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)

    No full text
    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)

    No full text
    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

    No full text
    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>

    No full text
    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>

    No full text
    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>

    No full text
    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
    corecore