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Porous materials / INTRODUCTORY EXPLORER

Adsorption isotherm shapes.

Compare six broad isotherm families and connect their shapes with possible adsorption processes.

Shape is evidence, not a unique diagnosis

Adsorption isotherm shapesEnable JavaScript to display the interactive diagram.

Explore the relationship.

The relationship

The model and its limits.

prel=pp0(T)p_{\mathrm{rel}}=\frac{p}{p_0(T)}

An isotherm records uptake as pressure changes at fixed temperature. Here p₀ is saturation vapor pressure at that temperature. Relative pressure is appropriate for a subcritical adsorptive, not every gas-storage experiment.

These curves are illustrative drawings generated from shape functions, not measured data or adsorption-model fits. Uptake is in arbitrary units. Heights do not compare capacities; the cursor is a reading aid. The endpoint at relative pressure 1 is illustrative, not a prediction at bulk saturation.

Reading the families

The descriptions above summarize six broad IUPAC families. Types I(a) and I(b) distinguish microporous shapes. IV(a) has hysteresis; IV(b) can be reversible. The plotted IV illustrates IV(a). Loop branches represent different adsorption and desorption paths.

Classification describes morphology. Choosing a fitting equation such as Langmuir or BET requires appropriate assumptions and a valid pressure range. Shape alone does not determine pore size or identify a material.

Why this matters for MOFs

Flexible MOFs can change structure as gas enters or leaves. Gate opening and structural transitions can create steps and hysteresis. A loop is not sufficient evidence for capillary condensation: structural measurements and experimental conditions matter. This explorer does not model framework flexibility or infer a mechanism from an unknown curve.

For measured high-pressure methane curves, explore methane storage.

Literature