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. 2006 Mar 23;573(Pt 2):291–304. doi: 10.1113/jphysiol.2006.108332

Figure 2. EAG family S5P chimaera characteristics.

Figure 2

Upper panel, alignment of the residues of the S5P linker of hERG, rELK2 and hEAG is shown at the top of the figure below a cartoon depicting wt hERG structure. The demonstrated α-helical region (Torres et al. 2003) is boxed. The charged residues of interest within the α-helical region of rELK2 are highlighted. Aa, steady-state inactivation of hERG/hEAG S5P chimaera. Typical example of currents recorded from hERG/hEAG S5P channels during a steady-state inactivation voltage protocol (see Fig. 1A) are shown. Arrow indicates zero current. Ab, the conductance–voltage plot of hERG/hEAG S5P (•). The curve fitted to the hERG/hEAG S5P data is a Boltzmann function with a V0.5 of inactivation of −57 mV and a slope factor of −31 mV (n = 5). The dotted line shows the Boltzmann fit to the wt hERG data from Fig. 1B. Ba, typical example of currents recorded from hERG/rELK2 S5P chimaera channels during a steady-state inactivation voltage protocol (see Fig. 1A). Arrow indicates zero current. Bb, the conductance–voltage plot of hERG/rELK2 S5P (•) compared with wt hERG (dotted line) and wt rELK2 (•). The curve fitted to the hERG/rELK2 S5P data is a Boltzmann function with a V0.5 of inactivation of 27 mV and a slope factor of −34 mV (n = 4). The data for wt hERG and wt rELK2 are reproduced from Fig. 1B.