4 research outputs found
Correlation Effects on the Relative Stabilities of Alkanes
The āalkane branching effectā
denotes the fact that
simple alkanes with more highly branched carbon skeletons, for example,
isobutane and neopentane, are more stable than their normal isomers,
for example, <i>n</i>-butane and <i>n</i>-pentane.
Although <i>n</i>-alkanes have no branches, the ākinksā
(or āprotobranchesā) in their chains (defined as the
composite of 1,3-alkylāalkyl interactionsīøincluding
methine, methylene, and methyl groups as alkyl entitiesīøpresent
in most linear, cyclic, and branched alkanes, but not methane or ethane)
also are associated with lower energies. Branching and protobranching
stabilization energies are evaluated by isodesmic comparisons of protobranched
alkanes with ethane. Accurate ab initio characterization of branching
and protobranching stability requires post-self-consistent field (SCF)
treatments, which account for medium range (ā¼1.5ā3.0
Ć
) electron correlation. Localized molecular orbital second-order
MĆøllerāPlesset (LMO-MP2) partitioning of the correlation
energies of simple alkanes into localized contributions indicates
that correlation effects between electrons in 1,3-alkyl groups are
largely responsible for the enhanced correlation energies and general
stabilities of branched and protobranched alkanes
A HuĢckel Theory Perspective on MoĢbius Aromaticity
Heilbronnerās HuĢckel molecular orbital treatment of MoĢbius 4nāĻ annulenes is revisited. When uneven twisting in Ļ-systems of small MoĢbius rings is accounted for, their resonance energies become comparable to iso-Ļ-electronic linear alkenes with the same number of carbon atoms. Larger MoĢbius rings distribute Ļ-twisting more evenly but exhibit only modest aromatic stabilization. Dissected nucleus independent chemical shifts (NICS), based on the LMO (localized molecular orbital)āNICS(0)<sub>Ļ</sub> index confirm the magnetic aromaticity of the MoĢbius annulenes considered
Why Do Two ĻāElectron Four-Membered HuĢckel Rings Pucker?
Notwithstanding their two (i.e., 4<i>n</i> + 2) Ļ electrons, four-membered ring systems, <b>1</b>ā<b>4</b>, favor puckered geometries (<b>1a</b>ā<b>4a</b>) despite the reduction in vicinal Ļ overlap and in the ring atom bond angles. This nonplanar preference is due to Ļ ā Ļ* hyperconjugative interactions across the ring (A) rather than to partial 1,3-bonding (B). Electronegative substituents (e.g., F in C<sub>4</sub>F<sub>4</sub><sup>2+</sup>) reduce the Ļ ā Ļ* electron delocalization, and planar geometries result. In contrast, electropositive groups (e.g., SiH<sub>3</sub> in C<sub>4</sub>(SiH<sub>3</sub>)<sub>4</sub><sup>2+</sup>) enhance hyperconjugation and increase the ring inversion barriers substantially
Potential-Dependent Generation of O<sub>2</sub><sup>ā</sup> and LiO<sub>2</sub> and Their Critical Roles in O<sub>2</sub> Reduction to Li<sub>2</sub>O<sub>2</sub> in Aprotic LiāO<sub>2</sub> Batteries
Discharging of the aprotic LiāO<sub>2</sub> battery relies
on the oxygen reduction reaction (ORR) producing Li<sub>2</sub>O<sub>2</sub> in the positive electrode, which remains incompletely understood.
Here, we report a mechanistic study of the Li-ORR on a model system,
i.e., an Au electrode in a Li<sup>+</sup> dimethyl sulfoxide (DMSO)
electrolyte. By spectroscopic identification of the reaction intermediates
coupled with density functional theory calculations, we conclude that
the formation of O<sub>2</sub><sup>ā</sup> and LiO<sub>2</sub> in the Li-ORR critically depends on electrode potentials and determines
the Li<sub>2</sub>O<sub>2</sub> formation mechanism. At low overpotentials
(> 2.0 V vs Li/Li<sup>+</sup>) O<sub>2</sub><sup>ā</sup> is
identified to be the first surface intermediate, which diffuses into
the bulk electrolyte and forms Li<sub>2</sub>O<sub>2</sub> therein
via a solution-mediated disproportionation mechanism. At high overpotentials
(ca. 2.0ā1.6 V vs Li/Li<sup>+</sup>) LiO<sub>2</sub> has been
observed, which can rapidly transform to Li<sub>2</sub>O<sub>2</sub> by further electro-reduction, suggesting a surface-mediated mechanism.
The solution-mediated Li<sub>2</sub>O<sub>2</sub> formation that can
account for the widely observed toroid-shaped discharged Li<sub>2</sub>O<sub>2</sub> particles has also been thoroughly examined. Thus,
O<sub>2</sub><sup>ā</sup> formation controls the overall reaction
onset potential, and LiO<sub>2</sub> formation demarcates the change
from a solution- to surface-mediated reaction mechanism. The new findings
and improved understandings of the Li-ORR in DMSO will contribute
to the further development of aprotic LiāO<sub>2</sub> batteries