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<prism:eIssn>1540-7748</prism:eIssn>
<prism:publicationName>The Journal of General Physiology</prism:publicationName>
<prism:issn>0022-1295</prism:issn>
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<title>The Journal of General Physiology</title>
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<link>http://www.jgp.org</link>
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<item rdf:about="http://www.jgp.org/cgi/content/short/jgp.200810024v1?rss=1">
<title><![CDATA[Nav1.4 Deregulation in Dystrophic Skeletal Muscle Leads to Na+ Overload and Enhanced Cell Death]]></title>
<link>http://www.jgp.org/cgi/content/short/jgp.200810024v1?rss=1</link>
<description><![CDATA[<p>Duchenne muscular dystrophy (DMD) is a hereditary degenerative disease manifested by the absence of dystrophin, a structural, cytoskeletal protein, leading to muscle degeneration and early death through respiratory and cardiac muscle failure. Whereas the rise of cytosolic Ca<sup>2+</sup> concentrations in muscles of <I>mdx</I> mouse, an animal model of DMD, has been extensively documented, little is known about the mechanisms causing alterations in Na<sup>+</sup> concentrations. Here we show that the skeletal muscle isoform of the voltage-gated sodium channel, Na<SUB>v</SUB>1.4, which represents over 90% of voltage-gated sodium channels in muscle, plays an important role in development of abnormally high Na<sup>+</sup> concentrations found in muscle from <I>mdx</I> mice. The absence of dystrophin modifies the expression level and gating properties of Na<SUB>v</SUB>1.4, leading to an increased Na<sup>+</sup> concentration under the sarcolemma. Moreover, the distribution of Na<SUB>v</SUB>1.4 is altered in <I>mdx</I> muscle while maintaining the colocalization with one of the dystrophin-associated proteins, syntrophin -1, thus suggesting that syntrophin is an important linker between dystrophin and Na<SUB>v</SUB>1.4. Additionally, we show that these modifications of Na<SUB>v</SUB>1.4 gating properties and increased Na<sup>+</sup> concentrations are strongly correlated with increased cell death in <I>mdx</I> fibers and that both cell death and Na<sup>+</sup> overload can be reversed by 3 nM tetrodotoxin, a specific Na<SUB>v</SUB>1.4 blocker.</p>]]></description>
<dc:creator><![CDATA[Hirn, C., Shapovalov, G., Petermann, O., Roulet, E., Ruegg, U. T.]]></dc:creator>
<dc:date>2008-07-14</dc:date>
<dc:identifier>info:doi/10.1085/jgp.200810024</dc:identifier>
<dc:title><![CDATA[Nav1.4 Deregulation in Dystrophic Skeletal Muscle Leads to Na+ Overload and Enhanced Cell Death]]></dc:title>
<dc:publisher>The Rockefeller University Press</dc:publisher>
<prism:publicationDate>2008-07-14</prism:publicationDate>
<prism:section>Articles</prism:section>
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<item rdf:about="http://www.jgp.org/cgi/content/short/jgp.200810008v1?rss=1">
<title><![CDATA[Linking Exponential Components to Kinetic States in Markov Models for Single-Channel Gating]]></title>
<link>http://www.jgp.org/cgi/content/short/jgp.200810008v1?rss=1</link>
<description><![CDATA[<p>Discrete state Markov models have proven useful for describing the gating of single ion channels. Such models predict that the dwell-time distributions of open and closed interval durations are described by mixtures of exponential components, with the number of exponential components equal to the number of states in the kinetic gating mechanism. Although the exponential components are readily calculated (Colquhoun and Hawkes, 1982, <I>Phil. Trans. R. Soc</I>. <I>Lond</I>. <I>B</I>. 