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Crystal structure of deracoxib, C17H14F3N3O3S

Published online by Cambridge University Press:  09 January 2023

James A. Kaduk*
Affiliation:
Illinois Institute of Technology, 3101 S. Dearborn St., Chicago, IL 60616, USA North Central College, 131 S. Loomis St., Naperville, IL 60540, USA
Amy M. Gindhart
Affiliation:
ICDD, 12 Campus Blvd., Newtown Square, PA 19073-3273, USA
Stacy Gates-Rector
Affiliation:
ICDD, 12 Campus Blvd., Newtown Square, PA 19073-3273, USA
Thomas N. Blanton
Affiliation:
ICDD, 12 Campus Blvd., Newtown Square, PA 19073-3273, USA
*
a)Author to whom correspondence should be addressed. Electronic mail: [email protected]
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Abstract

The crystal structure of deracoxib has been solved and refined using synchrotron X-ray powder diffraction data, and optimized using density functional theory techniques. Deracoxib crystallizes in space group Pbca (#61) with a = 9.68338(11), b = 9.50690(5), c = 38.2934(4) Å, V = 3525.25(3) Å3, and Z = 8. The molecules stack in layers parallel to the ab-plane. N–H⋯O hydrogen bonds link the molecules along the b-axis, in chains with the graph set C1,1(4), as well as more-complex patterns. N–H⋯N hydrogen bonds link the layers. The powder pattern has been submitted to ICDD for inclusion in the Powder Diffraction File™ (PDF®).

Type
New Diffraction Data
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited
Copyright
Copyright © The Author(s), 2023. Published by Cambridge University Press on behalf of International Centre for Diffraction Data

I. INTRODUCTION

Deracoxib (sold under the brand name Deramaxx) is a selective cyclooxygenase 2 inhibitor, used in veterinary medicine for the control of pain and inflammation associated with osteoarthritis in dogs. Deracoxib is also used after canine dental procedures and is not recommended for use in cats. The systematic name (CAS Registry Number 169590-41-4) is 4-[3-(difluoromethyl)-5-(3-fluoro-4-methoxyphenyl)pyrazol-1-yl]benzenesulfonamide. A two-dimensional molecular diagram is shown in Figure 1.

Figure 1. The 2D molecular structure of deracoxib.

We are unaware of any published powder diffraction data on deracoxib. This work was carried out as part of a project (Kaduk et al., Reference Kaduk, Crowder, Zhong, Fawcett and Suchomel2014) to determine the crystal structures of large-volume commercial pharmaceuticals, and include high-quality powder diffraction data for them in the Powder Diffraction File (Gates-Rector and Blanton, Reference Gates-Rector and Blanton2019).

II. EXPERIMENTAL AND REFINEMENTS

Deracoxib was a commercial reagent, purchased from TargetMol (Batch #113281), and was used as-received. The white powder was packed into a 1.5 mm diameter Kapton capillary and rotated during the measurement at ~50 Hz. The powder pattern was measured at 295 K at beamline 11-BM (Antao et al., Reference Antao, Hassan, Wang, Lee and Toby2008; Lee et al., Reference Lee, Shu, Ramanathan, Preissner, Wang, Beno, Von Dreele, Ribaud, Kurtz, Antao, Jiao and Toby2008; Wang et al., Reference Wang, Toby, Lee, Ribaud, Antao, Kurtz, Ramanathan, Von Dreele and Beno2008) of the Advanced Photon Source at Argonne National Laboratory using a wavelength of 0.458208(2) Å from 0.5 to 50° 2θ with a step size of 0.001° and a counting time of 0.1 s step−1. The high-resolution powder diffraction data were collected using twelve silicon crystal analyzers that allow for high angular resolution, high precision, and accurate peak positions. A mixture of silicon (NIST SRM 640c) and alumina (NIST SRM 676a) standards (ratio Al2O3:Si = 2:1 by weight) was used to calibrate the instrument and refine the monochromatic wavelength used in the experiment.

