10 research outputs found

    Exceptional Structural Compliance of the B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup> Superweak Anion

    No full text
    The single-crystal X-ray structures, thermogravimetric analyses, and/or FTIR spectra of a series of salts of the B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup> anion and homoleptic AgĀ­(L)<sub><i>n</i></sub><sup>+</sup> cations are reported (L = CH<sub>2</sub>Cl<sub>2</sub>, <i>n</i> = 2; L = PhCH<sub>3</sub>, <i>n</i> = 3; L = CH<sub>3</sub>CN; <i>n</i> = 2ā€“4; L = CO, <i>n</i> = 1, 2). The superweak-anion nature of B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup> (Y<sup>2ā€“</sup>) was demonstrated by the rapid reaction of microcrystalline Ag<sub>2</sub>(Y) with 1 atm of CO to form a nonclassical silverĀ­(I) carbonyl compound with an FTIR Ī½Ā­(CO) band at 2198 cm<sup>ā€“1</sup> (and with the proposed formula [AgĀ­(CO)<sub><i>n</i></sub>]<sub>2</sub>[Y]). In contrast, microcrystalline Ag<sub>2</sub>(B<sub>12</sub>Cl<sub>12</sub>) did not exhibit Ī½Ā­(CO) bands and therefore did not form AgĀ­(CO)<sup>+</sup> species, even after 32 h under 24 atm of CO. When Ag<sub>2</sub>(Y) was treated with carbon monoxide pressures higher than 1 atm, a new Ī½Ā­(CO) band at 2190 cm<sup>ā€“1</sup> appeared, which is characteristic of a AgĀ­(CO)<sub>2</sub><sup>+</sup> dicarbonyl cation. Both Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>8</sub>(Y) and Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>5</sub>(Y) rapidly lost coordinated CH<sub>3</sub>CN at 25 Ā°C to form Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>4</sub>(Y), which formed solvent-free Ag<sub>2</sub>(Y) only after heating above 100 Ā°C. Similarly, Ag<sub>2</sub>(PhCH<sub>3</sub>)<sub>6</sub>(Y) rapidly lost coordinated PhCH<sub>3</sub> at 25 Ā°C to form Ag<sub>2</sub>(PhCH<sub>3</sub>)<sub>2</sub>(Y), which formed Ag<sub>2</sub>(Y) after heating above 150 Ā°C, and Ag<sub>2</sub>(CH<sub>2</sub>Cl<sub>2</sub>)<sub>4</sub>(Y) rapidly lost three of the four coordinated CH<sub>2</sub>Cl<sub>2</sub> ligands between 25 and 100 Ā°C and formed Ag<sub>2</sub>(Y) when it was heated above 200 Ā°C. Solvent-free Ag<sub>2</sub>(Y) was stable until it was heated above 380 Ā°C. The rapid evaporative loss of coordinated ligands at 25 Ā°C from nonporous crystalline solids requires equally rapid structural reorganization of the lattice and is one of three manifestations of the structural compliance of the Y<sup>2ā€“</sup> anion reported in this work. The second, more quantitative, manifestation is that Ag<sup>+</sup> bond-valence sums for Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub><i>n</i></sub>(Y) are virtually constant, 1.20 Ā± 0.03, for <i>n</i> = 8, 5, 4, because the Y<sup>2ā€“</sup> anion precisely compensated for the lost CH<sub>3</sub>CN ligands by readily forming the necessary number of weak Agā€“FĀ­(B) bonds. The third, and most exceptional, manifestation is that the idealized structural reorganization accompanying the conceptual transformations Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>8</sub>(Y) ā†’ Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>5</sub>(Y) ā†’ Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>4</sub>(Y) involve close-packed layers of Y<sup>2ā€“</sup> anions that sandwich the AgĀ­(CH<sub>3</sub>CN)<sub>4</sub><sup>+</sup> complexes splitting into staggered flat ribbons of interconnected (Y<sup>2ā€“</sup>)<sub>3</sub> triangles that surround the Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>5</sub><sup>2+</sup> complexes on four sides, conceptually re-forming close-packed layers of anions that sandwich the AgĀ­(CH<sub>3</sub>CN)<sub>2</sub><sup>+</sup> complexes. The interconnected (Y<sup>2ā€“</sup>)<sub>3</sub> triangle lattice of anions in Ag<sub>2</sub>(CH<sub>3</sub>CN)<sub>5</sub>(Y) may be the first example of this structure type

