TY - JOUR
T1 - Effects of surface-charge regulation, convection, and slip lengths on the electrical conductance of charged nanopores
AU - Green, Yoav
N1 - Funding Information:
We thank Mr. John Sebastian for proofreading this paper. This work was supported by the Israel Science Foundation (Grants No. 337/20 and No. 1953/20). We thank the Ilse Katz Institute for Nanoscale Science and Technology for their support. We thank the anonymous referee for referring us to Ref. , with which we were not familiar.
Funding Information:
We thank Mr. John Sebastian for proofreading this paper. This work was supported by the Israel Science Foundation (Grants No. 337/20 and No. 1953/20). We thank the Ilse Katz Institute for Nanoscale Science and Technology for their support. We thank the anonymous referee for referring us to Ref. [61], with which we were not familiar.
Publisher Copyright:
© 2022 American Physical Society
PY - 2022/1/1
Y1 - 2022/1/1
N2 - The electric conductance characterizes the response of a nanochannel or nanopore to an electrical potential drop. It has long been known that at low concentrations the electric conductance is independent of the bulk electrolyte concentration but depends on the surface-charge density. In recent years, several works have demonstrated that the low-concentration conductance is concentration dependent. This dependence is implicit through the mechanism known as surface-charge regulation which causes the surface-charge density to depend on the concentration, Formula Presented. As a result, the conductance, Formula Presented, has power-law dependency such that Formula Presented with a slope of Formula Presented. It is typically assumed the slope takes on the particular values Formula Presented. Here, we will analytically show that slope varies continuously from 0 to Formula Presented as the system parameters vary. Thereafter, we will account for convection and the effects of a slip length at the channel surface. We will show that convection without slip increases the conductance but does not vary the slope Formula Presented. The inclusion of slip not only increases the conductance but also increases the slope to Formula Presented. Direct numerical simulations confirm our theoretical predictions. The consequences of these findings are important in the design of any electrokinetically driven nanofluidic system insofar as they provide the experimentalist an accurate prediction of the system response as a function of the material properties.
AB - The electric conductance characterizes the response of a nanochannel or nanopore to an electrical potential drop. It has long been known that at low concentrations the electric conductance is independent of the bulk electrolyte concentration but depends on the surface-charge density. In recent years, several works have demonstrated that the low-concentration conductance is concentration dependent. This dependence is implicit through the mechanism known as surface-charge regulation which causes the surface-charge density to depend on the concentration, Formula Presented. As a result, the conductance, Formula Presented, has power-law dependency such that Formula Presented with a slope of Formula Presented. It is typically assumed the slope takes on the particular values Formula Presented. Here, we will analytically show that slope varies continuously from 0 to Formula Presented as the system parameters vary. Thereafter, we will account for convection and the effects of a slip length at the channel surface. We will show that convection without slip increases the conductance but does not vary the slope Formula Presented. The inclusion of slip not only increases the conductance but also increases the slope to Formula Presented. Direct numerical simulations confirm our theoretical predictions. The consequences of these findings are important in the design of any electrokinetically driven nanofluidic system insofar as they provide the experimentalist an accurate prediction of the system response as a function of the material properties.
UR - http://www.scopus.com/inward/record.url?scp=85124454315&partnerID=8YFLogxK
U2 - 10.1103/PhysRevFluids.7.013702
DO - 10.1103/PhysRevFluids.7.013702
M3 - Article
AN - SCOPUS:85124454315
SN - 2469-990X
VL - 7
JO - Physical Review Fluids
JF - Physical Review Fluids
IS - 1
M1 - 013702
ER -