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II International Symposium on Carbon for Catalysis ABSTRACTS

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PP-I-50<br />

DENSITY FUNCTIONAL CALCULATIONS ON THE FORMATION OF CARBON<br />

NANOFIBERS<br />

Zhu Y., Dai Y., Zhou J., Sui Zh., Yuan W.<br />

State Key Laboratory of Chemical Reacti<strong>on</strong> Engineering, East China University of Science<br />

and Technology, Shanghai 200237, China<br />

e-mail: yanzhu@ecust.edu.cn<br />

Introducti<strong>on</strong><br />

Carb<strong>on</strong> nanofiber (CNF) is attracting increased attenti<strong>on</strong>. There are two major reas<strong>on</strong>s <strong>for</strong><br />

studying this particular kind of carb<strong>on</strong>. On the <strong>on</strong>e hand, filamentous carb<strong>on</strong> is <strong>for</strong>med in a<br />

temperature range where reacti<strong>on</strong>s of great technical importance, e.g., Fisher-Tropsch<br />

synthesis, methanati<strong>on</strong>, and steam-re<strong>for</strong>ming, are usually carried out. On the other hand,<br />

because of the unique chemical and physical properties induced by the CNF geometric and<br />

electr<strong>on</strong>ic structure, CNF has been applied in many fields such as catalysts, catalyst supports,<br />

gas storage materials, electrodes <strong>for</strong> fuel cell, and polymer additives. CNFs are synthesized<br />

mainly by chemical vapor depositi<strong>on</strong> (CVD). The global evoluti<strong>on</strong> of the growth is divided<br />

into three stages: firstly, carb<strong>on</strong> atoms and hydrogen molecules are <strong>for</strong>med with the<br />

decompositi<strong>on</strong> of carb<strong>on</strong>-c<strong>on</strong>taining gas <strong>on</strong> certain transiti<strong>on</strong> metal surface; sec<strong>on</strong>dly, the<br />

generated carb<strong>on</strong> atoms dissolve into the metal particle and diffuse through the bulk or al<strong>on</strong>g<br />

the surface; finally, the carb<strong>on</strong> atoms precipitate in the <strong>for</strong>m of graphene layer <strong>on</strong> the rear side<br />

of the metal particle. The sec<strong>on</strong>d stage is generally regarded as the rate-determining step<br />

because the activati<strong>on</strong> energy <strong>for</strong> carb<strong>on</strong> diffusi<strong>on</strong> is in reas<strong>on</strong>able agreement with that <strong>for</strong> the<br />

CNF <strong>for</strong>mati<strong>on</strong> in a range of 1.3-1.5eV. However, in fact, the CNF growth mechanism at the<br />

atomic scale is still unclear.<br />

As suggested microdiffracti<strong>on</strong> data, the [100] crystallographic directi<strong>on</strong> of the FCC Ni lattice<br />

coincided with the filament axis, and (111) planes which were parallel to the graphite sheet<br />

accounted <strong>for</strong> the nucleati<strong>on</strong> of the filament. This point was also c<strong>on</strong>firmed by Yang and<br />

Chen who per<strong>for</strong>med both experimental and theoretical studies <strong>on</strong> carb<strong>on</strong> filament growth,<br />

and verified that the Ni(100) and Ni(110) were am<strong>on</strong>g the gas/metal interface, while the<br />

Ni(111) and Ni(311) were am<strong>on</strong>g the graphite/metal interface. In this paper, the diffusi<strong>on</strong> of<br />

carb<strong>on</strong> atoms <strong>on</strong> Ni(111) is focused.<br />

220

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