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. Author manuscript; available in PMC: 2016 May 4.
Published in final edited form as: Nat Commun. 2013;4:1541. doi: 10.1038/ncomms2496

Table 1.

Best-fitting parameters describing the voltage-dependence of charge movement.

Qmax (nC µF−1) VQ1/2 (mV) K
WT (n = 13) 30 ± 8 −14 ± 2.2 16 ± 1.5
DKO 35 ±11 −24±1.7 14 ± 1.9
(n = 15) (P = 0.724) (P = 0.001) (P = 0.426)

Data points were fitted to a Boltzmann equation of the form: Qon = Qmax/[1 + exp(VQ1/2 − Vm)/K], where Qmax is the maximum charge, Vm is the membrane potential, VQ1/2 is the charge movement half-activation potential and K is the steepness of the curve as described in ref. 27. The number of FDB fibres from three to four mice is between parentheses. Results are expressed as the mean ± s.e.m. Statistical significance was assessed using Student’s t-test. The α-level was set at P=0.05.