Anomalous mole fraction effect induced by mutation of the H5 pore region in the Shaker K+ channel

P-loop residues critical for selectivity in K channels fail to confer selectivity to rabbit HCN4 channels

HCN channels are thought to be structurally similar to K_v channels, but show much lower selectivity for K⁺. The ∼3.3 Å selectivity filter of K⁺ channels is formed by the pore-lining sequence XT(V/I)GYG, with X usually T, and is held stable by key residues in the P-loop. Differences in the P-loop sequence of HCN channels (eg. the pore-lining sequence L₄₇₈C₄₇₉IGYG) suggest these residues could account for differences in selectivity between these channel families. Despite being expressed, L478T/C479T HCN4 channels did not produce current. Since threonine in the second position is highly conserved in K⁺ channels, we also studied C479T channels. Based on permeability ratios (P_X/P_K), C479T HCN4 channels (K⁺(1)>Rb⁺(0.85)>Cs⁺(0.59)>Li⁺(0.50)≥Na⁺(0.49)) were less selective than WT rabbit HCN4 (K⁺(1)>Rb⁺(0.48)>Cs⁺(0.31)≥Na⁺(0.29)>Li⁺(0.03)), indicating that the TIGYG sequence is insufficient to confer K⁺ selectivity to HCN channels. C479T HCN4 channels had an increased permeability to large organic cations than WT HCN4 channels, as well as increased unitary K⁺ conductance, and altered channel gating. Collectively, these results suggest that HCN4 channels have larger pores than K⁺ channels and replacement of the cysteine at position 479 with threonine further increases pore size. Furthermore, selected mutations in other regions linked previously to pore stability in K⁺ channels (ie. S475D, S475E and F471W/K472W) were also unable to confer K⁺ selectivity to C479T HCN4 channels. Our findings establish the presence of the TIGYG pore-lining sequence does not confer K⁺ selectivity to rabbit HCN4 channels, and suggests that differences in selectivity of HCN4 versus K⁺ channels originate from differences outside the P-loop region.

Ionic permeation and conduction properties of neuronal KCNQ2/KCNQ3 potassium channels

Heteromeric KCNQ2/3 potassium channels are thought to underlie the M-current, a subthreshold potassium current involved in the regulation of neuronal excitability. KCNQ channel subunits are structurally unique, but it is unknown whether these structural differences result in unique conduction properties. Heterologously expressed KCNQ2/3 channels showed a permeation sequence of while showing a conduction sequence of A differential contribution of component subunits to the properties of heteromeric KCNQ2/3 channels was demonstrated by studying homomeric KCNQ2 and KCNQ3 channels, which displayed contrasting ionic selectivities. KCNQ2/3 channels did not exhibit an anomalous mole-fraction effect in mixtures of K(+) and Rb(+). However, extreme voltage-dependence of block by external Cs(+) was indicative of multi-ion pore behavior. Block of KCNQ2/3 channels by external Ba(2+) ions was voltage-independent, demonstrating unusual ionic occupation of the outer pore. Selectivity properties and block of KCNQ2 were altered by mutation of outer pore residues in a manner consistent with the presence of multiple ion-binding sites. KCNQ2/3 channel deactivation kinetics were slowed exclusively by Rb(+), whereas activation of KCNQ2/3 channels was altered by a variety of external permeant ions. These data indicate that KCNQ2/3 channels are multi-ion pores which exhibit distinctive mechanisms of ion conduction and gating.

Permeation properties of inward-rectifier potassium channels and their molecular determinants

The structural domains contributing to ion permeation and selectivity in K channels were examined in inward-rectifier K(+) channels ROMK2 (Kir1.1b), IRK1 (Kir2.1), and their chimeras using heterologous expression in Xenopus oocytes. Patch-clamp recordings of single channels were obtained in the cell-attached mode with different permeant cations in the pipette. For inward K(+) conduction, replacing the extracellular loop of ROMK2 with that of IRK1 increased single-channel conductance by 25 pS (from 39 to 63 pS), whereas replacing the COOH terminus of ROMK2 with that of IRK1 decreased conductance by 16 pS (from 39 to 22 pS). These effects were additive and independent of the origin of the NH(2) terminus or transmembrane domains, suggesting that the two domains form two resistors in series. The larger conductance of the extracellular loop of IRK1 was attributable to a single amino acid difference (Thr versus Val) at the 3P position, three residues in front of the GYG motif. Permeability sequences for the conducted ions were similar for the two channels: Tl(+) > K(+) > Rb(+) > NH(4)(+). The ion selectivity sequence for ROMK2 based on conductance ratios was NH(4)(+) (1.6) > K(+) (1) > Tl(+) (0.5) > Rb(+) (0.4). For IRK1, the sequence was K(+) (1) > Tl(+) (0.8) > NH(4)(+) (0.6) >> Rb(+) (0.1). The difference in the NH(4)(+)/ K(+) conductance (1.6) and permeability (0.09) ratios can be explained if NH(4)(+) binds with lower affinity than K(+) to sites within the pore. The relatively low conductances of NH(4)(+) and Rb(+) through IRK1 were again attributable to the 3P position within the P region. Site-directed mutagenesis showed that the IRK1 selectivity pattern required either Thr or Ser at this position. In contrast, the COOH-terminal domain conferred the relatively high Tl(+) conductance in IRK1. We propose that the P-region and the COOH terminus contribute independently to the conductance and selectivity properties of the pore.

