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Previous calculations using continuum electrostatic calculations showed that a fully hydrated monovalent cation is electrostatically stabilized at the center of the cavity of the KcsA potassium channel. Further analysis demonstrated that this cavity stabilization was controlled by a balance between the unfavorable reaction field due to the finite size of the cavity and the favorable electrostatic field arising from the pore helices. In the present study, continuum electrostatic calculations are used to investigate how the stability of an ion in the intracellular vestibular cavity common to known potassium channels is affected as the inner channel gate opens and the cavity becomes larger and contiguous with the intracellular solution. The X-ray structure of the calcium-activated potassium channel MthK, which was crystallized in the open state, is used to construct models of the KcsA channel in the open state. It is found that, as the channel opens, the barrier at the helix bundle crossing decreases to approximately 0 kcal/mol, but that the ion in the cavity is also significantly destabilized. The results are compared and contrasted with additional calculations performed on the KvAP (voltage-activated) and KirBac1.1 (inward rectifier) channels, as well as models of the pore domain of Shaker in the open and closed state. In conclusion, electrostatic factors give rise to energetic constraints on ion permeation that have important functional consequences on the various K+ channels, and partly explain the presence or absence of charged residues near the inner vestibular entry.  相似文献   
2.
KvAP is a voltage-gated tetrameric K(+) channel with six transmembrane (S1-S6) segments in each monomer from the archaeon Aeropyrum pernix. The objective of the present investigation was to understand the plausible role of the S6 segment, which has been proposed to form the inner lining of the pore, in the membrane assembly and functional properties of KvAP channel. For this purpose, a 22-residue peptide, corresponding to the S6 transmembrane segment of KvAP (amino acids 218-239), and a scrambled peptide (S6-SCR) with rearrangement of only hydrophobic amino acids but without changing its composition were synthesized and characterized structurally and functionally. Although both peptides bound to the negatively charged phosphatidylcholine/phosphatidylglycerol model membrane with comparable affinity, significant differences were observed between these peptides in their localization, self-assembly, and aggregation properties onto this membrane. S6-SCR also exhibited reduced helical structures in SDS micelles and phosphatidylcholine/phosphatidylglycerol lipid vesicles as compared with the S6 peptide. Furthermore, the S6 peptide showed significant membrane-permeabilizing capability as evidenced by the release of calcein from the calcein-entrapped lipid vesicles, whereas S6-SCR showed much weaker efficacy. Interestingly, although the S6 peptide showed ion channel activity in the bilayer lipid membrane, despite having the same amino acid composition, S6-SCR was significantly inactive. The results demonstrated sequence-specific structural and functional properties of the S6 wild type peptide. The selected S6 segment is probably an important structural element that could play an important role in the membrane interaction, membrane assembly, and functional property of the KvAP channel.  相似文献   
3.
Inactivation is a fundamental property of voltage-gated ion channels. Fast inactivation of Na(+) channels involves channel block by the III-IV cytoplasmic interdomain linker. The mechanisms of nonfast types of inactivation (intermediate, slow, and ultraslow) are unclear, although the ionic environment and P-loops rearrangement appear to be involved. In this study, we employed a TTX-based P-loop domain model of a sodium channel and the MCM method to investigate a possible role of P-loop rearrangement in the nonfast inactivation. Our modeling predicts that Na(+) ions can bind between neighboring domains in the outer-carboxylates ring EEDD, forming an ordered structure with interdomain contacts that stabilize the conducting conformation of the outer pore. In this model, the permeant ions can transit between the EEDD ring and the selectivity filter ring DEKA, retaining contacts with at least two carboxylates. In the absence of Na(+), the electrostatic repulsion between the EEDD carboxylates disrupts the permeable configuration. In this Na(+)-deficient model, the region between the EEDD and DEKA rings is inaccessible for Na(+) but is accessible for TMA. Taken together, these results suggest that Na(+)-saturated models are consistent with experimental characteristics of the open channels, whereas Na(+)-deficient models are consistent with experimentally defined properties of the slow-inactivated channels. Our calculations further predict that binding of LAs to the inner pore would depend on whether Na(+) occupies the DEKA ring. In the absence of Na(+) in the DEKA ring, the cationic group of lidocaine occurs in the focus of the pore helices' macrodipoles and would prevent occupation of the ring by Na(+). Loading the DEKA ring with Na(+) results in the electrostatic repulsion with lidocaine. Thus, there are antagonistic relations between a cationic ligand bound in the inner pore and Na(+) in the DEKA ring.  相似文献   
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