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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 27;67(Pt 9):o2424. doi: 10.1107/S1600536811033435

4-(5-Phenyl-3-trifluoro­meth­yl-1H-pyrazol-1-­yl)benzene­sulfonamide

Abdullah M Asiri a,b,, Abdulrahman O Al-Youbi a, Hassan M Faidallah a, Seik Weng Ng c,a, Edward R T Tiekink c,*
PMCID: PMC3200877  PMID: 22059006

Abstract

Significant twists between the aromatic rings are evident in the structure of the title compound, C16H12F3N3O2S. With reference to the pyrazole plane, the N- and C-bound benzene rings form dihedral angles of 57.12 (11) and 29.75 (11)°, respectively. The dihedral angle between the benzene rings is 52.82 (11)°. The presence of N—H⋯O(sulfonamide) and N—H⋯N(pyrazole) hydrogen bonds lead to supra­molecular tubes along the b-axis direction. These are connected into layers via C—H⋯O inter­actions involving a bifurcated O atom (not involved in the N—H⋯O hydrogen bonding). Layers stack along the a-axis direction.

Related literature

For background to the biological applications of related species, see: Faidallah et al. (2007); Al-Saadi et al. (2008). For the crystal structure of a related species, see: Dev et al. (1999).graphic file with name e-67-o2424-scheme1.jpg

Experimental

Crystal data

  • C16H12F3N3O2S

  • M r = 367.35

  • Monoclinic, Inline graphic

  • a = 16.2430 (7) Å

  • b = 4.9461 (2) Å

  • c = 21.2383 (8) Å

  • β = 111.231 (5)°

  • V = 1590.47 (11) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.25 mm−1

  • T = 100 K

  • 0.40 × 0.10 × 0.05 mm

Data collection

  • Agilent SuperNova Dual diffractometer with an Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) T min = 0.735, T max = 1.000

  • 7901 measured reflections

  • 3560 independent reflections

  • 2876 reflections with I > 2σ(I)

  • R int = 0.031

Refinement

  • R[F 2 > 2σ(F 2)] = 0.043

  • wR(F 2) = 0.113

  • S = 1.06

  • 3560 reflections

  • 234 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.34 e Å−3

  • Δρmin = −0.49 e Å−3

Data collection: CrysAlis PRO (Agilent, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811033435/hg5083sup1.cif

e-67-o2424-sup1.cif (19.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033435/hg5083Isup2.hkl

e-67-o2424-Isup2.hkl (174.6KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811033435/hg5083Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H1⋯O1i 0.84 (3) 2.14 (3) 2.911 (2) 153 (2)
N3—H2⋯N2ii 0.87 (2) 2.21 (3) 3.049 (3) 164 (2)
C9—H9⋯O2iii 0.95 2.49 3.376 (3) 155
C16—H16⋯O2iv 0.95 2.55 3.137 (2) 120

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic.

Acknowledgments

The authors thank King Abdulaziz University and the University of Malaya for supporting this study.

supplementary crystallographic information

Comment

The crystallographic study of the title compound, (I), which is related to the anti-inflammatory drug, Celecoxib (Dev et al., 1999), was motivated by the recent reports of the biological activities exhibited by related pyrazole compounds (Faidallah et al., 2007; Al-Saadi et al., 2008).

Significant twists are evident in the molecule of (I), Fig. 1. With reference to the pyrazole (N1,N2,C2—C4) plane (r.m.s. deviation = 0,003 Å), the N-bound benzene ring (C11–C16) forms a dihedral angle of 57.12 (11) ° whereas the C-bound benzene ring (C5–C10) forms a dihedral angle of 29.75 (11) °; the dihedral angle formed between the two benzene rings is 52.82 (11) °. The orientations of the benzene rings in (I) differ from those in Celecoxib (Dev et al., 1999), the 4-methylphenyl derivative, with the dihedral angles formed between the N– and C-bound benzene rings and the pyrazole plane being 86.00 (12) and 15.25 (13) °, respectively.

Supramolecular tubes along the b axis feature in the crystal packing, Fig. 2. These are stabilized by amino-H hydrogen bonds to the pyrazole-N and to one of the sulfonamide-O atoms, Table 1. Tubes are linked into layers in the bc plane by C—H···O interactions whereby the sulfonamide-O2 atom is bifurcated, Table 1 and Fig. 3. Layers stack along the a axis, Fig. 4.

Experimental

A solution of 4,4,4-trifluoro-1-phenyl-1,3-butanedione (2.01 g, 10 mmol) in ethanol (50 ml) was refluxed with 4-hydrazinobenzenesulfonamide hydrochloride (2.2 g, 10 mmol) for 4 h, cooled and diluted with water. The precipitated crude product was filtered and recrystallized from ethanol as colourless crystals; M.pt. 431–433 K.