The pattern was indexed using JADE Pro 8.1 (MDI, 2021) on a high-quality primitive orthorhombic unit cell with a = 9.71606, b = 9.54339, c = 38.43565 Å, V = 3563.91 Å3, and Z = 8. The suggested space group was Pbca, which was confirmed by successful solution and refinement of the structure. A reduced cell search in the Cambridge Structural Database (Groom et al., Reference Groom, Bruno, Lightfoot and Ward2016) combined with only C, H, F, N, O, and S elements, yielded no hits.

A deracoxib molecule was downloaded from PubChem (Kim et al., Reference Kim, Chen, Cheng, Gindulyte, He, He, Li, Shoemaker, Thiessen, Yu, Zaslavsky, Zhang and Bolton2019) as Conformer3D_CID_3058754.sdf. It was converted to a *.mol2 file using Mercury (Macrae et al., Reference Macrae, Sovago, Cottrell, Galek, McCabe, Pidcock, Platings, Shields, Stevens, Towler and Wood2020) and to a Fenske-Hall Z-matrix using Open Babel (O'Boyle et al., Reference O'Boyle, Banck, James, Morley, Vandermeersch and Hutchison2011). The structure was solved using FOX (Favre-Nicolin and Černý, Reference Favre-Nicolin and Černý2002) using sinθ/λ max = 0.32 Å−1 (2θ max = 16.9°).

Rietveld refinement was carried out using GSAS-II (Toby and Von Dreele, Reference Toby and Von Dreele2013). Only the 1.0–25.0° portion of the pattern was included in the refinement (d min = 1.058 Å). The region 1.50–2.12°, which contained a peak from the Kapton capillary, was excluded from the refinement. All non-H bond distances and angles were subjected to restraints, based on a Mercury/Mogul Geometry Check (Bruno et al., Reference Bruno, Cole, Kessler, Luo, Sam Motherwell, Purkis, Smith, Taylor, Cooper, Harris and Guy Orpen2004; Sykes et al., Reference Sykes, McCabe, Allen, Battle, Bruno and Wood2011). The Mogul average and standard deviation for each quantity were used as the restraint parameters. The restraints contributed 4.2% to the final χ 2. The hydrogen atoms were included in calculated positions, which were recalculated during the refinement using Materials Studio (Dassault, 2021). The U iso were grouped by chemical similarity. The U iso for the H atoms were fixed at 1.3× the U iso of the heavy atoms to which they are attached. A second-order spherical harmonic model was included in the refinement. The texture index was 1.032(0). The peak profiles were described using the generalized microstrain model. The background was modeled using a 6-term shifted Chebyshev polynomial, plus a peak at 5.81° 2θ to model the scattering from the Kapton capillary and any amorphous component.

The final refinement of 106 variables using 23 413 observations and 72 restraints yielded the residuals R wp = 0.0589 and GOF = 1.26. The largest peak (1.09 Å from C19) and hole (1.01 Å from C17) in the difference Fourier map were 0.19(5) and −0.23(5) eÅ3, respectively. The largest errors in the difference plot (Figure 2) are in the shapes of some of the strong low-angle peaks.

Figure 2. The Rietveld plot for the refinement of deracoxib. The blue crosses represent the observed data points, and the green line is the calculated pattern. The cyan curve is the normalized error plot, and the red line is the background curve. The vertical scale has been multiplied by a factor of 5× for 2θ > 9.5° and by 20× for 2θ > 18.0°. The two vertical magenta dashed lines indicate the excluded region 1.50–2.12° 2θ, which contains a peak from the Kapton capillary.

The structure of deracoxib was optimized using VASP (Kresse and Furthmüller, Reference Kresse and Furthmüller1996) (fixed experimental unit cell) through the MedeA graphical interface (Materials Design, 2016). The calculation was carried out on 16 2.4 GHz processors (each with 4 GB RAM) of a 64-processor HP Proliant DL580 Generation 7 Linux cluster at North Central College. The calculation used the GGA-PBE functional, a plane wave cutoff energy of 400.0 eV, and a k-point spacing of 0.5 Å−1 leading to a 2 × 2 × 1 mesh, and took ~17 h. A single-point density functional theory calculation (fixed experimental cell) and population analysis were carried out using CRYSTAL17 (Dovesi et al., Reference Dovesi, Erba, Orlando, Zicovich-Wilson, Civalleri, Maschio, Rérat, Casassa, Baima, Salustro and Kirtman2018). The basis sets for the H, C, N, and O atoms in the calculation were those of Gatti et al. (Reference Gatti, Saunders and Roetti1994), and those for F and S were those of Peintinger et al. (Reference Peintinger, Oliveira and Bredow2013). The calculations were run on a 3.5 GHz PC using 8 k-points and the B3LYP functional, and took ~3.1 h.

