Zusammenfassung
Die Ladungen an der Oberfläche eines Teilchens erzeugen ein Potential ψ, das unmittelbar an der Grenzfläche den Wert ψ 0 hat und zur Lösung hin abfällt. Weit weg vom Teilchen ist ψ = 0 (Kap. 2.3.1). Wie sich das Potential mit zunehmendem Abstand von der Grenzfläche ändert, hängt von der Verteilung der Ionen zwischen Grenzfläche und Lösung ab. Modelle, die diese Verteilung beschreiben, wurden bereits diskutiert (Kap. 2.3.2, 9.4).
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Lagaly, G., Schulz, O., Zimehl, R. (1997). Oberflächenpotential und elektrokinetisches Potential. In: Dispersionen und Emulsionen. Steinkopff, Heidelberg. https://doi.org/10.1007/978-3-642-59248-5_10
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