To evaluate the contribution of Kir channels to the membrane potential (
V m), we recorded
V m from native BCE cell clusters in whole-cell configuration under the zero-current clamp condition while testing the effects of elevated [K
+]
o and K
+ channel blockers.
Figure 7A depicts the
V m response of a representative BCE cell cluster to increases in [K
+]
o. Increasing [K
+]
o from 5 to 140 mM caused a significant depolarization, indicating that
V m was determined in part by a K
+ conductance.
Figure 7B summarizes the results of similar experiments on 14 native BCE cell clusters. In the presence of 5 mM K
+,
V m averaged −40.0 ± 4.1 (mean ± SEM; range: −23 to −73 mV) and in the presence of 140 mM K
+, it averaged −7.4 ± 1.8 (range: −18 to +2.4 mV). To obtain a quantitative estimate of the contribution of Kir conductance to
V m, we applied the chord conductance equation
\[V_{\mathrm{m}}\ {=}\ (g_{\mathrm{K}}/g_{\mathrm{T}})E_{\mathrm{K}}\ {+}\ (1\ {-}\ g_{\mathrm{K}}/g_{\mathrm{T}})E_{\mathrm{r}}\]
where
g K is the inwardly rectifying K
+ conductance,
g T is the total conductance, 1 −
g K/
g T is residual conductance normalized to the total conductance,
E K is the K
+ equilibrium potential, and
E r is the reversal potential of the residual current. Assuming that 10 mM Ba
2+ blocks
g K specifically and completely,
E r can be taken to be −28 mV (discussed later). This value of
E r is close to the equilibrium potential for Cl
− (−32.5 mV), suggesting the residual current is primarily Cl
− current. We used this value and
equation 2 to calculate that the relative Kir conductance (
g K/
g T) of BCE cells bathed in 5 mM K
+ averages 0.22 and can be as high as 0.81. The depolarization of
V m to near 0 by 140 mM K
+ can be accounted for by a K
+-induced increase in
g K, combined with the depolarization of
E K to 0 mV.