Šindelka Karel, Limpouchová Zuzana, Procházka Karel
Department of Molecular and Mesoscopic Modelling, Czech Academy of Sciences, Institute of Chemical Process Fundamentals, Rozvojová 1, 165 02 Prague, Czech Republic.
Department of Physical Chemistry, Faculty of Science, Charles University, Hlavova 8, 128 00 Prague, Czech Republic.
Polymers (Basel). 2021 Feb 6;13(4):502. doi: 10.3390/polym13040502.
Using coarse-grained dissipative particle dynamics (DPD) with explicit electrostatics, we performed (i) an extensive series of simulations of the electrostatic co-assembly of asymmetric oppositely charged copolymers composed of one (either positively or negatively charged) polyelectrolyte (PE) block A and one water-soluble block B and (ii) studied the solubilization of positively charged porphyrin derivatives (P+) in the interpolyelectrolyte complex (IPEC) cores of co-assembled nanoparticles. We studied the stoichiometric mixtures of 137 A10+B25 and 137 A10-B25 chains with moderately hydrophobic A blocks (DPD interaction parameter aAS=35) and hydrophilic B blocks (aBS=25) with 10 to 120 P+ added (aPS=39). The P+ interactions with other components were set to match literature information on their limited solubility and aggregation behavior. The study shows that the moderately soluble P+ molecules easily solubilize in IPEC cores, where they partly replace PE+ and electrostatically crosslink PE- blocks. As the large P+ rings are apt to aggregate, P+ molecules aggregate in IPEC cores. The aggregation, which starts at very low loadings, is promoted by increasing the number of P+ in the mixture. The positively charged copolymers repelled from the central part of IPEC core partially concentrate at the core-shell interface and partially escape into bulk solvent depending on the amount of P+ in the mixture and on their association number, AS. If AS is lower than the ensemble average ⟨AS⟩n, the copolymer chains released from IPEC preferentially concentrate at the core-shell interface, thus increasing AS, which approaches ⟨AS⟩n. If AS>⟨AS⟩n, they escape into the bulk solvent.
我们使用具有显式静电作用的粗粒化耗散粒子动力学(DPD)方法,(i)对由一个(带正电或负电)聚电解质(PE)嵌段A和一个水溶性嵌段B组成的不对称带相反电荷共聚物的静电共组装进行了一系列广泛的模拟,(ii)研究了带正电的卟啉衍生物(P+)在共组装纳米颗粒的聚电解质复合物(IPEC)核中的增溶作用。我们研究了137条A10+B25和137条A10 - B25链的化学计量混合物,其中A嵌段具有中等疏水性(DPD相互作用参数aAS = 35),B嵌段具有亲水性(aBS = 25),并添加了10至120个P+(aPS = 39)。P+与其他组分的相互作用设置为与关于它们有限的溶解度和聚集行为的文献信息相匹配。研究表明,中等溶解度的P+分子很容易在IPEC核中增溶,在那里它们部分取代PE+并静电交联PE - 嵌段。由于大的P+环易于聚集,P+分子在IPEC核中聚集。这种聚集在非常低的负载量时就开始,通过增加混合物中P+的数量而促进。带正电的共聚物从IPEC核的中心部分排斥出来,部分聚集在核 - 壳界面,部分根据混合物中P+的量及其缔合数AS逃逸到本体溶剂中。如果AS低于系综平均值⟨AS⟩n,从IPEC释放的共聚物链优先聚集在核 - 壳界面,从而增加AS,使其接近⟨AS⟩n。如果AS>⟨AS⟩n,它们逃逸到本体溶剂中。