Coincident detection of CSF Na+ and osmotic pressure in osmoregulatory neurons of the supraoptic nucleus

Behavioral and neuroendocrine responses underlying systemic osmoregulation are under the concerted control of centrally located osmoreceptors and cerebrospinal fluid (CSF) Na+ concentration ([Na+]) detectors. Although the process underlying osmoreception is understood, the mechanism by which [Na+] is detected and integrated with cellular information derived from osmoreceptors is unknown. Here, we show that shifts in extracellular [Na+] ([Na+]0) cause proportional changes in the relative Na+ permeability of mechanosensitive cation channels responsible for signal transduction in the osmosensory neurons of the supraoptic nucleus. This effect causes the generation of Na+ specific receptor potentials under isotonic conditions and modulates osmoreceptor potentials and electrical responsiveness during osmotic perturbation. These results provide a cellular basis for Na+-sensing and for the coordinated detection of CSF [Na+] and osmolality in central osmoregulatory neurons.

Anomalous mole fraction effect, electrostatics, and binding in ionic channels

Ionic channels bathed in mixed solutions of two permeant electrolytes often conduct less current than channels bathed in pure solutions of either. For many years, this anomalous mole fraction effect (AMFE) has been thought to occur only in single-file pores containing two or more ions at a time. Most thinking about channels incorporates this view. We show here that the AMFE arises naturally, as an electrostatic consequence of localized ion specific binding, if the average current through a channel is described by a theory (Poisson-Nernst-Planck, PNP) that computes the average electric field from the average concentration of charges in and near the channel. The theory contains only those ion-ion interactions mediated by the mean field, and it does not enforce single filing. The AMFE is predicted by PNP over a wide range of mean concentrations of ions in the channel; for example, it is predicted when (on the average) less, or much less, than one ion is found in the channel's pore. In this treatment, the AMFE arises, in large measure, from a depletion layer produced near a region of ion-specific binding. The small excess concentration of ions in the binding region repels all nearby ions of like charge, thereby creating a depletion layer. The overall conductance of the channel arises in effect from resistors in series, one from the binding region, one from the depletion zone, and one from the unbinding region. The highest value resistor (which occurs in the depletion zone) limits the overall series conductance. Here the AMFE is not the result of single filing or multiple occupancy, and so previous views of permeation need to be revised: the presence of an AMFE does not imply that ions permeate single file through a multiply occupied pore.

Selectivity changes during activation of mutant Shaker potassium channels

Mutations of the pore-region residue T442 in Shaker channels result in large effects on channel kinetics. We studied mutations at this position in the backgrounds of NH2-terminal-truncated Shaker H4 and a Shaker -NGK2 chimeric channel having high conductance (Lopez, G.A., Y.N. Jan, and L.Y. Jan. 1994. Nature (Lond.). 367: 179-182). While mutations of T442 to C, D, H, V, or Y resulted in undetectable expression in Xenopus oocytes, S and G mutants yielded functional channels having deactivation time constants and channel open times two to three orders of magnitude longer than those of the parental channel. Activation time courses at depolarized potentials were unaffected by the mutations, as were first-latency distributions in the T442S chimeric channel. The mutant channels show two subconductance levels, 37 and 70% of full conductance. From single-channel analysis, we concluded that channels always pass through the larger subconductance state on the way to and from the open state. The smaller subconductance state is traversed in approximately 40% of activation time courses. These states apparently represent kinetic intermediates in channel gating having voltage-dependent transitions with apparent charge movements of approximately 1.6 e0. The fully open T442S chimeric channel has the conductance sequence Rb+ > NH4+ > K+. The opposite conductance sequence, K+ > NH4+ > Rb+, is observed in each of the subconductance states, with the smaller subconductance state discriminating most strongly against Rb+.