Crystal structure of Diaqua(1,10-phenanthroline)copper(II) sulfate

1984 ◽  
Vol 37 (5) ◽  
pp. 1111 ◽  
Author(s):  
PC Healy ◽  
JM Patrick ◽  
AH White

The crystal structure of the title compound, [Cu(OH2)2(phen)] (SO4) (phen = 1,10-phenanthroline), has been determined by single-crystal X-ray diffraction methods at room temperature, being refined by full matrix least-squares methods to a residual of 0.033 for 1445 'observed' reflections. Crystals are monoclinic, C2/c, a 14.883(8), b 13.843(9), c 7.019(4) �, β 108.60(4)�, Z 4. As in a number of other copper(II) and nickel(II) derivatives with (CuL4)(SO4) stoichiometry, the pseudo-square planar copper environments [Cu-N,O: 2.009(2), 1.970(2) � in the present case] are bridged through the two axial coordination positions by sulfate groups: O.SO2.O[Cu(OH2)2(phen)]O.SO2.0, etc. to give a linear polymeric array [Cu-O(SO4), 2.468(3) �]; a crystallographic twofold axis passes through the copper atom.

1994 ◽  
Vol 47 (2) ◽  
pp. 391 ◽  
Author(s):  
CJ Kepert ◽  
BW Skeleton ◽  
AH White

The room-temperature single-crystal X-ray structural characterization of the title compound (tpyH2)2[Tb(OH2)8]Cl7.~2⅓H2O is recorded. Crystals are triclinic, Pī , a 17.063(5), b 16.243(3), c 7.878(3) Ǻ, α 84.78(2), β 84.39(3), γ 87.81(2)°, Z = 2 formula units; 3167 'observed' diffractometer reflections were refined by full-matrix least-squares procedures to a residual of 0.057. Notable features of interest of the compound are the 'chelation' of chloride ions by the terpyridinium cations , and the existence of a free [Tb(OH2)8]2+ cation in the presence of an abundance of chloride ions.


1978 ◽  
Vol 31 (9) ◽  
pp. 1927 ◽  
Author(s):  
DL Kepert ◽  
CL Raston ◽  
NK Roberts ◽  
AH White

The crystal structure of the title compound, [Tl(S2CNEt2)3], has been determined by single-crystal X-ray diffraction methods at 295 K and refined by full-matrix least squares to a residual of 0.050 for 2517 'observed' reflections. Crystals are monoclinic, with space group A2/a, a 14.789(7), b 10.428(4), c 18.207(9) Ǻ, β 118.11(4)°, Z 4, and are isostructural with those of the previously determined gallium and indium analogues, the molecule having 2 symmetry with <Tl-S> 2.666 Ǻ. As in the dimethyl/thallium analogue, the departure of the TlS6 core symmetry from 3 is large and is examined in terms of electron-pair repulsion theory.


1983 ◽  
Vol 36 (8) ◽  
pp. 1527 ◽  
Author(s):  
BN Figgis ◽  
ES Kucharski ◽  
AH White

The crystal structure of the title compound, [CO(C15H11N3)2] 12.2H2O, has been determined by single crystal X-ray diffraction methods at 295 K and at 120 K, being refined by least squares to residuals of 0.051 and 0.035 respectively for 982 and 1024 'observed' reflections at these temperatures. Both structures are based on a P42/n tetragonal cell, a c. 8.9, c c. 19.4 �, Z 2, in which only a quarter of the cation is independent, being located about a site of 4 symmetry. At room temperature (μoff c. 3.2 BM) Co-N (central, distal) are 1.942(7), 2.104(5) � diminishing to 1.912(5), 2.083(4) � at 120 K, with μoff c. 2.2 BM, corresponding to a fully populated low-spin ground state.


1978 ◽  
Vol 31 (12) ◽  
pp. 2717 ◽  
Author(s):  
BN Figgis ◽  
CL Raston ◽  
RP Sharma ◽  
AH White

The crystal structure of the title compound, (NH4)2 [FeCl5(H2O)], has been redetermined by single-crystal X-ray diffraction at 295 K and refined by full matrix least squares to a residual of 0.054 for 1662 'observed' reflections. Crystals are orthorhombic, Pnma, a 13.706(2), b 9.924(1), c 7.024(1)Ǻ Z 4. Fe-O is 2.110(4)Ǻ; Fe-Cl range between 2.323(1)Ǻ (trans to OH2) and 2.350(1)-2.390(1) Ǻ (cis), the latter distances being very dependent upon hydrogen-bonded interactions with nearby species.


