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具有类异戊二烯型疏水链的葡萄糖基表面活性剂水溶液中的胶束结构。

Micelle structures in aqueous solutions of glucose-based surfactants having an isoprenoid-type hydrophobic chain.

作者信息

Kato Taiki, Kawabata Youhei, Fujii Masatoshi, Kato Tadashi, Hato Masakatsu, Minamikawa Hiroyuki

机构信息

Department of Chemistry, Tokyo Metropolitan University, Minamiohsawa, Hachioji, Tokyo 192-0397, Japan.

出版信息

J Colloid Interface Sci. 2007 Aug 1;312(1):122-9. doi: 10.1016/j.jcis.2006.09.030. Epub 2006 Sep 20.

Abstract

Surfactant self-diffusion coefficients have been measured on a binary system of 1-O-beta-3,7-dimethyloctyl-D-maltopyranoside (beta-Mal(2)(Ger))/water and a mixed surfactant system of beta-Mal(2)(Ger)/1-O-beta-3,7-dimethyloctyl-D-glucopyranoside (beta-Glc(Ger))/water at 25 degrees C. For comparison, measurements have also been made on 1-O-beta-decyl-D-maltopyranoside (beta-Mal(2)C(10))/water and beta-Mal(2)C(10)/1-O-beta-decyl-D-glucopyranoside (beta-GlcC(10))/water. The hydrodynamic radius of beta-Mal(2)(Ger) micelles obtained from the micellar diffusion coefficient is around 3 nm and nearly equal to that of beta-GlcC(10) micelles within experimental error. In the mixed surfactant systems, the hydrodynamic radii for both systems increase with increasing X(G) (the mole fraction of beta-Glc(Ger) or beta-GlcC(10) in the total mixed solute) above X(G) congruent with 0.4 when the total surfactant concentration is kept constant at 2 wt%. The R(H) of beta-Glc(Ger)/Mal(2)(Ger) micelles increases more rapidly than beta-GlcC(10)/beta-Mal(2)C(10) micelles, and then phase separation occurs at X(G) congruent with 0.65. On the other hand, the R(H) of beta-GlcC(10)/beta-Mal(2)C(10) micelles continues to increase until the phase separation occurs at X(G) congruent with 0.92. Measurements have also been performed as a function of total surfactant concentration at constant X(G) (=0.6). The CMC of the beta-Glc(Ger)/Mal(2)(Ger) system is larger than that of the beta-GlcC(10)/beta-Mal(2)C(10) system as expected from the results of the pure surfactant systems published previously. The R(H) increases with increasing total surfactant concentration for both systems. At higher concentrations, the R(H) of beta-Glc(Ger)/Mal(2)(Ger) micelles increases more rapidly than beta-GlcC(10)/beta-Mal(2)C(10) micelles. These results can be explained by the fact that the geranyl and decyl chains have the same volume but different chain lengths.

摘要

已在25℃下测量了1-O-β-3,7-二甲基辛基-D-麦芽吡喃糖苷(β-Mal(2)(Ger))/水的二元体系以及β-Mal(2)(Ger)/1-O-β-3,7-二甲基辛基-D-葡萄糖吡喃糖苷(β-Glc(Ger))/水的混合表面活性剂体系中的表面活性剂自扩散系数。为作比较,还对1-O-β-癸基-D-麦芽吡喃糖苷(β-Mal(2)C(10))/水以及β-Mal(2)C(10)/1-O-β-癸基-D-葡萄糖吡喃糖苷(β-GlcC(10))/水进行了测量。由胶束扩散系数得到的β-Mal(2)(Ger)胶束的流体力学半径约为3nm,在实验误差范围内几乎与β-GlcC(10)胶束的流体力学半径相等。在混合表面活性剂体系中,当总表面活性剂浓度保持在2wt%不变时,对于两个体系,在X(G)(β-Glc(Ger)或β-GlcC(10)在总混合溶质中的摩尔分数)大于约0.4时,流体力学半径均随X(G)的增加而增大。β-Glc(Ger)/Mal(2)(Ger)胶束的R(H)比β-GlcC(10)/β-Mal(2)C(10)胶束增加得更快,然后在X(G)约为0.65时发生相分离。另一方面,β-GlcC(10)/β-Mal(2)C(10)胶束的R(H)持续增加,直到在X(G)约为0.92时发生相分离。还在X(G)恒定(=0.6)时作为总表面活性剂浓度的函数进行了测量。正如先前发表的纯表面活性剂体系的结果所预期的那样,β-Glc(Ger)/Mal(2)(Ger)体系的临界胶束浓度大于β-GlcC(10)/β-Mal(2)C(10)体系。对于两个体系,R(H)均随总表面活性剂浓度的增加而增大。在较高浓度下,β-Glc(Ger)/Mal(2)(Ger)胶束的R(H)比β-GlcC(10)/β-Mal(2)C(10)胶束增加得更快。这些结果可以用香叶基链和癸基链具有相同体积但链长不同这一事实来解释。

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