“…For such a channel, the whole cell current amplitude ( I ) depends on the number of channels in the surface membrane ( N ), the single channel pore amplitude ( i ) and the open probabilities of the two protopore gates ( P p ) and the common gate ( P c ) (Accardi and Pusch, 2000; Fischer et al, 2010):
Random opening and closing of ion channels produce a Lorentzian type of noise (σ 2 ) that depends on the number of channels as well as its unitary current amplitude and its open probability. For a double-barreled channel σ 2 can be calculated as Fischer et al (2010), Weinberger et al (2012) and Stölting et al (2014a):
In the case of ClC-Ka/barttin channels the common gate was found permanently open using single channel recordings and noise analysis (Fischer et al, 2010), thus simplifying (2) to
which is equivalent to:
Based on an ohmic current-voltage relationship, this relationship can be further simplified to:
here with V the applied voltage, V rev the reversal potential, N the number of functional channels in the surface membrane and γ the single channel pore conductance (Sesti and Goldstein, 1998). The voltage-independent background noise was recorded at the reversal potential, where ClC-Ka/barttin currents do not contribute, averaged and subtracted from the otherwise measured variance.…”