    Formation of a Cationic Vinylimido Group upon Cā€“H Activation of Nitriles by Trialkylamines in the Presence of TaCl<sub>5</sub>

    No full text
    We report a new CH<sub>3</sub>CN activation mode where an imido group is directly formed by deprotonation of the nitrile coordinated to the highly Lewis acidic Ta<sup>V</sup> center. The unexpected deprotonation of TaCl<sub>5</sub>(CH<sub>3</sub>CN) by NEt<sub>3</sub> resulted in isolation of the triethylammonium vinylimido complex [HNEt<sub>3</sub>]Ā­[TaĀ­(NCĀ­(CH<sub>2</sub>)Ā­NEt<sub>3</sub>)Ā­Cl<sub>5</sub>]. The reaction is proposed to proceed through rearrangement of the initial nucleophilic carbanion to the electrophilic azaallene/carbocation intermediate. The use of more sterically hindered (<i>i</i>-Pr)Ā­CN and weakly nucleophilic NĀ­(<i>i</i>-Pr)<sub>2</sub>Et resulted in the isolation of a vinylimido group formed upon dimerization of deprotonated nitriles, suggesting deprotonation as the first step of the transformation

    Metal- and Ligand-Centered Reactivity of <i>meta</i>-Carboranyl-Backbone Pincer Complexes of Rhodium

    No full text
    We report the synthesis of the chelating phosphinite-arm carboranyl POBOP-H (POBOP = 1,7-OPĀ­(<i>i</i>-Pr)<sub>2</sub>-<i>m</i>-carboranyl) ligand precursor, preparation of its rhodium complexes, and their reactivity in oxidative addition/reductive elimination reactions. The oxidative addition of iodobenzene to the low-valent (POBOP)Ā­RhĀ­(PPh<sub>3</sub>) resulted in the selective formation of the 16-electron complex (POBOP)Ā­RhĀ­(Ph)Ā­(I), featuring a highly strained exohedral rhodiumā€“boron bond. The complex (POBOP)Ā­RhĀ­(Ph)Ā­(I) is the first example of a B-carboranyl aryl metal complex, which is a proposed intermediate in metal-promoted Bā€“C coupling reactions. The complex (POBOP)Ā­RhĀ­(Ph)Ā­(I) was selectively and directly converted, in the presence of acetonitrile, to (POBĀ­(BPh)Ā­OP)Ā­RhĀ­(H)Ā­(I)Ā­(CH<sub>3</sub>CN) (POBĀ­(BPh)Ā­OP = 1,7-OPĀ­(<i>i</i>-Pr)<sub>2</sub>-2-Ph-<i>m</i>-carboranyl) through unprecedented cascade reductive elimination of the phenyl-<i>B</i>-carboranyl and the oxidative addition of a vicinal Bā€“H bond of the boron cluster to the metal center, exhibiting both metal- and cluster-centered reactivity

    Opening of Carborane Cages by Metal Cluster Complexes: The Reaction of a Thiolate-Substituted Carborane with Triosmium Carbonyl Cluster Complexes

