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. 2018 Nov 5;14:1744806918815007. doi: 10.1177/1744806918815007

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© The Author(s) 2018

Creative Commons Non Commercial CC BY-NC: This article is distributed under the terms of the Creative Commons Attribution-NonCommercial 4.0 License (http://www.creativecommons.org/licenses/by-nc/4.0/) which permits non-commercial use, reproduction and distribution of the work without further permission provided the original work is attributed as specified on the SAGE and Open Access pages (https://us.sagepub.com/en-us/nam/open-access-at-sage).

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Figure 3. — V810M has no effect on inactivation of Na_v1.7. (a) Steady-state fast inactivation of WT (black squares, n = 18) and V810M (red circles, n = 17) channels. Currents were normalized to maximum current amplitude and fit to a Boltzmann equation. (b) Steady-state slow inactivation of WT (black squares, n = 8) and V810M (red circles, n = 7) channels. Currents were normalized to maximum current amplitude and fit to a Boltzmann equation. Data are expressed as means ± SEM.