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The internal vestibule of large-conductance [Ca.sup.2+] voltage-activated [K.sup.+] (BK) channels contains a ring of eight negative charges not present in [K.sup.+] channels of lower conductance (Glu386 and Glu389 in hSlo) that modulates channel conductance through an electrostatic mechanism (Brelidze, T.I., X. Niu, and K.L. Magleby. 2003. Proc. NatL Acad. Sci. USA. 100:9017-9022). In BK channels there are also two acidic amino acid residues in an extracellular loop (Asp326 and Glu329 in hSlo). To determine the electrostatic influence of these charges on channel conductance, we expressed wild-type BK channels and mutants E386N/E389N, D326N, E329Q, and D326N/E329Q channels on Xenopus laevis oocytes, and measured the expressed currents under patch clamp. Contribution of E329 to the conductance is negligible and single channel conductance of D326N/E329Q channels measured at 0 mV in symmetrical 110 mM [K.sup.+] was 18% lower than the control. Current-voltage curves displayed weak outward rectification for D326N and the double mutant. The conductance differences between the mutants and wild-type BK were caused by an electrostatic effect since they were enhanced at low [K.sup.+] (30 mM) and vanished at high [K.sup.+] (1 M [K.sup.+]). We determine the electrostatic potential change, [DELTA][phi], caused by the charge neutralization using [TEA.sup.+] block for the extracellular charges and [Ba.sup.2+] for intracellular charges. We measured 13 [+ or -] 2 mV for [DELTA][phi] at the [TEA.sup.+] site when turning off the extracellular charges, and 17 [+ or -] 2 mV for the [DELTA][phi] at the [Ba.sup.2+] site when the intracellular charges were turned off. To understand the electrostatic effect of charge neutralizations, we determined [DELTA][phi] using a BK channel molecular model embedded in a lipid bilayer and solving the Poisson-Boltzmann equation. The model explains the experimental results adequately and, in particular, gives an economical explanation to the differential effect on the conductance of the neutralization of charges D326 and E329.

In neurosecretion, allosteric communication between voltage sensors and Ca2+ binding in BK channels is crucially involved in damping excitatory stimuli. Nevertheless, the voltage-sensing mechanism of BK channels is still under debate. Here, based on gating current measurements, we demonstrate that two arginines in the transmembrane segment S4 (R210 and R213) function as the BK gating charges. Significantly, the energy landscape of the gating particles is electrostatically tuned by a network of salt bridges contained in the voltage sensor domain (VSD). Molecular dynamics simulations and proton transport experiments in the hyperpolarization-activated R210H mutant suggest that the electric field drops off within a narrow septum whose boundaries are defined by the gating charges. Unlike Kv channels, the charge movement in BK appears to be limited to a small displacement of the guanidinium moieties of R210 and R213, without significant movement of the S4. [ABSTRACT FROM AUTHOR]

Research has been conducted on Saccharomyces cerevisiae lysine 213 and histidine 233. The role of these residues in Mn (super)2+ binding and in catalysis has been investigated and the results demonstrate that mutation of lysine 213 and histidine 233 affects catalysis and that they are required for proper Mn (super)2+ binding.

The differential pulse polarography was used to analyze the molecular interactions of progesterone with [beta]-cyclodextrin ([beta]-CD). The preferred orientation for the complex formation was found to be at positions where the acetyl group of the progesterone is nearer to the primary hydroxyl rim to the cyclodextrin cavity.

Large-conductance Ca2+- and voltage-activated K+ (BK) channels are involved in a large variety of physiological processes. Regulatory β-subunits are one of the mechanisms responsible for creating BK channel diversity fundamental to the adequate function of many tissues. However, little is known about the structure of its voltage sensor domain. Here, we present the external architectural details of BK channels using lanthanide-based resonance energy transfer (LRET). We used a genetically encoded lanthanide-binding tag (LBT) to bind terbium as a LRET donor and a fluorophore-labeled iberiotoxin as the LRET acceptor for measurements of distances within the BK channel structure in a living cell. By introducing LBTs in the extracellular region of the α- or β1-subunit, we determined (i) a basic extracellular map of the BK channel, (ii) β1-subunit-induced rearrangements of the voltage sensor in α-subunits, and (iii) the relative position of the β1-subunit within the α/β1-subunit complex. [ABSTRACT FROM AUTHOR]

Large-conductance Ca(2+)- and voltage-activated K(+) (BK) channels are involved in a large variety of physiological processes. Regulatory β-subunits are one of the mechanisms responsible for creating BK channel diversity fundamental to the adequate function of many tissues. However, little is known about the structure of its voltage sensor domain. Here, we present the external architectural details of BK channels using lanthanide-based resonance energy transfer (LRET). We used a genetically encoded lanthanide-binding tag (LBT) to bind terbium as a LRET donor and a fluorophore-labeled iberiotoxin as the LRET acceptor for measurements of distances within the BK channel structure in a living cell. By introducing LBTs in the extracellular region of the α- or β1-subunit, we determined (i) a basic extracellular map of the BK channel, (ii) β1-subunit-induced rearrangements of the voltage sensor in α-subunits, and (iii) the relative position of the β1-subunit within the α/β1-subunit complex.