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. 2015 May 26;17(3):285–296. doi: 10.1007/s12017-015-8356-8

Table 1.

Boltzmann parameters of activation relationships of wild-type hClC-1 channel and MC variants

[Cl−]i Variants N V 0.5 (mV) S (mV) Min
134 mM WT 11 −72.0 ± 3.3 47.2 ± 3.3 0.13 ± 0.02
p.T82A 12 −74.2 ± 1.6 42.2 ± 1.5 0.08 ± 0.01
p.R453W 13 −73.8 ± 1.7 34.1 ± 1.6 0.08 ± 0.01
p.G190S 9 +116.2 ± 3.1 33.1 ± 2.1 0.11 ± 0.01
p.G270V 13 +92.7 ± 5.9 52.6 ± 5.1 0.22 ± 0.01
p.T82A + p.G190S 9 −22.1 ± 2.5 69.3 ± 2.9 0.06 ± 0.02
p.R453W + p.G190S 6 +45.2 ± 1.9 56.4 ± 1.8 0.14 ± 0.01
4 mM WT 14 −14.8 ± 2.4 43.5 ± 2.7 <0.01
p.T82A 17 −4.1 ± 2.1 40.3 ± 2.3 <0.01
p.R453W 12 −8.6 ± 3.0 56.3 ± 3.8 0.03 ± 0.01
p.G270V 13 +84.4 ± 14.2 45.8 ± 8.3 0.07 ± 0.02

The averaged activation relationships obtained from n cells are fitted with a Boltzmann equation [P 0(V) = Min + (1 − Min)/(1 + exp((V − V 0.5)/S)], where V 0.5 is the half-maximal activation potential, S is the slope factor, and Min is the minimal value of P 0. The parameters are expressed as the calculated fit value ± the standard error of the fit