Very specific protein-salt interactions are involved in a multitude of biological phenomena such as protein folding/stability, enzymatic activity, and signal transduction events. In this work, we used two very simple, protein-mimic model biopolymers to obtain a better understanding of specific cation effects operating in aqueous protein environments. The two biopolymers used were Elastin-like Polypeptides (ELPs) and poly(N-isopropylacrylamide) (PNIPAM). ELPs are an especially an ideal model system as these polypeptides can be easily genetically engineered to observe the effect of specific amino acid residues and peptide chain length on these salt interactions. Both of these biopolymers are also highly thermoresponsive as their aqueous solutions undergo a hydrophobic collapse/aggregation induced phase transition process above a lower critical solution temperature (LCST). Thermodynamic measurements of these biopolymers were carried out under various salt solution conditions. Additionally, both of these biopolymers are suitable for making surface specific spectroscopic measurements. Vibrational sum frequeny spectroscopy (VSFS), a non-linear interface sensitive spectroscopic technique, was employed here to investigate biologically relevant cation interactions which occur at peptide/protein surfaces. First, the LCST response of a non-polar ELP and a neutral biopolymer, PNIPAM, was investigated in the presence of 12 different alkali, alkaline-earth metal and transition metal chloride salts. Even though the salt interactions for uncharged proteins are dominated by anions, subtle specific cation effects were also observed. The results followed a direct Hofmeister series for cations. Most alkali cations are excluded from the polar amide regions of proteins. More polarizable cations, however, can solvate the hydrophobic moieties and somewhat counter the salting-out effect of the chloride anion. More charged and hydrated ions like lithium and divalent cations showed a weak interaction to the amide moiety through their hydration shell. The role of acidic amino acid residues in inducing cation specificities was investigated using an aspartate-rich ELP system. Both thermodynamic and spectroscopic data conclusively proved that the negative charge on protein surfaces is the main driving force for cation partitioning and specificity under physiological relevant concentration regimes. Apparent binding constants of carboxylate moieties with cations were determined. This is the first quantitative and thoroughly systematic study of such biologically relevant cation-carboxylate interactions prevalent in enzyme active sites and protein surfaces.

he extent of BiInO₃ substitution in the perovskite system xBiInO(₃)-(1 - x)PbTiO₃ and the corresponding raise in the transition temperature were investigated using thermal analysis, dielectric measurements, x-ray diffraction, and electron microscopy. Maximum tetragonal perovskite distortion (c/a = 1.082) was obtained for x = 0.20, with a corresponding Curie temperature of 582°C. Phase-pure tetragonal perovskite was obtained for x less than or equal to 0.25. Compound formation after calcining mixed oxide powders resulted in agglomerated cube-shaped tetragonal perovskite particles, which could be fired to 94.7% of theoretical density (TD). Niobium-modified BIPT ceramics with PT contents of 80% and 85% were found to possess significantly lower dielectric loss at elevated temperatures, making it possible to polarize the materials. Piezoelectric properties were measured for a 1.5 mol% Nb -0.15BI-0.85PT composition with a transition temperature of 542°C; the longitudinal piezoelectric coefficient and coercive field were found to be 60 pC/N and 125 kV/cm, respectively. Compositions of xBiLaO₃-(1 − x)PbTiO₃ over the range 0 < x < 0.225 were calcined and sintered. Dielectric constant with temperature and differential scanning calorimetry measurements were in excellent agreement with respect to a Curie-like tetragonal to cubic transformations starting at 495°C for pure PbTiO₃, shifting to lower temperatures with increasing x. For compositions of x > 0.05, a second higher-temperature (∼600°C) endotherm, and matching dielectric anomaly, were consistently observed, for which there were no structural changes indicated by hot-stage x-ray diffraction. This transformation was interpreted to be similar to a Curie transformation in relaxor ferroelectrics in which localized segregation of B-site cations (below the resolution limit of x-ray diffraction) facilitated ferroelectric behavior.

Thesis (Ph. D.)--University of Texas at Austin, 2008. / Vita. Includes bibliographical references.

Thesis (Ph. D.)--University of Washington, 2004. / Vita. Includes bibliographical references (p. 153-161).

Thesis (Ph. D.)--University of Missouri-Columbia, 1998. / Typescript. Vita. Includes bibliographical references (leaves 217-223). Also available on the Internet.

Thesis (Ph. D.)--University of Missouri-Columbia, 1998. / Typescript. Vita. Includes bibliographical references (leaves 217-223). Also available on the Internet.

Thesis (Ph. D.)--University of Texas at Austin, 2004. / Supervisor: Peter F. Green. Vita. Includes bibliographical references.

Thesis (Ph. D.)--University of Texas at Austin, 2006. / Vita. Includes bibliographical references.

O estudo do processo de fusão e solidificação da água contida dentro de materiais confinantes tem sido amplamente discutido em química, biologia, física, geologia, e com diversas aplicações tecnológicas, tais como aplicação na fabricação de etanol de segunda geração, ou etanol celulósico, separação de fases, fabricação de nanomateriais. Pesquisas mostraram que as temperaturas de transição da água nanoconfinada são muito sensíveis ao diâmetro do poro, mas que podem ser pouco afetadas pela natureza, hidrofóbica ou hidrofílica, da superfície do poro. Outra importante constatação em experimentos de fusão e congelamento em nanoporos é que nem toda água presente nos poros pode ser cristalizada até gelo. A existência de uma camada de água pré-fundida em nanoporos tem sido confirmada através de experimentos. Com o objetivo de entender mais profundamente como a temperatura de transição da água confinada depende da natureza da parede confinante e do tamanho do confinamento, propõe-se um modelo de nanoporos de celulose para o confinamento, onde varia-se o diâmetro e comprimento do nanoporo, além da natureza da parede do nanoporo. Nossos estudos, mostram que para sistemas hidrofóbicos, com formação de camada de água líquida na parede, as temperaturas de transição variam desde relativamente baixas, para menores valores de calor latente, até atingindo a temperatura de transição da água bulk, para calor latente mais alto. Enquanto que para sistemas hidrofílicos, para nenhum dos valores de calor latente trabalhados, e para nenhum tamanho do sistema, a temperatura de transição atinge o valor de bulk. / The study of the fusion process and water solidification inside confining materials has been widely discussed in Chemistry, Biology, Physics, and Geology, and has various technological applications as the usage and fabrication of second generation ethanol or cellulosic ethanol, phase separation, and nanomaterials fabrications. Researches have shown that nanoconfined water’s transition temperature are highly sensitive to the pore. Another interesting remark on freezing and fusion experiments on nanopores is that not all water present in pores can be crystallized into ice. The existence of a water layer pre-melted on nanopores has been confirmed through experiments. Aiming at understanding deeply how water’s transition temperature depends on the nature of the confining wall and size, a cellulose nanopore model is proposed to the confinement, where the nanopore diameter and length are varied, besides the nature of the wall of the nanopore. Our studies show that for hydrophobic systems, with the liquid water layer formation on the wall, the transition temperatures vary from relatively low latent heat to smaller values, even reaching the temperature transition on bulk water to higher latent heat. While for hydrophilic systems, for none of the latent heat used and no system size the transition temperature reaches bulk value.

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