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Polyferrocenylsilane crystals in nanoconfinement: Fragmentation, dissolution, and regrowth of cylindrical block copolymer micelles with a crystalline core

机译:纳米约束中的聚二茂铁基硅烷晶体:具有晶体核的圆柱形嵌段共聚物胶束的断裂,溶解和再生

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Two samples of rod-like micelles in decane were prepared by seeded growth from a sample of a poly(isoprene-b-ferrocenyldimethylsilane) diblock copolymer (PI _(1000)-PFS _(50), where the subscripts indicate the degree of polymerization). These micelles were uniform in length with a mass/length of 1.9 moleculesm. The longer micelles (L-1250) had a number-average length L _n = 1243 nm, whereas the shorter micelles (L-250) had L _n = 256 nm. We used transmission electron microscopy (TEM) to examine the behavior of these micelles when dilute solutions of L-1250 or L-250 or their mixtures were heated at temperatures ranging from 40 to 75 °C and then cooled to room temperature. At 55 °C, the L-1250 sample underwent kinetically controlled fragmentation to give a broad distribution of micelle lengths. At this temperature, fragmentation was much less prominent in the L-250 sample. At higher temperatures, micelles with narrow distributions of lengths were obtained in each case (L _w/L _n ≈ 1.01). This process operates under thermodynamic control, and L _n values increased strongly with an increase in temperature. These results indicate that the micelles fragment, and polymer molecules dissolve, as the samples were heated. The fraction of surviving fragments decreased significantly at elevated temperatures, presumably reflecting a distribution of crystallinity in the cores of the micelle precursor. When the solutions were cooled, the surviving fragments served as seeds for the epitaxial growth of the micelles as the polymer solubility decreased. The most striking result of these experiments was the finding that fragments formed from the L-1250 micelles had a distribution of dissolution temperatures shifted by about 5 °C to higher temperature than the shorter L-250 micelles.
机译:通过从聚(异戊二烯-b-二茂铁基二甲基硅烷)二嵌段共聚物(PI _(1000)-PFS _(50))的种子中进行接种生长来制备癸烷中的两个棒状胶束样品。 )。这些胶束的长度均匀,质量/长度为1.9分子/ nm。较长的胶束(L-1250)的数均长度L _n = 1243 nm,而较短的胶束(L-250)的L_n = 256 nm。当将L-1250或L-250的稀溶液或其混合物在40至75°C的温度下加热然后冷却至室温时,我们使用透射电子显微镜(TEM)来检查这些胶束的行为。在55°C下,对L-1250样品进行了动力学控制的裂解,从而使胶束长度分布更广。在此温度下,碎片在L-250样品中不明显。在更高的温度下,在每种情况下均获得了长度分布较窄的胶束(L _w / L _n≈1.01)。该过程在热力学控制下进行,并且L _n值随着温度的升高而强烈增加。这些结果表明,随着样品的加热,胶束碎片和聚合物分子溶解。在高温下,幸存碎片的比例显着下降,大概反映了胶束前体核心中结晶度的分布。当溶液冷却时,随着聚合物溶解度的降低,幸存的碎片成为胶束外延生长的种子。这些实验最惊人的结果是发现,与较短的L-250胶束相比,由L-1250胶束形成的碎片的溶解温度分布向较高的温度移动了约5°C。

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