2 research outputs found
Formation of 6‑Methyl-1,4-dihydronaphthalene in the Reaction of the <i>p</i>‑Tolyl Radical with 1,3-Butadiene under Single-Collision Conditions
Crossed molecular
beam reactions of <i>p</i>-tolyl (C<sub>7</sub>H<sub>7</sub>) plus 1,3-butadiene (C<sub>4</sub>H<sub>6</sub>), <i>p</i>-tolyl (C<sub>7</sub>H<sub>7</sub>) plus 1,3-butadiene-<i>d</i><sub>6</sub> (C<sub>4</sub>D<sub>6</sub>), and <i>p</i>-tolyl-<i>d</i><sub>7</sub> (C<sub>7</sub>D<sub>7</sub>) plus 1,3-butadiene (C<sub>4</sub>H<sub>6</sub>) were carried
out under single-collision conditions at collision energies of about
55 kJ mol<sup>–1</sup>. 6-Methyl-1,4-dihydronaphthalene was
identified as the major reaction product formed at fractions of about
94% with the monocyclic isomer (<i>trans</i>-1-<i>p</i>-tolyl-1,3-butadiene) contributing only about 6%. The reaction is
initiated by <i>barrierless</i> addition of the <i>p</i>-tolyl radical to the terminal carbon atom of the 1,3-butadiene
via a van der Waals complex. The collision complex isomerizes via
cyclization to a bicyclic intermediate, which then ejects a hydrogen
atom from the bridging carbon to form 6-methyl-1,4-dihydronaphthalene
through a tight exit transition state located about 27 kJ mol<sup>–1</sup> above the separated products. This is the dominant
channel under the present experimental conditions. Alternatively,
the collision complex can also undergo hydrogen ejection to form <i>trans</i>-1-<i>p</i>-tolyl-1,3-butadiene; this is
a minor contributor to the present experiment. The de facto barrierless
formation of a methyl-substituted aromatic hydrocarbons by dehydrogenation
via a single event represents an important step in the formation of
polycyclic aromatic hydrocarbons (PAHs) and their partially hydrogenated
analogues in combustion flames and the interstellar medium
Combined Crossed Molecular Beam and Ab Initio Investigation of the Reaction of Boron Monoxide (BO; X<sup>2</sup>Σ<sup>+</sup>) with 1,3-Butadiene (CH<sub>2</sub>CHCHCH<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>) and Its Deuterated Counterparts
The reactions of the boron monoxide
(<sup>11</sup>BO; X<sup>2</sup>Σ<sup>+</sup>) radical with 1,3-butadiene
(CH<sub>2</sub>CHCHCH<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>) and
its partially deuterated
counterparts, 1,3-butadiene-<i>d</i><sub>2</sub> (CH<sub>2</sub>CDCDCH<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>) and 1,3-butadiene-<i>d</i><sub>4</sub> (CD<sub>2</sub>CHCHCD<sub>2</sub>; X<sup>1</sup>A<sub>g</sub>), were investigated under single collision conditions
exploiting a crossed molecular beams machine. The experimental data
were combined with the state-of-the-art ab initio electronic structure
calculations and statistical RRKM calculations to investigate the
underlying chemical reaction dynamics and reaction mechanisms computationally.
Our investigations revealed that the reaction followed indirect scattering
dynamics through the formation of <sup>11</sup>BOC<sub>4</sub>H<sub>6</sub> doublet radical intermediates via the barrierless addition
of the <sup>11</sup>BO radical to the terminal carbon atom (C1/C4)
and/or the central carbon atom (C2/C3) of 1,3-butadiene. The resulting
long-lived <sup>11</sup>BOC<sub>4</sub>H<sub>6</sub> intermediate(s)
underwent isomerization and/or unimolecular decomposition involving
eventually at least two distinct atomic hydrogen loss pathways to
1,3-butadienyl-1-oxoboranes (CH<sub>2</sub>CHCHCH<sup>11</sup>BO)
and 1,3-butadienyl-2-oxoboranes (CH<sub>2</sub>C (<sup>11</sup>BO)ÂCHCH<sub>2</sub>) in overall exoergic reactions via tight exit transition
states. Utilizing partially deuterated 1,3-butadiene-<i>d</i><sub>2</sub> and -<i>d</i><sub>4</sub>, we revealed that
the hydrogen loss from the methylene moiety (CH<sub>2</sub>) dominated
with 70 ± 10% compared to an atomic hydrogen loss from the methylidyne
group (CH) of only 30 ± 10%; these data agree nicely with the
theoretically predicted branching ratio of 80% versus 19%