Das Bijan, Maitra Basanti, Mercer Sean M, Everist Michelle, Leaist Derek G
Department of Chemistry, St. Francis Xavier University, Antigonish, Nova Scotia, CanadaB2G 2W5.
Phys Chem Chem Phys. 2008 Jun 7;10(21):3083-92. doi: 10.1039/b801393d. Epub 2008 Apr 3.
Taylor dispersion is used to measure ternary mutual diffusion coefficients (D(ik)) for aqueous solutions of decylsulfobetaine (SB10) (1) + dodecylsulfobetaine (SB12) (2), SB10 (1) + SB14 (2), and SB12 (1) + SB14 (2) mixed zwitterionic micelles. Cross-coefficient D(21) for the coupled flow of surfactant 1 produced by a concentration gradient in surfactant 2 is relatively small for these solutions, but D(12) reaches values as large as the main D(ii) coefficients. The results are interpreted by using the equation D(ik) = partial differential(C(i)D(i))/ partial differentialC(k) to relate the ternary mutual diffusion coefficients to the concentration-weighted average diffusion coefficients D(i) of the micellar and free-monomer forms of the surfactants. The macroscopic-gradient Taylor measurements are compared with diffusion coefficients measured by dynamic light scattering (DLS), which monitors microscopic concentration fluctuations. At most compositions, the intensity autocorrelation function G(tau) is a single exponential decay in D((2)), the smaller eigenvalue of the mutual diffusion coefficient matrix. A contribution from D((1)) is identified at high solute fractions of surfactant 1. The DLS results are consistent with contributions to G(tau) from uncoupled fluctuations in the concentrations of eigencomponents defined as the linear combinations of surfactants 1 and 2 that diagonalize the D(ik) matrix. A procedure for the rapid and convenient DLS measurement of ternary mutual diffusion coefficients, including the cross-coefficients for coupled diffusion, is suggested, using the Onsager reciprocal relation together with the eigenvalues and pre-exponential factors from G(tau).
泰勒色散法用于测量癸基磺基甜菜碱(SB10)(1)+十二烷基磺基甜菜碱(SB12)(2)、SB10(1)+SB14(2)以及SB12(1)+SB14(2)混合两性离子胶束的水溶液的三元互扩散系数(D(ik))。对于这些溶液,由表面活性剂2中的浓度梯度产生的表面活性剂1的耦合流的交叉系数D(21)相对较小,但D(12)的值可高达主要的D(ii)系数。通过使用方程D(ik) = ∂(C(i)D(i))/∂C(k)将三元互扩散系数与表面活性剂胶束形式和游离单体形式的浓度加权平均扩散系数D(i)相关联来解释结果。将宏观梯度泰勒测量结果与通过动态光散射(DLS)测量的扩散系数进行比较,动态光散射监测微观浓度波动。在大多数组成下,强度自相关函数G(τ)在互扩散系数矩阵较小的特征值D((2))中呈单指数衰减。在表面活性剂1的高溶质分数下可识别出D((1))的贡献。DLS结果与由定义为使D(ik)矩阵对角化的表面活性剂1和2的线性组合的本征组分浓度的非耦合波动对G(τ)的贡献一致。提出了一种使用昂萨格互易关系以及来自G(τ)的特征值和预指数因子快速便捷地通过DLS测量三元互扩散系数(包括耦合扩散的交叉系数)的方法。