    No full text
    The reaction of Os<sub>3</sub>(CO)<sub>10</sub>(NCMe)<sub>2</sub> with closo-<i>o</i>-(1-SCH<sub>3</sub>)Ā­C<sub>2</sub>B<sub>10</sub>H<sub>11</sub> has yielded the complex Os<sub>3</sub>(CO)<sub>9</sub>[Ī¼<sub>3</sub>-Ī·<sup>3</sup>-C<sub>2</sub>B<sub>10</sub>H<sub>9</sub>(SCH<sub>3</sub>)]Ā­(Ī¼-H)<sub>2</sub>, <b>1</b>, by the loss of the two NCMe ligands and one CO ligand from the Os<sub>3</sub> cluster and the coordination of the sulfur atom and the activation of two Bā€“H bonds with transfer of the hydrogen atoms to the cluster. Reaction of <b>1</b> with a second equivalent of Os<sub>3</sub>(CO)<sub>10</sub>(NCMe)<sub>2</sub> yielded the complex Os<sub>3</sub>(CO)<sub>9</sub>(Ī¼-H)Ā­[(Ī¼<sub>3</sub>-Ī·<sup>3</sup>-1,4,5-Ī¼<sub>3</sub>-Ī·<sup>3</sup>-6,10,11-C<sub>2</sub>B<sub>10</sub>H<sub>8</sub>SĀ­(CH<sub>3</sub>)]Ā­Os<sub>3</sub>(CO)<sub>9</sub>(Ī¼-H)<sub>2</sub>, <b>2</b>, that contains two triosmium triangles attached to the same carborane cage. The carborane cage was opened by cleavage of two Bā€“C bonds and one Bā€“B bond. The Bā€“H group that was pulled out of the cage became a triply bridging group on one of the Os<sub>3</sub> triangles but remains bonded to the cage by two Bā€“B bonds. When heated to 150 Ā°C, <b>2</b> was transformed into the complex Os<sub>3</sub>(CO)<sub>9</sub>(Ī¼-H)Ā­[(Ī¼<sub>3</sub>-Ī·<sup>3</sup>-Ī¼<sub>3</sub>-Ī·<sup>3</sup>-C<sub>2</sub>B<sub>10</sub>H<sub>7</sub>SĀ­(CH<sub>3</sub>)]Ā­Os<sub>3</sub>(CO)<sub>9</sub>(Ī¼-H), <b>3</b>, by the loss of two hydrogen atoms and a rearrangement that led to further opening of the carborane cage. Reaction of <b>1</b> with a second equivalent of closo-<i>o</i>-(1-SCH<sub>3</sub>)Ā­C<sub>2</sub>B<sub>10</sub>H<sub>11</sub> has yielded the complex Os<sub>3</sub>(CO)<sub>6</sub>)Ā­(Ī¼<sub>3</sub>-Ī·<sup>3</sup>-C<sub>2</sub>B<sub>10</sub>H<sub>9</sub>-<i>R</i>-SCH<sub>3</sub>) (Ī¼<sub>3</sub>-Ī·<sup>3</sup>-C<sub>2</sub>B<sub>10</sub>H<sub>10</sub>-<i>S</i>-SCH<sub>3</sub>)Ā­(Ī¼-H)<sub>3</sub>, <b>4a</b>, containing two carborane cages coordinated to one Os<sub>3</sub> cluster. Compound <b>4a</b> was isomerized to the compound Os<sub>3</sub>(CO)<sub>6</sub>(Ī¼<sub>3</sub>-Ī·<sup>3</sup>-C<sub>2</sub>B<sub>10</sub>H<sub>9</sub>-<i>R</i>-SCH<sub>3</sub>)Ā­(Ī¼<sub>3</sub>-Ī·<sup>3</sup>-C<sub>2</sub>B<sub>10</sub>H<sub>10</sub>-<i>R</i>-SCH<sub>3</sub>)Ā­(Ī¼-H)<sub>3</sub>, <b>4b</b>, by an inversion of stereochemistry at one of the sulfur atoms by heating to 174 Ā°C

    (BB)-Carboryne Complex of Ruthenium: Synthesis by Double Bā€“H Activation at a Single Metal Center

    Get PDF
    The first example of a transition metal (BB)-carboryne complex containing two boron atoms of the icosahedral cage connected to a single exohedral metal center (POBBOP)Ā­RuĀ­(CO)<sub>2</sub> (POBBOP = 1,7-OPĀ­(<i>i</i>-Pr)<sub>2</sub>-2,6-dehydro-<i>m</i>-carborane) was synthesized by double Bā€“H activation within the strained <i>m</i>-carboranyl pincer framework. Theoretical calculations revealed that the unique three-membered (BB)>Ru metalacycle is formed by two bent Bā€“Ru Ļƒ-bonds with the concomitant increase of the bond order between the two metalated boron atoms. The reactivity of the highly strained electron-rich (BB)-carboryne fragment with small molecules was probed by reactions with electrophiles. The carboryneā€“carboranyl transformations reported herein represent a new mode of cooperative metalā€“ligand reactivity of boron-based complexes

