Nandigana Vishal V R, Jo Kyoo, Timperman Aaron, Aluru Narayana R
Department of Mechanical Engineering, Indian Institute of Technology, Madras, Chennai, 600036, India.
U.S. Army Corps of Engineers, Construction Engineering Research Laboratory, 2902 Newmark Drive, Champaign, Illinois, 61826, USA.
Sci Rep. 2018 Sep 17;8(1):13941. doi: 10.1038/s41598-018-32284-7.
We demonstrate a novel nanofluidic diode that produces rectification factors in excess of 1000. The nanofluidic diode consists of ion permselective nanopores that connect two reservoirs of different diameters- a micropore reservoir and a macropore reservoir. On the application of +100 V to the micropore, a low OFF state current is observed. The OFF state is caused by formation of the ion depleted zone in the micropore because the anions are prevented from entering the nanopores from the micropore and the cations are depleted in this region to maintain charge neutrality. On the application of -100 V, we observe a high ON state current. The ON state is caused by formation of the ion enriched zone in the microchannel because the anions cannot pass through the nanopores and accumulate in the microchannel. To maintain charge neutrality the cations also become enriched in the microchannel. The ratio of ON state current to the OFF state current gives the rectification of current. Here, plasma oxidation is used to achieve a nanopore with a large wall surface charge density of σ = -55 mC/m which yields a rectification of current on the order of 3500 that is nearly two orders of magnitude higher than those reported thus far. In contrast to the other nanofluidic diodes, this nanofluidic diode does not introduce asymmetry to the nanopore, but asymmetry is produced by having the nanopores join a micropore and a macropore. Introduction of asymmetry into the fluidic reservoirs which the nanopores connect is quite simple. Hence, the nanofluidic diode is easy to scale up to industrial level.
我们展示了一种新型纳米流体二极管,其整流因子超过1000。该纳米流体二极管由离子选择性渗透纳米孔组成,这些纳米孔连接两个不同直径的储液器——一个微孔储液器和一个大孔储液器。在向微孔施加+100 V电压时,观察到低关态电流。关态是由微孔中离子耗尽区的形成引起的,因为阴离子被阻止从微孔进入纳米孔,并且阳离子在该区域耗尽以保持电荷中性。在施加-100 V电压时,我们观察到高开态电流。开态是由微通道中离子富集区的形成引起的,因为阴离子不能通过纳米孔并在微通道中积累。为了保持电荷中性,阳离子也在微通道中富集。开态电流与关态电流之比给出了电流的整流。在这里,等离子体氧化用于实现具有大壁面电荷密度σ = -55 mC/m²的纳米孔,其产生的电流整流约为3500,比迄今为止报道的高出近两个数量级。与其他纳米流体二极管不同,这种纳米流体二极管没有给纳米孔引入不对称性,而是通过使纳米孔连接一个微孔和一个大孔产生不对称性。将不对称性引入纳米孔所连接的流体储液器中非常简单。因此,这种纳米流体二极管易于扩大到工业规模。