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Transition between collapsed state phases and the critical swelling of a hydrogen bonding gel: Poly(methacrylic acid-co-dimethyl acrylamide)

机译:塌陷状态相与氢键合凝胶的临界溶胀之间的过渡:聚(甲基丙烯酸-共二甲基丙烯酰胺)

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Transition between collapsed state phases and discontinuous volume phase transition for a hydrogen bonding gel, poly(methacrylic acid-co-dimethyl acrylamide), were observed by using both the volume measurements and fluorescence intensity of the pyranine fluoroprobe (8-hydroxypyrene-1,3,6-trisulfonic acid trisodium salt) bonded to the gel by means of electrostatic interactions. In the collapsed state, while there is no appreciable change in the volume of the gel, a considerable variation in the fluorescence intensity occurred around 30 degrees C signaling a second order phase transition between collapsed state phases, from relatively frozen to a fluctuating phase. Our analysis of the data around 30 degrees C indicates that the critical point of gel volume transition belongs to the so-called mean-field universality class, as predicted in Onuki [Phys. Rev. A 38, 2192 (1988)] and by Golubovic and Lubensky [Phys. Rev. Lett. 63, 1082 (1989)]. The relaxation time for the equilibrium swelling critically depends on the temperature and diverges near 60 degrees C, where both fluorescence intensity and the volume of the gel change drastically and indicate the discontinuous volume phase transition. The swelling kinetics of the critical gel during the discontinuous volume phase transition can be modeled best with the first term in the expansion of the Li-Tanaka equation for a long initial period of the swelling time. (c) 2007 American Institute of Physics.
机译:氢键凝胶聚(甲基丙烯酸-共-二甲基丙烯酰胺)的塌陷状态相和不连续体积相变之间的过渡通过使用吡喃类氟探针(8-羟基-1-1,3)的体积测量和荧光强度来观察(6-6-三磺酸三钠盐)通过静电相互作用结合到凝胶上。在塌陷状态下,虽然凝胶的体积没有明显变化,但是荧光强度发生了相当大的变化,大约在30摄氏度时发生了塌陷状态相之间的第二阶相变,从相对冻结的状态转变为波动的状态。我们在30摄氏度左右的数据分析表明,凝胶体积转变的临界点属于所谓的平均场通用性类别,正如Onuki [Phys。 Rev. A 38,2192(1988)]和Golubovic和Lubensky [物理学报。牧师63,1082(1989)]。平衡膨胀的弛豫时间主要取决于温度,并且在60摄氏度附近发散,在该温度下,荧光强度和凝胶体积均急剧变化,并指示不连续的体积相变。临界凝胶在不连续的体积相变过程中的溶胀动力学可以在溶胀时间较长的初期用Li-Tanaka方程扩展中的第一项进行最佳建模。 (c)2007年美国物理研究所。

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