    (BB)-Carboryne Complex of Ruthenium: Synthesis by Double Bā€“H Activation at a Single Metal Center

    No full text
    The first example of a transition metal (BB)-carboryne complex containing two boron atoms of the icosahedral cage connected to a single exohedral metal center (POBBOP)Ā­RuĀ­(CO)<sub>2</sub> (POBBOP = 1,7-OPĀ­(<i>i</i>-Pr)<sub>2</sub>-2,6-dehydro-<i>m</i>-carborane) was synthesized by double Bā€“H activation within the strained <i>m</i>-carboranyl pincer framework. Theoretical calculations revealed that the unique three-membered (BB)>Ru metalacycle is formed by two bent Bā€“Ru Ļƒ-bonds with the concomitant increase of the bond order between the two metalated boron atoms. The reactivity of the highly strained electron-rich (BB)-carboryne fragment with small molecules was probed by reactions with electrophiles. The carboryneā€“carboranyl transformations reported herein represent a new mode of cooperative metalā€“ligand reactivity of boron-based complexes

    Structures of M<sub>2</sub>(SO<sub>2</sub>)<sub>6</sub>B<sub>12</sub>F<sub>12</sub> (M = Ag or K) and Ag<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>B<sub>12</sub>F<sub>12</sub>: Comparison of the Coordination of SO<sub>2</sub> versus H<sub>2</sub>O and of B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup> versus Other Weakly Coordinating Anions to Metal Ions in the Solid State

    No full text
    The structures of three solvated monovalent cation salts of the superweak anion B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup> (Y<sup>2ā€“</sup>), K<sub>2</sub>(SO<sub>2</sub>)<sub>6</sub>Y, Ag<sub>2</sub>Ā­(SO<sub>2</sub>)<sub>6</sub>Y, and Ag<sub>2</sub>Ā­(H<sub>2</sub>O)<sub>4</sub>Y, are reported and discussed with respect to previously reported structures of Ag<sup>+</sup> and K<sup>+</sup> with other weakly coordinating anions. The structures of K<sub>2</sub>(SO<sub>2</sub>)<sub>6</sub>Y and Ag<sub>2</sub>Ā­(SO<sub>2</sub>)<sub>6</sub>Y are isomorphous and are based on expanded cubic close-packed arrays of Y<sup>2ā€“</sup> anions with MĀ­(OSO)<sub>6</sub><sup>+</sup> complexes centered in the trigonal holes of one expanded close-packed layer of B<sub>12</sub> centroids (āŠ™). The K<sup>+</sup> and Ag<sup>+</sup> ions have virtually identical bicapped trigonal prism MO<sub>6</sub>F<sub>2</sub> coordination spheres, with Mā€“O distances of 2.735(1)ā€“3.032(2) ƅ for the potassium salt and 2.526(5)ā€“2.790(5) ƅ for the silver salt. Each MĀ­(OSO)<sub>6</sub><sup>+</sup> complex is connected to three other cationic complexes through their six Ī¼-SO<sub>2</sub>-Īŗ<sup>1</sup><i>O</i>,Īŗ<sup>2</sup><i>O</i>ā€² ligands. The structure of Ag<sub>2</sub>Ā­(H<sub>2</sub>O)<sub>4</sub>Y is unique [different from that of K<sub>2</sub>Ā­(H<sub>2</sub>O)<sub>4</sub>Y]. Planes of close-packed arrays of anions are offset from neighboring planes along only one of the linear āŠ™Ā·Ā·Ā·āŠ™Ā·Ā·Ā·āŠ™ directions of the close-packed arrays, with [AgĀ­(Ī¼-H<sub>2</sub>O)<sub>2</sub>Ā­AgĀ­(Ī¼-H<sub>2</sub>O)<sub>2</sub>)]<sub>āˆž</sub> infinite chains between the planes of anions. There are two nearly identical AgO<sub>4</sub>F<sub>2</sub> coordination spheres, with Agā€“O distances of 2.371(5)ā€“2.524(5) ƅ and Agā€“F distances of 2.734(4)ā€“2.751(4) ƅ. This is only the second structurally characterized compound with four H<sub>2</sub>O molecules coordinated to a Ag<sup>+</sup> ion in the solid state. Comparisons with crystalline H<sub>2</sub>O and SO<sub>2</sub> solvates of other Ag<sup>+</sup> and K<sup>+</sup> salts of weakly coordinating anions show that (i) NĀ­[(SO<sub>2</sub>)<sub>2</sub>Ā­(1,2-C<sub>6</sub>H<sub>4</sub>)]<sup>āˆ’</sup>, BF<sub>4</sub><sup>ā€“</sup>, SbF<sub>6</sub><sup>ā€“</sup>, and AlĀ­(OCĀ­(CF<sub>3</sub>)<sub>3</sub>)<sub>4</sub><sup>ā€“</sup> coordinate much more strongly to Ag<sup>+</sup> than does Y<sup>2ā€“</sup>, (ii) SnF<sub>6</sub><sup>2ā€“</sup> coordinates somewhat more strongly to K<sup>+</sup> than does Y<sup>2ā€“</sup>, and (iii) B<sub>12</sub>Cl<sub>12</sub><sup>2ā€“</sup> coordinates to K<sup>+</sup> about the same as, if not slightly weaker than, Y<sup>2ā€“</sup>

