Spreading of dipalmitoyl phosphatidylcholine on the surface of sodium deoxycholate aqueous solution

The surface pressure vs. mokcular surface area relations for dipalmitoyl phosphatidylcholine (DPPC) insoluble monolayer and sodium deoxycholate (SDC) adsorbed monolayer,L and D1, respectively, were obtained from the analyses of surface tensions measured by the Wilhelmy glass plate. Also, D1 was obtained by a drop-weight method. Next, the surface pressure time course,(t), of the SDC aq. was measured by the Wilhelmy plate before and after DPPC was spread on the liquid surface. At DPPC spreading,(t) jumped to a maximum,, and decreased along an exponential curve. The values of with various surface amounts of DPPC and bulk concentrations of SDC were analyzed using a dual surface-region model. The model enabled the estimation of. For better fitting, modified relations were constructed in place of D1. The exponential decrease of(t) was also observed on the SDC adsorbed monolayer which was rapidly compressed by a moving barrier. The(t) relaxation rate constants of the SDC monolayers which were compressed by DPPC spreading and the moving barrier agreed with each other, suggesting a desorption of SDC from the surface.     

Diffusion-controlled stress-relaxation in polymers,I

Summary The “chemical” relaxation of stress either in Amilan (6-Nylon) or polyvinyl alcohol caused by penetration of water vapor was studied at 40% R. H. and temperatures 15, 30, and 50° C. A theory was presented of the chemical relaxation in a polymer which comprises penetrant-sensitive bonds as the crosslinkages between the molecular chains. This theory assumes the diffusion coefficient of penetrant in the polymer to he independent of concentration and any other factors. It was found that the system Amilan-water behaves in exact conformity with the theory over the ranges of elongation and temperature studied. The diffusion coefficient,D, of water in Amilan could thus be evaluated from the chemical relaxation data, using the theory presented, as functions of elongation and temperature. An ordinary sorption experiment was carried out for this system at 40% R. H. and 16.8° C and demonstrated that the diffusion of water in Amilan was Fickian with a constant diffusion coefficient. Both diffusion coefficients from the chemical relaxation data and the sorption. data were found to agree quite well when the former was extrapolated to zero-strain. The chemical relaxation behavior in the system polyvinyl alcohol-water was markedly different from that expected from the theory, suggesting primarily that the diffusion coefficient of water in this polymer was not constant. A parallel evidence for this fact was obtained from sorption measurements on this system, which demonstrated the diffusion in this system to be dependent both on concentration and time. From these results it may be concluded that the chemical relaxation technique, when combined properly with an adequate theory, can be used not only to evaluate the diffusion coefficient of penetrant in a given polymer solid but also to investigate, at least qualitatively, the type of sorption behavior characteristic of the system under given experimental conditions.

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Zusammenfassung Die chemische Spannungsrelaxation in Amilan (6-Nylon) und Polyvinylalkohol, verursacht durch Eindringen von Wasserdampf, wurde bei 40% r. F. und Temperaturen von 15, 30 und 50° C untersucht. Es wird eine Theorie der chemischen Relaxation von Polymeren vorgelegt, die als empfindliche Bindungen auf das eindringende Niedermolekulare die Vernetzungen zwischen den molekularen Ketten betrachtet. Diese Theorie setzt voraus, da? der Diffusionskoeffizient im Polymeren für die eindringende Substanz unabh?ngig von Konzentration und anderen Faktoren ist. Das System Amilan-Wasser benimmt sich vollkommen entsprechend dieser Theorie in den studierten Verstreckungs- und Temperaturbereiche. Der Diffusionskoeffizient von Wasser in Amilan konnte daher aus der chemischen Relaxation als Funktion von Dehnung und Temperatur ausgewertet werden. Ein normales Quellungsexperiment wurde für das System bei 40% r. F. und 16,8° C ausgeführt und zeigte, da? die Diffusion von Wasser in Amilan dem Fickschen Gesetz mit konstantem Diffusionskoeffizienten folgt. Beide Diffusionskoeffizienten, der aus chemischer Relaxation und der aus Quellungsdaten gewonnene, stimmten sehr gut überein, falls der erstere auf die Dehnung 0 extrapoliert wurde. Die chemische Relaxation des Systems Polyvinylalkohol-Wasser war merklich anders als nach der Theorie erwartet und lie? in erster Linie vermuten, da? der Diffusionskoeffizient von Wasser in diesem Polymeren nicht konstant ist. Eine entsprechende Andeutung wurde aus Quellungsmessungen an diesem System erhalten. Die Diffusion h?ngt von Konzentration und Zeit ab. Aus diesen Resultaten kann gefolgert werden, da? die Technik der Untersuchungen der chemischen Relaxation unter Verwendung einer geeigneten Theorie nicht nur dazu angewendet werden kann, Diffusionskoeffizienten von kleinen Molekülen in einem gegebenen festen Polymeren zu messen, sondern zumindest auch qualitativ den Typ des Quellungsverhaltens festzustellen, der das System unter den gegebenen experimentellen Bedingungen charakterisiert.

