6 research outputs found
Near-Perfect CO<sub>2</sub>/CH<sub>4</sub> Selectivity Achieved through Reversible Guest Templating in the Flexible Metal–Organic Framework Co(bdp)
Metal–organic
frameworks are among the most promising materials
for industrial gas separations, including the removal of carbon dioxide
from natural gas, although substantial improvements in adsorption
selectivity are still sought. Herein, we use equilibrium adsorption
experiments to demonstrate that the flexible metal–organic
framework Co(bdp) (bdp<sup>2–</sup> = 1,4-benzenedipyrazolate)
exhibits a large CO<sub>2</sub> adsorption capacity and approaches
complete exclusion of CH<sub>4</sub> under 50:50 mixtures of the two
gases, leading to outstanding CO<sub>2</sub>/CH<sub>4</sub> selectivity
under these conditions. <i>In situ</i> powder X-ray diffraction
data indicate that this selectivity arises from reversible guest templating,
in which the framework expands to form a CO<sub>2</sub> clathrate
and then collapses to the nontemplated phase upon desorption. Under
an atmosphere dominated by CH<sub>4</sub>, Co(bdp) adsorbs minor amounts
of CH<sub>4</sub> along with CO<sub>2</sub>, highlighting the importance
of studying all relevant pressure and composition ranges via multicomponent
measurements when examining mixed-gas selectivity in structurally
flexible materials. Altogether, these results show that Co(bdp) may
be a promising CO<sub>2</sub>/CH<sub>4</sub> separation material and
provide insights for the further study of flexible adsorbents for
gas separations
Near-Perfect CO<sub>2</sub>/CH<sub>4</sub> Selectivity Achieved through Reversible Guest Templating in the Flexible Metal–Organic Framework Co(bdp)
Metal–organic
frameworks are among the most promising materials
for industrial gas separations, including the removal of carbon dioxide
from natural gas, although substantial improvements in adsorption
selectivity are still sought. Herein, we use equilibrium adsorption
experiments to demonstrate that the flexible metal–organic
framework Co(bdp) (bdp<sup>2–</sup> = 1,4-benzenedipyrazolate)
exhibits a large CO<sub>2</sub> adsorption capacity and approaches
complete exclusion of CH<sub>4</sub> under 50:50 mixtures of the two
gases, leading to outstanding CO<sub>2</sub>/CH<sub>4</sub> selectivity
under these conditions. <i>In situ</i> powder X-ray diffraction
data indicate that this selectivity arises from reversible guest templating,
in which the framework expands to form a CO<sub>2</sub> clathrate
and then collapses to the nontemplated phase upon desorption. Under
an atmosphere dominated by CH<sub>4</sub>, Co(bdp) adsorbs minor amounts
of CH<sub>4</sub> along with CO<sub>2</sub>, highlighting the importance
of studying all relevant pressure and composition ranges via multicomponent
measurements when examining mixed-gas selectivity in structurally
flexible materials. Altogether, these results show that Co(bdp) may
be a promising CO<sub>2</sub>/CH<sub>4</sub> separation material and
provide insights for the further study of flexible adsorbents for
gas separations
Reversible Capture and Release of Cl<sub>2</sub> and Br<sub>2</sub> with a Redox-Active Metal–Organic Framework
Extreme toxicity, corrosiveness,
and volatility pose serious challenges
for the safe storage and transportation of elemental chlorine and
bromine, which play critical roles in the chemical industry. Solid
materials capable of forming stable nonvolatile compounds upon reaction
with elemental halogens may partially mitigate these challenges by
allowing safe halogen release on demand. Here we demonstrate that
elemental halogens quantitatively oxidize coordinatively unsaturated
Co(II) ions in a robust azolate metal–organic framework (MOF)
to produce stable and safe-to-handle Co(III) materials featuring terminal
Co(III)–halogen bonds. Thermal treatment of the oxidized MOF
causes homolytic cleavage of the Co(III)–halogen bonds, reduction
to Co(II), and concomitant release of elemental halogens. The reversible
chemical storage and thermal release of elemental halogens occur with
no significant losses of structural integrity, as the parent cobaltous
MOF retains its crystallinity and porosity even after three oxidation/reduction
cycles. These results highlight a material operating via redox mechanism
that may find utility in the storage and capture of other noxious
and corrosive gases
Nature of Decahydro-<i>closo</i>-decaborate Anion Reorientations in an Ordered Alkali-Metal Salt: Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub>
The
ordered monoclinic phase of the alkali-metal decahydro-<i>closo</i>-decaborate salt Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> was found
to be stable from about 250 K all the way up to
an order–disorder phase transition temperature of ≈762
K. The broad temperature range for this phase allowed for a detailed
quasielastic neutron scattering (QENS) and nuclear magnetic resonance
(NMR) study of the protypical B<sub>10</sub>H<sub>10</sub><sup>2–</sup> anion reorientational dynamics. The QENS and NMR combined results
are consistent with an anion reorientational mechanism comprised of
two types of rotational jumps expected from the anion geometry and
lattice structure, namely, more rapid 90° jumps around the anion <i>C</i><sub>4</sub> symmetry axis (e.g., with correlation frequencies
of ≈2.6 × 10<sup>10</sup> s<sup>–1</sup> at 530
K) combined with order of magnitude slower orthogonal 180° reorientational
flips (e.g., ≈3.1 × 10<sup>9</sup> s<sup>–1</sup> at 530 K) resulting in an exchange of the apical H (and apical B)
positions. Each latter flip requires a concomitant 45° twist
around the <i>C</i><sub>4</sub> symmetry axis to preserve
the ordered Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> monoclinic
structural symmetry. This result is consistent with previous NMR data
for ordered monoclinic Na<sub>2</sub>B<sub>10</sub>H<sub>10</sub>,
which also pointed to two types of anion reorientational motions.