1989 ◽  
Vol 42 (10) ◽  
pp. 1795 ◽  
Author(s):  
JM Harrowfield ◽  
BW Skelton ◽  
AA Soudi ◽  
AH White

The structure of the title compound, C4H4N2O5, has been redetermined by single-crystal X-ray diffraction methods at c. 295 K. Crystals are triclinic, P1, a 8.217(2), b 6.809(2), c 5.765(4) �, α 66.49(3),β 81.87(3), γ 74.35(2)�, Z= 2; the structure was refined by full-matrix least squares to a residual of 0.042 for 2190 independent 'observed' reflections, typical non-hydrogen interatomic distances being determined with estimated standard deviations of 0.001 �. Together with the recent precise redetermination of the structure of alloxan , these results allow comparison of the geometries of essentially planar polycarbonyl (-hydrate) arrays with those of long-chain arrays previously recorded.


1973 ◽  
Vol 51 (7) ◽  
pp. 1116-1122 ◽  
Author(s):  
M. C. Fredette ◽  
C. J. L. Lock

The title compound, [Re(CO)3Cl(C6H5•COH•CH•CO•CH3)]2, is one of a series of compounds obtained by the reaction of chloropentacarbonylrhenium(I) with β-diketones and has been characterized by n.m.r. and infrared spectroscopy and single crystal X-ray diffraction. The crystals are monoclinic with lattice parameters a = 14.77(2), b = 17.98(2), c = 13.48(2) Å, β = 124.34(9)°; C2/c, Z = 4. A total of 1293 independent reflections were measured on a single crystal X-ray diffractometer and the structure was refined by full matrix least squares analysis to a weighted R2 value of 0.0444. The dimeric halves of the molecules are held together by two chlorine atoms symmetrically bridging the rhenium atoms (Re—Cl = 2.511(5) Å The structure is thus very like that of [Re(CO)4Cl]2, except that two neutral β-ketoenol molecules replace two carbon monoxide molecules (one on each rhenium) and are bonded through the ketone group (Re—O = 2.16(1) Å). The arrangement of the keto and enol groups is such that hydrogen bonding can occur between them.


1979 ◽  
Vol 32 (2) ◽  
pp. 297
Author(s):  
BW Skelton ◽  
AH White

The crystal structure of the title compound, NaAg(NO2)2, has been determined by single-crystal X-ray diffraction at 295(1) K and refined by full-matrix least squares to a residual of 0.043 for 449 'observed' reflections. Crystals are orthorhombic, space group Fd2d, a 7.913(2), b 10.721(2), c 10.857(3) �, Z 8. The structure is closely related to that of sodium and silver nitrites; the silver environment is dominated by the 'linear' coordination of a nitro group (Ag-N 2.25(2) �) and a 'chelating' pair of oxygen atoms from another NO2- species (Ag-O 2.422(8)�), the O2N-Ag-O2N group containing a crystallographic 2 axis.


1978 ◽  
Vol 31 (7) ◽  
pp. 1619 ◽  
Author(s):  
SR Hall ◽  
BW Skelton ◽  
AH White

The crystal structure of the title compound, [Fe(CO)3(C9H6O)], has been determined from single-crystal X-ray diffraction data at 295 K and refined by full-matrix least squares to a residual of 0.039 (2160 'observed' reflections). Crystals are monoclinic, P21/c, a 9.326(5), b 12.293(5), c 10.342(4) Ǻ, β 115.77(3)°, Z 4. The iron atom is symmetrically bound to the four atoms of the cyclobutadiene ring (<Fe- C> 2.055 Ǻ).


1979 ◽  
Vol 32 (5) ◽  
pp. 1165 ◽  
Author(s):  
AJ Canty ◽  
CL Raston ◽  
AH White

The crystal structure of the title compound, MeSHgCl, has been determined by single-crystal X-ray diffraction at 295 K and refined by full-matrix least squares to a residual of 0.048 for 787 'observed' reflections. Crystals are monoclinic, P21/c, a 7.490(4), b 7.395(2), c 7.815(3) �,β 92.93(4)�, Z 4, and are isostructural with the previously described MeSHgBr.


1980 ◽  
Vol 33 (2) ◽  
pp. 431 ◽  
Author(s):  
A Farrand ◽  
AK Gregson ◽  
BW Skelton ◽  
AH White

The crystal structure of the title compound, K2Cu(CO3)2, has been determined by single-crystal X-ray diffraction at 295(1) K, and refined by least squares to a residual of 0.027 for 1441 'observed' reflections. Crystals are orthorhombic, space group Fdd2, a 11.425(3), b 17.658(4), c 6.154(2) A, Z 8. The structure comprises potassium cations embedded in an infinite three-dimensional polymeric anionic array of square-planar coordinated copper atoms with bridging carbonate groups [Cu-O 1.934(2), 1.936(2) Ǻ]. Within the latter, the non- coordinating oxygen-carbon bond is shorter [1.259(3) Ǻ] than the other two [1.303(3), 1.307(2) Ǻ] and the O-C-O angle opposite it is correspondingly reduced to 117.1(2)°. The CO3 plane lies at 83.9° to the CuO4 'plane'.


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