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J Gen Physiol
2005 Sep 01;1263:205-12. doi: 10.1085/jgp.200509293.
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Localization of the activation gate of a voltage-gated Ca2+ channel.
Xie C
,
Zhen XG
,
Yang J
.
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Ion channels open and close in response to changes in transmembrane voltage or ligand concentration. Recent studies show that K+ channels possess two gates, one at the intracellular end of the pore and the other at the selectivity filter. In this study we determined the location of the activation gate in a voltage-gated Ca2+ channel (VGCC) by examining the open/closed state dependence of the rate of modification by intracellular methanethiosulfonate ethyltrimethylammonium (MTSET) of pore-lining cysteines engineered in the S6 segments of the alpha1 subunit of P/Q type Ca2+ channels. We found that positions above the putative membrane/cytoplasm interface, including two positions below the corresponding S6 bundle crossing in K+ channels, showed pronounced state-dependent accessibility to internal MTSET, reacting approximately 1,000-fold faster with MTSET in the open state than in the closed state. In contrast, a position at or below the putative membrane/cytoplasm interface was modified equally rapidly in both the open and closed states. Our results suggest that the S6 helices of the alpha1 subunit of VGCCs undergo conformation changes during gating and the activation gate is located at the intracellular end of the pore.
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16129771
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Figure 1. Pore-lining residues in S6. Amino acid sequence alignment of the four S6 segments in the Cav2.1 subunit and the M2/S6 segment of KcsA and Shaker K+ channels. Amino acid numbers are given on both sides. For Ca2+ channel S6 segments, the amino acid numbering defined in this study is shown on the top. Position 0 presumably represents the membrane/cytoplasm interface. Bold positions denote those that can be modified by internal MTSET. Underlined positions were studied in this work. For K+ channel M2/S6 segments, bold residues denote pore-lining positions defined either structurally or by MTS reagent accessibility. Arrow marks the M2/S6 bundle crossing.
Figure 2. Closed-state modification of a cysteine above the putative membrane/cytoplasm interface. (A) Voltage protocol for closed-state modification by internal MTSET and representative current traces. Current was evoked by a 20-ms test pulse before and after MTSET (1 mM) application. Voltage was held at â80 mV when MTSET was applied for 2 min and then washed out for 1 min. (B) An exemplar time course of closed-state modification of IIIS6-V9C. Each point represents the peak current evoked by the 20-ms test pulse. Pulsing was stopped during MTSET application and washout. (C) Cartoon of S5 and S6 transmembrane helices and P-loop in the closed state. The thiol group of a pore-lining cysteine above the membrane/cytoplasm interface is shown. Dark gray spheres represent MTSET molecules.
Figure 3. Open-state modification of a cysteine above the putative membrane/cytoplasm interface. (A) Voltage protocol for open-state modification by internal MTSET and representative current traces. Current was evoked every 6 s by a 500-ms test pulse. MTSET (1 mM) was applied continuously in both the open and closed states until steady-state inhibition was reached. (B) An exemplar time course of open-state modification of IIIS6-V9C. (C) Cartoon of S5 and S6 transmembrane helices and P-loop in the open state. The thiol group of a pore-lining cysteine above the membrane/cytoplasm interface is shown. Dark gray spheres represent MTSET molecules.
Figure 4. Comparison of open- and closed-state modification of a cysteine above the putative membrane/cytoplasm interface. (A) Voltage protocol for closed-state modification using fast perfusion. Current was evoked every 20 s by a 20-ms test pulse. Between the test pulses MTSET (1 mM) was applied for 10 s and subsequently washed out for 10 s. (B and D) Time course of MTSET modification of a representative cysteine (IIS6-A4C) in closed state (B) and open state (D). (C and E) The MTSET inhibition phase in B and D plotted against the cumulative time in MTSET or the cumulative channel open time, respectively, superimposed with a single-exponential fitting curve.
Figure 5. MTSET modification rates in open and closed states. (A) Apparent second-order rate constants for MTSET modification of selected pore-lining residues. Filled circles represent rate constants measured in the closed state (â80 mV) and open circles represent those measured in the open state (at +20 or +30 mV for different mutant channels). (B) Cartoon of the closed-state conformation of S5 and S6 helices, showing that cysteines below the membrane/cytoplasm interface can be accessed by MTSET (dark gray spheres) in the closed state.
Figure 6. Voltage dependence of MTSET modification. Data were collected from IIS6-A4C. Filled squares and open circles represent, respectively, the mean modification rates (n = 3â5) and channel open probability measured at different voltages. The solid line is the Boltzmann fit to the voltage-activation curves obtained from 10 experiments (midpoint = â44.8 ± 0.6 mV and slope factor = 9.6 ± 0.5 mV).
Figure 7. Trapping of MTSET in the inner pore in the closed state. (A) Two voltage protocols for measuring MTSET modification. Currents were evoked by a depolarizing pulse to +30 mV every 6 s from a holding potential of â80 mV. The duration of the depolarizing pulse was either 500 ms or 10 ms. (B) Time course of MTSET inhibition of currents evoked by the 500-ms test pulse (filled circles) or the 10-ms test pulse (open circles) in the IIS6-A4C mutant channel. (C) The MTSET inhibition phase in B plotted against the cumulative channel open time, superimposed with a single-exponential fitting curve with the indicated time constant.
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