Kuhlman William A, Olivetti Elsa A, Griffith Linda G, Mayes Anne M
Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts, 02139, USA.
Macromolecules. 2006 Jul 25;39(15):5122-5126. doi: 10.1021/ma060132y.
Comb copolymers comprising a poly(methyl methacrylate) (PMMA) backbone and short, polyethylene oxide (PEO) side chains, PMMA-g-PEO, have been proposed to self-organize at the polymer/water interface, resulting in the quasi-2D confinement of the backbone for chains at the immediate surface of PMMA-g-PEO films (D.J. Irvine et al., Biomacromolecules2001, 2, 85-94). To directly probe such 2D conformations, combs modified with maleimide groups on the PEO chain ends were blended at 0.5-10 wt% into unmodified PMMA-g-PEO (M(n) 142 kg/mol, PDI 3.2, 32 wt% PEO) and cast into films ∼35 nm thick. Films were immersed in aqueous solution to induce orientation of surface molecules, and maleimide-functionalized chains at the film/water interface were labeled with 1.4 nm dia. Au nanoparticles. Transmission electron microscopy (TEM) was then used to trace the 2D trajectories of nanoparticle-decorated chains. The distribution of observed chain lengths was in good agreement with that from gel permeation chromatography. The 2D radius of gyration (R(g)) calculated from the observed conformations scaled with number of backbone segments (N) as R(g)∼N(0.69±0.02). Monte Carlo simulations of a 2D melt of comparable chain length distribution yielded a scaling exponent ν=0.67±0.03, suggesting that the deviation from 2D melt behavior arose from polydispersity.
由聚甲基丙烯酸甲酯(PMMA)主链和短聚环氧乙烷(PEO)侧链组成的梳状共聚物PMMA-g-PEO,被认为可在聚合物/水界面处自组装,从而使主链在PMMA-g-PEO薄膜的紧邻表面处受到准二维限制(D.J. 欧文等人,《生物大分子》,2001年,第2卷,第85 - 94页)。为了直接探测这种二维构象,将在PEO链端用马来酰亚胺基团修饰的梳状共聚物以0.5 - 10 wt%的比例与未修饰的PMMA-g-PEO(M(n) = 142 kg/mol,PDI = 3.2,PEO含量32 wt%)混合,并浇铸成约35纳米厚的薄膜。将薄膜浸入水溶液中以诱导表面分子取向,并用直径1.4纳米的金纳米颗粒标记薄膜/水界面处带有马来酰亚胺官能团的链。然后使用透射电子显微镜(TEM)追踪纳米颗粒修饰链的二维轨迹。观察到的链长分布与凝胶渗透色谱法得到的结果高度一致。根据观察到的构象计算出的二维回转半径(R(g))与主链段数(N)的关系为R(g)∼N(0.69±0.02)。对具有可比链长分布的二维熔体进行的蒙特卡罗模拟得出标度指数ν = 0.67±0.03,这表明与二维熔体行为的偏差源于多分散性。