300:1&ndash;59), there is little practical understanding of the relationship between components and states, as every rate constant in the gating mechanism contributes to each exponential component. We now resolve this problem for simple models. As a tutorial we first illustrate how the dwell-time distribution of all closed intervals arises from the sum of constituent distributions, each arising from a specific gating sequence. The contribution of constituent distributions to the exponential components is then determined, giving the relationship between components and states. Finally, the relationship between components and states is quantified by defining and calculating the linkage of components to states. The relationship between components and states is found to be both intuitive and paradoxical, depending on the ratios of the state lifetimes. Nevertheless, both the intuitive and paradoxical observations can be described within a consistent framework. The approach used here allows the exponential components to be interpreted in terms of underlying states for all possible values of the rate constants, something not previously possible.</p>]]></description>
<dc:creator><![CDATA[Shelley, C., Magleby, K. L.]]></dc:creator>
<dc:date>2008-07-14</dc:date>
<dc:identifier>info:doi/10.1085/jgp.200810008</dc:identifier>
<dc:title><![CDATA[Linking Exponential Components to Kinetic States in Markov Models for Single-Channel Gating]]></dc:title>
<dc:publisher>The Rockefeller University Press</dc:publisher>
<prism:publicationDate>2008-07-14</prism:publicationDate>
<prism:section>TUTORIAL RESEARCH ARTICLE</prism:section>
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<item rdf:about="http://www.jgp.org/cgi/content/short/jgp.200809978v1?rss=1">
<title><![CDATA[Voltage Clamp Fluorimetry Reveals a Novel Outer Pore Instability in a Mammalian Voltage-gated Potassium Channel]]></title>
<link>http://www.jgp.org/cgi/content/short/jgp.200809978v1?rss=1</link>
<description><![CDATA[<p>Voltage-gated potassium (Kv) channel gating involves complex structural rearrangements that regulate the ability of channels to conduct K<sup>+</sup> ions. Fluorescence-based approaches provide a powerful technique to directly report structural dynamics underlying these gating processes in <I>Shaker</I> Kv channels. Here, we apply voltage clamp fluorimetry, for the first time, to study voltage sensor motions in mammalian Kv1.5 channels. Despite the homology between Kv1.5 and the <I>Shaker</I> channel, attaching TMRM or PyMPO fluorescent probes to substituted cysteine residues in the S3&ndash;S4 linker of Kv1.5 (M394C-V401C) revealed unique and unusual fluorescence signals. Whereas the fluorescence during voltage sensor movement in <I>Shaker</I> channels was monoexponential and occurred with a similar time course to ionic current activation, the fluorescence report of Kv1.5 voltage sensor motions was transient with a prominent rapidly dequenching component that, with TMRM at A397C (equivalent to <I>Shaker</I> A359C), represented 36 &plusmn; 3% of the total signal and occurred with a <I></I> of 3.4 &plusmn; 0.6 ms at +60 mV (<I>n</I> = 4). Using a number of approaches, including 4-AP drug block and the ILT triple mutation, which dissociate channel opening from voltage sensor movement, we demonstrate that the unique dequenching component of fluorescence is associated with channel opening. By regulating the outer pore structure using raised (99 mM) external K<sup>+</sup> to stabilize the conducting configuration of the selectivity filter, or the mutations W472F (equivalent to <I>Shaker</I> W434F) and H463G to stabilize the nonconducting (P-type inactivated) configuration of the selectivity filter, we show that the dequenching of fluorescence reflects rapid structural events at the selectivity filter gate rather than the intracellular pore gate.</p>]]></description>
<dc:creator><![CDATA[Vaid, M., Claydon, T. W., Rezazadeh, S., Fedida, D.]]></dc:creator>
<dc:date>2008-07-14</dc:date>
<dc:identifier>info:doi/10.1085/jgp.200809978</dc:identifier>
<dc:title><![CDATA[Voltage Clamp Fluorimetry Reveals a Novel Outer Pore Instability in a Mammalian Voltage-gated Potassium Channel]]></dc:title>
<dc:publisher>The Rockefeller University Press</dc:publisher>
<prism:publicationDate>2008-07-14</prism:publicationDate>
<prism:section>Articles</prism:section>
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