| 1. | In 1980, Stigter extended Booth's model to allow for higher surface potentials.
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| 2. | We see that the surface potential has a direct relationship with the temperature.
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| 3. | This involves the equations being solved with simple boundary conditions such as constant surface potential.
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| 4. | Electric potential difference between the fluid bulk and the surface is called the electric surface potential.
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| 5. | Surface functionalization can largely change the surface potential.
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| 6. | As a result, the Hamiltonian is a quadratic functional of the surface potential " ? ".
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| 7. | The properties of this ion are strongly related to the surface potential present on a corresponding solid.
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| 8. | And the corresponding equation for the free-surface potential is identical, with \ zeta replaced by \ varphi.
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| 9. | If the partition function has no special surface potential terms, this is the surface of a hard solid.
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| 10. | Accounting for non-Coulombic interactions increases the ion concentration at the surface and leads to a reduced surface potential.
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