    Activation of Cā€“H Bonds of Alkyl- and Arylnitriles by the TaCl<sub>5</sub>ā€“PPh<sub>3</sub> Lewis Pair

    No full text
    A new pathway of activation of Cā€“H bonds of alkyl- and arylnitriles by a cooperative action of TaCl<sub>5</sub> and PPh<sub>3</sub> under mild conditions is reported. Coordination of nitriles to the highly Lewis acidic TaĀ­(V) center resulted in an activation of their aliphatic and aromatic Cā€“H bonds, allowing nucleophilic attack and deprotonation by the relatively weak base PPh<sub>3</sub>. The propensity of TaĀ­(V) to form multiple bonds to nitrogen-containing ligands is an important driving force of the reaction as it led to a sequence of bond rearrangements and the emergence of, in the case of benzonitrile, a zwitterionic enediimido complex of TaĀ­(V) through Cī—»C double bond formation between two activated nitrile fragments. These transformations highlight the special role of the high-valent transition metal halide in substrate activation and distinguish the reactivity of the TaCl<sub>5</sub>ā€“PPh<sub>3</sub> system from both non-metal- and late transition metal-based frustrated Lewis pairs

    Comparison of the Coordination of B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup>, B<sub>12</sub>Cl<sub>12</sub><sup>2ā€“</sup>, and B<sub>12</sub>H<sub>12</sub><sup>2ā€“</sup> to Na<sup>+</sup> in the Solid State: Crystal Structures and Thermal Behavior of Na<sub>2</sub>(B<sub>12</sub>F<sub>12</sub>), Na<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>(B<sub>12</sub>F<sub>12</sub>), Na<sub>2</sub>(B<sub>12</sub>Cl<sub>12</sub>), and Na<sub>2</sub>(H<sub>2</sub>O)<sub>6</sub>(B<sub>12</sub>Cl<sub>12</sub>)

