Pial Turash Haque, Das Siddhartha
Department of Mechanical Engineering, University of Maryland, College Park, Maryland20742, United States.
J Phys Chem B. 2022 Dec 15;126(49):10543-10553. doi: 10.1021/acs.jpcb.2c05524. Epub 2022 Dec 1.
Controlling ion distribution inside a charged nanochannel is central to using such channels in diverse applications. Here, we show the possibility of using a charged polyelectrolyte (PE) brush-grafted nanochannel for triggering diverse nanoscopic ion distribution and nanofluidic electroosmotic transport by controlling the valence and size of the counterions (that screen the charges of the PE brushes) and the strength of an externally applied axial electric field. We atomistically simulate separate cases of fully charged polyacrylic acid (PAA) brush functionalized nanochannels with Na, Cs, Ca, Ba, and Y counterions screening the PE charges. Four key findings emerge from our simulations. First, we find that the counterions with a greater valence and a smaller size prefer to remain localized inside the brush layer. Second, for the case where there is an added chloride salt with the same cation (as the screening counterions), there are more coions (Cl ions) in the brush-free bulk than counterions (for counterions Na, Ca, Ba, Y): this is a manifestation of the overscreening (OS) of the PE brush layer. Contrastingly, the number of Cs ions remain higher than the Cl ions inside the brush-free bulk, ensuring that there is no OS effect for this case. Third, large applied electric field enables a few Na, Cs, and Ba counterions to leave the brush layer and to go to the bulk: this makes the OS of the PE brush layer disappear for the cases of PE brushes being screened by the Na and Ba ions. On the other hand, no such electric-field-mediated disappearance of OS is observed for the cases of Ca and Y screening counterions; we attribute this to the firm attachment of these counterions to the negatively charged monomers. Free energy associated with a counterion binding to a PE chain corroborates this diversity in the counterion-specific response to the applied electric field. Finally, we demonstrate that such diverse ion distributions, along with specific electric-field-strength-dependent ion properties, lead to (1) electroosmotic (EOS) transport in nanochannels grafted with PAA brushes screened with Cs ions to be always counterion dominated, (2) EOS transport in nanochannels grafted with PAA brushes screened with Ca and Y ions to be always coion-dominated, and (3) EOS transport in nanochannels grafted with PAA brushes screened with Na and Ba ions to be coion dominated for smaller electric fields and counterion dominated for larger electric fields.
控制带电纳米通道内的离子分布是在各种应用中使用此类通道的核心。在此,我们展示了通过控制抗衡离子(即屏蔽聚电解质刷电荷的离子)的价态和大小以及外部施加的轴向电场强度,利用接枝有带电聚电解质(PE)刷的纳米通道来触发各种纳米级离子分布和纳米流体电渗传输的可能性。我们通过原子模拟分别研究了用Na、Cs、Ca、Ba和Y抗衡离子屏蔽PE电荷的完全带电聚丙烯酸(PAA)刷功能化纳米通道的情况。我们的模拟得出了四个关键发现。第一,我们发现价态更高且尺寸更小的抗衡离子更倾向于局域在刷层内部。第二,对于添加了与屏蔽抗衡离子相同阳离子的氯化物盐的情况,在无刷本体中同离子(Cl离子)比抗衡离子(对于抗衡离子Na、Ca、Ba、Y)更多:这是PE刷层过屏蔽(OS)的一种表现。相反,在无刷本体中Cs离子的数量高于Cl离子,确保了这种情况下不存在OS效应。第三,大的外加电场能使一些Na、Cs和Ba抗衡离子离开刷层进入本体:这使得对于由Na和Ba离子屏蔽的PE刷情况,PE刷层的OS消失。另一方面,对于Ca和Y屏蔽抗衡离子的情况,未观察到这种由电场介导的OS消失;我们将此归因于这些抗衡离子与带负电单体的牢固结合。与抗衡离子与PE链结合相关的自由能证实了抗衡离子对施加电场的特定响应中的这种多样性。最后,我们证明,这种多样的离子分布以及特定电场强度依赖的离子性质导致:(1)用Cs离子屏蔽的接枝有PAA刷的纳米通道中的电渗(EOS)传输始终以抗衡离子为主导;(2)用Ca和Y离子屏蔽的接枝有PAA刷的纳米通道中的EOS传输始终以同离子为主导;(3)用Na和Ba离子屏蔽的接枝有PAA刷的纳米通道中的EOS传输在较小电场下以同离子为主导,在较大电场下以抗衡离子为主导。