Refinement

Carbon-bound H-atoms were placed in calculated positions [C—H 0.95 Å, Uiso(H) 1.2Ueq(C)] and were included in the refinement in the riding model approximation. The amino-H atoms were located in a difference Fourier map, and subsequently refined freely.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

Supramolecular tube aligned along the b axis in (I) mediated by N—H···O and N—H···N hydrogen bonds shown as orange and blue dashed lines, respectively.

Fig. 3.

Fig. 3.

A view in projection down the a axis of the unit-cell contents of (I). The N—H···O and N—H···N hydrogen bonds and C—H···O interactions are shown as orange, blue and purple dashed lines, respectively.

Fig. 4.

Fig. 4.

A view in projection down the b axis of the unit-cell contents of (I) highlighting the stacking of layers along the a direction. The N—H···O and N—H···N hydrogen bonds and C—H···O interactions are shown as orange, blue and purple dashed lines, respectively.

Crystal data

C16H12F3N3O2S F(000) = 752
Mr = 367.35 Dx = 1.534 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 3338 reflections
a = 16.2430 (7) Å θ = 2.5–29.3°
b = 4.9461 (2) Å µ = 0.25 mm1
c = 21.2383 (8) Å T = 100 K
β = 111.231 (5)° Prism, colourless
V = 1590.47 (11) Å3 0.40 × 0.10 × 0.05 mm
Z = 4

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector 3560 independent reflections
Radiation source: SuperNova (Mo) X-ray Source 2876 reflections with I > 2σ(I)
mirror Rint = 0.031
Detector resolution: 10.4041 pixels mm-1 θmax = 27.5°, θmin = 2.7°
ω scans h = −16→21
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) k = −6→4
Tmin = 0.735, Tmax = 1.000 l = −27→27
7901 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.113 H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0453P)2 + 1.0489P] where P = (Fo2 + 2Fc2)/3
3560 reflections (Δ/σ)max < 0.001
234 parameters Δρmax = 0.34 e Å3
0 restraints Δρmin = −0.49 e Å3

