ABSTRACT
In less than one minute the catalytic activity and selectivity of a single catalyst was measured in combinatorial libraries of ternary Rh-Pd-Pt-Cu alloys. Only slightly more than two hours were needed to complete a library with 136 elements. The elements of the libraries (ca. 2-4 µg of material) are contained in a two-dimensional array synthesized by a thin-film technique. The analysis was performed by a scanning mass spectrometer (see picture).
ABSTRACT
Six aluminum phenylphosphonates have been synthesized depending upon the synthetic conditions: Al(2)(O(3)PC(6)H(5))(3).2H(2)O (I), Al(2)(O(3)PC(6)H(5))(3) (II), alpha-Al(HO(3)PC(6)H(5))(O(3)PC(6)H(5)).H(2)O (III), beta-Al(HO(3)PC(6)H(5))(O(3)PC(6)H(5)).H(2)O (IV), Al(HO(3)PC(6)H(5))(3).H(2)O (V), and Al(OH)(O(3)PC(6)H(5)) (VI). Thermal analysis, X-ray powder thermodiffractometry, IR spectroscopy, and (27)Al and (31)P MAS NMR data have been obtained to study the structure and thermal stability of these materials. III crystallizes in the orthorhombic system, space group Pbca, with a = 9.7952(1) Å, b = 29.3878(4) Å, c = 9.3537(3) Å, and Z = 8. The structure was solved ab initio, from synchrotron data (lambda approximately 0.4 Å), using direct methods, and refined by Rietveld methods. The final agreement factors were R(wP) = 6.73%, R(P) = 5.24%, and R(F)() = 6.8%. The compound is layered with the aluminum atoms in an octahedral environment of oxygens and two crystallographically independent phosphonate groups, one being protonated. The powder patterns of V and VI have been indexed, and the experimental observations are consistent with layered structures. The unit cell of V contains one octahedral site for Al and three tetrahedral sites for P. Phosphonate I seems to have a three-dimensional tubular structure with aluminum atoms in both octahedral and tetrahedral environments and phosphorus atoms in three different types of sites.
ABSTRACT
A zirconium trisilicate compound, with composition K(2)ZrSi(3)O(9).H(2)O (1), was prepared under mild hydrothermal conditions and was structurally characterized by using its X-ray powder diffraction data. The compound crystallizes in the space group P2(1)2(1)2(1) with a = 10.2977(2) Å, b = 13.3207(3) Å, c = 7.1956(1) Å, and Z = 4. The asymmetric unit consists of a metal atom, a trisilicate group, and three lattice positions corresponding to two cations and a water oxygen atom. In the structure, the Zr atom is octahedrally coordinated by the six terminal oxygens of the trisilicate group. The trisilicate groups exist as linear chain polymers connected to each other through the Zr atoms. This arrangement leads to channels and cavities in the structure that are occupied by the cations and water molecules. The K(+) ions in compound 1 were exchanged for Cs(+) ions in two steps. In the first case about 50% of the K(+) ions were exchanged to give a compound with composition K(0.9)Cs(1.1)ZrSi(3)O(9).H(2)O (2). Compound 2 was then loaded with additional Cs(+) ions which resulted in a phase K(0.5)Cs(1.5)ZrSi(3)O(9).H(2)O (3). These exchanged phases retain the crystal symmetry of compound 1, but their unit cell dimensions have expanded as a result of large Cs(+) ions replacing the smaller K(+) ions. Structure analyses of the exchanged phases show that the cations found in the cavities of compound 1 are highly selective for Cs(+) ions. A small amount of Cs ions also go to a site in the large channel that is very close to that occupied by the water oxygen in compound 1. In the absence of Cs, this site is filled with water molecules. The second cation found in the channel of 1 is partially occupied by water and K(+) ions. The K(+) ions in compound 1 were completely exchanged for Na(+) ions, and the compound thus obtained, Na(2)ZrSi(3)O(9).H(2)O (4), was treated with Cs(+) ions in a manner similar to that carried out for compound 1. The low Cs(+) ion phase, Na(0.98)Cs(1.02)ZrSi(3)O(9).H(2)O (5), and the high Cs(+) ion phase, Na(0.6)Cs(1.4)ZrSi(3)O(9).H(2)O (6), show ion distributions very similar to compounds 2 and 3 except for the fact that in the Na phases a small amount Cs(+) ion also goes to the second cation site. Compound 1 on heating releases the lattice water and transforms into a hexagonal phase, K(2)ZrSi(3)O(9), corresponding to the mineral wadeite. In the high-temperature phase the silicate group exists as a condensed cyclic group and the K(+) ions are sandwiched between trisilicate groups. A possible pathway for this conversion is also discussed.
