39 research outputs found

    Mapping alterations to the endogenous elemental distribution within the lateral ventricles and choroid plexus in brain disorders using X-ray fluorescence imaging

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    The choroid plexus and cerebral ventricles are critical structures for the production of cerebral spinal fluid (CSF) and play an important role in regulating ion and metal transport in the brain, however many aspects of its roles in normal physiology and disease states, such as psychiatric illness, remain unknown. The choroid plexus is difficult to examine in vivo, and in situ ex vivo, and as such has typically been examined indirectly with radiolabeled tracers or ex vivo stains, making measurements of the endogenous K+, Cl-, and Ca+ distributions unreliable. In the present study, we directly examined the distribution of endogenous ions and biologically relevant transition metals in the choroid plexus and regions surrounding the ventricles (ventricle wall, cortex, corpus callosum, striatum) using X-ray fluorescence imaging (XFI). We find that the choroid plexus was rich in Cl- and Fe while K+ levels increase further from the ventricle as Cl- levels decrease, consistent with the known role of ion transporters in the choroid plexus CSF production. A polyI:C offspring displayed enlarged ventricles, elevated Cl- surrounding the ventricles, and intraventricular calcifications. These observations fit with clinical findings in patients with schizophrenia and suggest maternal treatment with polyI:C may lead to dysfunctional ion regulation in offspring. This study demonstrates the power of XFI for examining the endogenous elemental distributions of the ventricular system in healthy brain tissue as well as disease models

    Elemental and chemically specific x-ray fluorescence imaging of biological systems

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    Modeling by Assembly and Molecular Dynamics Simulations of the Low Cu2+ Occupancy Form of the Mammalian Prion Protein Octarepeat Region: Gaining Insight into Cu2+-Mediated β-Cleavage

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    The prion protein has garnered considerable interest because of its involvement in prion disease as well as its unresolved cellular function. The octarepeat region in the flexible N-domain is capable of binding copper through multiple coordination modes. Under conditions of low pH and low Cu2+ concentration, the four octarepeats (ORs) cooperatively coordinate a single copper ion. Based on the average structure of the PHGG and GWGQ portions of a copper-free OR2 model from molecular dynamics simulations, the starting structures of the OR4 complex could be constructed by assembling the repeating structure of PHGG and GWGQ fragments. The resulting model contains a preformed site suitable for Cu2+ coordination. Molecular dynamics simulations of Cu2+ bound to the assembled OR4 model (Cu:OR4) reveal a close association of specific Trp and Gly residues with the Cu2+ center. This low Cu2+-occupancy form of prion protein is redox-active and can readily initiate cleavage of the OR region, mediated by reactive oxygen species generated by Cu+. The OR region is known to be required for β-cleavage, as are the Trp residues within the OR region. The β-cleaved form of the prion protein accumulates in amyloid fibrils. Hence, the close approach of Trp and Gly residues to the Cu2+ coordination site in the low Cu2+-occupancy form of the OR region may signal an important interaction for the initiation of prion disease

    High Affinity Binding of Indium and Ruthenium Ions by Gastrins

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    <div><p>The peptide hormone gastrin binds two ferric ions with high affinity, and iron binding is essential for the biological activity of non-amidated forms of the hormone. Since gastrins act as growth factors in gastrointestinal cancers, and as peptides labelled with Ga and In isotopes are increasingly used for cancer diagnosis, the ability of gastrins to bind other metal ions was investigated systematically by absorption spectroscopy. The coordination structures of the complexes were characterized by extended X-ray absorption fine structure (EXAFS) spectroscopy. Changes in the absorption of gastrin in the presence of increasing concentrations of Ga<sup>3+</sup> were fitted by a 2 site model with dissociation constants (K<sub>d</sub>) of 3.3 x 10<sup>−7</sup> and 1.1 x 10<sup>−6</sup> M. Although the absorption of gastrin did not change upon the addition of In<sup>3+</sup> ions, the changes in absorbance on Fe<sup>3+</sup> ion binding in the presence of indium ions were fitted by a 2 site model with K<sub>d</sub> values for In<sup>3+</sup> of 6.5 x 10<sup>−15</sup> and 1.7 x 10<sup>−7</sup> M. Similar results were obtained with Ru<sup>3+</sup> ions, although the K<sub>d</sub> values for Ru<sup>3+</sup> of 2.6 x 10<sup>−13</sup> and 1.2 x 10<sup>−5</sup> M were slightly larger than observed for In<sup>3+</sup>. The structures determined by EXAFS all had metal:gastrin stoichiometries of 2:1 but, while the metal ions in the Fe, Ga and In complexes were bridged by a carboxylate and an oxygen with a metal-metal separation of 3.0–3.3 Å, the Ru complex clearly demonstrated a short range Ru—Ru separation, which was significantly shorter, at 2.4 Å, indicative of a metal-metal bond. We conclude that gastrin selectively binds two In<sup>3+</sup> or Ru<sup>3+</sup> ions, and that the affinity of the first site for In<sup>3+</sup> or Ru<sup>3+</sup> ions is higher than for ferric ions. Some of the metal ion-gastrin complexes may be useful for cancer diagnosis and therapy.</p></div

