Allosteric Voltage Gating of Potassium Channels I: Mslo Ionic Currents in the Absence of Ca2+

FT Horrigan, J Cui, RW Aldrich - The Journal of general physiology, 1999 - rupress.org
FT Horrigan, J Cui, RW Aldrich
The Journal of general physiology, 1999rupress.org
Activation of large conductance Ca2+-activated K+ channels is controlled by both
cytoplasmic Ca2+ and membrane potential. To study the mechanism of voltage-dependent
gating, we examined mSlo Ca2+-activated K+ currents in excised macropatches from
Xenopus oocytes in the virtual absence of Ca2+ (< 1 nM). In response to a voltage step, IK
activates with an exponential time course, following a brief delay. The delay suggests that
rapid transitions precede channel opening. The later exponential time course suggests that …
Activation of large conductance Ca2+-activated K+ channels is controlled by both cytoplasmic Ca2+ and membrane potential. To study the mechanism of voltage-dependent gating, we examined mSlo Ca2+-activated K+ currents in excised macropatches from Xenopus oocytes in the virtual absence of Ca2+ (<1 nM). In response to a voltage step, IK activates with an exponential time course, following a brief delay. The delay suggests that rapid transitions precede channel opening. The later exponential time course suggests that activation also involves a slower rate-limiting step. However, the time constant of IK relaxation [τ(IK)] exhibits a complex voltage dependence that is inconsistent with models that contain a single rate limiting step. τ(IK) increases weakly with voltage from −500 to −20 mV, with an equivalent charge (z) of only 0.14 e, and displays a stronger voltage dependence from +30 to +140 mV (z = 0.49 e), which then decreases from +180 to +240 mV (z = −0.29 e). Similarly, the steady state GK–V relationship exhibits a maximum voltage dependence (z = 2 e) from 0 to +100 mV, and is weakly voltage dependent (z ≅ 0.4 e) at more negative voltages, where Po = 10−5–10−6. These results can be understood in terms of a gating scheme where a central transition between a closed and an open conformation is allosterically regulated by the state of four independent and identical voltage sensors. In the absence of Ca2+, this allosteric mechanism results in a gating scheme with five closed (C) and five open (O) states, where the majority of the channel's voltage dependence results from rapid C–C and O–O transitions, whereas the C–O transitions are rate limiting and weakly voltage dependent. These conclusions not only provide a framework for interpreting studies of large conductance Ca2+-activated K+ channel voltage gating, but also have important implications for understanding the mechanism of Ca2+ sensitivity.
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