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. 1999 Feb 16;96(4):1357–1362. doi: 10.1073/pnas.96.4.1357

Table 2.

Voltage-dependence of wild-type and mutant channels

Activation
Inactivation
Vmid, mV Slope, mV Vmid, mV Slope, mV
Wild type 8.4 ± 0.7 6.7 ± 0.3 −1.8 ± 1.6 12.0 ± 0.5
P215L 7.1 ± 2.0 9.1 ± 0.2 −7.7 ± 3.5 13.5 ± 0.3
P976L 17.8 ± 0.8 7.4 ± 0.6 0.0 ± 1.5 11.9 ± 0.9
P215L-P976L 18.0 ± 0.8 10.6 ± 0.2 1.2 ± 3.0 14.4 ± 0.3
I598P 0.5 ± 1.1 6.3 ± 0.2 −13.4 ± 2.4 9.1 ± 0.9
L1306P 5.6 ± 1.0 8.5 ± 0.4 −2.0 ± 1.1 7.0 ± 0.6
I598P-L1307P −2.0 ± 0.8 8.3 ± 0.1 −25.1 ± 0.8 9.8 ± 0.7

Current-voltage relationships or current-prepulse voltage relationships were fitted to Boltzmann distributions to derive values for the midpoint (Vmid) and the slope (mV/e-fold change in G/Gmax) of the curves for steady-state activation and steady-state inactivation. The prepulses were 5,000 ms long. Data represent means ± standard error obtained from 7–14 (activation) and 4–9 (inactivation) measurements. Underlining indicates statistically significant differences from values for the wild type, with P < 0.05.