© A.W.Marczewski 2002

A Practical Guide to Isotherms of ADSORPTION on Heterogeneous Surfaces

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Global Heterogeneity, H: local heterogeneity function h(q): Jovanovic
(see global heterogeneity calc. plot)

Local heterogeneity - model lines for Jovanovic, Jov-m, Freundlich ,Langmuir and GF equations Local heterogeneity function, h(q), for Jovanovic and Jov-m (Jovanovic + heterogeneity) compared with Langmuir, Generalized Freundlich (GF)/Sips and Freundlich (F) equations.

All equations (Jov-m, GF and F) corresponding to heterogeneous surfaces and characterized by the same value of heterogeneity parameter m for low surface coverages q behave in the same way :
hhet(q → 0) = 1/m
However, for medium and high coverages q) the differences become clear. For Freundlich and Jovanovic-derived isotherms:
hhet(q → 1) = 0
as opposed to Langmuir-based GF isotherm:
(hGF(q → 1) = hL(q) = 1).
For other Langmuir-based isotherms (see model picture for GL): hGL(q) ≥ hL(q) = 1
Those differences result partially from their implied local isotherms, i.e. different adsorption/interaction models (Langmuir, Jovanovic, Freundlich), partially from the magnitude of heterogeneity effects (heterogeneous or homogeneous: Jov-m / Jov; GF / L) or shape of energy distribution function corresponding to apparently identical heterogeneity parameters or other factors (e.g. Freundlich should be used for weakly soluble substances with c ≤ cs).

For Freundlich equation point q=1 corresponds to p=po , for other equations q=1 is reached for p→∞ or [p/(1-x)]→∞ (for vapors x = p/ps and for weakly soluble solutes; x=c/cs).
NOTE. Replace p with c for dilute solute adsorption.


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