III. RESULTS AND DISCUSSION

The root-mean-square (rms) Cartesian displacement between the Rietveld-refined and DFT-optimized structures of deracoxib is 0.070 Å (Figure 3). The excellent agreement provides strong evidence that the structure is correct (van de Streek and Neumann, Reference van de Streek and Neumann2014). This discussion concentrates on the DFT-optimized structure. The asymmetric unit (with atom numbering) is illustrated in Figure 4. The best view of the crystal structure is down the a-axis (Figure 5). The molecules stack in layers parallel to the ab-plane.

Figure 3. Comparison of the Rietveld-refined (red) and VASP-optimized (blue) structures of deracoxib. The rms Cartesian displacement is 0.070 Å. Image generated using Mercury (Macrae et al., Reference Macrae, Sovago, Cottrell, Galek, McCabe, Pidcock, Platings, Shields, Stevens, Towler and Wood2020).

Figure 4. The asymmetric unit of deracoxib, with the atom numbering. The atoms are represented by 50% probability spheroids/ellipsoids. Image generated using Mercury (Macrae et al., Reference Macrae, Sovago, Cottrell, Galek, McCabe, Pidcock, Platings, Shields, Stevens, Towler and Wood2020).

Figure 5. The crystal structure of deracoxib, viewed down the a-axis. Image generated using Diamond (Crystal Impact, 2022).

All of the bond distances and angles fall within the normal ranges indicated by a Mercury/Mogul Geometry Check (Macrae et al., Reference Macrae, Sovago, Cottrell, Galek, McCabe, Pidcock, Platings, Shields, Stevens, Towler and Wood2020). The quantum chemical geometry optimization of the deracoxib molecule (DFT/B3LYP/6-31G*/water) using Spartan ‘18 (Wavefunction, 2020) indicated that the observed conformation is very close to a local minimum in energy. A conformational analysis (MMFF force field) indicates that the minimum-energy conformation is 5.9 kcal mol−1 lower in energy, and has a different orientation of the phenyl ring containing the sulfonamide group (~180° rotation). Intermolecular interactions, thus, affect the solid-state conformation.

Analysis of the contributions to the total crystal energy of the structure using the Forcite module of Materials Studio (Dassault, 2021) suggests that the intramolecular deformation energy is dominated by angle deformation terms. The intermolecular energy is dominated by van der Waals and electrostatic attractions, which in this force field analysis also include hydrogen bonds. The hydrogen bonds are better analyzed using the results of the DFT calculation.

There are three traditional hydrogen bonds in the structure (Table I), between the amino group H37–N10–H38 and the sulfonyl group O6–S1–O7, as well as the ring nitrogen atom N9. The energies of the N–H⋯O hydrogen bonds were calculated using the correlation of Wheatley and Kaduk (Reference Wheatley and Kaduk2019). The N–H⋯O hydrogen bonds link the molecules along the b-axis, in chains with the graph set (Etter, Reference Etter1990; Bernstein et al., Reference Bernstein, Davis, Shimoni and Chang1995; Shields et al., Reference Shields, Raithby, Allen and Samuel Motherwell2000) C1,1(4), as well as more-complex patterns. The N–H⋯N hydrogen bonds link the layers. Several intramolecular and intermolecular C–H⋯O and C–H⋯N hydrogen bonds contribute to the crystal energy.

TABLE I. Hydrogen bonds (CRYSTAL17) in deracoxib.

a Intramolecular.