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
S1 0.38822 (3) 0.81404 (10) 0.32626 (2) 0.01565 (14)
F1 0.90203 (11) 0.1680 (3) 0.69086 (6) 0.0425 (4)
F2 0.94604 (9) −0.1249 (3) 0.63638 (7) 0.0399 (4)
F3 0.81737 (9) −0.1604 (3) 0.64239 (8) 0.0432 (4)
O1 0.37971 (9) 1.0737 (3) 0.35369 (8) 0.0244 (4)
O2 0.38267 (9) 0.7931 (3) 0.25777 (7) 0.0231 (3)
N1 0.74390 (11) 0.3994 (3) 0.49401 (8) 0.0156 (4)
N2 0.75444 (11) 0.2540 (4) 0.55074 (8) 0.0177 (4)
N3 0.31318 (11) 0.6258 (4) 0.33572 (9) 0.0164 (4)
H1 0.3186 (17) 0.461 (6) 0.3280 (12) 0.030 (7)*
H2 0.3050 (15) 0.658 (5) 0.3732 (12) 0.020 (6)*
C1 0.87573 (14) 0.0151 (5) 0.63544 (11) 0.0243 (5)
C2 0.83889 (13) 0.1780 (4) 0.57227 (10) 0.0179 (4)
C3 0.88288 (13) 0.2711 (4) 0.53112 (10) 0.0183 (4)
H3 0.9429 0.2415 0.5367 0.022*
C4 0.82048 (13) 0.4154 (4) 0.48055 (10) 0.0163 (4)
C5 0.82969 (13) 0.5586 (4) 0.42273 (9) 0.0159 (4)
C6 0.89089 (13) 0.4628 (4) 0.39583 (10) 0.0195 (4)
H6 0.9266 0.3111 0.4160 0.023*
C7 0.90027 (14) 0.5854 (5) 0.34033 (10) 0.0225 (5)
H7 0.9422 0.5181 0.3226 0.027*
C8 0.84853 (14) 0.8061 (4) 0.31056 (10) 0.0224 (5)
H8 0.8542 0.8885 0.2719 0.027*
C9 0.78859 (14) 0.9066 (4) 0.33714 (11) 0.0229 (5)
H9 0.7532 1.0587 0.3168 0.027*
C10 0.77983 (14) 0.7863 (4) 0.39346 (10) 0.0201 (4)
H10 0.7397 0.8595 0.4122 0.024*
C11 0.65665 (12) 0.4914 (4) 0.45432 (9) 0.0151 (4)
C12 0.61316 (15) 0.6612 (5) 0.48304 (11) 0.0324 (6)
H12 0.6395 0.7133 0.5291 0.039*
C13 0.52997 (16) 0.7552 (6) 0.44350 (12) 0.0372 (7)
H13 0.4985 0.8704 0.4627 0.045*
C14 0.49304 (12) 0.6820 (4) 0.37671 (10) 0.0157 (4)
C15 0.53662 (14) 0.5093 (4) 0.34853 (10) 0.0207 (5)
H15 0.5103 0.4580 0.3024 0.025*
C16 0.61907 (14) 0.4107 (4) 0.38786 (10) 0.0209 (4)
H16 0.6494 0.2889 0.3692 0.025*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0135 (2) 0.0142 (3) 0.0179 (2) 0.00119 (19) 0.00409 (19) 0.00217 (18)
F1 0.0559 (10) 0.0483 (9) 0.0155 (6) 0.0101 (8) 0.0035 (6) 0.0034 (6)
F2 0.0336 (8) 0.0494 (9) 0.0404 (8) 0.0254 (7) 0.0179 (7) 0.0220 (7)
F3 0.0308 (8) 0.0513 (10) 0.0446 (9) −0.0026 (7) 0.0104 (7) 0.0283 (7)
O1 0.0196 (8) 0.0133 (7) 0.0360 (9) 0.0023 (6) 0.0051 (7) −0.0020 (6)
O2 0.0185 (7) 0.0320 (9) 0.0189 (7) 0.0016 (7) 0.0068 (6) 0.0080 (6)
N1 0.0152 (8) 0.0185 (9) 0.0130 (8) 0.0028 (7) 0.0050 (6) 0.0008 (7)
N2 0.0190 (9) 0.0194 (9) 0.0143 (8) 0.0009 (7) 0.0056 (7) 0.0017 (7)
N3 0.0170 (9) 0.0144 (9) 0.0187 (9) 0.0009 (7) 0.0075 (7) −0.0001 (7)
C1 0.0202 (11) 0.0282 (12) 0.0247 (11) 0.0059 (9) 0.0083 (9) 0.0065 (9)
C2 0.0174 (10) 0.0186 (10) 0.0167 (9) 0.0034 (8) 0.0048 (8) 0.0006 (8)
C3 0.0147 (10) 0.0214 (10) 0.0187 (10) 0.0024 (8) 0.0061 (8) −0.0001 (8)
C4 0.0136 (9) 0.0174 (10) 0.0175 (9) 0.0005 (8) 0.0053 (8) −0.0026 (8)
C5 0.0137 (9) 0.0180 (10) 0.0145 (9) −0.0032 (8) 0.0034 (7) −0.0013 (8)
C6 0.0150 (10) 0.0226 (11) 0.0195 (10) 0.0024 (8) 0.0043 (8) 0.0015 (8)
C7 0.0224 (11) 0.0276 (12) 0.0201 (10) 0.0000 (9) 0.0110 (9) −0.0006 (9)
C8 0.0234 (11) 0.0266 (11) 0.0173 (10) −0.0043 (9) 0.0073 (9) 0.0025 (9)
C9 0.0213 (11) 0.0205 (11) 0.0243 (11) 0.0018 (9) 0.0052 (9) 0.0048 (9)
C10 0.0191 (10) 0.0199 (11) 0.0231 (10) 0.0010 (9) 0.0099 (9) −0.0015 (9)
C11 0.0129 (9) 0.0166 (10) 0.0152 (9) 0.0010 (8) 0.0043 (8) 0.0025 (8)
C12 0.0244 (12) 0.0470 (15) 0.0183 (10) 0.0133 (11) −0.0013 (9) −0.0148 (10)
C13 0.0272 (13) 0.0526 (16) 0.0243 (12) 0.0208 (12) 0.0003 (10) −0.0182 (11)
C14 0.0134 (9) 0.0151 (10) 0.0176 (9) 0.0004 (8) 0.0046 (8) 0.0013 (8)
C15 0.0191 (10) 0.0263 (11) 0.0151 (9) 0.0022 (9) 0.0045 (8) −0.0036 (9)
C16 0.0185 (10) 0.0249 (11) 0.0194 (10) 0.0065 (9) 0.0070 (8) −0.0034 (9)

Geometric parameters (Å, °)

