Aachener Verfahrenstechnik, RWTH Aachen University , Turmstrasse 46, D-52064 Aachen, Germany.
Wallenberg Wood Science Center, and the Department of Fibre and Polymer Technology, KTH Royal Institute of Technology , SE-10044 Stockholm, Sweden.
J Phys Chem B. 2017 Mar 16;121(10):2244-2251. doi: 10.1021/acs.jpcb.6b11914. Epub 2017 Mar 8.
The adsorption of urea on cellulose at room temperature has been studied using adsorption isotherm experiments and molecular dynamics (MD) simulations. The immersion of cotton cellulose into bulk urea solutions with concentrations between 0.01 and 0.30 g/mL led to a decrease in urea concentration in all solutions, allowing the adsorption of urea on the cellulose surface to be measured quantitatively. MD simulations suggest that urea molecules form sorption layers on both hydrophobic and hydrophilic surfaces. Although electrostatic interactions accounted for the majority of the calculated interaction energy between urea and cellulose, dispersion interactions were revealed to be the key driving force for the accumulation of urea around cellulose. The preferred orientation of urea and water molecules in the first solvation shell varied depending on the nature of the cellulose surface, but urea molecules were systematically oriented parallel to the hydrophobic plane of cellulose. The translational entropies of urea and water molecules, calculated from the velocity spectrum of the trajectory, are lower near the cellulose surface than in bulk. As urea molecules adsorb on cellulose and expel surface water into the bulk, the increase in the translational entropy of the water compensated for the decrease in the entropy of urea, resulting in a total entropy gain of the solvent system. Therefore, the cellulose-urea dispersion energy and the translational entropy gain of water are the main factors that drive the adsorption of urea on cellulose.
本研究采用吸附等温线实验和分子动力学(MD)模拟,研究了尿素在纤维素上的室温吸附。将棉纤维素浸入浓度在 0.01 到 0.30 g/mL 之间的尿素本体溶液中,导致所有溶液中尿素浓度降低,从而可以定量测量尿素在纤维素表面的吸附。MD 模拟表明,尿素分子在疏水面和亲水面上都形成了吸附层。尽管静电相互作用解释了计算出的尿素与纤维素之间的大部分相互作用能,但发现色散相互作用是尿素在纤维素周围聚集的关键驱动力。在第一个溶剂化壳中,尿素和水分子的优先取向取决于纤维素表面的性质,但尿素分子系统地平行于纤维素的疏水面取向。根据轨迹速度谱计算得到的尿素和水分子的平动熵,在纤维素表面附近比在本体中低。当尿素分子吸附在纤维素上并将表面水逐出本体时,水分子的平动熵增加补偿了尿素熵的减少,导致溶剂体系的总熵增加。因此,纤维素-尿素的色散能和水的平动熵增加是推动尿素在纤维素上吸附的主要因素。