    No full text
    The synthesis of high-purity Na<sub>2</sub>B<sub>12</sub>F<sub>12</sub> and the crystal structures of Na<sub>2</sub>(B<sub>12</sub>F<sub>12</sub>) (5 K neutron powder diffraction (NPD)), Na<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>(B<sub>12</sub>F<sub>12</sub>) (120 K single-crystal X-ray diffraction (SC-XRD)), Na<sub>2</sub>(B<sub>12</sub>Cl<sub>12</sub>) (5 and 295 K NPD), and Na<sub>2</sub>(H<sub>2</sub>O)<sub>6</sub>Ā­(B<sub>12</sub>Cl<sub>12</sub>) (100 K SC-XRD) are reported. The compound Na<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>(B<sub>12</sub>F<sub>12</sub>) contains {[(NaĀ­(Ī¼-H<sub>2</sub>O)<sub>2</sub>NaĀ­(Ī¼-H<sub>2</sub>O)<sub>2</sub>)]<sup>2+</sup>}<sub>āˆž</sub> infinite chains; the compound Na<sub>2</sub>(H<sub>2</sub>O)<sub>6</sub>Ā­(B<sub>12</sub>Cl<sub>12</sub>) contains discrete [(H<sub>2</sub>O)<sub>2</sub>NaĀ­(Ī¼-H<sub>2</sub>O)<sub>2</sub>NaĀ­(H<sub>2</sub>O)<sub>2</sub>]<sup>2+</sup> cations with OHĀ·Ā·Ā·O hydrogen bonds linking the terminal H<sub>2</sub>O ligands. The structures of the two hydrates and the previously published structure of Na<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>(B<sub>12</sub>H<sub>12</sub>) are analyzed with respect to the relative coordinating ability of B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup>, B<sub>12</sub>H<sub>12</sub><sup>2ā€“</sup>, and B<sub>12</sub>Cl<sub>12</sub><sup>2ā€“</sup> toward Na<sup>+</sup> ions in the solid state (i.e., the relative ability of these anions to satisfy the valence of Na<sup>+</sup>). All three hydrated structures have distorted octahedral NaX<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub> coordination spheres (X = F, H, Cl). The sums of the four Naā€“O bond valence contributions are 71, 75, and 89% of the total bond valences for the X = F, H, and Cl hydrated compounds, respectively, demonstrating that the relative coordinating ability by this criterion is B<sub>12</sub>Cl<sub>12</sub><sup>2ā€“</sup> ā‰Ŗ B<sub>12</sub>H<sub>12</sub><sup>2ā€“</sup> < B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup>. Differential scanning calorimetry experiments demonstrate that Na<sub>2</sub>(B<sub>12</sub>F<sub>12</sub>) undergoes a reversible, presumably orderā€“disorder, phase transition at ca. 560 K (287 Ā°C), between the 529 and 730 K transition temperatures previously reported for Na<sub>2</sub>(B<sub>12</sub>H<sub>12</sub>) and Na<sub>2</sub>(B<sub>12</sub>Cl<sub>12</sub>), respectively. Thermogravimetric analysis demonstrates that Na<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>Ā­(B<sub>12</sub>F<sub>12</sub>) and Na<sub>2</sub>(H<sub>2</sub>O)<sub>6</sub>Ā­(B<sub>12</sub>Cl<sub>12</sub>) undergo partial dehydration at 25 Ā°C to Na<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Ā­(B<sub>12</sub>F<sub>12</sub>) and Na<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Ā­(B<sub>12</sub>Cl<sub>12</sub>) in ca. 30 min and 2 h, respectively, and essentially complete dehydration to Na<sub>2</sub>(B<sub>12</sub>F<sub>12</sub>) and Na<sub>2</sub>(B<sub>12</sub>Cl<sub>12</sub>) within minutes at 150 and 75 Ā°C, respectively (the remaining trace amounts of H<sub>2</sub>O, if any, were not quantified). The changes in structure upon dehydration and the different vapor pressures of H<sub>2</sub>O needed to fully hydrate the respective Na<sub>2</sub>(B<sub>12</sub>X<sub>12</sub>) compounds provide additional evidence that B<sub>12</sub>Cl<sub>12</sub><sup>2ā€“</sup> is more weakly coordinating than B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup> to Na<sup>+</sup> in the solid state. Taken together, the results suggest that the anhydrous, halogenated <i>closo</i>-borane compounds Na<sub>2</sub>(B<sub>12</sub>F<sub>12</sub>) and Na<sub>2</sub>(B<sub>12</sub>Cl<sub>12</sub>), in appropriately modified forms, may be viable component materials for fast-ion-conducting solid electrolytes in future energy-storage devices

