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Adsorption Modeling of physisorption in porous materials Part 1

European Master. Adsorption Modeling of physisorption in porous materials Part 1. Bogdan Kucht a Laboratoire MADIREL Université Aix - Marseille. Notion of Interface. Interface: Separation between two (volume) phases .

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Adsorption Modeling of physisorption in porous materials Part 1

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  1. European Master Adsorption Modeling of physisorption in porous materials Part 1 Bogdan Kuchta Laboratoire MADIREL Université Aix-Marseille

  2. Notion of Interface Interface: Separation between two (volume) phases. Although words ‘interface’ and ‘surface’ mean practically the same, the word "interface" is often used when 2 condensed phases are in contact or when two phase are explicitly considered. ex : interface solid/liquid; interface solid/gaz. The word "surface"is used to describe interface of solid (when it is (or not) in a contact with different phase)

  3. Adsorption • Phenomenon of adsorption • When a fluid is in the vicinity of solid surface, its concentration increases close to the interface. • Definition • Adsorption is a process that occurs when a gas or liquid solute accumulates on the surface of a solid or, more rarely, a liquid (adsorbent), forming a molecular or atomic film (adsorbate). • Word "adsorption" is also used to describe the transition of a fluid when it transforms into an adsorbed phase.

  4. Concentration of the adsorbed phase [c] Concentration of the gas phase z What is adsorption ?

  5. Gaz phase Adsorbate Adsorbed phase Adsorbent Adsorption Adsorption – a phenomenon general which involves the preferential partitioning of substances from the gaseous or liquid phase onto the surface of a solid substrate Physical adsorption is caused mainly by van der Waals forces and electrostatic forces between adsorbate molecules and the atoms which compose the adsorbent surface. Thus adsorbents are characterized first by surface properties such as surface area, structure (roughness) and polarity.

  6. Adsorption physique Adsorption chimique Energie Energie d’activation Adsorption physique Adsorption chimique Adsorption Chemical (chemisorption) versus physical (physisorption) adsorption. In chemisorptionthere is an exchange of electrons between the surface and the adsorbed molecules . n / ms Theenergy of chemisorption is stronger. P = const. Tadsorption

  7. Adsorbed quantity na Adsorbed quantity: va Gas : vg t 0 How do we represent the adsorbed quantity?(a) interface layer Surface : A Solide : vs c z

  8. How do we represent the adsorbed quantity ?(b) GIBBS representation c Surface of Gibbs Solide : vs Excess adsorbed quantity: n Excess quantity on surface n Volume (total) : vg,0 cg na = ns + cg.va cg.va z T : na n

  9. Representations of adsorption equilibrium Gibbs representation Interface layer solide gaz c couche solide gaz adsorbée GDS V S,0 V g,0 Surface V V V S a g (imaginary surface) c = dn/dV I II c = dn/dV I II III gas in volumeVg,0 (measured with He) gas in volume Vg (unknown) c g F c g F C = 0 S z 0 C = 0 S z t 0 Excess quantity on surface n Adsorbed quantity na:

  10. Equilibre d'adsorption An equilibrium of adsorption , at temperature T, is characterized par quantity that depends on pressure of gas , p : •  = n /A • n  est la quantité d'excès en surface • A est l'étendue de l'interface • a est l'aire spécifique (= A /m s)

  11. p / po Isotherm of argon at 77.4 K

  12. p / po Isotherme d'adsorption (définition) Isotherm of adsorption: is an ensemble of equilibrium states, at temperature T, for all pressures p between 0 et p° (pressure of saturated vapor of adsorbate at temperature T ). p/p° is called « relative equilibrium pressure".

