Electric Double Layer at the Membrane/Solution Interface: Distribution of Electric Potential and Estimation of the Charge Stored

1992 ◽  
Vol 96 (4) ◽  
pp. 538-544 ◽  
Author(s):  
J. A. Manzanares ◽  
S. Mafé ◽  
J. Bisquert
Nanoscale ◽  
2018 ◽  
Vol 10 (30) ◽  
pp. 14736-14746 ◽  
Author(s):  
Kaito Hirata ◽  
Takuya Kitagawa ◽  
Keisuke Miyazawa ◽  
Takahiro Okamoto ◽  
Akira Fukunaga ◽  
...  

Charge accumulation behavior at the Au–electrolyte interface was visualized by three-dimensional open-loop electric potential microscopy with a varying electrode potential.


2016 ◽  
Vol 18 (1) ◽  
pp. 234-243 ◽  
Author(s):  
Jun-Sik Sin ◽  
Hak-Chol Pak ◽  
Kwang-Il Kim ◽  
Kuk-Chol Ri ◽  
Dok-Yong Ju ◽  
...  

Non-uniform size effects and orientational ordering of water dipoles influence the relative permittivity and electric potential in suspension.


2015 ◽  
Vol 17 (7) ◽  
pp. 5207-5218 ◽  
Author(s):  
A. A. Moya

The study of the formation of the electric double layer at the membrane–solution interface based on the Nernst–Planck and Poisson equations including different diffusion coefficient and dielectric constant values in the solution and membrane phases.


Author(s):  
Neeraj Sharma ◽  
Gerardo Diaz ◽  
Edbertho Leal-Quiros

Joule heating of liquid films in the presence of an externally applied electric field is influenced by the formation of the electric double layer. The thickness and charge distribution inside the electric double layer determine the extent of interaction of the charge in the electric double layer with the externally applied electric field and the Joule heating of the electrolyte layer. For this reason, the effects of externally applied electric field (both parallel and along the normal to the surface) on the electric double layer are being studied in the present paper. In the absence of the externally applied electric field, the distribution of the electric potential in the double layer is given by Poisson equation. Assuming Boltzmann distribution for the ionic concentration in the double layer, one arrives at Poisson-Boltzmann equation for the electric potential distribution. The externally applied electric field changes this electric potential distribution. Hence, the contribution of the externally applied electric field is studied by including it in the Poisson-Boltzmann equation.


2008 ◽  
Vol 77 (24) ◽  
Author(s):  
Yugo Nosaka ◽  
Masashi Hirabayashi ◽  
Takayoshi Kobayashi ◽  
Eiji Tokunaga

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