|
|
Research |
|
|||||||||
|
Life Style |
|||||||||||
|
Theoretical investigation on the liquid junction potential
in a slit-like microchannel Kwan Hyoung
Kang* and In Seok Kang¢Ó Department
of Mechanical Engineering* and Department of Chemical Engineering,¢Ó Pohang University of Science
and Technology, San 31, Hyoja-dong, Pohang 790-784, (Submitted
to the J. Electroanalytical Chemistry) The liquid junction potential (LJP) is generated
at the interface of the two electrolyte solutions of different ionic concentrations
(see Fig. 1). It can be applied to generate electricity (Fig. 2) and it can
also be applied to passive control of the trajectory of the charged micro-
and nanoparticles in the micro total analysis systems. In this
work, an analytical model is provided to predict the LJP and the associated
electrostatic field generated by the contacting two electrolyte layers in a
slit-like channel, for the case of the simple 1:1 electrolyte system. The
one-dimensional Nernst–Planck equation is analyzed to investigate the
temporal evolution of the concentration distribution.
Fig.
1 Diffusivity difference of ionic
species induces the concentration polarization.
Fig.
2 Application of the LJP for the membraneless fuel cell
As a
result, comprehensive analytical formulas for the LJP, the electric field, and
the charge density are obtained. The LJP is obtained by introducing the
concentrations at the boundary surfaces to the Planck¡¯s equation
written for the finite domain. The analytical result for the LJP is compared
with the existing experimental result of Lagger et al. [2], which shows a
reasonable agreement as shown in Fig. 3. Of particular interest is the influence of the initial concentration ratio and the thickness ratio of the two electrolyte layers. It is shown that there exist limiting profiles in the temporal evolution of the LJP, with respect to the variation of the concentration ratio and the thickness ratio, respectively. The implication of the electric field produced by the charge separation is discussed concerning the behavior of the charged particles in the micro total analysis systems.
Fig. 3. Validation of the theory. x and y-axes
represents the non-dimensional time and the LJP. The experiment of Lagger et
al. [2] is performed in a mini channel shown in Fig. 2(b). The lines indicate
the theoretical prediction and the symbols represent the experimental results
obtained for different concentrations and the location of the electrode in
the channel. References
[1] R. Ferrigno, A. D. Strook, T. D. Clark, M.
Mayer, G. M. Whitesides ¡°Membraneless
Vanadium Redox Fuel Cell Using Laminar Flow,¡±
J. Am. Chem. Soc. 124 (2002) 12930. [2] G. Lagger, H. Jensen, J. Josserand, H. H.
Girault ¡°Hydro-voltaic cells. Part I. Concentration
cells,¡±
J. Electroanal. Chem. 545 (2003) 1. Lastly
Modified in October 13, 2003 |
|||||||||||