Gambi C M C, Giordano R, Chittofrati A, Pieri R, Baglioni P, Teixeira J
Department of Physics, University of Florence and I.N.F.M., v. G. Sansone 1, 50019 Sesto Fiorentino, Firenze, Italy.
J Phys Chem B. 2005 May 12;109(18):8592-8. doi: 10.1021/jp0405815.
This paper reports a small-angle neutron scattering (SANS) characterization of perfluoropolyether (PFPE) aqueous micellar solutions with lithium, sodium, cesium and diethanol ammonium salts obtained from a chlorine terminated carboxylic acid and with two perfluoroisopropoxy units in the tail (n(2)). The counterion and temperature effects on the micelle formation and micellar growth extend our previous work on ammonium and potassium salts n(2) micellar solutions. Lithium, sodium, cesium and diethanol ammonium salts are studied at 0.1 and 0.2 M surfactant concentration in the temperature interval 28-67 degrees C. SANS spectra have been analyzed by a two-shell model for the micellar form factor and a screened Coulombic plus steric repulsion potential for the structure factor in the frame of the mean spherical approximation of a multicomponent system reduced to a generalized one component macroions system (GOCM). At 28 degrees C, for all the salts, the micelles are ellipsoidal with an axial ratio that increases from 1.6 to 4.2 as the counterion volume increases. The micellar core short axis is 13 A and the shell thickness 4.0 A for the alkali micelles, and 14 and 5.1 A for the diethanol ammonium micelles. Therefore, the core short axis mainly depends on the surfactant tail length and the shell thickness on the carboxylate polar head. The bulky diethanol ammonium counterion solely influences the shell thickness. Micellar charge and average aggregation number depend on concentration, temperature and counterion. At 28 degrees C, the fractional ionization decreases vs the counterion volume (or molecular weight) increase at constant concentration for both C = 0.1 M and C = 0.2 M. The increase of the counterion volume leads also to more ellipsoidal shapes. At C = 0.2 M, at 67 degrees C, for sodium and cesium micelles the axial ratio changes significantly, leading to spherical micelles with a core radius of 15 A, lower average aggregation number, and larger fractional ionization.
本文报道了全氟聚醚(PFPE)水性胶束溶液的小角中子散射(SANS)表征,该溶液含有由氯封端羧酸制得的锂盐、钠盐、铯盐和二乙醇铵盐,且尾部含有两个全氟异丙氧基单元(n(2))。抗衡离子和温度对胶束形成及胶束生长的影响扩展了我们之前关于铵盐和钾盐n(2)胶束溶液的研究工作。在28 - 67℃的温度区间内,研究了表面活性剂浓度为0.1 M和0.2 M时的锂盐、钠盐、铯盐和二乙醇铵盐。在多组分体系简化为广义单组分大离子体系(GOCM)的平均球近似框架下,通过胶束形状因子的双壳模型和结构因子的屏蔽库仑加空间排斥势对SANS光谱进行了分析。在28℃时,对于所有盐类,胶束呈椭球形,随着抗衡离子体积增加,轴比从1.6增大到4.2。碱金属胶束的胶束核短轴为13 Å,壳厚度为4.0 Å,二乙醇铵胶束的胶束核短轴为14 Å,壳厚度为5.1 Å。因此,核短轴主要取决于表面活性剂尾部长度,壳厚度取决于羧酸盐极性头。体积较大的二乙醇铵抗衡离子仅影响壳厚度。胶束电荷和平均聚集数取决于浓度、温度和抗衡离子。在28℃时,对于C = 0.1 M和C = 0.2 M,在恒定浓度下,随着抗衡离子体积(或分子量)增加,电离分数降低。抗衡离子体积增加还会导致更接近椭球形的形状。在C = 0.2 M、67℃时,对于钠和铯胶束,轴比发生显著变化,形成核半径为15 Å的球形胶束,平均聚集数较低,电离分数较大。