Figure 4.

Extracellular D2O does not alter the midpoint of the voltage dependence of steady-state activation of Shaker-IR mutant channels expressed in tsA201 cells. (A–C) Cells were held at −120 mV and depolarized to gradually increasing test potentials ranging from −100 to +70 mV in steps of 10 mV in every 45 s. The duration of the depolarizing pulses was 150 ms. G–V curves were constructed from current–voltage relationships using G(V) = Ipeak/(Vtest − EK) with the following parameters: peak current (Ipeak) at a test potential of Vtest and a K+ reversal potential of EK = −85 mV. The conductance values were normalized to the maximum (G/G0) and plotted as a function of the test potential (Em). The voltage dependencies of steady-state activation curves were determined in the absence (filled symbols, H2O//H2O condition) or presence of extracellular D2O (empty symbols, H2O//D2O condition). The superimposed solid lines show the best-fit Boltzmann functions to the averaged data points. (D) Bars and error bars indicate the mean ± SEM (n ≥ 4) of the midpoint voltages (V1/2) of steady-state activation obtained for the indicated clones. Symbols indicate individual data points (circles, T449A; down triangles, T449A/I470A; up triangles, T449K/I470C) obtained in H2O//H2O (filled symbols) and H2O//D2O (empty symbols).

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