    Latent Porosity in Alkali-Metal M<sub>2</sub>B<sub>12</sub>F<sub>12</sub> Salts: Structures and Rapid Room-Temperature Hydration/Dehydration Cycles

    No full text
    Structures of the alkali-metal hydrates Li<sub>2</sub>(H<sub>2</sub>O)<sub>4</sub>Z, LiKĀ­(H<sub>2</sub>O)<sub>4</sub>Z, Na<sub>2</sub>(H<sub>2</sub>O)<sub>3</sub>Z, and Rb<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z, unit cell parameters for Rb<sub>2</sub>Z and Rb<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z, and the density functional theory (DFT)-optimized structures of K<sub>2</sub>Z, K<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z, Rb<sub>2</sub>Z, Rb<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z, Cs<sub>2</sub>Z, and Cs<sub>2</sub>(H<sub>2</sub>O)Ā­Z are reported (Z<sup>2ā€“</sup> = B<sub>12</sub>F<sub>12</sub><sup>2ā€“</sup>) and compared with previously reported X-ray structures of Na<sub>2</sub>(H<sub>2</sub>O)<sub>0,4</sub>Z, K<sub>2</sub>(H<sub>2</sub>O)<sub>0,2,4</sub>Z, and Cs<sub>2</sub>(H<sub>2</sub>O)Ā­Z. Unusually rapid room-temperature hydration/dehydration cycles of several M<sub>2</sub>Z/M<sub>2</sub>(H<sub>2</sub>O)<sub><i>n</i></sub>Z salt hydrate pairs, which were studied by isothermal gravimetry, are also reported. Finely ground samples of K<sub>2</sub>Z, Rb<sub>2</sub>Z, and Cs<sub>2</sub>Z, which are not microporous, exhibited latent porosity by undergoing hydration at 24ā€“25 Ā°C in the presence of 18 Torr of H<sub>2</sub>OĀ­(g) to K<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z, Rb<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z, and Cs<sub>2</sub>(H<sub>2</sub>O)Ā­Z in 18, 40, and 16 min, respectively. These hydrates were dehydrated at 24ā€“25 Ā°C in dry N<sub>2</sub> to the original anhydrous M<sub>2</sub>Z compounds in 61, 25, and 76 min, respectively (the exact times varied from sample to sample depending on the particle size). The hydrate Na<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z also exhibited latent porosity by undergoing multiple 90 min cycles of hydration to Na<sub>2</sub>(H<sub>2</sub>O)<sub>3</sub>Z and dehydration back to Na<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z at 23 Ā°C. For the K<sub>2</sub>Z, Rb<sub>2</sub>Z, and Cs<sub>2</sub>Z transformations, the maximum rate of hydration (rh<sub>max</sub>) decreased, and the absolute value of the maximum rate of dehydration (rd<sub>max</sub>) increased, as <i>T</i> increased. For K<sub>2</sub>Z ā†” K<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z hydration/dehydration cycles with the same sample, the ratio rh<sub>max</sub>/rd<sub>max</sub> decreased 26 times over 8.6 Ā°C, from 3.7 at 23.4 Ā°C to 0.14 at 32.0 Ā°C. For Rb<sub>2</sub>Z ā†” Rb<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z cycles, rh<sub>max</sub>/rd<sub>max</sub> decreased from 0.88 at 23 Ā°C to 0.23 at 27 Ā°C. For Cs<sub>2</sub>Z ā†” Cs<sub>2</sub>(H<sub>2</sub>O)Ā­Z cycles, rh<sub>max</sub>/rd<sub>max</sub> decreased 20 times over 8 Ā°C, from 6.7 at 24 Ā°C to 0.34 at 32 Ā°C. In addition, the reversible substitution of D<sub>2</sub>O for H<sub>2</sub>O in fully hydrated Rb<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>Z in the presence of N<sub>2</sub>/16 Torr of D<sub>2</sub>OĀ­(g) was complete in only 60 min at 23 Ā°C
    corecore