Graduate School of Life and Environmental Sciences, University of Tsukuba , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8572, Japan.
Flexible Electronics Research Center, National Institute of Advanced Industrial Study and Technology , 1-1-1 Higashi, Tsukuba, Ibaraki 305-8565, Japan.
Langmuir. 2017 Nov 7;33(44):12660-12669. doi: 10.1021/acs.langmuir.7b02742. Epub 2017 Oct 23.
To understand the charging and aggregation of cellulose nanofibers (CNFs), we performed the following experimental and theoretical studies. The charging behavior of CNFs was characterized by potentiometric acid-base titration measuring the density of deprotonated carboxyl groups at different KCl concentrations. The charging behavior from the titration was quantitatively described by the 1-pK Poisson-Boltzmann (PB) model for a cylinder. The electrophoretic mobility of CNFs was measured as a function of pH by electrophoretic light scattering. The mobility was analyzed with the equation for an infinitely long cylinder considering the relaxation of the electric double layer. Good agreement between experimental mobilities and theoretical calculation was obtained by assuming a reasonable distance from the surface to the slipping plane. The result demonstrated that the negative charge of CNFs originates from the deprotonation of β(1-4)-d-glucuronan on the surface. The aggregation behavior of CNFs was studied by measuring the hydrodynamic diameter of CNFs at different pH and KCl concentrations. Also, we calculated the capture efficiencies of aggregation, using interaction energies of perpendicularly and parallelly oriented cylinders. The interaction energies between cylinders in both orientations were obtained by the Derjaguin, Landau, Verwey, and Overbeek theory, where the electrostatic repulsion was calculated from the surface potential obtained by the 1-pK PB model. From comparison of the theoretical capture efficiency with the measured hydrodynamic diameter, we suggest that CNFs can be aggregated in perpendicular orientation at low pH and low salt concentration, and the fast aggregation regime of CNFs is realized by the reduction of electric repulsion for both perpendicularly and parallelly interacting CNFs. Meanwhile, the application of Smoluchowski's equation to the mobility of CNFs results in the underestimation of the zeta potential.
为了理解纤维素纳米纤维(CNF)的荷电和聚集行为,我们进行了以下实验和理论研究。通过测定不同 KCl 浓度下的脱质子化羧基密度,用等电滴定法对 CNF 的荷电行为进行了表征。通过 1-pK 泊松-玻尔兹曼(PB)模型对圆柱进行定量描述,对滴定的荷电行为进行了定量描述。通过电泳光散射测量 CNF 的电泳迁移率作为 pH 的函数。通过考虑双电层弛豫的无限长圆柱方程对迁移率进行了分析。通过假设从表面到滑移面的合理距离,实验迁移率与理论计算之间得到了很好的一致性。结果表明,CNF 的负电荷来源于表面上 β(1-4)-d-葡糖醛酸的脱质子化。通过测量不同 pH 和 KCl 浓度下 CNF 的水动力直径,研究了 CNF 的聚集行为。此外,我们还使用垂直和平行取向的圆柱的相互作用能计算了聚集的捕获效率。通过德贾古因、朗道、维韦和奥弗贝克理论获得了两个取向的圆柱之间的相互作用能,其中静电排斥由 1-pK PB 模型得到的表面电位计算得出。通过将理论捕获效率与测量的水动力直径进行比较,我们提出在低 pH 和低盐浓度下,CNF 可以以垂直取向聚集,并且通过降低垂直和平行相互作用的 CNF 的电排斥,可以实现 CNF 的快速聚集状态。同时,将斯莫卢霍夫斯基方程应用于 CNF 的迁移率会导致 ζ 电位的低估。