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. Author manuscript; available in PMC: 2010 Mar 30.
Published in final edited form as: Channels (Austin). 2008 Feb 19;1(6):429–437. doi: 10.4161/chan.1.6.5760

Table 1.

Deactivation time constants for HERG and mutant constructs in the absence and presence of 10 mM Mg2+

0 mM Mg2+ 10 mM Mg2+ n Vtest
WT (slow)** 2567 ± 129 789 ± 82 11 +40 mV
WT (fast)** 480 ± 25 219 ± 21 11 +40 mV
D456A (slow) 201 ± 21 165 ± 10 6 +40 mV
D456A (fast)** 52 ± 2 39 ± 1 6 +40 mV
D460A* 99 ± 5 76 ± 3 8 +40 mV
D466A* 111 ± 5 84 ± 7 5 +40 mV
D509A* 47 ± 1 42 ± 1 8 +40 mV
D456A/D460A (slow) 163 ± 7 166 ± 9 8 +60 mV
D456A/D460A (fast) 24 ± 1 26 ± 2 8 +60 mV
D456A/D509A 63 ± 3 59 ± 3 7 +60 mV
D460A/D509A* 50 ± 2 44 ± 1 5 +60 mV
D466A/D509A** 76 ± 2 53 ± 2 11 +60 mV

Values for the deactivation time constants (in ms, mean ± SEM) were derived from single or double exponential fits to the tail currents (see Figs. 1A and 3B). The number of experiments, n, and the test pulse, Vtest, are indicated.

*

and ** denote significant differences in the presence and absence of 10 mM Mg2+ p < 0.001 and p < 0.05, respectively, using one-way ANOVA.