ABSTRACT
The reaction of 2,5-bis(2-pyridyl)pyrazine (bppz) with nickel(II) sulfate in aqueous solution yielded a binuclear complex, [Ni(2)(bppz)(H(2)O)(8)](SO(4))(2).2H(2)O (1), whose structure was solved by single-crystal methods. The compound crystallizes in the monoclinic space group P2(1)/n with a = 8.372(2) Å, b = 18.301(2) Å, c = 17.197(2) Å, beta = 97.54(2) degrees, and Z = 4. The bppz ligand chelates the two octahedrally coordinated nickel atoms through its nitrogen donors. The four remaining coordination sites are occupied by water oxygen atoms. The binuclear [Ni(2)(bppz)(H(2)O)(8)](4+) cations are held together by hydrogen bonds involving sulfate anions and water molecules. Similar reactions with nickel(II) or copper(II) chloride in less polar solvents resulted in the formation of two new coordination polymers, {[Ni(2)Cl(2)(bppz)(H(2)O)(2)(CH(3)OH)(2)]Cl(2)}(n)() (2) and [Cu(2)Cl(4)(bppz)](n)() (3). These polymers could be obtained only in microcrystalline form. Their structures were determined ab initio from X-ray powder diffraction data. The complex {[Ni(2)Cl(2)(bppz)(H(2)O)(2)(CH(3)OH)(2)]Cl(2)}(n)() (2) belongs to the triclinic space group P&onemacr; with a = 8.7014(4) Å, b = 10.1465(5) Å, c = 8.0303(3) Å, alpha = 116.095(2) degrees, beta = 112.713(3) degrees, gamma = 64.056(3) degrees, and Z = 1. The octahedral coordination of the nickel atom is achieved by two nitrogens of the ligand bppz, two chloride ions, and two oxygens from the solvent molecules. The bridging nature of the chloride ions and the bis-bidentate ligands (bppz) leads to a one-dimensional polymer. The compound [Cu(2)Cl(4)(bppz)](n)() (3) crystallizes in the monoclinic space group C2/m with a = 13.9124(5) Å, b = 6.1844(2) Å, c = 10.1572(3) Å, beta = 112.952(3) degrees, and Z = 2. The copper atoms display a distorted octahedral geometry where four of the coordination sites are occupied by chloride ions and the remaining two by nitrogen atoms of bppz. The metal atoms are bridged by two chlorine atoms and the bppz ligands, forming a two-dimensional coordination polymer.
ABSTRACT
Reaction of copper salts with 1,4-phenylenebis(phosphonic acid) yielded a conventional layered compound, Cu(2)[(O(3)PC(6)H(4)PO(3))(H(2)O)(2)], while a similar reaction with 4,4'-biphenylenebis(phosphonic acid) resulted in a new lamellar structure with composition Cu[HO(3)P(C(6)H(4))(2)PO(3)H]. The structures of these compounds were solved ab initio by using X-ray powder diffraction data. The crystals of the phenylenebis(phosphonate) compound are monoclinic, space group C2/c, with a = 18.8892(4) Å, b = 7.6222(2) Å, c = 7.4641(2) Å, beta = 90.402(2) degrees, and Z = 4. The layer structure in this case is similar to that in copper phenylphosphonate, Cu[O(3)PC(6)H(5)]. The metal atoms display a distorted square pyramidal geometry where four of the coordination sites are occupied by the phosphonate oxygens. The remaining site is filled by an oxygen atom of the water molecule. Adjacent metal-O(3)PC layers are covalently pillared by the phenyl group of the phosphonates to create a 3-dimensional structure. Cu[HO(3)P(C(6)H(4))(2)PO(3)H] is triclinic, space group P&onemacr;, with a = 4.856(2) Å, b = 14.225(5) Å, c = 4.788(2) Å, alpha = 97.85(1) degrees, beta = 110.14(1) degrees, gamma = 89.38(1) degrees, and Z = 1. The structure in this case, ideally consists of linear chains of copper atoms. The copper atoms are bridged by centrosymmetrically related phosphonate groups utilizing two of their oxygen atoms. This binding mode leads to square planar geometry for the copper atoms. The third oxygen atom of the phosphonate is protonated and is involved in linking adjacent linear chains through hydrogen bonds. At the same time, these hydroxyl oxygens interact weakly (Cu-O = 3.14 Å) with the copper atoms of the adjacent chain. Considering these long Cu-O interactions, the geometry of the copper atom may be described as distorted square bipyramidal. As in the phenylphosphonate structure, the biphenyl groups covalently link the Cu-O(3)PC networks in the perpendicular direction.
ABSTRACT
The novel dimeric compounds [Ph(2)Sb(O(2)PR(2))O](2).2CH(2)Cl(2) [R = cycl-C(6)H(11) (2) and cycl-C(8)H(15) (3)] have been synthesized by reacting diphenylantimony trichloride (1) with 3 mol equiv of silver acetate followed by 1 mol equiv of the phosphinic acid. By the same route under more stringent conditions to exclude moisture, the mixed phosphinate-acetate [Ph(2)Sb(O(2)P(C(6)H(11))(2))(O(2)CMe)](2)O (4) was isolated and characterized. Treatment of 2 with acetic acid/water affords the tetranuclear cage Ph(8)Sb(4)O(4)(OH)(2)(O(2)P(C(6)H(11))(2))(2).CH(3)COOH.CH(2)Cl(2) (5); it is possible to convert 5 to 2 by heating it with an excess of the phosphinic acid. Compounds 2, 3, and 5 have been characterized by X-ray structural analysis. All of them possess four membered Sb(2)O(2) rings with hexacoordinated antimony. In 5 the antimony atoms in the two Sb(2)O(2) rings are connected by oxo bridges on two sides to give an Sb(4)O(6) cage. These structures are correlated with those of known tin cages.
ABSTRACT
The three-dimensional structure of a complex tubular uranyl phosphonate, (UO(2))(3)(HO(3)PC(6)H(5))(2)(O(3)PC(6)H(5))(2).H(2)O, was determined ab initio from laboratory X-ray powder diffraction data and refined by the Rietveld method. The crystals belong to the space group P2(1)2(1)2(1), with a = 17.1966(2) Å, b = 7.2125(2) Å, c = 27.8282(4) Å, and Z = 4. The structure consists of three independent uranium atoms, among which two are seven-coordinated and the third is eight-coordinated. These metal atoms are connected by four different phosphonate groups to form a one-dimensional channel structure along the b axis. The phenyl groups are arranged on the outer periphery of the channels, and their stacking forces keep the channels intact in the lattice. The determination of this structure which contains 50 non-hydrogen atoms in the asymmetric unit, from conventional X-ray powder data, represents significant progress in the application of powder techniques to structure solution of complex inorganic compounds, including organometallic compounds.
