9.8
The charge distribution across the interface between a solid electrode and an electrolyte solution forms an electrical double layer.
The primitive model considers two idealized charge sheets: a positive sheet on the electrode surface and a negative sheet in the solution.
In reality, ions in solution are solvated and cannot reside directly at the electrode surface. Helmholtz refined the model by introducing solvated ions at the electrode surface, held apart by hydration spheres, with the outer Helmholtz plane marking the ionic charge sheet.
Here, the electric potential linearly shifts from ϕM at the metal to ϕS at the OHP. However, it neglects the disruptive effect of thermal motion on the rigid charge plane.
Considering the thermal motion, the Gouy–Chapman model features a diffuse double layer where the oppositely charged ions cluster at the electrode by diffusing into the solution, causing a non-linear potential change.
Combining both ideas, Stern proposed that some negative ions adhere to the electrode, maintaining a fixed distance based on the ionic radius.
Simultaneously, thermal motion disperses the remaining excess negative ions throughout the interphase region, leading to a gradual change in electric potential.
In the region where two bulk phases meet, an intricate electric charge distribution arises due to charge transfer, ion adsorption, molecular orientati…
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