6 research outputs found
Ca<sub>11</sub>E<sub>3</sub>C<sub>8</sub> (E = Sn, Pb): New Complex Carbide Zintl Phases Grown from Ca/Li Flux
New
carbide Zintl phases Ca<sub>11</sub>E<sub>3</sub>C<sub>8</sub> (E
= Sn, Pb) were grown from reactions of carbon and heavy tetrelides
in Ca/Li flux. They form with a new structure type in space group <i>P</i>2<sub>1</sub>/<i>c</i> (<i>a</i> =
13.1877(9)ÂÃ…, <i>b</i> = 10.6915(7)ÂÃ…, <i>c</i> = 14.2148(9)ÂÃ…, β = 105.649(1)°, and <i>R</i><sub>1</sub> = 0.019 for the Ca<sub>11</sub>Sn<sub>3</sub>C<sub>8</sub> analog). The structure features isolated E<sup>4–</sup> anions
as well as acetylide (C<sub>2</sub><sup>2–</sup>) and allenylide
(C<sub>3</sub><sup>4–</sup>) anions; the vibrational modes
of the carbide anions are observed in the Raman spectrum. The charge-balanced
nature of these phases is confirmed by DOS calculations which indicate
that the tin analog has a small band gap (<i>E</i><sub>g</sub> < 0.1 eV) and the lead analog has a pseudogap at the Fermi level.
Reactions of these compounds with water produce acetylene and allene
Ca<sub>11</sub>E<sub>3</sub>C<sub>8</sub> (E = Sn, Pb): New Complex Carbide Zintl Phases Grown from Ca/Li Flux
New
carbide Zintl phases Ca<sub>11</sub>E<sub>3</sub>C<sub>8</sub> (E
= Sn, Pb) were grown from reactions of carbon and heavy tetrelides
in Ca/Li flux. They form with a new structure type in space group <i>P</i>2<sub>1</sub>/<i>c</i> (<i>a</i> =
13.1877(9)ÂÃ…, <i>b</i> = 10.6915(7)ÂÃ…, <i>c</i> = 14.2148(9)ÂÃ…, β = 105.649(1)°, and <i>R</i><sub>1</sub> = 0.019 for the Ca<sub>11</sub>Sn<sub>3</sub>C<sub>8</sub> analog). The structure features isolated E<sup>4–</sup> anions
as well as acetylide (C<sub>2</sub><sup>2–</sup>) and allenylide
(C<sub>3</sub><sup>4–</sup>) anions; the vibrational modes
of the carbide anions are observed in the Raman spectrum. The charge-balanced
nature of these phases is confirmed by DOS calculations which indicate
that the tin analog has a small band gap (<i>E</i><sub>g</sub> < 0.1 eV) and the lead analog has a pseudogap at the Fermi level.
Reactions of these compounds with water produce acetylene and allene
Reaction of Methane with Bulk Intermetallics Containing Iron Clusters Yields Carbon Nanotubes
Reaction
of Methane with Bulk Intermetallics Containing
Iron Clusters Yields Carbon Nanotube
Microwave-Specific Enhancement of the Carbon–Carbon Dioxide (Boudouard) Reaction
The Boudouard reaction, which is
the reaction of carbon and carbon
dioxide to produce carbon monoxide, represents a simple and straightforward
method for the remediation of carbon dioxide in the environment through
reduction: CO<sub>2</sub>(g) + C(s) ⇌ 2CO. However, due to
the large positive enthalpy, typically reported to be 172 kJ/mol under
standard conditions at 298 K, the equilibrium does not favor CO production
until temperatures >700 °C, when the entropic term, −<i>T</i>Δ<i>S</i>, begins to dominate and the free
energy becomes negative. We have found that, under microwave irradiation
to selectively heat the carbon, dramatically different thermodynamics
for the reaction are observed. During kinetic studies of the reaction
under conditions of flowing CO<sub>2</sub>, the apparent activation
energy dropped from 118.4 kJ/mol under conventional convective heating
to 38.5 kJ/mol under microwave irradiation. From measurement of the
equilibrium constants as a function of temperature, the enthalpy of
the reaction dropped from 183.3 kJ/mol at ∼1100 K to 33.4 kJ/mol
at the same temperature under microwave irradiation. This changes
the position of the equilibrium so that the temperature at which CO
becomes the major product drops from 643 °C in the conventional
thermal reaction to 213 °C in the microwave. The observed reduction
in the apparent enthalpy of the microwave driven reaction, compared