The volume enclosed by the Hirshfeld surface of the deracoxib molecule (Figure 6; Hirshfeld, Reference Hirshfeld1977; Turner et al., Reference Turner, McKinnon, Wolff, Grimwood, Spackman, Jayatilaka and Spackman2017) is 433.26 Å3, 98.32% of 1/8 the unit cell volume. The packing density is thus fairly typical. The only significant close contacts (red in Figure 6) involve the hydrogen bonds. The volume/non-hydrogen atom is 16.3 Å3.

Figure 6. The Hirshfeld surface of deracoxib. Intermolecular contacts longer than the sums of the van der Waals radii are colored blue, and contacts shorter than the sums of the radii are colored red. Contacts equal to the sums of radii are white.

The Bravais–Friedel–Donnay–Harker (Bravais, Reference Bravais1866; Friedel, Reference Friedel1907; Donnay and Harker, Reference Donnay and Harker1937) morphology suggests that we might expect platy morphology for deracoxib, with {001} as the major faces. A second-order spherical harmonic model was included in the refinement. The texture index was 1.032(0), indicating that preferred orientation was small in this rotated capillary specimen.

IV. DEPOSITED DATA

The powder pattern of deracoxib from this synchrotron data set has been submitted to ICDD for inclusion in the Powder Diffraction File. The Crystallographic Information Framework (CIF) files containing the results of the Rietveld refinement (including the raw data) and the DFT geometry optimization were deposited with the ICDD. The data can be requested at .

ACKNOWLEDGEMENTS

The use of the Advanced Photon Source at Argonne National Laboratory was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357. This work was partially supported by the International Centre for Diffraction Data. We thank Lynn Ribaud and Saul Lapidus for their assistance in the data collection.

CONFLICT OF INTEREST

The authors have no conflict of interest to declare.