The QENS-derived reorientational activation energies are 197(2) and
288(3) meV for the <i>C</i><sub>4</sub> fourfold jumps and
apical exchanges, respectively, between 400 and 680 K. Below this
temperature range, NMR (and QENS) both indicate a shift to significantly
larger reorientational barriers, for example, 485(8) meV for the apical
exchanges. Finally, subambient diffraction measurements identify a
subtle change in the Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> structure
from monoclinic to triclinic symmetry as the temperature is decreased
from around 250 to 210 K
Nature of Decahydro-<i>closo</i>-decaborate Anion Reorientations in an Ordered Alkali-Metal Salt: Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub>
The
ordered monoclinic phase of the alkali-metal decahydro-<i>closo</i>-decaborate salt Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> was found
to be stable from about 250 K all the way up to
an order–disorder phase transition temperature of ≈762
K. The broad temperature range for this phase allowed for a detailed
quasielastic neutron scattering (QENS) and nuclear magnetic resonance
(NMR) study of the protypical B<sub>10</sub>H<sub>10</sub><sup>2–</sup> anion reorientational dynamics. The QENS and NMR combined results
are consistent with an anion reorientational mechanism comprised of
two types of rotational jumps expected from the anion geometry and
lattice structure, namely, more rapid 90° jumps around the anion <i>C</i><sub>4</sub> symmetry axis (e.g., with correlation frequencies
of ≈2.6 × 10<sup>10</sup> s<sup>–1</sup> at 530
K) combined with order of magnitude slower orthogonal 180° reorientational
flips (e.g., ≈3.1 × 10<sup>9</sup> s<sup>–1</sup> at 530 K) resulting in an exchange of the apical H (and apical B)
positions. Each latter flip requires a concomitant 45° twist
around the <i>C</i><sub>4</sub> symmetry axis to preserve
the ordered Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> monoclinic
structural symmetry. This result is consistent with previous NMR data
for ordered monoclinic Na<sub>2</sub>B<sub>10</sub>H<sub>10</sub>,
which also pointed to two types of anion reorientational motions.
The QENS-derived reorientational activation energies are 197(2) and
288(3) meV for the <i>C</i><sub>4</sub> fourfold jumps and
apical exchanges, respectively, between 400 and 680 K. Below this
temperature range, NMR (and QENS) both indicate a shift to significantly
larger reorientational barriers, for example, 485(8) meV for the apical
exchanges. Finally, subambient diffraction measurements identify a
subtle change in the Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> structure
from monoclinic to triclinic symmetry as the temperature is decreased
from around 250 to 210 K
Nature of Decahydro-<i>closo</i>-decaborate Anion Reorientations in an Ordered Alkali-Metal Salt: Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub>
The
ordered monoclinic phase of the alkali-metal decahydro-<i>closo</i>-decaborate salt Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> was found
to be stable from about 250 K all the way up to
an order–disorder phase transition temperature of ≈762
K. The broad temperature range for this phase allowed for a detailed
quasielastic neutron scattering (QENS) and nuclear magnetic resonance
(NMR) study of the protypical B<sub>10</sub>H<sub>10</sub><sup>2–</sup> anion reorientational dynamics. The QENS and NMR combined results
are consistent with an anion reorientational mechanism comprised of
two types of rotational jumps expected from the anion geometry and
lattice structure, namely, more rapid 90° jumps around the anion <i>C</i><sub>4</sub> symmetry axis (e.g., with correlation frequencies
of ≈2.6 × 10<sup>10</sup> s<sup>–1</sup> at 530
K) combined with order of magnitude slower orthogonal 180° reorientational
flips (e.g., ≈3.1 × 10<sup>9</sup> s<sup>–1</sup> at 530 K) resulting in an exchange of the apical H (and apical B)
positions. Each latter flip requires a concomitant 45° twist
around the <i>C</i><sub>4</sub> symmetry axis to preserve
the ordered Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> monoclinic
structural symmetry. This result is consistent with previous NMR data
for ordered monoclinic Na<sub>2</sub>B<sub>10</sub>H<sub>10</sub>,
which also pointed to two types of anion reorientational motions.
The QENS-derived reorientational activation energies are 197(2) and
288(3) meV for the <i>C</i><sub>4</sub> fourfold jumps and
apical exchanges, respectively, between 400 and 680 K. Below this
temperature range, NMR (and QENS) both indicate a shift to significantly
larger reorientational barriers, for example, 485(8) meV for the apical
exchanges. Finally, subambient diffraction measurements identify a
subtle change in the Rb<sub>2</sub>B<sub>10</sub>H<sub>10</sub> structure
from monoclinic to triclinic symmetry as the temperature is decreased
from around 250 to 210 K