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Figure 1. . Phenotype of mutations. Glutamate 148 of the StCLC channel (Dutzler et al., 2002) marks the beginning of helix F and is part of a highly conserved structural motif of CLC channels. The phenotype of mutations E166A and E166D are illustrated in C and D. Mutant E166S (not depicted) was indistinguishable from mutant E166A, and mutant E166K (not depicted) was similar to E166A. voltage-clamp traces obtained from whole oocytes from the indicated constructs are shown. Single traces in 100 mM NaCl (thin trace) and 100 mM NaI (thick trace) measured from the same oocyte are shown superimposed. They were evoked by a pulse to 60 mV followed by a pulse to â140 mV. Horizontal bars, 50 ms. Vertical bars: 2 μA (B), 16 μA (C), 4 μA (D). Similar results were obtained for at least five oocytes for each mutant.
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Figure 2. . Inhibition of mutant E166A by CPA. Patch-clamp data from a representative inside-out patch are shown in the absence of CPA (A), and in the presence of 0.1 mM CPA (B) and 5 mM CPA (C). The pulse protocol consists of a prepulse to 80 mV, a test pulse to various potentials (the responses to â140, â100, â60, â20, 20, 60, and 100 mV are shown) and a âtailâ pulse to 80 mV. The chemical structure of CPA is shown in C as an inset. Nearly identical results were obtained for the mutation E166S (not depicted).
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Figure 3. . Steady-state inhibition by CPA. The inhibition seen at steady-state is shown in A as a function of [CPA] (filled circles, â140 mV; open circles, â120 mV; filled squares, â100 mV; open squares, â80 mV; filled triangles up, â60 mV, open triangles up, â40 mV; filled triangles down, â20 mV; open triangles down, 20 mV; filled diamonds, 40 mV; open diamonds, 60 mV; filled hexagon, 80 mV; open hexagon, 100 mV; cross, 120 mV; star, 140 mV). Data were obtained by averages from 5 patches. Lines in A are best fits of Eq. 1. The resulting KDapp is shown in B (filled circles) as a function of voltage. The solid line represents a best exponential fit to the data from â120 to 120 mV of the form KDapp(V) = KDapp(0)*exp(z*V/(RT)) with a valence z = 0.96 and KDapp(0) = 0.48 mM. Diamonds represent the open channel KD estimated by the fit of Eq. 3 to the relaxation rates shown in Fig. 8 A and the dotted line indicates an exponential function of the form KD (V) = KD (0)*exp(zO*V/(RT)) with zO = 0.23 and KD(0) = 11 mM. Open squares are calculated from Eq. 2 using the parameters obtained by fitting Eq. 3 to the relaxation rates (see Fig. 8).
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Figure 4. . Block of E166A in low intracellular chloride. The steady-state block was evaluated using an intracellular solution in which 90 mM chloride was replaced by glutamate resulting in a solution with 14 mM Clâ (filled squares). For comparison, the data from Fig. 3 obtained in the regular Clâ solution are also shown (open circles). Data in low Clâ were obtained by the average from three patches.
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Figure 5. . Nonstationary noise analysis of mutant E166A in the presence of CPA. Examples of nonstationary noise analysis are shown under different conditions from different patches (A, test pulse to 80 mV after a prepulse to â140 mV in the presence of 1 mM CPA; B, test pulse to 80 mV after a prepulse to â140 mV in the presence of 0.1 mM CPA; C, test pulse to â100 mV after a prepulse to 80 mV in the presence of 0.1 mM CPA). On the left are shown the mean (top trace) and the variance (bottom trace), while on the right the variance is plotted versus the mean (symbols) and fitted with a parabola (line) as described in materials and methods. The parameters obtained by the fit are, A, i = 0.37 pA, N = 123, pmax = 0.88; B, i = 0.40 pA, N = 96, pmax = 0.95; C, i = 0.91, N = 89, pmax = 0.94. Bars: 5 ms, 10 pA, 1 pA2 (A and B); 10 ms, 30 pA, 5 pA2 (C). Similar results were obtained in a total of four patches.
