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1.
Fig. 6.

Fig. 6. From: Sequential formation of ion pairs during activation of a sodium channel voltage sensor.

Full atom and molecular surface representation of the voltage-sensing module of NaChBac in three sequential activated states. Segments S1 through S4 colored individually and labeled. Side chains of gating-charge-carrying arginines (labeled R1 through R4 and colored blue) in S4, and D60 and E70 (colored red) in S2 shown in space filling representation. A probe radius of 1.4 Å was used to scan the molecular surface of each structural model. Figure generated using Chimera.

Paul G. DeCaen, et al. Proc Natl Acad Sci U S A. 2009 Dec 29;106(52):22498-22503.
2.
Fig. 2.

Fig. 2. From: Sequential formation of ion pairs during activation of a sodium channel voltage sensor.

Disulfide locking the D60C:R4C voltage sensor. Mean normalized peak INa elicited by trains to 40 mV positive to the potential of half activation (V1/2 + 40 mV). Holding potential = −120 mV. (A) Effect of 10 mM H2O2 (n = 7). (B and C) Reversal of H2O2 effect with 10 mM DTT (B) or 1 mM TCEP (C) (V = +80 mV; n = 8). (D) Test for disulfide locking with H2O2 during 2 min (t = 1–3 min, bar) at −120 mV without pulsing.

Paul G. DeCaen, et al. Proc Natl Acad Sci U S A. 2009 Dec 29;106(52):22498-22503.
3.
Fig. 1.

Fig. 1. From: Sequential formation of ion pairs during activation of a sodium channel voltage sensor.

Disulfide locking the E70C:R4C voltage-sensor. (A) INa from the first and last pulses in a 2-min 0.1 Hz train of 500-ms depolarizations to 0 mV from a holding potential of −120 mV. (B) Mean normalized peak currents during trains (n = 7). After 3 min, pulsing was stopped for 5 min to test for channel recovery. (C) Effect of 10 mM H2O2 (bar; n = 5). (D and E) Effects of 10 mM βME (D) or 1 mM TCEP (E) (Bars; holding potential = −140 mV; n = 6.)

Paul G. DeCaen, et al. Proc Natl Acad Sci U S A. 2009 Dec 29;106(52):22498-22503.
4.
Fig. 4.

Fig. 4. From: Sequential formation of ion pairs during activation of a sodium channel voltage sensor.

Time course of disulfide locking. (A) Voltage protocol. Channels were unlocked by a 5-s prepulse to −160 mV. Cells were then depolarized by prepulses to (V1/2 + 40 mV) of the indicated duration. Following 5 s at −120 mV, disulfide-locked channels were assayed with a 100-ms test pulse to V1/2 + 40 mV (WT, 0 mV; D60C, 20 mV; E70C, −30 mV; R4C, 60 mV; D60C:R4C, 80 mV; E70C:R4C, −40 mV). (B) Peak test pulse currents were normalized to the test pulse current in the absence of a prepulse. Mean values (±SEM) were plotted versus prepulse duration (n = 6). (C–E) Comparison of the rate of disulfide locking (red circles) and channel activation (blue line) for (C) E70C:R4C, control, (D) E70C:R4C, 2 mM H2O2, and (E) D60C:R4C, 2 mM H2O2. (F) Ratio of the time constant for disulfide locking (τS–S) to the time constant for activation (τAct) for E70C:R4C and D60C:R4C channels in 2 mM H2O2. For E70C:R4C, τS–S = 33 ± 2 ms, τact = 20 ± 2 ms (n = 6). For D60C:R4C, τS–S = 45 ms ± 2 ms (n = 7), τact = 4 ± 0.5 ms (n = 7).

Paul G. DeCaen, et al. Proc Natl Acad Sci U S A. 2009 Dec 29;106(52):22498-22503.
5.
Fig. 3.

Fig. 3. From: Sequential formation of ion pairs during activation of a sodium channel voltage sensor.

Reversal of disulfide locking of E70C:R4C by hyperpolarization. (A) Voltage dependence of reversal of disulfide locking. Before each trial, five 500-ms pulses to 0 mV were applied to disulfide-lock and fully inactivate all voltage sensors. Fully locked channels were hyperpolarized for 5 s to potentials from −200 to −120 mV followed by a 500-ms depolarization to 0 mV to assay the unlocked channels. Each cell was tested in control and in 10 mM βME or 10 mM H2O2, and currents were normalized to the largest current in control. Mean normalized peak currents were plotted against prepulse potential (n = 6; ±SEM). (B) Time-course of reversal of disulfide locking. Fully locked channels were hyperpolarized to −160 mV for the indicated times followed by a test pulse to 0 mV. Each cell was tested in control and then in the presence of 10 mM βME or 10 mM H2O2; peak test pulse currents were normalized to the peak current following the 32-s hyperpolarization in control. Mean normalized peak currents (±SEM) are plotted against prepulse duration and fit to a single exponential (n = 6). Error bars are smaller than data points where not visible. (C) Rate constants for disulfide locking. Assuming a bimolecular reaction, inset, forward α (black circles), and reverse β (green squares), rate constants were calculated from the rate and extent of reversal of unlocking at −160 mV from (B) as detailed in SI Methods.

Paul G. DeCaen, et al. Proc Natl Acad Sci U S A. 2009 Dec 29;106(52):22498-22503.
6.
Fig. 5.

Fig. 5. From: Sequential formation of ion pairs during activation of a sodium channel voltage sensor.

Voltage dependence of disulfide locking and rates of inactivation of disulfide-locked states. The voltage dependence of channel activation (white circles) and of disulfide locking (blue circles) measured in the presence of 2 mM H2O2 are compared for E70C:R4C (A) and D60C:R4C (B). The voltages for half-maximal channel activation and disulfide locking were determined from fits of a Boltzmann equation to the data. To measure the voltage dependence of disulfide locking of E70C:R4C (n = 9), channels were unlocked by a 5 s pulse to −160 mV, then depolarized with 500-ms prepulses to the indicated potentials. After 5 s at −120 mV, the number of channels locked during the prepulse was assessed with a 100-ms test pulse to +80 mV. Since H2O2-induced disulfide locking of D60C:R4C channels cannot be reversed by hyperpolarization, disulfide locking could only be tested at one potential for each cell (n = 5–6 for each potential). (C) Rates of inactivation of disulfide-locked channels. Sodium current traces from the indicated NaChBac channels elicited by 500-ms depolarizations to V = V1/2 + 40 mV from −120 mV (black traces). The time constant of inactivation was determined by an exponential fit to the decay of INa (red lines). INa is outward for D60C:R4C because its positive voltage dependence of activation requires test pulses to V = V1/2 + 40 mV, that are beyond the reversal potential. (D) Mean time constants of inactivation measured at the indicated potentials (WT, n = 10; D60C:R4C, n = 8; E70C:R4C, n = 10; ± SEM).

Paul G. DeCaen, et al. Proc Natl Acad Sci U S A. 2009 Dec 29;106(52):22498-22503.

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