Table 2.
Activation GV |
Deactivation GV |
Mode-shift |
Deactivation τ—τf (ms) |
|||||||
---|---|---|---|---|---|---|---|---|---|---|
Vh (mV) | k (mV) | n | Vh (mV) | k (mV) | n | Vh (mV) | n | −110 mV | n | |
WT | −22.8 ± 1.1 | 10.8 ± 0.7 | 13 | −54.2 ± 1.6 | 7.8 ± 0.4 | 13 | −31.4 ± 2.1 | 13 | 94.8 ± 9.3 | 8 |
R4D | −14.9 ± 1.0 | 9.2 ± 0.3 | 5 | −22.8 ± 1.1 | 7.5 ± 0.8 | 5 | −7.8 ± 1.6 | 5 | 27.5 ± 2.5 | 4 |
R5E | −17.6 ± 2.0 | 9.6 ± 0.3 | 5 | −30.1 ± 1.4 | 7.8 ± 0.5 | 5 | −12.5 ± 1.0 | 5 | 47.9 ± 5.7 | 4 |
D456A | −1.0 ± 1.2 | 7.5 ± 0.4 | 5 | −7.0 ± 1.0 | 7.5 ± 0.6 | 5 | −6.0 ± 0.9 | 5 | 35.8 ± 2.5 | 5 |
E480R | −2.8 ± 0.6 | 10.0 ± 0.2 | 5 | −14.0 ± 1.7 | 8.4 ± 0.5 | 5 | −11.8 ± 2.3 | 5 | 47.0 ± 3.5 | 5 |
D509A | 14.3 ± 1.5 | 11.0 ± 0.2 | 4 | 8.3 ± 0.7 | 9.9 ± 0.7 | 4 | −6.0 ± 1.4 | 4 | 22.0 ± 2.0 | 4 |
R537K | −8.6 ± 3.7 | 8.0 ± 0.3 | 6 | −9.8 ± 3.7 | 8.3 ± 0.4 | 6 | −1.2 ± 0.7 | 6 | 55.2 ± 2.3 | 5 |
R541G | −35.2 ± 1.5 | 13.2 ± 0.5 | 5 | −41.7 ± 1.2 | 11.7 ± 0.4 | 5 | −6.5 ± 0.6 | 5 | 42.8 ± 1.6 | 7 |
Y542G | −4.9 ± 2.1 | 14.8 ± 1.0 | 5 | −14.9 ± 1.4 | 11.1 ± 0.7 | 5 | −10.0 ± 1.6 | 5 | 12.9 ± 0.5 | 9 |
E544G | −22.4 ± 0.5 | 8.5 ± 0.1 | 7 | −25.3 ± 0.8 | 7.5 ± 0.2 | 7 | −2.9 ± 0.6 | 7 | 18.9 ± 0.6 | 5 |
Activation GV relations were collected from oocytes held at −80 mV and subjected to 2 s depolarizing steps to +50 mV in 10 mV increments followed by a 2 s step to −110 mV. Deactivation GV relations were collected from oocytes held at −80 mV and subjected to a 500 ms depolarizing step +60 mV followed by 8 s steps from –110 mV to +40 mV in 10 mV increments followed by a repolarizing step to −110 mV. Boltzmann fits were used to obtain the Vh and k values. Deactivation τ was obtained by fitting the deactivation tail current decay with a double exponential function. The value τfast is reported, because current decay at −110 mV was dominated (>85%) by the fast component.