Institut Charles Gerhardt, UMR 5253 CNRS/ENSCM/UM2/UM1, 8 Rue de L'Ecole Normale, 34296 Montpellier Cedex 5, France.
Langmuir. 2012 Feb 28;28(8):3773-82. doi: 10.1021/la204562t. Epub 2012 Feb 13.
Hybrid polyion complex (HPIC) micelles are nanoaggregates obtained by complexation of multivalent metal ions by double hydrophilic block copolymers (DHBC). Solutions of DHBC such as the poly(acrylic acid)-block-poly(acrylamide) (PAA-b-PAM) or poly(acrylic acid)-block-poly(2-hydroxyethylacrylate) (PAA-b-PHEA), constituted of an ionizable complexing block and a neutral stabilizing block, were mixed with solutions of metal ions, which are either monoatomic ions or metal polycations, such as Al(3+), La(3+), or Al(13)(7+). The physicochemical properties of the HPIC micelles were investigated by small angle neutron scattering (SANS) and dynamic light scattering (DLS) as a function of the polymer block lengths and the nature of the cation. Mixtures of metal cations and asymmetric block copolymers with a complexing block smaller than the stabilizing block lead to the formation of stable colloidal HPIC micelles. The hydrodynamic radius of the HPIC micelles varies with the polymer molecular weight as M(0.6). In addition, the variation of R(h) of the HPIC micelle is stronger when the complexing block length is increased than when the neutral block length is increased. R(h) is highly sensitive to the polymer asymmetry degree (block weight ratio), and this is even more true when the polymer asymmetry degree goes down to values close to 3. SANS experiments reveal that HPIC micelles exhibit a well-defined core-corona nanostructure; the core is formed by the insoluble dense poly(acrylate)/metal cation complex, and the diffuse corona is constituted of swollen neutral polymer chains. The scattering curves were modeled by an analytical function of the form factor; the fitting parameters of the Pedersen's model provide information on the core size, the corona thickness, and the aggregation number of the micelles. For a given metal ion, the micelle core radius increases as the PAA block length. The radius of gyration of the micelle is very close to the value of the core radius, while it varies very weakly with the neutral block length. Nevertheless, the radius of gyration of the micelle is highly dependent on the asymmetry degree of the polymer: if the neutral block length increases in a large extent, the micelle radius of gyration decreases due to a decrease of the micelle aggregation number. The variation of the R(g)/R(h) ratio as a function of the polymer block lengths confirms the nanostructure associating a dense spherical core and a diffuse corona. Finally, the high stability of HPIC micelles with increasing concentration is the result of the nature of the coordination complex bonds in the micelle core.
杂化聚离子复合物(HPIC)胶束是通过多价金属离子与双亲水嵌段共聚物(DHBC)的络合作用得到的纳米聚集体。DHBC 的溶液,如聚丙烯酸-嵌段-聚丙烯酰胺(PAA-b-PAM)或聚丙烯酸-嵌段-聚(2-羟乙基丙烯酸)(PAA-b-PHEA),由可离解的络合嵌段和中性稳定嵌段组成,与金属离子溶液混合,金属离子可以是单价离子或多价金属阳离子,如 Al(3+)、La(3+)或 Al(13)(7+)。HPIC 胶束的物理化学性质通过小角中子散射(SANS)和动态光散射(DLS)进行研究,作为聚合物链段长度和阳离子性质的函数。具有比稳定嵌段小的络合嵌段的金属阳离子和不对称嵌段共聚物的混合物导致稳定的胶体 HPIC 胶束的形成。HPIC 胶束的水动力半径随聚合物分子量呈 M(0.6)变化。此外,当增加络合嵌段长度时,HPIC 胶束的 R(h)变化比增加中性嵌段长度时更强。R(h)对聚合物不对称度(块重比)非常敏感,当聚合物不对称度接近 3 时,这种情况更为明显。SANS 实验表明,HPIC 胶束具有明确定义的核-冠纳米结构;核由不溶性致密聚丙烯酸/金属阳离子复合物组成,扩散冠由溶胀的中性聚合物链组成。散射曲线通过形式因子的解析函数进行建模;佩德森模型的拟合参数提供了有关胶束核大小、冠状厚度和聚集数的信息。对于给定的金属离子,胶束核半径随 PAA 嵌段长度的增加而增加。胶束的回转半径非常接近核半径的值,而它随中性嵌段长度的变化非常微弱。然而,胶束的回转半径高度依赖于聚合物的不对称度:如果中性嵌段长度大大增加,由于胶束聚集数的减少,胶束的回转半径减小。作为聚合物嵌段长度的函数的 R(g)/R(h) 比值的变化证实了与致密球形核和扩散冠状相关的纳米结构。最后,HPIC 胶束在浓度增加时的高稳定性是胶束核中配位络合键性质的结果。