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II International Symposium on Carbon for Catalysis ABSTRACTS

II International Symposium on Carbon for Catalysis ABSTRACTS

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PL-3<br />

developed NLDFT model, which allowed us to determine the solid–fluid potential as a<br />

functi<strong>on</strong> of the distance from the surface. It turned out that the adsorpti<strong>on</strong> in the first<br />

molecular layer is localized and c<strong>on</strong>trolled by short-range <strong>for</strong>ces, with the surface being<br />

highly heterogeneous. Bey<strong>on</strong>d the first molecular layer the solid–fluid potential obeys the<br />

power law and decays inversely the third power of the distance. Interestingly enough that the<br />

absolute value of the potential outside the first molecular layer is several times smaller than it<br />

is predicted by the LJ pair potential. This means that the individuality of a n<strong>on</strong>porous material<br />

is mainly restricted by the first molecular layer (more exact estimati<strong>on</strong> is 1.3 of m<strong>on</strong>olayer<br />

capacity) and partly explains the universality of adsorpti<strong>on</strong> isotherms at relative pressures<br />

above approximately 0.1, which is reflected in so-called t-curve. Some additi<strong>on</strong>al in<strong>for</strong>mati<strong>on</strong><br />

we have obtained by the comparis<strong>on</strong> of the behavior of nitrogen adsorbed <strong>on</strong> n<strong>on</strong>graphitized<br />

carb<strong>on</strong> black and n<strong>on</strong>porous silica. In the latter case the solid–fluid potential decays inversely<br />

the fourth power of the distance, meaning that, as opposed to carb<strong>on</strong> blacks, the potential is<br />

exerted by surface (oxygen) atoms. Analysis of N 2 adsorpti<strong>on</strong> in highly ordered MCM-41<br />

silica samples has shown a startling result that the effect of the surface curvature <strong>on</strong> the solid–<br />

fluid potential is nearly absent, which indirectly c<strong>on</strong>firms the c<strong>on</strong>clusi<strong>on</strong> that the adsorpti<strong>on</strong><br />

potential of amorphous solids in c<strong>on</strong>tact layer is short-range.<br />

Applicati<strong>on</strong> of the developed NLDFT to activated carb<strong>on</strong>s has c<strong>on</strong>vincingly shown that<br />

the use of n<strong>on</strong>graphitized carb<strong>on</strong> black as a reference system leads to much more reliable PSD<br />

functi<strong>on</strong>s and excellent fitting of experimental adsorpti<strong>on</strong> isotherms. For example, the PSD<br />

functi<strong>on</strong>s have become smoother and do not show any artificial peaks and gaps. Thus, the<br />

pore structure of carb<strong>on</strong>aceous materials, the surface area and its distributi<strong>on</strong> over the pore<br />

size can now be reliably disclosed with the developed approach. Additi<strong>on</strong>ally, this technique<br />

provides the predicti<strong>on</strong> of differential heat of adsorpti<strong>on</strong> and adsorpti<strong>on</strong> de<strong>for</strong>mati<strong>on</strong><br />

(adsorpti<strong>on</strong>-induced c<strong>on</strong>tracti<strong>on</strong> and swelling). The latter is important <strong>for</strong> the problem of<br />

methane and hydrogen storage. At present we carry out further investigati<strong>on</strong>s to develop a<br />

NLDFT-based tool to determine the surface chemistry of n<strong>on</strong>porous and porous carb<strong>on</strong>aceous<br />

materials. In particular, it will allow us to identify different functi<strong>on</strong>al surface groups,<br />

crystalline defects, relati<strong>on</strong> of basal, prismatic, and defect surfaces, which is important <strong>for</strong> the<br />

applicati<strong>on</strong> of those materials in catalysis. To summarize, <strong>on</strong>e can state that the analysis of<br />

adsorpti<strong>on</strong> isotherms with NLDFT is a promising tool <strong>for</strong> determinati<strong>on</strong> of porous materials<br />

structure and further ef<strong>for</strong>ts are needed.<br />

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