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. 2012 Aug 27;7(8):e43587. doi: 10.1371/journal.pone.0043587

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© 2012 Qu, Chung

This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are properly credited.

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A. The quasi-steady state whole-cell current (I_Q) vs. voltage in the original model with = 0.15 mS/cm² with x set at different constant values (as marked). B. I_Q vs. voltage with x = 0 for the original model (Δ = 0), 10 mV shift in f_∞ (Δ = 10 mV), and f_∞ slope reduced (β = 18). C. I_Q vs. voltage with x = 0 for different V_trunc. D. Activation time constant (τ_x) and the steady-state action curve (x_∞) of I_K vs. voltage from the original LR1 model.

Inline graphic — A. The quasi-steady state whole-cell current (I_Q) vs. voltage in the original model with = 0.15 mS/cm² with x set at different constant values (as marked). B. I_Q vs. voltage with x = 0 for the original model (Δ = 0), 10 mV shift in f_∞ (Δ = 10 mV), and f_∞ slope reduced (β = 18). C. I_Q vs. voltage with x = 0 for different V_trunc. D. Activation time constant (τ_x) and the steady-state action curve (x_∞) of I_K vs. voltage from the original LR1 model.