The Markovnikov regioselectivity rule in the light of site activation models
Author
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Aizman, Arie
Author
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Contreras Ramos, Renato
Author
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Galván, M.
Author
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Cedillo, Andrés
Author
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Santos, J. C.
Author
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Chamorro, E.
Admission date
dc.date.accessioned
2019-01-29T13:47:38Z
Available date
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2019-01-29T13:47:38Z
Publication date
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2002
Cita de ítem
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Journal of Physical Chemistry A, Volumen 106, Issue 34, 2002, Pages 7844-7849
Identifier
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10895639
Identifier
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10.1021/jp020214y
Identifier
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https://repositorio.uchile.cl/handle/2250/159774
Abstract
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The electrophilic addition of HCl to a series of asymmetric alkenes-propene, 2-methyl-2-butene, styrene, 2-phenylpropene, and 1-cyanopropene-is used as a model system to study the regioselectivity Markovnikov rule using density functional theory reactivity descriptors. The results show that this rule may be interpreted on the basis of a site activation model that goes beyond the Li-Evans model of selectivity if both the fluctuations in global softness and Fukui functions at the active site are taken into account. A local static analysis based on the condensed Fukui function at the ground state of alkenes was also performed. For all the systems considered, the Markovnikov carbon (M) atom (i.e., the less substituted one) displays electrophilic Fukui function values that are larger than those associated with the more substituted anti-Markovnikov (AM) carbon atom at the double bond. In most cases, they are also larger than the corresponding nucleophilic
Fukui function values at both carbon centers of the ethylenic functionality. Site activation at the nucleophilic
and electrophilic centers of the alkenes considered was probed by changes in regional softness with reference
to the transition state structures. The results are consistent with the empirical Markovnikov rule. A global
analysis of involved structures in the electrophilic addition of HCl shows that while the ground state and
transition state structures display relative values of the energy and molecular hardness ordered in a way that
is consistent with the maximum hardness principle (MHP), the comparison between the Markovnikov and
anti-Markovnikov transition state structures do not: the Markovnikov channel presents a transition state which
is lower in energy and softer than the one corresponding to the anti-Markovnikov addition.