Table 1.

Fitted parameters for WT and mutant channels

 z1 z2 V1 (mV) V2 (mV) r2 
WT 2.37 4.19 −49.6 −33.9 n.d. 
R4K 2.03 ± 0.11 0.93 ± 0.06 −60.7 ± 0.9 46.4 ± 3.2 0.9973 
I241W 2.07 ± 0.04 1.91 ± 0.04 −74.4 ± 0.4 9.8 ± 0.4 0.9995 
I241W/R1K 1.53 ± 0.04 2.01 ± 0.05 −68.0 ± 0.7 49.6 ± 0.5 0.9995 
I241W/R2K 1.62 ± 0.02 1.48 ± 0.02 −59.2 ± 0.3 4.4 ± 0.3 0.9999 
I241W/R2Q 1.23 ± 0.07 2.11 ± 0.11 −89.9 ± 2.2 18.8 ± 0.9 0.9974 
I241W/R3K 1.84 ± 0.04 2.12 ± 0.04 −93.0 ± 0.5 57.7 ± 0.4 0.9997 
I241W/R4K 1.91 ± 0.08 1.75 ± 0.07 −79.1 ± 0.8 88.9 ± 0.1 0.9978 
F244W 2.65 ± 0.10 2.29 ± 0.09 −63.4 ± 0.5 −2.3 ± 0.7 0.9993 
F244W/R2K 2.61 ± 0.04 2.17 ± 0.03 −53.7 ± 0.2 −12.7 ± 0.2 0.9999 
F244W/R3K 2.01 ± 0.09 2.39 ± 0.11 −87.6 ± 1.1 8.6 ± 0.8 0.9978 
Deac I241W 2.62 ± 0.19 1.89 ± 0.15 −71.7 ± 0.1 −9.9 ± 1.7 0.9976 
Deac F244W 3.56 ± 0.15 2.99 ± 0.15 −64.5 ± 0.4 −15.0 ± 0.6 0.9986 
Deac I241W/R2K 2.52 ± 0.12 2.31 ± 0.11 −37.7 ± 0.7 6.2 ± 0.7 0.9994 
Deac I241W/R3K 2.25 ± 0.15 2.02 ± 0.14 −91.5 ± 1.2 −20.7 ± 1.4 0.9972 
 z1 z2 V1 (mV) V2 (mV) r2 
WT 2.37 4.19 −49.6 −33.9 n.d. 
R4K 2.03 ± 0.11 0.93 ± 0.06 −60.7 ± 0.9 46.4 ± 3.2 0.9973 
I241W 2.07 ± 0.04 1.91 ± 0.04 −74.4 ± 0.4 9.8 ± 0.4 0.9995 
I241W/R1K 1.53 ± 0.04 2.01 ± 0.05 −68.0 ± 0.7 49.6 ± 0.5 0.9995 
I241W/R2K 1.62 ± 0.02 1.48 ± 0.02 −59.2 ± 0.3 4.4 ± 0.3 0.9999 
I241W/R2Q 1.23 ± 0.07 2.11 ± 0.11 −89.9 ± 2.2 18.8 ± 0.9 0.9974 
I241W/R3K 1.84 ± 0.04 2.12 ± 0.04 −93.0 ± 0.5 57.7 ± 0.4 0.9997 
I241W/R4K 1.91 ± 0.08 1.75 ± 0.07 −79.1 ± 0.8 88.9 ± 0.1 0.9978 
F244W 2.65 ± 0.10 2.29 ± 0.09 −63.4 ± 0.5 −2.3 ± 0.7 0.9993 
F244W/R2K 2.61 ± 0.04 2.17 ± 0.03 −53.7 ± 0.2 −12.7 ± 0.2 0.9999 
F244W/R3K 2.01 ± 0.09 2.39 ± 0.11 −87.6 ± 1.1 8.6 ± 0.8 0.9978 
Deac I241W 2.62 ± 0.19 1.89 ± 0.15 −71.7 ± 0.1 −9.9 ± 1.7 0.9976 
Deac F244W 3.56 ± 0.15 2.99 ± 0.15 −64.5 ± 0.4 −15.0 ± 0.6 0.9986 
Deac I241W/R2K 2.52 ± 0.12 2.31 ± 0.11 −37.7 ± 0.7 6.2 ± 0.7 0.9994 
Deac I241W/R3K 2.25 ± 0.15 2.02 ± 0.14 −91.5 ± 1.2 −20.7 ± 1.4 0.9972 

The Q-V curves of the single or double mutants were fitted using a 3-state model equation (see Appendix). The parameters for WT were from a previous work (Bezanilla and Stefani, 1996). The fitted parameters for deactivation (Deac) were obtained from experiments done at 28°C.

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