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njit-etd2003-111 - New Jersey Institute of Technology

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10<br />

exchange-correlation term is, itself, also divided into separate exchange and correlation<br />

components in most actual DFT functions). A variety <strong>of</strong> functionals have been defined,<br />

generally distinguished by the way that they treat exchange and correlation components. 19<br />

• Local exchange and correlation functionals involve only the values <strong>of</strong> the electron<br />

spin densities.<br />

• Gradient-corrected functionals involve both the values <strong>of</strong> electron spin densities<br />

and their gradients. 5uch functionals are also referred to as non-local in literature.<br />

A popular gradient-corrected exchange functional is one proposed by Becke 2<br />

; a<br />

widely used gradient-corrected correlation functional is the LYP functional <strong>of</strong><br />

Lee, Yang and Parr. The combination <strong>of</strong> the two forms the B-LYP method.<br />

B3LYP is Becke-style 3-parameter density functional theory (using the Lee-<br />

Yang-Parr correlation functional).<br />

2.3 Kinetics<br />

2.3.1 Lindemann-Hinshelwood Mechanism for Unimolecular Reactions<br />

A general theory for thermal unimolecular reactions that forms the basis for the current<br />

theory <strong>of</strong> thermal unimolecular rates was proposed by Lindemann 21 in 1922. He proposed<br />

that molecules become energized by bimolecular collisions, with a time lag between the<br />

moment <strong>of</strong> collisional energy transfer and the time the molecule decomposes. Energized<br />

molecules could then undergo deactivating collisions before decomposition occurred.<br />

5teinfeld et al. 22 indicated that "A major achievement <strong>of</strong> Lindemann's theory is its ability<br />

to explain the experimental finding that the reaction rate changes from first to second<br />

order in going from the high- to low-pressure limit."

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