10 research outputs found
Exceptional Structural Compliance of the B<sub>12</sub>F<sub>12</sub><sup>2ā</sup> Superweak Anion
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> = 2ā4; 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>ā1</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>ā1</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 AgāFĀ(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 CāH Activation of Nitriles by Trialkylamines in the Presence of TaCl<sub>5</sub>
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
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 rhodiumāboron 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 BāC 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 BāH 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
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 BāH 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 BāC
bonds and one BāB bond. The BāH 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 BāB
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 BāH Activation at a Single Metal Center
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 BāH 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 BāRu Ļ-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 carboryneācarboranyl transformations reported herein represent
a new mode of cooperative metalāligand reactivity of boron-based
complexes
(BB)-Carboryne Complex of Ruthenium: Synthesis by Double BāH Activation at a Single Metal Center
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 BāH 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 BāRu Ļ-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 carboryneācarboranyl transformations reported herein represent
a new mode of cooperative metalāligand 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
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 (ā). 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 MāO distances of 2.735(1)ā3.032(2)
Ć
for the potassium salt and 2.526(5)ā2.790(5) Ć
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>ā² 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 āĀ·Ā·Ā·āĀ·Ā·Ā·ā
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>ā</sub> infinite chains between the planes of anions. There
are two nearly identical AgO<sub>4</sub>F<sub>2</sub> coordination
spheres, with AgāO distances of 2.371(5)ā2.524(5) Ć
and AgāF distances of 2.734(4)ā2.751(4) Ć
. 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>ā</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 CāH Bonds of Alkyl- and Arylnitriles by the TaCl<sub>5</sub>āPPh<sub>3</sub> Lewis Pair
A new pathway of
activation of CāH 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 CāH
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>āPPh<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>)
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>ā</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 NaāO 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> āŖ 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 orderādisorder,
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
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 24ā25 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 24ā25 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