     

Development of a cooled He*(23S) beam source for measurements of state-resolved collision energy dependence of Penning ionization cross sections: Evidence for a stereospecific attractive well around methyl group in CH3CN

A low-temperature discharge nozzle source with a liquid-N(2) circulator for He*(2(3)S) metastable atoms has been developed in order to obtain the state-resolved collision energy dependence of Penning ionization cross sections in a low collision energy range from 20 to 80 meV. By controlling the discharge condition, we have made it possible to measure the collision energy dependence of partial ionization cross sections (CEDPICS) for a well-studied system of CH(3)CN+He*(2(3)S) in a wide energy range from 20 to 350 meV. The anisotropic interaction potential energy surface for the present system was obtained starting from an ab initio model potential via an optimization procedure based on classical trajectory calculations for the observed CEDPICS. A dominant attractive well depth was found to be 423 meV (ca. 10 kcal/mol) at a distance of 3.20 A from the center of mass of CH(3)CN in the N-atom side along the CCN axis. In addition, a weak attractive well (ca. 0.9 kcal/mol) surrounding the methyl group (-CH(3)) has been found and ascribed to the interaction between an unoccupied molecular orbital of CH(3)CN and 2s atomic orbital of He*(2(3)S).     

Intermediate state during the crystal transition in aspartame, studied with thermal analysis, solid-state NMR, and molecular dynamics simulation

Aspartame (L-alpha-aspartyl-L-phenylalanine methyl ester) is a dipeptide sweetener about 200 times as sweet as sugar. It exists in crystal forms such as IA, IB, IIA, and IIB, which differ in crystal structure and in the degree of hydration. Among these, IIA is the most stable crystal form, and its crystal structure has been well determined (Hatada et al., J. Am. Chem. Soc., 107, 4279-4282 (1985)). To elucidate the structural factors of thermal stability in the IIA form of aspartame and to examine the physical process in the crystal transformation between the IIA and IIB forms, we performed a thermal analysis and solid-state NMR measurements. We found that a quasi-stable intermediate state exists in the transformation, and it has the same crystal lattice as the usual IIA form, despite the dehydration from 1/2 mol to 1/3 mol per 1 mol of aspartame. The results of the energy component analysis and the molecular dynamics simulation suggest that the entropic effect promotes the generation of the intermediate state, which is presumably caused by the evaporation of the water of crystallization and the increase of molecular motion in aspartame. Thus, the thermal stability of the IIA form is attributable to a structural property, i.e., the crystal lattice itself is retained during the above dehydration. Moreover, the molecular dynamics simulations suggest that the aspartame molecules have two kinds of conformational flexibility in the intermediate state.     

A distance-controlled oligopeptide linker as a novel photo-induced energy transfer switch by secondary structural transition

By using an oligopeptide chain as a functional linker and introducing coumarin 2 and coumarin 343 at the chain ends, an effective photo-induced energy transfer system was constructed and energy transfer from coumarin 2 to coumarin 343 was switched on and off by a solvent-induced helix-coil secondary transition of the oligopeptide chain.     

Penning ionization electron spectroscopy of C6H6 by collision with He*(2 3 S) metastable atoms and classical trajectory calculations: optimization of ab initio model potentials

The potential energy surface of benzene (C(6)H(6)) with a He*(2(3)S) atom was obtained by comparison of experimental data in collision-energy-resolved two-dimensional Penning ionization electron spectroscopy with classical trajectory calculations. The ab initio model interaction potentials for C(6)H(6)+He*(2(3)S) were successfully optimized by the overlap expansion method; the model potentials were effectively modified by correction terms proportional to the overlap integrals between orbitals of the interacting system, C(6)H(6) and He*(2(3)S). Classical trajectory calculations with optimized potentials gave excellent agreement with the observed collision-energy dependence of partial ionization cross sections. Important contributions to corrections were found to be due to interactions between unoccupied molecular orbitals and the He*2s orbital. A C(6)H(6) molecule attracts a He*(2(3)S) atom widely at the region where pi electrons distribute, and the interaction of -80 meV (ca. -1.8 kcal/mol) just cover the carbon hexagon. The binding energy of a C(6)H(6) molecule and a He* atom was 107 meV at a distance of 2.40 A on the sixfold axis from the center of a C(6)H(6) molecule, which is similar to that of C(6)H(6)+Li and is much larger than those of the C(6)H(6)+[He,Ne,Ar] systems.     

2′,4′-BNA/LNA with 9-(2-Aminoethoxy)-1,3-diaza-2-oxophenoxazine Efficiently Forms Duplexes and Has Enhanced Enzymatic Resistance**

Artificial nucleic acids are widely used in various technologies, such as nucleic acid therapeutics and DNA nanotechnologies requiring excellent duplex-forming abilities and enhanced nuclease resistance. 2′-O,4′-C-Methylene-bridged nucleic acid/locked nucleic acid (2′,4′-BNA/LNA) with 1,3-diaza-2-oxophenoxazine (BNAP ( B^H )) was previously reported. Herein, a novel B^H analogue, 2′,4′-BNA/LNA with 9-(2-aminoethoxy)-1,3-diaza-2-oxophenoxazine (G-clamp), named BNAP-AEO ( B^AEO ), was designed. The B^AEO nucleoside was successfully synthesized and incorporated into oligodeoxynucleotides (ODNs). ODNs containing B^AEO possessed up to 10⁴-, 152-, and 11-fold higher binding affinities for complementary (c) RNA than those of ODNs containing 2′-deoxycytidine ( C ), 2′,4′-BNA/LNA with 5-methylcytosine ( L ), or 2′-deoxyribonucleoside with G-clamp ( P^AEO ), respectively. Moreover, duplexes formed by ODN bearing B^AEO with cDNA and cRNA were thermally stable, even under molecular crowding conditions induced by the addition of polyethylene glycol. Furthermore, ODN bearing B^AEO was more resistant to 3′-exonuclease than ODNs with phosphorothioate linkages.