Crystal structure of bretylium tosylate (Bretylol®), C18H24BrNO3S

2018 ◽  
Vol 33 (4) ◽  
pp. 298-302
Author(s):  
Austin M. Wheatley ◽  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of bretylium tosylate has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional techniques. Bretylium tosylate crystallizes in space group C2/c (#15) with a = 32.6238(4), b = 12.40353(14), c = 9.93864(12) Å, β = 101.4676(10), V = 3941.39(5) Å3, and Z = 8. The sample exhibited visible decomposition in the X-ray beam. The unusual displacement ellipsoid of the Br atom probably indicates that the decomposition in the beam involves the Br atom. The crystal structure can be viewed as layered parallel to the bc plane. The layers are double, the center consisting of the cation/anion polar interactions and the outer surface of the double layers consists of hydrocarbon interactions. In the absence of normal hydrogen bond donors, the only hydrogen bonds in the bretylium tosylate structure are C–H…O hydrogen bonds. The powder pattern has been submitted to ICDD® for inclusion in the Powder Diffraction File™.

2019 ◽  
Vol 34 (2) ◽  
pp. 189-195
Author(s):  
Samantha C. Diulus ◽  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of bumetanide has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional techniques. Bumetanide crystallizes in space group P-1 (#2) with a = 5.00168(4), b = 9.22649(3), c = 19.59924(14) Å, α = 80.7941(5), β = 82.8401(7), γ = 86.8148(7)°, V = 885.268(9) Å3, and Z = 2. The crystal structure is layered with the double layers parallel to the ab plane. The exterior of the layer is composed of hydrocarbon portions of the molecule, both phenyl rings and butyl side chains. The central portion of the bilayer contains the hydrogen-bonding regions, both the carboxylic acid dimers and the hydrogen bonds involving the sulfonamide groups. The molecular conformations of bumetanide in this current triclinic structure and the previously-determined monoclinic polymorph FEDGON are very similar, as are the energies of the two polymorphs. The powder pattern is included in the Powder Diffraction File™ as entry 00-066-1609.


2015 ◽  
Vol 30 (4) ◽  
pp. 333-339 ◽  
Author(s):  
James A. Kaduk ◽  
Kai Zhong ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of salmeterol xinafoate has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional techniques. Salmeterol xinafoate crystallizes in space group P−1 (#2) with a = 9.173 89(13), b = 9.483 79(14), c = 21.3666(4) Å, α = 82.2646(13), β = 85.2531(12), γ = 62.1565(11)°, V = 1628.37(5) Å3, and Z = 2. Key to the structure solution was linking the two fragments by a Li atom along the expected N–H···O hydrogen bond. The salmeterol cation and xinafoate anion are linked by N–H···O and O–H···O hydrogen bonds, interactions which cause the salmeterol to adjust its conformation. The hydrogen bonds result in complex chains along the b-axis. The powder pattern is included in the Powder Diffraction File™ as entry 00-065-1430.


2021 ◽  
Vol 36 (1) ◽  
pp. 56-62
Author(s):  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of tezacaftor Form A has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional techniques. Tezacaftor Form A crystallizes in space group C2 (#5) with a = 21.05142(6), b = 6.60851(2), c = 17.76032(5) Å, β = 95.8255(2)°, V = 2458.027(7) Å3, and Z = 4. The crystal structure is dominated by van der Waals interactions. O–H⋯O hydrogen bonds link the molecules in chains along the b-axis, and there are a variety of C–H⋯O hydrogen bonds, both intra- and intermolecular. The powder pattern has been submitted to ICDD® for inclusion in the Powder Diffraction File™ (PDF®).


2021 ◽  
pp. 1-3
Author(s):  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of pazopanib hydrochloride Form 1 has been refined using synchrotron X-ray powder diffraction data and optimized using density functional theory techniques. Pazopanib hydrochloride crystallizes in space group P-1 (#2) with a = 8.45008(6), b = 8.71310(12), c = 16.05489(35) Å, α = 79.5996(9), β = 86.4784(5), γ = 87.3764(3)°, V = 1159.724(9) Å3, and Z = 2. The crystal structure is essentially identical to that of CSD Refcode CEVYEK. There are four strong N–H⋯Cl hydrogen bonds to the chloride anion. Several additional weaker N–H⋯Cl and C–H⋯Cl hydrogen bonds are also present. A variety of C–H⋯O, C–H⋯N, and N–H⋯S hydrogen bonds also contribute to the lattice energy. The powder pattern has been submitted to ICDD® for inclusion in the Powder Diffraction File™.


