Department of Chemistry, University of Minnesota, Minneapolis, 55455, USA.
Biomacromolecules. 2013 Aug 12;14(8):2484-8. doi: 10.1021/bm400694r. Epub 2013 Jul 26.
It is well established that aqueous solutions of methylcellulose (MC) can form hydrogels on heating, with the rheological gel point closely correlated to the appearance of optical turbidity. However, the detailed gelation mechanism and the resulting gel structure remain poorly understood. Herein the fibrillar structure of aqueous MC gels was precisely quantified with a powerful combination of (real space) cryogenic transmission electron microscopy (cryo-TEM) and (reciprocal space) small-angle neutron scattering (SANS) techniques. The cryo-TEM images reveal that MC chains with a molecular weight of 300 000 g/mol associate into fibrils upon heating, with a remarkably uniform diameter of 15 ± 2 nm over a range of concentrations. Vitrified gels also exhibit heterogeneity in the fibril density on the length scale of hundreds of nanometers, consistent with the observed optical turbidity of MC hydrogels. The SANS curves of gels exhibit no characteristic peaks or plateaus over a broad range of wavevector, q, from 0.001-0.2 Å(-1). The major feature is a change in slope from I ∼ q(-1.7) in the intermediate q range (0.001 - 0.01 Å(-1)) to I ∼ q(-4) above q ≈ 0.015 Å(-1). The fibrillar nature of the gel structure was confirmed by fitting the SANS data consistently with a model based on the form factor for flexible cylinders with a polydisperse radius. This model was found to capture the scattering features quantitatively for MC gels varying in concentration from 0.09-1.3 wt %. In agreement with the microscopy results, the flexible cylinder model indicated fibril diameters of 14 ± 1 nm for samples at elevated temperatures. This combination of complementary experimental techniques provides a comprehensive nanoscale depiction of fibrillar morphology for MC gels, which correlates very well with macro-scale rheological behavior and optical turbidity previously observed for such systems.
众所周知,甲基纤维素(MC)的水溶液在加热时可以形成水凝胶,流变学凝胶点与光学浊度的出现密切相关。然而,详细的凝胶化机制和所得凝胶结构仍知之甚少。本文通过强大的(实空间)低温透射电子显微镜(cryo-TEM)和(倒空间)小角中子散射(SANS)技术组合,精确地量化了水性 MC 凝胶的纤维状结构。cryo-TEM 图像显示,分子量为 300000g/mol 的 MC 链在加热时缔合成纤维,在一系列浓度范围内,直径非常均匀,为 15 ± 2nm。玻璃态凝胶在数百纳米的长度尺度上,纤维密度也表现出不均匀性,与 MC 水凝胶的观察到的光学浊度一致。在宽的波矢 q 范围内(0.001-0.2Å(-1)),凝胶的 SANS 曲线没有特征峰或平台。主要特征是在中间 q 范围(0.001-0.01Å(-1))从 I∼q(-1.7)到 q ≈ 0.015Å(-1)以上的 I∼q(-4)斜率发生变化。凝胶结构的纤维状性质通过将 SANS 数据与基于具有多分散半径的柔性圆柱的形状因子的模型一致拟合得到了证实。该模型被发现可以定量地捕捉 MC 凝胶在浓度从 0.09-1.3wt%变化时的散射特征。与显微镜结果一致,柔性圆柱模型表明在高温下,样品的纤维直径为 14 ± 1nm。这种互补的实验技术的组合为 MC 凝胶提供了纤维形态的全面纳米级描述,与以前观察到的此类系统的宏观流变行为和光学浊度非常吻合。