    Proposed structural models of FeIII2Ggly and RuIII2Ggly.

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    <p>The model for Fe<sup>III</sup><sub>2</sub>Ggly (A) is based on the EXAFS data presented in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.g005" target="_blank">Fig 5B</a>, and is consistent with previous NMR and visible spectroscopic studies of Ggly and mutant peptides.[<a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.ref008" target="_blank">8</a>,<a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.ref009" target="_blank">9</a>,<a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.ref012" target="_blank">12</a>] The two Fe<sup>III</sup> ions are coordinated by the carboxylate side chains likely from glutamates 6, 7, 8, 9 and 10, with glutamate 7 acting as a ligand to both Fe<sup>III</sup> ions. One or more oxygens also act as bridging ligands between the two Fe<sup>III</sup> ions. The peptide backbone and non-coordinating side chains have been omitted for simplicity. The model for Ru<sup>III</sup><sub>2</sub>Ggly (B) is based on the EXAFS data presented in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.g005" target="_blank">Fig 5H</a>, and differs from the model for Fe<sup>III</sup><sub>2</sub>Ggly in the presence of a Ru≡Ru bond and a chloride ion ligand.</p

    Ruthenium ions compete with ferric ions for the gastrin binding sites.

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    <p>Addition of aliquots of ruthenium chloride (black ▼) to 10 μM Gamide or Gly in the buffer described in the <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.g002" target="_blank">Fig 2</a> legend resulted in an increase in absorbance at 280 nm which was significantly less than the changes seen on addition of aliquots of ferric chloride (red π). However in the presence of 5.30 (green ⬛) or 26.48 μM (blue •) ruthenium chloride the changes in absorbance seen on addition of aliquots of ferric chloride were considerably different from the changes seen in the absence of ruthenium chloride. The points are means from three separate experiments; bars represent the SEM. The lines were constructed with the dissociation constants and maximum absorbance values (<a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.t001" target="_blank">Table 1</a>) obtained by fitting the data to the 2 site competitive model shown in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.g001" target="_blank">Fig 1</a> with the program BioEqs.</p

    Models of metal ion binding.

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    <p>In the 2 site model gastrin binds two metal ions with dissociation constants K<sub>d1M</sub> and K<sub>d2M</sub>. In the 2 site competitive model gastrin binds two ferric ions with dissociation constants K<sub>d1Fe</sub> and K<sub>d2Fe</sub>, and two metal ions (M) to the same two sites with dissociation constants K<sub>d1M</sub> and K<sub>d2M</sub>. The dissociation constant K<sub>d3M</sub> describes the formation of the mixed FeGastrinM complex.</p

    Indium ions compete with ferric ions for the gastrin binding sites.

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    <p>Addition of aliquots of indium nitrate (black ▼) to 10 μM Gamide or Ggly in the buffer described in the <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.g002" target="_blank">Fig 2</a> legend resulted in little change in absorbance at 280 nm when compared to the changes seen on addition of aliquots of ferric chloride (red π). However in the presence of 3.99 (green ⬛) or 39.85 μM (blue •) indium nitrate the changes in absorbance seen on addition of aliquots of ferric chloride were considerably different from the changes seen in the absence of indium nitrate. The points are means from three separate experiments; bars represent the SEM. The lines were constructed with the dissociation constants and maximum absorbance values (<a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.t001" target="_blank">Table 1</a>) obtained by fitting the data to the 2 site competitive model shown in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0140126#pone.0140126.g001" target="_blank">Fig 1</a> with the program BioEqs.</p
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