Large-conductance Ca-activated potassium channels (BK channels) are uniquely sensitive to both membrane potential and intracellular Ca2+. Recent work has demonstrated that in the gating of these channels there are voltage-sensitive steps that are separate from Ca2+ binding steps. Based on this result and the macroscopic steady state and kinetic properties of the cloned BK channel mslo, we have recently proposed a general kinetic scheme to describe the interaction between voltage and Ca2+ in the gating of the mslo channel (Cui, J., D.H. Cox, and R.W. Aldrich. 1997. J. Gen. Physiol. In press.). This scheme supposes that the channel exists in two main conformations, closed and open. The conformational change between closed and open is voltage dependent. Ca2+ binds to both the closed and open conformations, but on average binds more tightly to the open conformation and thereby promotes channel opening. Here we describe the basic properties of models of this form and test their ability to mimic mslo macroscopic steady state and kinetic behavior. The simplest form of this scheme corresponds to a voltage-dependent version of the Monod-Wyman-Changeux (MWC) model of allosteric proteins. The success of voltage-dependent MWC models in describing many aspects of mslo gating suggests that these channels may share a common molecular mechanism with other allosteric proteins whose behaviors have been modeled using the MWC formalism. We also demonstrate how this scheme can arise as a simplification of a more complex scheme that is based on the premise that the channel is a homotetramer with a single Ca2+ binding site and a single voltage sensor in each subunit. Aspects of the mslo data not well fitted by the simplified scheme will likely be better accounted for by this more general scheme. The kinetic schemes discussed in this paper may be useful in interpreting the effects of BK channel modifications or mutations.
Allosteric Gating of a Large Conductance Ca-activated K+ Channel
Address correspondence to Dr. Richard W. Aldrich, Department of Molecular and Cellular Physiology, Beckman Center B171, Stanford, CA 94305-5426. Fax: 415-725-4463; E-mail: [email protected]
Abbreviations used in this paper: CNG, cyclic nucleotide–gated; KNF, Koshland-Nemethy-Filmer; MWC, Monod-Wyman-Changeux.
Although a single Boltzmann function often appears to fit the data well, somewhat better fits can be achieved by fitting to a Boltzmann function raised to a power >1 (Cui et al., 1997).
For each patch, the two-tiered KNF scheme fit significantly better than the voltage-dependent MWC scheme (P < 0.01), and the general 10-state scheme fit significantly better than the two-tiered KNF scheme (P < 0.05).
Models of the form of scheme II actually do not predict a change in Hill coefficient as a function of voltage. The change in model Hill coefficient with voltage in Fig. 8,D is due to a voltage-dependent shift in the region of the dose–response curve emphasized in the fitting. The true Hill coefficient, defined as the maximum slope of a plot of log (Popen/(Popen_max − Popen)) vs. log([Ca]), is a complicated function of [Ca] and all the Ca2+ dissociation constants in the model. It can be found by setting the second derivative of the function representing log (Popen/(Popen_max − Popen)) with respect to log([Ca]) equal to 0, solving for [Ca], and substituting this value of [Ca] into the expression for the first derivative with respect to log([Ca]). For the model in Fig. 8, this value is 2.10. As is well known, however, the model's Hill coefficient would change with L, and therefore voltage, if the fraction of binding sites occupied by Ca2+ is measured instead of Popen (Wyman and Gill, 1990).
D.H. Cox, J. Cui, R.W. Aldrich; Allosteric Gating of a Large Conductance Ca-activated K+ Channel . J Gen Physiol 1 September 1997; 110 (3): 257–281. doi: https://doi.org/10.1085/jgp.110.3.257
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