References

REFERENCES

Antao, Sytle M., Hassan, Ishmael, Wang, Jun, Lee, Peter L., and Toby, Brian H.. 2008. “State-of-the-Art High-Resolution Powder X-Ray Diffraction (HRPXRD) Illustrated with Rietveld Structure Refinement of Quartz, Sodalite, Tremolite, and Meionite.” The Canadian Mineralogist 46 (6): 1501–9.CrossRefGoogle Scholar
Bernstein, Joel, Davis, Raymond E., Shimoni, Liat, and Chang, Ning-Leh. 1995. “Patterns in Hydrogen Bonding: Functionality and Graph Set Analysis in Crystals.” Angewandte Chemie International Edition in English 34 (15): 1555–73.CrossRefGoogle Scholar
Bravais, Auguste. 1866. Etudes Cristallographiques. Paris, Gauthier-Villars.Google Scholar
Bruno, Ian J., Cole, Jason C., Kessler, Magnus, Luo, Jie, Sam Motherwell, WD, Purkis, Lucy H., Smith, Barry R., Taylor, Robin, Cooper, Richard I., Harris, Stephanie E., and Guy Orpen, A.. 2004. “Retrieval of Crystallographically-Derived Molecular Geometry Information.” Journal of Chemical Information and Computer Sciences 44 (6): 2133–44.CrossRefGoogle ScholarPubMed
Crystal Impact. 2022. Diamond. V. 4.6.8. Crystal Impact - Dr. H. Putz & Dr. K. Brandenburg. Windows.Google Scholar
Dassault Systèmes. 2021. Materials Studio 2021. San Diego, CA, BIOVIA.Google Scholar
Donnay, J. D H., and Harker, David. 1937. “A New Law of Crystal Morphology Extending the Law of Bravais.” American Mineralogist: Journal of Earth and Planetary Materials 22 (5): 446–67.Google Scholar
Dovesi, Roberto, Erba, Alessandro, Orlando, Roberto, Zicovich-Wilson, Claudio M., Civalleri, Bartolomeo, Maschio, Lorenzo, Rérat, Michel, Casassa, Silvia, Baima, Jacopo, Salustro, Simone, and Kirtman, Bernard. 2018. “Quantum-Mechanical Condensed Matter Simulations with CRYSTAL.” Wiley Interdisciplinary Reviews: Computational Molecular Science 8 (4): e1360.Google Scholar
Etter, Margaret C. 1990. “Encoding and Decoding Hydrogen-Bond Patterns of Organic Compounds.” Accounts of Chemical Research 23 (4): 120–6.CrossRefGoogle Scholar
Favre-Nicolin, Vincent, and Černý, Radovan. “FOX, ‘Free Objects for Crystallography': A Modular Approach to ab initio Structure Determination from Powder Diffraction.” Journal of Applied Crystallography 35 (6): 734–43.CrossRefGoogle Scholar
Friedel, Georges. 1907. “Etudes sur la loi de Bravais.” Bulletin de Minéralogie 30 (9): 326455.Google Scholar
Gates-Rector, Stacy, and Blanton, Thomas. 2019. “The Powder Diffraction File: A Quality Materials Characterization Database.” Powder Diffraction 34 (4): 352–60.CrossRefGoogle Scholar
Gatti, C., Saunders, V. R., and Roetti, C.. 1994. “Crystal Field Effects on the Topological Properties of the Electron Density in Molecular Crystals: The Case of Urea.” The Journal of Chemical Physics 101 (12): 10686–96.CrossRefGoogle Scholar
Groom, C. R., Bruno, I. J., Lightfoot, M. P., and Ward, S. C. 2016. “The Cambridge Structural Database.” Acta Crystallographica Section B. Structural Science, Crystal Engineering and Materials 72, 171–9.CrossRefGoogle ScholarPubMed
Hirshfeld, Fred L. 1977. “Bonded-Atom Fragments for Describing Molecular Charge Densities.” Theoretica Chimica Acta 44 (2): 129–38.CrossRefGoogle Scholar
Kaduk, James A., Crowder, Cyrus E., Zhong, Kai, Fawcett, Timothy G., and Suchomel, Matthew R.. 2014. “Crystal Structure of Atomoxetine Hydrochloride (Strattera), C17H22NOCl.” Powder Diffraction 29 (3): 269–73.CrossRefGoogle Scholar
Kim, Sunghwan, Chen, Jie, Cheng, Tiejun, Gindulyte, Asta, He, Jia, He, Siqian, Li, Qingliang, Shoemaker, Benjamin A., Thiessen, Paul A., Yu, Bo, Zaslavsky, Leonid, Zhang, Jian, and Bolton, Evan E.. 2019. “PubChem 2019 Update: Improved Access to Chemical Data.” Nucleic Acids Research 47 (D1): D1102–9. doi:10.1093/nar/gky1033.CrossRefGoogle ScholarPubMed
Kresse, Georg, and Furthmüller, Jürgen. 1996. “Efficiency of ab-initio Total Energy Calculations for Metals and Semiconductors Using a Plane-Wave Basis Set.” Computational Materials Science 6 (1): 1550.CrossRefGoogle Scholar
Lee, Peter L., Shu, Deming, Ramanathan, Mohan, Preissner, Curt, Wang, Jun, Beno, Mark A., Von Dreele, Robert B., Ribaud, Lynn, Kurtz, Charles, Antao, Sytle M., Jiao, Xuesong, and Toby, Brian H.. 2008. “A Twelve-Analyzer Detector System for High-Resolution Powder Diffraction.” Journal of Synchrotron Radiation 15 (5): 427–32.CrossRefGoogle ScholarPubMed
Macrae, Clare F., Sovago, Ioana, Cottrell, Simon J., Galek, Peter TA, McCabe, Patrick, Pidcock, Elna, Platings, Michael, Shields, Greg P., Stevens, Joanna S., Towler, Matthew, and Wood, Peter A.. 2020. “Mercury 4.0: From Visualization to Analysis, Design and Prediction.” Journal of Applied Crystallography 53 (1): 226–35.CrossRefGoogle ScholarPubMed
Materials Design Inc. 2016. MedeA 2.20.4. Angel Fire, NM, Materials Design Inc.Google Scholar
MDI Materials Data. 2022. JADE Pro Version 8.2. MDI Materials Data, Livermore, CA, USA.Google Scholar
O'Boyle, Noel M., Banck, Michael, James, Craig A., Morley, Chris, Vandermeersch, Tim, and Hutchison, Geoffrey R.. “Open Babel: An open chemical toolbox.” Journal of cheminformatics 3, no. 1 (2011): 114.CrossRefGoogle ScholarPubMed
Peintinger, Michael F., Oliveira, Daniel Vilela, and Bredow, Thomas. 2013. “Consistent Gaussian Basis Sets of Triple-Zeta Valence with Polarization Quality for Solid-State Calculations.” Journal of Computational Chemistry 34 (6): 451–9.CrossRefGoogle ScholarPubMed
Shields, Gregory P., Raithby, Paul R., Allen, Frank H., and Samuel Motherwell, WD. 2000 “The Assignment and Validation of Metal Oxidation States in the Cambridge Structural Database.” Acta Crystallographica Section B: Structural Science 56 (3): 455–65.CrossRefGoogle Scholar
Sykes, Richard A., McCabe, Patrick, Allen, Frank H., Battle, Gary M., Bruno, Ian J., and Wood, Peter A.. 2011. “New Software for Statistical Analysis of Cambridge Structural Database Data.” Journal of Applied Crystallography 44 (4): 882–6.CrossRefGoogle Scholar
Toby, Brian H., and Von Dreele, Robert B.. 2013. “GSAS-II: The Genesis of a Modern Open-Source all Purpose Crystallography Software Package.” Journal of Applied Crystallography 46 (2): 544–9.CrossRefGoogle Scholar
Turner, M. J., McKinnon, J. J., Wolff, S. K., Grimwood, D. J., Spackman, P. R., Jayatilaka, D., and Spackman, M. A.. “CrystalExplorer17.” (2017): 76730. http://hirshfeldsurface.net.Google Scholar
van de Streek, Jacco van de, and Neumann, Marcus A.. 2014. “Validation of Molecular Crystal Structures from Powder Diffraction Data with Dispersion-Corrected Density Functional Theory (DFT-D).” Acta Crystallographica. Section B, Structural Science, Crystal Engineering and Materials 70 (Pt 6): 1020–32.CrossRefGoogle ScholarPubMed
Wang, Jun, Toby, Brian H., Lee, Peter L., Ribaud, Lynn, Antao, Sytle M., Kurtz, Charles, Ramanathan, Mohan, Von Dreele, Robert B., and Beno, Mark A.. 2008. “A Dedicated Powder Diffraction Beamline at the Advanced Photon Source: Commissioning and Early Operational Results.” Review of Scientific Instruments 79 (8): 085105.CrossRefGoogle ScholarPubMed
Wavefunction, Inc. 2020. “Spartan ’18” Version 1.4.5. Wavefunction, Inc., Irvine, CA.Google Scholar
Wheatley, Austin M., and Kaduk, James A.. 2019. “Crystal Structures of Ammonium Citrates.” Powder Diffraction 34 (1): 3543.CrossRefGoogle Scholar
Figure 0

