1997
DOI: 10.1063/1.473378
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The influence of image interactions on the structure of water and electrolytes in front of a metal surface

Abstract: Structure of the metal-aqueous electrolyte solution interface

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Cited by 19 publications
(12 citation statements)
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“…With respect to the solvent-induced oscillatory behavior of the SRISM counterion density profiles, it is worth mentioning that such layering effects have not only been observed in alternative double layer theories involving dipolar or multipolar hard sphere water models or the central force water model as solvent, but surprisingly occur in macroscopic−thermodynamic continuum models as well if both the finite volumes of ions and water and the dielectric saturation of the latter are taken into account. …”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…With respect to the solvent-induced oscillatory behavior of the SRISM counterion density profiles, it is worth mentioning that such layering effects have not only been observed in alternative double layer theories involving dipolar or multipolar hard sphere water models or the central force water model as solvent, but surprisingly occur in macroscopic−thermodynamic continuum models as well if both the finite volumes of ions and water and the dielectric saturation of the latter are taken into account. …”
Section: Resultsmentioning
confidence: 99%
“…With respect to the solvent-induced oscillatory behavior of the SRISM counterion density profiles, it is worth mentioning that such layering effects have not only been observed in alternative double layer theories involving dipolar [25][26][27][28][29][30][31][32][33][34][35] or multipolar [36][37][38][39] hard sphere water models or the central force water model [40][41][42][43] as solvent, but surprisingly occur in macroscopic-thermodynamic continuum models as well if both the finite volumes of ions and water and the dielectric saturation of the latter are taken into account. [44][45][46] The corresponding SRISM/KH (left panel) and SRISM/HNC (right panel) coion density profiles for cations at cathodes (dashed lines), anions at anodes (dashed-dotted lines), and the corresponding SOZ results (solid lines) are shown in Figure 6.…”
Section: Resultsmentioning
confidence: 99%
“…In the present work we will compute the inhomogeneous density distribution of the vortices in front of a planar surface using the Wertheim-Lovett-Mou-Buff (WLMB) equation [7] together with a mean-field treatment of the image-forces. [8] The same method has recently successfully been applied in a different context, namely the structure of liquid water at a metallic interface [9]. From the equilibrium vortex-density profiles at the surface we calculate the local magnetic field which together with the image interactions determines the potential energy barrier [10] for pan-cake vortices entering into the sample.…”
mentioning
confidence: 99%
“…The electrode/solution interface phenomena have been a hot subject of theoretical simulations, to which various theoretical approaches based on classical mechanics have been applied, such as Canonical Monte Carlo [33,34], Wertheim-Lovett-Mou-Buff (WLMB) integral equation [35,36], modified Poisson-Boltzmann [37][38][39], and molecular dynamics [40,41]. Using these approaches, some features of the electrode/solution interface, such as the dynamic ordering of the interfacial water [41,42] and the structure of the electrochemical double layer, [33] have been elucidated.…”
Section: Theoretical Methods For Electrochemical Reactionsmentioning
confidence: 99%