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Figure 6. . Recordings from a patch with only a few channels. Representative traces from a single patch held at â100 mV (AâC) or 60 mV (EâG) in the absence of CPA (gray trace in A and E), with 0.1 mM CPA (black trace in A and F), or 5 mM CPA (B, C, and G) are shown. In C a short stretch of the trace in B is shown at a higher time-resolution (filtered at 500 Hz, while the longer traces were filtered at 200 Hz before display). In D a raw amplitude histogram of the recording at â100 mV in the presence of 0.1 mM CPA (gray trace) and 5 mM CPA (black trace) is shown. The vertical lines are drawn at current values of â0.8 and â0.61 pA to highlight the first nonzero peaks of the respective amplitude histograms. The bin-width for the amplitude histograms was 5 fA. The vertical scale bar in A also applies to B and C, and the scale bars in F also apply to E and G. The patch most likely contained two channels with four pores. Similar results were obtained in a total of four patches.
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SCHEME III.
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Figure 7. . Single-exponential relaxations of mutant E166A in the presence of CPA. Examples of relaxations in the presence of CPA (A and B, 5 mM; C, 0.1 mM) at 80 mV (prepulse to â140 mV) (A), â120 mV (prepulse to 80 mV) (B), and â140 mV (prepulse to 80 mV) (C) are shown (thin lines) superimposed with single exponential fits (thick gray traces) (time constants, A, 2.2 ms; B, 2.7 ms; C, 17.5 ms).
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Figure 8. . Kinetic analysis of CPA inhibition of mutant E166A. A shows relaxation rates obtained by fitting single exponential functions to the relaxations of the currents in the presence of CPA for exemplary voltages (circles, â140 mV; squares, â100 mV; triangles up, â60 mV; triangles down, â20 mV; diamond, 20 mV; open hexagons, 80 mV). Lines are fits of Eq. 3 to the data with the parameters α, β, and KD for each voltage. In the positive voltage-range essentially only the opening rate, α, could be determined because the affinity for CPA is too low, so that the second term in Eq. 3 is small compared with α. The resulting open channel KD is shown in Fig. 3 B (diamonds), while α (circles) and β (squares) are displayed in B as a function of voltage. The line in B is a function of the form α(V) = α(0)*exp(zα*V/(RT)) with zα = 0.58 and α(0) = 75 sâ1.
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SCHEME IV.
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SCHEME I.
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SCHEME V.
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Figure 9. . Effect of reduced [Clâ]ext on CPA block of E166A. The main graph shows the open-probability as a function of voltage of E166A channels with 0.1 mM intracellular CPA in 110 mM [Clâ]ext (circles) and 20 mM [Clâ]ext (squares) (n = 4 each). The inset shows a typical family of voltage-clamp traces measured from an outside-out patch in high (top traces) and low (bottom traces) [Clâ]ext. The asterisk indicates the constant tail pulse at â140 mV. At 0.1 mM CPA practically no inhibition is seen at voltages >80 mV and thus the normalized initial currents at the constant âtailâ pulse directly reflect the apparent open-probability at the end of a previous conditioning pulse. The normalized initial current values at this test pulse were thus used to calculate the open-probability. The lines are fits of a Boltzmann function with a voltage of half-maximal activation of â71 mV (high Clâ) and â41 mV (low Clâ). Scale bars in the inset indicate 50 ms and 50 pA, respectively.
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SCHEME VI.
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Figure 10. . Effect of additional mutations on the kinetics of CPA block of mutant E166A. Shown are representative current traces measured with 1 mM CPA for mutant E166A (thin black trace), mutant E166A/S123T (dashed gray trace), and mutant E166A/K519E (dashed black trace). None of the mutants show any relaxation in the absence of CPA. The currents are normalized to have similar amplitude at the 80-mV prepulse, that is followed by a pulse to â140 mV, and a repolarization to 80 mV. Note also the strong outward rectification of mutant E166A/K519E, compatible with the known alterations of the open channel properties of the mutant K519E (Pusch et al., 1995; Ludewig et al., 1997a). Similar results were obtained in a total of five patches for each mutant (E166A/S123T and E166A/K519E).
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SCHEME II.
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SCHEME VII.
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