Figure 1. The 2D molecular structure of deracoxib.

Figure 1

Figure 2. The Rietveld plot for the refinement of deracoxib. The blue crosses represent the observed data points, and the green line is the calculated pattern. The cyan curve is the normalized error plot, and the red line is the background curve. The vertical scale has been multiplied by a factor of 5× for 2θ > 9.5° and by 20× for 2θ > 18.0°. The two vertical magenta dashed lines indicate the excluded region 1.50–2.12° 2θ, which contains a peak from the Kapton capillary.

Figure 2

Figure 3. Comparison of the Rietveld-refined (red) and VASP-optimized (blue) structures of deracoxib. The rms Cartesian displacement is 0.070 Å. Image generated using Mercury (Macrae et al., 2020).

Figure 3

Figure 4. The asymmetric unit of deracoxib, with the atom numbering. The atoms are represented by 50% probability spheroids/ellipsoids. Image generated using Mercury (Macrae et al., 2020).

Figure 4

Figure 5. The crystal structure of deracoxib, viewed down the a-axis. Image generated using Diamond (Crystal Impact, 2022).

Figure 5

TABLE I. Hydrogen bonds (CRYSTAL17) in deracoxib.

Figure 6

Figure 6. The Hirshfeld surface of deracoxib. Intermolecular contacts longer than the sums of the van der Waals radii are colored blue, and contacts shorter than the sums of the radii are colored red. Contacts equal to the sums of radii are white.