CRYSTAL STRUCTURE OF ZIRCONYL PERCHLORATE DIHYDRATE BY X-RAY POWDER DIFFRACTION METHOD

1963 ◽  
Vol 67 (6) ◽  
pp. 1357-1358 ◽  
Author(s):  
P. Rama Murthy ◽  
C. C. Patel
2014 ◽  
Vol 70 (a1) ◽  
pp. C1560-C1560
Author(s):  
Fumiko Kimura ◽  
Wataru Oshima ◽  
Hiroko Matsumoto ◽  
Hidehiro Uekusa ◽  
Kazuaki Aburaya ◽  
...  

In pharmaceutical sciences, the crystal structure is of primary importance because it influences drug efficacy. Due to difficulties of growing a large single crystal suitable for the single crystal X-ray diffraction analysis, powder diffraction method is widely used. In powder method, two-dimensional diffraction information is projected onto one dimension, which impairs the accuracy of the resulting crystal structure. To overcome this problem, we recently proposed a novel method of fabricating a magnetically oriented microcrystal array (MOMA), a composite in which microcrystals are aligned three-dimensionally in a polymer matrix. The X-ray diffraction of the MOMA is equivalent to that of the corresponding large single crystal, enabling the determination of the crystal lattice parameters and crystal structure of the embedded microcrytals.[1-3] Because we make use of the diamagnetic anisotropy of crystal, those crystals that exhibit small magnetic anisotropy do not take sufficient three-dimensional alignment. However, even for these crystals that only align uniaxially, the determination of the crystal lattice parameters can be easily made compared with the determination by powder diffraction pattern. Once these parameters are determined, crystal structure can be determined by X-ray powder diffraction method. In this paper, we demonstrate possibility of the MOMA method to assist the structure analysis through X-ray powder and single crystal diffraction methods. We applied the MOMA method to various microcrystalline powders including L-alanine, 1,3,5-triphenyl benzene, and cellobiose. The obtained MOMAs exhibited well-resolved diffraction spots, and we succeeded in determination of the crystal lattice parameters and crystal structure analysis.


2007 ◽  
Vol 22 (3) ◽  
pp. 241-245 ◽  
Author(s):  
B. Włodarczyk-Gajda ◽  
A. Rafalska-Łasocha ◽  
W. Łasocha

A novel synthesis method of fibrillar trimolybdates with the use of Ag2Mo3O10∙2H2O as a precursor has been used successfully to synthesize methylammonium trimolybdate, (CH3NH3)2Mo3O10∙H2O. The crystal structure of this compound was determined by X-ray powder diffraction method and refined by the Rietveld method. The compound is orthorhombic, space group Pnma (62), with a=11.241(3), b=7.585(1), and c=15.516(4) Å. The redetermined crystal structure of the precursor and the structure of the title compound are compared and discussed.


2006 ◽  
Vol 21 (3) ◽  
pp. 225-228 ◽  
Author(s):  
R. Karray ◽  
A. Kabadou ◽  
A. Ben Salah ◽  
A. van der Lee

The crystal structure of cesium ammonium hexachlorotellurate [Cs0.86(NH4)0.14]2TeCl6, has been determined using X-ray powder diffraction techniques. At room temperature, the title compound crystallizes in the cubic space group Fm3m, with a lattice parameter a=10.470(17) Å. The Rietveld refinement of the structure led to final confidence factors Rp=0.0338 and Rwp=0.0487. The structure of [Cs0.86(NH4)0.14]2TeCl6 belongs to the large family of K2PtCl6-related structures. The H atoms of the ammonium group are orientated with its apex toward Te atoms as seen in the related compound (NH4)2SiF6. An IR spectroscopic study was performed to confirm the results of the diffraction method, notably concerning the presence of the ammonium group.


2015 ◽  
Vol 3 (2) ◽  
pp. 65-71
Author(s):  
Yuri Titov ◽  
Nadezhda Belyavina ◽  
Mykola Slobodyanik ◽  
Vitaly Polubinskii ◽  
Olesya Nakonechna

The Sr6Nb4ZrO18 niobatozirconate has been synthesized from the Sr5Nb4O15 four-layer perovskite and the SrZrO3 perovskite at T = 1670 K by ceramic technique. Crystal structure of the Sr6Nb4ZrO18 compound has been studied by the X-ray powder diffraction method. It was shown that crystal structure of the Sr6Nb4ZrO18 (a = 0.5687(1) nm, c = 4.146(1) nm, R-3m space group) belongs to the Ba6Nb4TiO18-type with five-layer perovskite-like structure. The crystal structure features of the Sr6Nb4BIVO18 compounds (BIV = Ti, Sn, Zr) has been analyzed. The correlation between composition and crystal structure features for all Sr6Nb4BIVO18 (BIV = Ti, Sn, Zr) compounds, which leads to destruction slab perovskite-like structure has been revealed.


