4,406 research outputs found

    Stochastic Modeling of Ca2+-Channel / BKCa-Channel Complexes

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    Frontiers in the Ca2+ Regulation of the BKca Channel

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    The BKCa Channel's Ca2+-binding Sites, Multiple Sites, Multiple Ions

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    Gating and Ionic Currents Reveal How the BKCa Channel's Ca2+ Sensitivity Is Enhanced by its β1 Subunit

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    Large-conductance Ca2+-activated K+ channels (BKCa channels) are regulated by the tissue-specific expression of auxiliary β subunits. β1 is predominately expressed in smooth muscle, where it greatly enhances the BKCa channel's Ca2+ sensitivity, an effect that is required for proper regulation of smooth muscle tone. Here, using gating current recordings, macroscopic ionic current recordings, and unitary ionic current recordings at very low open probabilities, we have investigated the mechanism that underlies this effect. Our results may be summarized as follows. The β1 subunit has little or no effect on the equilibrium constant of the conformational change by which the BKCa channel opens, and it does not affect the gating charge on the channel's voltage sensors, but it does stabilize voltage sensor activation, both when the channel is open and when it is closed, such that voltage sensor activation occurs at more negative voltages with β1 present. Furthermore, β1 stabilizes the active voltage sensor more when the channel is closed than when it is open, and this reduces the factor D by which voltage sensor activation promotes opening by ∼24% (16.8→12.8). The effects of β1 on voltage sensing enhance the BKCa channel's Ca2+ sensitivity by decreasing at most voltages the work that Ca2+ binding must do to open the channel. In addition, however, in order to fully account for the increase in efficacy and apparent Ca2+ affinity brought about by β1 at negative voltages, our studies suggest that β1 also decreases the true Ca2+ affinity of the closed channel, increasing its Ca2+ dissociation constant from ∼3.7 μM to between 4.7 and 7.1 μM, depending on how many binding sites are affected

    Small Energy Scale for Mixed-Valent Uranium Materials

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    We investigate a two-channel Anderson impurity model with a 5f15f^1 magnetic and a 5f25f^2 quadrupolar ground doublet, and a 5f25f^2 excited triplet. Using the numerical renormalization group method, we find a crossover to a non-Fermi liquid state below a temperature TT^* varying as the 5f25f^2 triplet-doublet splitting to the 7/2 power. To within numerical accuracy, the non-linear magnetic susceptibility and the 5f15f^1 contribution to the linear susceptibility are given by universal one-parameter scaling functions. These results may explain UBe13_{13} as mixed valent with a small crossover scale TT^*.Comment: 4 pages, 3 figures, REVTeX, to appear in Phys. Rev. Let

    Reply to ``Comment on `Insulating Behavior of λ\lambda-DNA on the Micron Scale' "

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    In our experiment, we found that the resistance of vacuum-dried λ\lambda-DNA exceeds 1014Ω10^{14} \Omega at 295 K. Bechhoefer and Sen have raised a number of objections to our conclusion. We provide counter arguments to support our original conclusion.Comment: 1 page reply to comment, 1 figur

    Measurements of the BKCa Channel's High-Affinity Ca2+ Binding Constants: Effects of Membrane Voltage

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    It has been established that the large conductance Ca2+-activated K+ channel contains two types of high-affinity Ca2+ binding sites, termed the Ca2+ bowl and the RCK1 site. The affinities of these sites, and how they change as the channel opens, is still a subject of some debate. Previous estimates of these affinities have relied on fitting a series of conductance–voltage relations determined over a series of Ca2+ concentrations with models of channel gating that include both voltage sensing and Ca2+ binding. This approach requires that some model of voltage sensing be chosen, and differences in the choice of voltage-sensing model may underlie the different estimates that have been produced. Here, to better determine these affinities we have measured Ca2+ dose–response curves of channel activity at constant voltage for the wild-type mSlo channel (minus its low-affinity Ca2+ binding site) and for channels that have had one or the other Ca2+ binding site disabled via mutation. To accurately determine these dose–response curves we have used a series of 22 Ca2+ concentrations, and we have used unitary current recordings, coupled with changes in channel expression level, to measure open probability over five orders of magnitude. Our results indicate that at −80 mV the Ca2+ bowl has higher affinity for Ca2+ than does the RCK1 site in both the opened and closed conformations of the channel, and that the binding of Ca2+ to the RCK1 site is voltage dependent, whereas at the Ca2+ bowl it is not

    Elimination of the BKCa Channel's High-Affinity Ca2+ Sensitivity

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    We report here a combination of site-directed mutations that eliminate the high-affinity Ca2+ response of the large-conductance Ca2+-activated K+ channel (BKCa), leaving only a low-affinity response blocked by high concentrations of Mg2+. Mutations at two sites are required, the “Ca2+ bowl,” which has been implicated previously in Ca2+ binding, and M513, at the end of the channel's seventh hydrophobic segment. Energetic analyses of mutations at these positions, alone and in combination, argue that the BKCa channel contains three types of Ca2+ binding sites, one of low affinity that is Mg2+ sensitive (as has been suggested previously) and two of higher affinity that have similar binding characteristics and contribute approximately equally to the power of Ca2+ to influence channel opening. Estimates of the binding characteristics of the BKCa channel's high-affinity Ca2+-binding sites are provided
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