2 resultados para Water ethanol 1-butyl-3-methylimidazolium bis(trifluoromethanesulfonyl)imide

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<p>The (He<sup>3</sup>, n) reactions on B<sup>11</sup>, N<sup>15</sup>, O<sup>16</sup>, and O<sup>18</sup> targets have been studied using a pulsed-beam time-of-flight spectrometer. Special emphasis was placed upon the determination of the excitation energies and properties of states with T = 1 (in Ne<sup>18</sup>), T = 3/2 (in N<sup>13</sup> and F<sup>17</sup>) and T = 2 (in Ne<sup>20</sup>). The identification of the T = 3/2 and T = 2 levels is based on the structure of these states as revealed by intensities and shapes of angular distributions. The reactions are interpreted in terms of double stripping theory. Angular distributions have been compared with plane and distorted wave stripping theories. Results for the four reactions are summarized below: </p> <p>1) O<sup>16</sup> (He<sup>3</sup>, n). The reaction has been studied at incident energies up to 13.5 MeV and two previously unreported levels in Ne<sup>18</sup> were observed at E<sub>x</sub> = 4.55 ± .015 MeV (Î = 70 ± 30 keV) and E<sub>x</sub> = 5.14 ± .018 MeV (Î = 100 ± 40 keV).</p> <p>2) B<sup>11</sup> (He<sup>3</sup>, n). The reaction has been studied at incident energies up to 13.5 MeV. Three T = 3/2 levels in N<sup>13</sup> have been identified at E<sub>x</sub> = 15.068 ± .008 MeV (Î Ë 15 keV), E<sub>x</sub> = 18.44 ± .04, and E<sub>x</sub> 18.98 ± .02 MeV (Î = 40 ± 20 keV).</p> <p>3) N<sup>15</sup> (He<sup>3</sup>, n). The reaction has been studied at incident energies up to 11.88 MeV. T = 3/2 levels in F<sup>17</sup> have been identified at E<sub>x</sub> = 11.195 ± .007 MeV (Î Ë 20 keV), E<sub>x</sub> = 12.540 ± .010 MeV (Î Ë 25 keV), and E<sub>x</sub> = 13.095 ± .009 MeV (Î Ë 25 keV). </p> <p>4) O<sup>18</sup> (He<sup>3</sup>, n). The reaction has been studied at incident energies up to 9.0 MeV. The excitation energy of the lowest T = 2 level in Ne<sup>20</sup> has been found to be 16.730 ± .006 MeV (Î Ë 20 keV). </p> <p>Angular distributions of the transitions leading to the above higher isospin states are well described by double stripping theory. Analog correspondences are established by comparing the present results with recent studies (t, p) and (He<sup>3</sup>, p) reactions on the same targets. </p>

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Meeting the world's growing energy demands while protecting our fragile environment is a challenging issue. Second generation biofuels are liquid fuels like long-chain alcohols produced from lignocellulosic biomass. To reduce the cost of biofuel production, we engineered fungal family 6 cellobiohydrolases (Cel6A) for enhanced thermostability using random mutagenesis and recombination of beneficial mutations. During long-time hydrolysis, engineered thermostable cellulases hydrolyze more sugars than wild-type Cel6A as single enzymes and binary mixtures at their respective optimum temperatures. Engineered thermostable cellulases exhibit synergy in binary mixtures similar to wild-type cellulases, demonstrating the utility of engineering individual cellulases to produce novel thermostable mixtures. Crystal structures of the engineered thermostable cellulases indicate that the stabilization comes from improved hydrophobic interactions and restricted loop conformations by proline substitutions. At high temperature, free cysteines contribute to irreversible thermal inactivation in engineered thermostable Cel6A and wild-type Cel6A. The mechanism of thermal inactivation in this cellulase family is consistent with disulfide bond degradation and thiol-disulfide exchange. Enhancing the thermostability of Cel6A also increases tolerance to pretreatment chemicals, demonstrated by the strong correlation between thermostability and tolerance to 1-ethyl-3-methylimidazolium acetate. Several semi-rational protein engineering approaches &#8211; on the basis of consensus sequence analysis, proline stabilization, FoldX energy calculation, and high B-factors &#8211; were evaluated to further enhance the thermostability of Cel6A.