2019 ◽  
Vol 35 (1) ◽  
pp. 34-40
Author(s):  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of bisoprolol fumarate Form I has been solved and refined using synchrotron X-ray powder diffraction data and optimized using density functional techniques. Bisoprolol fumarate Form I crystallizes in space group P-1 (#2) with a = 8.165 70(5) Å, b = 8.516 39(12) Å, c = 16.751 79(18) Å, α = 89.142(1)°, β = 78.155(1)°, γ = 81.763(1)°, V = 1128.265(10) Å3, and Z = 2. The neutral side chain of the bisoprolol cation is probably disordered. The cation and anion are linked by N–H⋯O and O–H⋯O hydrogen bonds. The cations are also linked by N–H⋯O hydrogen bonds. The result is alternating layers of hydrophilic and hydrophobic layers parallel to the ab-plane. The density of the structure is relatively low at 1.130 g cm−3, but there are no obvious voids in the structure. The powder pattern is included in the Powder Diffraction File™ as entry 00-066-1625.


2021 ◽  
pp. 1-7
Author(s):  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of eltrombopag olamine Form I has been solved and refined using synchrotron X-ray powder diffraction data and optimized using density functional techniques. Eltrombopag olamine crystallizes in the space group P21/n (#14) with a = 17.65884(13), b = 7.55980(2), c = 22.02908(16) Å, β = 105.8749(4)°, V = 2828.665(11) Å3, and Z = 4. The crystal structure is dominated by columns of hydrogen-bonded cations and anions along the short b-axis. van der Waals interactions bind the columns together. Two H atoms of each ammonium group in the ethanolammonium cations participate in strong hydrogen bonds, and the third H forms weaker bifurcated H-bonds. The powder pattern has been submitted to ICDD® for inclusion in the Powder Diffraction File™ (PDF®).


2015 ◽  
Vol 30 (3) ◽  
pp. 263-269
Author(s):  
James A. Kaduk ◽  
Kai Zhong ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of the potassium salt of raltegravir has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional techniques. Raltegravir potassium crystallizes in space group P21/c (#14) with a = 15.610 59(9), b = 8.148 19(3), c = 16.125 97(6) Å, β = 94.1848(5)°, V = 2045.72(1) Å3, and Z = 4. The most prominent feature of the crystal structure is the chains of edge-sharing 7-coordinate KO5N2 parallel to the b-axis. The crystal structure can be described as having K-containing layers in the bc-plane, with double layers of CH4F halfway between them. The raltegravir anion is not in the minimum-energy conformation, suggesting that coordination to the K and hydrogen bonds play a significant role in the solid-state structure. The powder pattern is included in the Powder Diffraction File™ as entry 00-064-1499.


2021 ◽  
pp. 1-3
Author(s):  
James A. Kaduk ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of varenicline hydrogen tartrate Form B (Chantix®) has been refined using synchrotron X-ray powder diffraction data and optimized using density functional techniques. Varenicline hydrogen tartrate Form B crystallizes in space group P212121 (#19) with a = 7.07616(2), b = 7.78357(2), c = 29.86149(7) Å, V = 1644.706(6) Å3, and Z = 4. The hydrogen bonds were identified and quantified. Hydrogen bonds link the cations and anions in zig-zag chains along the b-axis. The powder pattern has been submitted to ICDD® for inclusion in the Powder Diffraction File™ (PDF®).


2015 ◽  
Vol 30 (3) ◽  
pp. 270-277
Author(s):  
James A. Kaduk ◽  
Kai Zhong ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of nilotinib has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional techniques. Nilotinib crystallizes in space group P1 (#1) with a = 4.518 14(3), b = 10.638 01(5), c = 13.703 77(8) Å, α = 68.8607(4), β = 82.1486(5), γ = 84.1978(5)°, V = 607.62(1) Å3, and Z = 1. The most prominent feature of the structure is two strong hydrogen bonds. These form chains with a graph set C1,1(13); the chains run along [111]. Several weak C–H···O hydrogen bonds also contribute to the packing. The powder pattern has been submitted to ICDD for inclusion in future releases of the Powder Diffraction File™.


2015 ◽  
Vol 30 (3) ◽  
pp. 211-217
Author(s):  
James A. Kaduk ◽  
Joel W. Reid ◽  
Kai Zhong ◽  
Amy M. Gindhart ◽  
Thomas N. Blanton

The crystal structure of solifenacin hydrogen succinate [C23H27N2O2(HC4H4O4)] has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional techniques. Solifenacin hydrogen succinate crystallizes in space group P21 (#4) with a = 6.477 03(2), b = 7.830 95(2), c = 23.848 72(7) Å, β = 90.2373(3)°, V = 1209.63(1) Å3, and Z = 2. The hydrogen succinate anions form a chain linked by strong hydrogen bonds parallel to the a-axis. Discrete N–H···O hydrogen bonds lie on the sides of this chain, resulting in a layer parallel to the ab-plane rich in hydrogen bonds. Halfway between these layers the molecules meet in a herringbone packing of aromatic rings. The powder pattern has been submitted to ICDD for inclusion in future releases of the Powder Diffraction File™.


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