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在疏水/亲水弹性蛋白样多肽 (ELP) 嵌段共聚物的温度响应过程中对水合作用和纳米相分离的特性描述。

Characterisation of hydration and nanophase separation during the temperature response in hydrophobic/hydrophilic elastin-like polypeptide (ELP) diblock copolymers.

机构信息

Institut für Chemie, Martin-Luther-Universität Halle-Wittenberg, Von-Danckelmann-Platz 4, 06120 Halle (Saale), Germany.

Department of Biomedical Engineering, Duke University, 136 Hudson Hall, Campus Box 90281, Durham, North Carolina 27708, USA.

出版信息

Soft Matter. 2017 Mar 1;13(9):1816-1822. doi: 10.1039/c6sm02427k.

Abstract

To understand the complex nanoscale dehydration process during the lower critical solution temperature (LCST) based inverse phase transition of a class of thermoresponsive biopolymers, diblock elastin-like polypeptides (ELPs) were investigated by spin probing continuous wave electron paramagnetic resonance (CW EPR) spectroscopy. The diblock copolymers composed of a hydrophobic block and a hydrophilic block showed different mechanisms of a temperature-driven phase transition. While the phase transition temperature is a function of the hydrophobic mass fraction of the diblock ELPs, the hydrophilic block length determines the molecular structure of the polymer aggregates formed above the transition temperature. When the weight ratio of hydrophilic block length to hydrophobic block length is greater than or equal to 0.3, the polymer aggregates consist of a hydrophobic core and a hydrophilic corona. The interface of these two regions become permeable at temperatures above the transition temperature. In case of smaller ratios, the aggregating hydrophobic parts of the polymer enclose the hydrated hydrophilic blocks, that are too small to form a hydrophilic corona, leading to bigger and less dense aggregates of higher polarity.

摘要

为了理解一类温敏生物聚合物在低临界相转变温度(LCST)下的反相转变过程中复杂的纳米尺度脱水过程,通过自旋探测连续波电子顺磁共振(CW EPR)光谱研究了二嵌段弹性蛋白样多肽(ELP)。由疏水嵌段和亲水嵌段组成的二嵌段共聚物表现出不同的温度驱动相转变机制。虽然相转变温度是二嵌段 ELP 的疏水质量分数的函数,但亲水嵌段长度决定了高于转变温度时形成的聚合物聚集体的分子结构。当亲水嵌段长度与疏水嵌段长度的重量比大于或等于 0.3 时,聚合物聚集体由疏水核和亲水冠组成。在温度高于转变温度时,这两个区域的界面变得可渗透。在较小的比例下,聚合物的聚集疏水部分包围水合的亲水块,这些亲水块太小而无法形成亲水冠,导致更高极性的更大且更密集的聚集体。

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