10.01.2015 Views

II International Symposium on Carbon for Catalysis ABSTRACTS

II International Symposium on Carbon for Catalysis ABSTRACTS

II International Symposium on Carbon for Catalysis ABSTRACTS

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

KL-6<br />

THEORY OF MECHANICAL BEHAVIOR OF MICROPOROUS CARBON<br />

CATALYSTS<br />

Rusanov А.I.<br />

Mendeleev Center of St. Petersburg State University, St. Petersburg, Russia<br />

e-mail: rusanov@AR1047.spb.edu<br />

Researchers dealing with microporous carb<strong>on</strong> sorbents observed the sorpti<strong>on</strong>-stricti<strong>on</strong><br />

phenomen<strong>on</strong> (a change in the sorbent volume), which can take different <strong>for</strong>ms depending <strong>on</strong><br />

the external c<strong>on</strong>diti<strong>on</strong>s. When a sorbate enters a sorbent, the latter can expand at a high<br />

temperature, but also can c<strong>on</strong>tract at a sufficiently low temperature and a low amount of the<br />

sorbate with subsequent transiti<strong>on</strong> to expansi<strong>on</strong> at higher sorbate amounts. Naturally, the<br />

phenomen<strong>on</strong> is determined by molecular interacti<strong>on</strong>s of the sorbate matter with the micropore<br />

walls. A special case is chemisorpti<strong>on</strong> that is typical <strong>for</strong> catalysis.<br />

The theory of mechanical behavior of microporous carb<strong>on</strong> bodies reported in this<br />

presentati<strong>on</strong> includes three parts. The first part c<strong>on</strong>tains the calculati<strong>on</strong> of the pressure tensor<br />

inside a micropore where there cannot be the sorbate bulk phase, and the pressure tensor<br />

structure is determined by the micropore shape. Calculati<strong>on</strong>s have been carried out <strong>for</strong><br />

spherical cavities, cylindrical pores, and flat (slit-like) pores. Since carb<strong>on</strong> interacts with<br />

dispersi<strong>on</strong> <strong>for</strong>ces, all calculati<strong>on</strong>s were made <strong>on</strong> the basis of the pair potential<br />

−λ<br />

∅ () r =− A r<br />

(1)<br />

ij<br />

( λ )<br />

ij<br />

where r is the distance between molecules of sorts i and j,<br />

( )<br />

A λ<br />

ij<br />

is a c<strong>on</strong>stant of interacti<strong>on</strong>, λ<br />

= 6 <strong>for</strong> the ordinary van der Waals <strong>for</strong>ces (at r < 12 nm) and λ = 7 <strong>for</strong> the van der Waals<br />

<strong>for</strong>ces with electromagnetic retardati<strong>on</strong> (at r > 50 nm). As Equati<strong>on</strong> (1) itself, the whole<br />

computati<strong>on</strong>al scheme is based <strong>on</strong> the asymptotic theory of dispersi<strong>on</strong> interacti<strong>on</strong>s (presuming<br />

the pore diameter to be c<strong>on</strong>siderably larger than the molecular size). The calculati<strong>on</strong> yields a<br />

negative value <strong>for</strong> the normal (to the pore walls) pressure (leading to the self-c<strong>on</strong>tracti<strong>on</strong> of a<br />

porous body) in vacuum and establishes c<strong>on</strong>diti<strong>on</strong>s when the interacti<strong>on</strong> with the first porti<strong>on</strong><br />

of a sorbate provokes an additi<strong>on</strong>al c<strong>on</strong>tracti<strong>on</strong> (the most probable in the case of<br />

chemisorpti<strong>on</strong>). This additi<strong>on</strong>al c<strong>on</strong>tracti<strong>on</strong> is shown to be attained easier the smaller is the<br />

pore size and is best realizable <strong>for</strong> nanoporous solids.<br />

30

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!