1989 ◽  
Vol 03 (07) ◽  
pp. 561-569 ◽  
Author(s):  
J.K. LIANG ◽  
Y.L. ZHANG ◽  
J.Q. HUANG ◽  
S.S. XIE ◽  
G.C. CHE ◽  
...  

The crystal structure of TlBa 2 Ca 2 Cu 3 O 8.5(Tc=112 K) has been determined by means of X-ray powder diffraction method. It belongs to primary tetragonal symmetry with lattice parameters: a=3.847 Å, c=15.89 Å. Its space group is [Formula: see text]. Each unit cell contains one chemical formular unit. The arrangements of ions in a unit cell are as follows: 1Tl cation occupies 1(b) equivalent point position. 2Ca and 2Ba cations occupy 2(h) equivalent point positions with respective atomic parameters z=0.100 and 0.320. 3Cu occupy 1(a) and 2(g) (z=0.200) equivalent point positions. 8.50 anions occupy 1(d), 2(f), 2(g) (z=0.325) and 4(i) (z=0.200) equivalent point positions respectively. (Occupation factor is 0.945.) The crystal structure of TlBa2Ca2Cu3O8.5 is quite similar to those of the other superconducting phases. All cations are distributed at positions of (0,0,z) and (1 /2,1 /2,z) alternatively. The oxygen deficient pseudo-perovskite unit Ba-Cu-Ca-Cu-Ca-Cu-Ba is separated by double Tl-O layers in the crystal structure of Tl 2 Ba 2 Ca 2 Cu 3 O 10. However, the oxygen deficient pseudo-perovskite unit Ba-Cu-Ca-Cu-Ca-Cu-Ba is separated by single Tl-O layer in the crystal structure of TlBa 2 Ca 2 Cu 3 O 8.5. The relations among the crystal structure of the superconducting phases as well as the relation between the crystal structure and superconductivity are discussed.


1989 ◽  
Vol 03 (01) ◽  
pp. 41-46 ◽  
Author(s):  
J.Q. HUANG ◽  
J.K. LIANG ◽  
Y.L. ZHANG ◽  
S.S. XIE ◽  
X.R. CHEN ◽  
...  

We reported the crystal structures of TlBa 2 Ca 3 Cu 4 O 10.5 and Tl 2 Ba 2 CuO 6. The atomic parameters were determined by means of X-ray powder diffraction method. We also discussed the relationship between the crystal structure and properties as well as the relation among the crystal structures of the high T c superconductors.


2021 ◽  
Vol 36 (1) ◽  
pp. 35-42
Author(s):  
Shivang Bhaskar ◽  
Joseph T. Golab ◽  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of pimecrolimus Form B has been solved and refined using synchrotron X-ray powder diffraction data and optimized using density functional techniques. Pimecrolimus crystallizes in the space group P21 (#4) with a = 15.28864(7), b = 13.31111(4), c = 10.95529(5) Å, β = 96.1542(3)°, V = 2216.649(9) Å3, and Z = 2. Although there are an intramolecular six-ring hydrogen bond and some larger chain and ring patterns, the crystal structure is dominated by van der Waals interactions. There is a significant difference between the conformation of the Rietveld-refined and the DFT-optimized structures in one portion of the macrocyclic ring. Although weak, intermolecular interactions are apparently important in determining the solid-state conformation. The powder pattern is included in the Powder Diffraction File™ (PDF®) as entry 00-066-1619. This study provides the atomic coordinates to be added to the PDF entry.


1993 ◽  
Vol 102 (2) ◽  
pp. 340-348 ◽  
Author(s):  
Staffan Hansen ◽  
Kenny Ståhl ◽  
Roland Nilsson ◽  
Arne Andersson

2021 ◽  
pp. 1-3
Author(s):  
Carina Schlesinger ◽  
Edith Alig ◽  
Martin U. Schmidt

The structure of the anticancer drug carmustine (1,3-bis(2-chloroethyl)-1-nitrosourea, C5H9Cl2N3O2) was successfully determined from laboratory X-ray powder diffraction data recorded at 278 K and at 153 K. Carmustine crystallizes in the orthorhombic space group P212121 with Z = 4. The lattice parameters are a = 19.6935(2) Å, b = 9.8338(14) Å, c = 4.63542(6) Å, V = 897.71(2) ų at 153 K, and a = 19.8522(2) Å, b = 9.8843(15) Å, c = 4.69793(6) Å, V = 921.85(2) ų at 278 K. The Rietveld fits are very good, with low R-values and smooth difference curves of calculated and experimental powder data. The molecules form a one-dimensional hydrogen bond pattern. At room temperature, the investigated commercial sample of carmustine was amorphous.


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