Y. Chang, M.S. Nadal, U. Lin, M.J. Saganich, T. McCormack, K.O. Akinsanya, S.Y. Qi, and B. Rudy. 2005. J. Biol. Chem. 280:18853–18861). However, the underlying mechanism of action is unknown. We hypothesized that a unique interaction between the Kv4.2 channel and a DPLP found in brain (DPPX-S) may remodel the channel's voltage-sensing domain. To test this hypothesis, we implemented a robust experimental system to measure Kv4.2 gating currents and study gating charge dynamics in the absence and presence of DPPX-S. The results demonstrated that coexpression of Kv4.2 and DPPX-S causes a −26 mV parallel shift in the gating charge-voltage (Q-V) relationship. This shift is associated with faster outward movements of the gating charge over a broad range of relevant membrane potentials and accelerated gating charge return upon repolarization. In sharp contrast, DPPX-S had no effect on gating charge movements of the Shaker B Kv channel. We propose that DPPX-S destabilizes resting and intermediate states in the voltage-dependent activation pathway, which promotes the outward gating charge movement. The remodeling of gating charge dynamics may involve specific protein–protein interactions of the DPPX-S's transmembrane segment with the voltage-sensing and pore domains of the Kv4.2 channel. This mechanism may determine the characteristic fast operation of neuronal Kv4 channels in the subthreshold range of membrane potentials.

scholarly journals A gating charge interaction required for late slow inactivation of the bacterial sodium channel NavAb

2013 ◽  
Vol 142 (3) ◽  
pp. 181-190 ◽  
Author(s):  
Tamer M. Gamal El-Din ◽  
Gilbert Q. Martinez ◽  
Jian Payandeh ◽  
Todd Scheuer ◽  
William A. Catterall
Keyword(s):  
Sodium Channel ◽  
Sodium Channels ◽  
Late Phase ◽  
Membrane Potentials ◽  
Charge Movement ◽  
Slow Inactivation ◽  
Functional Studies ◽  
Voltage Gated Sodium Channels ◽  
Gating Charge ◽  
Charge Interaction

Voltage-gated sodium channels undergo slow inactivation during repetitive depolarizations, which controls the frequency and duration of bursts of action potentials and prevents excitotoxic cell death. Although homotetrameric bacterial sodium channels lack the intracellular linker-connecting homologous domains III and IV that causes fast inactivation of eukaryotic sodium channels, they retain the molecular mechanism for slow inactivation. Here, we examine the functional properties and slow inactivation of the bacterial sodium channel NavAb expressed in insect cells under conditions used for structural studies. NavAb activates at very negative membrane potentials (V1/2 of approximately −98 mV), and it has both an early phase of slow inactivation that arises during single depolarizations and reverses rapidly, and a late use-dependent phase of slow inactivation that reverses very slowly. Mutation of Asn49 to Lys in the S2 segment in the extracellular negative cluster of the voltage sensor shifts the activation curve ∼75 mV to more positive potentials and abolishes the late phase of slow inactivation. The gating charge R3 interacts with Asn49 in the crystal structure of NavAb, and mutation of this residue to Cys causes a similar positive shift in the voltage dependence of activation and block of the late phase of slow inactivation as mutation N49K. Prolonged depolarizations that induce slow inactivation also cause hysteresis of gating charge movement, which results in a requirement for very negative membrane potentials to return gating charges to their resting state. Unexpectedly, the mutation N49K does not alter hysteresis of gating charge movement, even though it prevents the late phase of slow inactivation. Our results reveal an important molecular interaction between R3 in S4 and Asn49 in S2 that is crucial for voltage-dependent activation and for late slow inactivation of NavAb, and they introduce a NavAb mutant that enables detailed functional studies in parallel with structural analysis.

scholarly journals Components of gating charge movement and S4 voltage-sensor exposure during activation of hERG channels

2013 ◽  
Vol 141 (4) ◽  
pp. 431-443 ◽  
Author(s):  
Zhuren Wang ◽  
Ying Dou ◽  
Samuel J. Goodchild ◽  
Zeineb Es-Salah-Lamoureux ◽  
David Fedida
Keyword(s):  
Mammalian Cells ◽  
Voltage Sensor ◽  
Delayed Rectifier ◽  
Charge Movement ◽  
Α Subunit ◽  
Time Constants ◽  
Gating Charge ◽  
Activation Gating ◽  
Pore Opening ◽  
Herg Channels

The human ether-á-go-go–related gene (hERG) K+ channel encodes the pore-forming α subunit of the rapid delayed rectifier current, IKr, and has unique activation gating kinetics, in that the α subunit of the channel activates and deactivates very slowly, which focuses the role of IKr current to a critical period during action potential repolarization in the heart. Despite its physiological importance, fundamental mechanistic properties of hERG channel activation gating remain unclear, including how voltage-sensor movement rate limits pore opening. Here, we study this directly by recording voltage-sensor domain currents in mammalian cells for the first time and measuring the rates of voltage-sensor modification by [2-(trimethylammonium)ethyl] methanethiosulfonate chloride (MTSET). Gating currents recorded from hERG channels expressed in mammalian tsA201 cells using low resistance pipettes show two charge systems, defined as Q1 and Q2, with V1/2’s of −55.7 (equivalent charge, z = 1.60) and −54.2 mV (z = 1.30), respectively, with the Q2 charge system carrying approximately two thirds of the overall gating charge. The time constants for charge movement at 0 mV were 2.5 and 36.2 ms for Q1 and Q2, decreasing to 4.3 ms for Q2 at +60 mV, an order of magnitude faster than the time constants of ionic current appearance at these potentials. The voltage and time dependence of Q2 movement closely correlated with the rate of MTSET modification of I521C in the outermost region of the S4 segment, which had a V1/2 of −64 mV and time constants of 36 ± 8.5 ms and 11.6 ± 6.3 ms at 0 and +60 mV, respectively. Modeling of Q1 and Q2 charge systems showed that a minimal scheme of three transitions is sufficient to account for the experimental findings. These data point to activation steps further downstream of voltage-sensor movement that provide the major delays to pore opening in hERG channels.

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