to what is determined for the thermal reaction from standard heats
of formation, can be thought of as arising from additional energy
being put into the carbon by the microwaves, effectively increasing
its apparent standard enthalpy. Mechanistically, it is hypothesized
that the enhanced reactivity arises from the interaction of CO<sub>2</sub> with the steady-state concentration of electron–hole
pairs that are present at the surface of the carbon due to the space-charge
mechanism, by which microwaves are known to heat carbon. Such a mechanism
is unique to microwave-induced heating and, given the effect it has
on the thermodynamics of the Boudouard reaction, suggests that its
use may yield energy savings in driving the general class of gas–carbon
reactions
Mechanism of Initiation in the Phillips Ethylene Polymerization Catalyst: Redox Processes Leading to the Active Site
The detailed mechanism by which ethylene
polymerization is initiated
by the inorganic Phillips catalyst (Cr/SiO<sub>2</sub>) without recourse
to an alkylating cocatalyst remains one of the great unsolved mysteries
of heterogeneous catalysis. Generation of the active catalyst starts
with reduction of Cr<sup>VI</sup> ions dispersed on silica. A lower
oxidation state, generally accepted to be Cr<sup>II</sup>, is required
to activate ethylene to form an organoCr active site. In this work,
a mesoporous, optically transparent monolith of Cr<sup>VI</sup>/SiO<sub>2</sub> was prepared using sol–gel chemistry in order to monitor
the reduction process spectroscopically. Using in situ UV–vis
spectroscopy, we observed a very clean, stepwise reduction by CO of
Cr<sup>VI</sup> first to Cr<sup>IV</sup>, then to Cr<sup>II</sup>.
Both the intermediate and final states show XANES consistent with
these oxidation state assignments, and aspects of their coordination
environments were deduced from Raman and UV–vis spectroscopies.
The intermediate Cr<sup>IV</sup> sites are inactive toward ethylene
at 80 °C. The Cr<sup>II</sup> sites, which have long been postulated
as the end point of CO reduction, were observed directly by high-frequency/high-field
EPR spectroscopy. They react quantitatively with ethylene to generate
the organoCr<sup>III</sup> active sites, characterized by X-ray absorption
and UV–vis spectroscopy, which initiate polymerization
Mechanism of Initiation in the Phillips Ethylene Polymerization Catalyst: Redox Processes Leading to the Active Site
The detailed mechanism by which ethylene
polymerization is initiated
by the inorganic Phillips catalyst (Cr/SiO<sub>2</sub>) without recourse
to an alkylating cocatalyst remains one of the great unsolved mysteries
of heterogeneous catalysis. Generation of the active catalyst starts
with reduction of Cr<sup>VI</sup> ions dispersed on silica. A lower
oxidation state, generally accepted to be Cr<sup>II</sup>, is required
to activate ethylene to form an organoCr active site. In this work,
a mesoporous, optically transparent monolith of Cr<sup>VI</sup>/SiO<sub>2</sub> was prepared using sol–gel chemistry in order to monitor
the reduction process spectroscopically. Using in situ UV–vis
spectroscopy, we observed a very clean, stepwise reduction by CO of
Cr<sup>VI</sup> first to Cr<sup>IV</sup>, then to Cr<sup>II</sup>.
Both the intermediate and final states show XANES consistent with
these oxidation state assignments, and aspects of their coordination
environments were deduced from Raman and UV–vis spectroscopies.
The intermediate Cr<sup>IV</sup> sites are inactive toward ethylene
at 80 °C. The Cr<sup>II</sup> sites, which have long been postulated
as the end point of CO reduction, were observed directly by high-frequency/high-field
EPR spectroscopy. They react quantitatively with ethylene to generate
the organoCr<sup>III</sup> active sites, characterized by X-ray absorption
and UV–vis spectroscopy, which initiate polymerization