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. 2003 Nov;122(5):541–556. doi: 10.1085/jgp.200308905

TABLE I.

Voltage Activation Relations for Shaker Kv Channels with Mutations at P475

Residue V50 z n
mV
P (Wt) −30.5 ± 0.6 3.8 ± 0.1 37
G 44.6 ± 1.3 2.2 ± 0.02 4
S 195.0 ± 5.7 1.2 ± 0.03 4
T −15.0 ± 1.5 3.3 ± 0.08 8
Y −48.3 ± 0.5 3.7 ± 0.1 10
V 64.8 ± 1.0 1.6 ± 0.08 6
I 63.9 ± 1.7 1.2 ± 0.04 5
M −11.9 ± 0.2 2.8 ± 0.06 9
C 146 ± 3.0 1.3 ± 0.07 3
F −21.6 ± 0.8 3.0 ± 0.09 10
W −49.4 ± 1.8 4.0 ± 0.3 14
Q −95.2 ± 1.0 2.6 ± 0.08 24
N −83.6 ± 0.9 3.2 ± 0.1 8
K −94.2 ± 3.6 2.6 ± 0.5 5
H −76.0 ± 6.3 3.1 ± 0.2 5
R −72.8 ± 2.8 3.0 ± 0.2 4
E −96.1 ± 3.2 3.1 ± 0.23 4
D −98.5 ± 2.3 3.3 ± 0.4 10

Tail current voltage-activation relations were obtained for most mutants using 50 mM Rb+ as the external charge carrier and fit with single Boltzmann functions. P475D was obtained using 50 mM K+ as the external charge carrier. P475L results in undetectable ionic or gating currents and P475A results in gating currents but no ionic currents (i.e., a nonconducting mutant). n corresponds to the number of experiments.