  13. a : corrugation b : bottle neck c : opening d : interconnection e : close-ended f : closed (isolated) b c f d e a Adsorption Special case – materials with large surface: porous materials: specific surface between 0.1 and 2600 m2g-1  mesopores (nano-pores): 2 – 50 nm in diameter  “nanomaterials” of technological interests with 1, 2 or 3 dimensions  100 nm Micropores <2 nm Macropores >50 nm

  14. Fundamental questions : 1. Mechanism of adsorption – influence of the geometry and pore structure 2. Influence of confined geometry (interaction with walls) on structural transformations 3. Capillary condensation 4. Hysteresis and metastability ns/ms p/p° Adsorption Adsorption mechanism: • localized adsorption • filling of micropores • monolayer adsorption • multilayer adsorption • capillary condensation Classification of isotherms of physical adsorption :

  15. Ultramicropore Specific sites External surface Mesopores (nanopores) Supermicropore Internal surface Different stages of adsorption on heterogeneous adsorbent

  16. n / ms • supermicropores • cooperative mechanism • Filling of micropores • ultramicropores p / p0 Adsorption on purely microporous samples: d  0.4 à 2 nm

  17. Building statistical monolayer • Multilayer • Adsorption n / ms B p / p0 Adsorption on purely non-porous sample

  18. Building statistical monolayer • Multilayer • Adsorption • Capillary • condensation • Hysteresis n / ms B p / p0 Adsorption on purely mesoporous sample : d  2 à 50 nm

  19. ns/ms p/p° Adsorption on heterogeneous sample

  20. Interpretation of isotherms of physicaladsorption • Generally, adsorption starts at lower pressure when the interaction between the surface and the adsorbed particles is stronger • When an adsorbate is in contact with an adsorbent, adsorption is first observed (that is, at lowest relative pressure, domain A) on the centers of adsorption that are the most strongly attractive (defaults, imperfections, etc..)

  21. Interpretation of isotherms of physicaladsorption The filling of the micropores happens also at pressures relatively low (domain B) Domain C corresponds to pressures where the adsorption monomolecular  is observed. At the end of this domain , statistically, the whole surface of solid is totally covered by a monolayer adsorbed on the surface.

  22. Interpretation of isotherms of physicaladsorption When the relative pressure increases, (domain D), the surface is covered by multilayer of increasing thickness: multilayer adsorption Starting at some pressure in the domain D, one can observe a rapid acceleration of adsorption, due to the phenomenon of capillary condensation (in nanopores)

  23. Capillary condensation Building of monolayer Multilayer adsorption Localised dsorption Filling of micropores Different domains of physical adsorption ns/ms p/p°

  24. I II III B n/ms V IV VI B p/p0 Classification de l'IUPAC des isothermes d'adsorption physique T < Tc

  25. I II III B n/ms V IV VI B p/p0 Classification (I) The isotherms of adsorption of type I are characterized par horizontal line which indicates saturation of the adsorbent. This isotherm is observed in adsorbents having only micropores that are filled at low pressures. Lower pressure of filling, smaller the size of the pores.

  26. I II III B n/ms V IV VI B p/p0 Classification (II) The isotherms of adsorption of type II are characterized par increase of the adsorbed quantity, in a continuous way, as a function of the equilibrium pressure. This type of isotherms is observed in non-porous adsorbents or in macropores. It indicates the multilayer adsorption..

  27. I II III B n/ms V IV VI B p/p0 Classification (III) Desorption is very often nonreversible; one observes a hysteresis of desorption with respect to adsorption. Isotherms of the type IV have the same shape as the type II at lower pressures (approximately, below 0.4 of the reduced pressure). At higher pressures it is characterized par saturation which is observed at different pressures. This type of isotherms is observed when adsorption happens in nanoporous (mesoporous) materials where the capillary condensation is observed.

  28. I II III B n/ms V IV VI B p/p0 Classification (IV) The isotherms of adsorption of type III and V are less frequently observed: they are similar to isotherm of type II and IV but they differ at low pressures. This difference is attributed to weak interaction between adsorbent and the adsorbed molecules. For example, it is observed for adsorption of water on hydrophobic surfaces.

  29. I II III B n/ms V IV VI B p/p0 Classification (V) Step-wise isotherms of adsorption (type VI) are observed in adsorption on homogeneous surfaces where the layers are formed one after another. The proposed classification shows the typical adsorbents. The real isotherms are very often composed of different types discussed above.

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