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. 2010 Aug 9;99(4):1110–1118. doi: 10.1016/j.bpj.2010.06.013

Figure 3.

Figure 3

(A) Kinetic model of hERG currents before and after PIP2 application. Activation and inactivation are modeled as uncoupled processes. The channel is open when it is in the O and NI states at the same time. To focus on activation properties, transition rates regarding inactivation (αI, βI) are determined before and after PIP2 addition from a concomitant fit of voltage-dependent inactivation rates and recovery-from-inactivation kinetics (Fig. S2). (B) Simulated and recorded hERG currents for the three protocols before and after PIP2 application. The transition rates and biophysical parameters determined from these simulations are shown in Table S1. Optimization of the late voltage-independent transitions (αP, βP), supposed to be related to the pore domain, leads to a reasonable fit of the PIP2 effect that is as good as the fit obtained by optimizing all transition rates. Conversely, optimization of early voltage-dependent transition rates (αVS1, βVS1, αVS2, βVS2), supposed to be mainly related to the voltage sensing of hERG, leads to a poor fit of the PIP2 effect.