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. 2015 Aug;88(2):273–280. doi: 10.1124/mol.115.098707

TABLE 2.

Voltage dependence of activation and inactivation of mosquito sodium channels

The voltage dependences of conductance and inactivation were fitted with a two-state Boltzmann equation to determine V1/2, the voltage for half-maximal conductance or inactivation, and k, the slope factor for conductance or inactivation. The values in the table represent the mean ± S.E.M., and the number of oocytes was 6–16. The asterisks indicate significant differences as determined by one-way analysis of variance (P < 0.05) with Scheffe’s post hoc analysis.

Na+ Channel Type Activation
Inactivation
V1/2 (mV) k (mV) V1/2 (mV) k (mV)
AaNav1-1 −29.2 ± 0.8 5.2 ± 0.3 −52.9 ± 0.4 4.9 ± 0.2
G1K9A −32.6 ± 1.2 5.0 ± 0.2 −51.9 ± 0.4 4.8 ± 0.1
G1K9I −32.8 ± 1.4 6.3 ± 0.6 −52.8 ± 1.2 4.6 ± 0.2
I1k12N −33.8 ± 0.9 5.1 ± 0.4 −51.8 ± 0.6 4.6 ± 0.1
I1k12N+ G1K9A −30.2 ± 1.0 5.5 ± 0.3 −55.5 ± 0.8 4.8 ± 0.3
I1k12N+ G1K9I −30.4 ± 0.5 6.2 ± 0.2 −55.5 ± 1.1 5.1 ± 0.2
S1o2A −32.9 ± 0.2 5.1 ± 0.1 −54.0 ± 0.4 4.5 ± 0.1
N1o5A −33.5 ± 0.8 4.5 ± 0.2 −52.1 ± 0.6 4.5 ± 0.1
1o6A −50.5 ± 1.8* 6.1 ± 0.6 −64.7 ± 0.7* 6.4 ± 0.3
R1o7A −31.0 ± 0.6 5.1 ± 0.3 −53.9 ± 0.7 5.1 ± 0.1
I1i22A −34.3 ± 1.1 5.5 ± 0.4 −52.9 ± 0.5 5.0 ± 0.1
I1i25A −30.0 ± 0.8 7.0 ± 0.6 −67.5 ± 0.8* 5.0 ± 0.1
S1i29A −33.0 ± 0.8 5.5 ± 0.4 −54.8 ± 0.5 5.1 ± 0.1
V2i12A −26.7 ± 0.7 5.6 ± 0.4 −53.5 ± 0.8 5.5 ± 0.1
V2i12L −32.7 ± 0.8 5.5 ± 0.1 −50.9 ± 0.5 4.8 ± 0.1
N2i15S −28.8 ± 1.3 5.1 ± 0.1 −52.9 ± 1.4 4.9 ± 0.2
N2i20A −30.8 ± 0.6 5.4 ± 0.2 −58.7 ± 0.5 5.3 ± 0.1
F2i22S −30.7 ± 0.9 5.3 ± 0.7 −51.3 ± 0.9 4.7 ± 0.1
L2i25A −28.5 ± 0.8 5.9 ± 0.3 −51.5 ± 0.8 4.8 ± 0.1
L2i26A −31.7 ± 1.1 7.2 ± 0.4 −63.1 ± 1.2* 6.0 ± 0.4