S1—O2 1.4283 (15) C6—C7 1.382 (3)
S1—O1 1.4373 (15) C6—H6 0.9500
S1—N3 1.6033 (18) C7—C8 1.383 (3)
S1—C14 1.7754 (19) C7—H7 0.9500
F1—C1 1.332 (3) C8—C9 1.383 (3)
F2—C1 1.330 (2) C8—H8 0.9500
F3—C1 1.332 (3) C9—C10 1.389 (3)
N1—N2 1.359 (2) C9—H9 0.9500
N1—C4 1.376 (3) C10—H10 0.9500
N1—C11 1.436 (2) C11—C12 1.374 (3)
N2—C2 1.333 (3) C11—C16 1.378 (3)
N3—H1 0.84 (3) C12—C13 1.387 (3)
N3—H2 0.87 (2) C12—H12 0.9500
C1—C2 1.492 (3) C13—C14 1.374 (3)
C2—C3 1.392 (3) C13—H13 0.9500
C3—C4 1.379 (3) C14—C15 1.377 (3)
C3—H3 0.9500 C15—C16 1.385 (3)
C4—C5 1.471 (3) C15—H15 0.9500
C5—C6 1.397 (3) C16—H16 0.9500
C5—C10 1.395 (3)
O2—S1—O1 119.85 (9) C7—C6—H6 119.5
O2—S1—N3 108.36 (9) C5—C6—H6 119.5
O1—S1—N3 106.20 (10) C6—C7—C8 120.0 (2)
O2—S1—C14 106.32 (9) C6—C7—H7 120.0
O1—S1—C14 107.22 (9) C8—C7—H7 120.0
N3—S1—C14 108.50 (9) C9—C8—C7 119.9 (2)
N2—N1—C4 112.43 (16) C9—C8—H8 120.1
N2—N1—C11 117.95 (15) C7—C8—H8 120.1
C4—N1—C11 129.36 (16) C8—C9—C10 120.3 (2)
C2—N2—N1 103.70 (16) C8—C9—H9 119.9
S1—N3—H1 113.6 (18) C10—C9—H9 119.9
S1—N3—H2 112.6 (16) C9—C10—C5 120.4 (2)
H1—N3—H2 115 (2) C9—C10—H10 119.8
F2—C1—F1 106.47 (18) C5—C10—H10 119.8
F2—C1—F3 107.48 (19) C12—C11—C16 121.55 (19)
F1—C1—F3 106.57 (18) C12—C11—N1 119.34 (17)
F2—C1—C2 110.94 (18) C16—C11—N1 119.11 (18)
F1—C1—C2 112.57 (19) C11—C12—C13 118.7 (2)
F3—C1—C2 112.45 (18) C11—C12—H12 120.6
N2—C2—C3 112.93 (18) C13—C12—H12 120.6
N2—C2—C1 119.24 (18) C14—C13—C12 120.1 (2)
C3—C2—C1 127.82 (19) C14—C13—H13 119.9
C4—C3—C2 105.10 (18) C12—C13—H13 119.9
C4—C3—H3 127.5 C13—C14—C15 120.76 (19)
C2—C3—H3 127.5 C13—C14—S1 119.41 (16)
N1—C4—C3 105.85 (17) C15—C14—S1 119.83 (15)
N1—C4—C5 125.03 (17) C14—C15—C16 119.55 (19)
C3—C4—C5 129.12 (18) C14—C15—H15 120.2
C6—C5—C10 118.42 (19) C16—C15—H15 120.2
C6—C5—C4 118.74 (18) C11—C16—C15 119.24 (19)
C10—C5—C4 122.85 (18) C11—C16—H16 120.4
C7—C6—C5 121.0 (2) C15—C16—H16 120.4
C4—N1—N2—C2 −0.4 (2) C6—C7—C8—C9 1.1 (3)
C11—N1—N2—C2 174.33 (17) C7—C8—C9—C10 −0.3 (3)
N1—N2—C2—C3 0.2 (2) C8—C9—C10—C5 −1.7 (3)
N1—N2—C2—C1 179.01 (18) C6—C5—C10—C9 2.7 (3)
F2—C1—C2—N2 156.75 (19) C4—C5—C10—C9 −177.26 (19)
F1—C1—C2—N2 −84.1 (2) N2—N1—C11—C12 60.5 (3)
F3—C1—C2—N2 36.3 (3) C4—N1—C11—C12 −125.9 (2)
F2—C1—C2—C3 −24.6 (3) N2—N1—C11—C16 −120.6 (2)
F1—C1—C2—C3 94.6 (3) C4—N1—C11—C16 53.0 (3)
F3—C1—C2—C3 −145.0 (2) C16—C11—C12—C13 −0.8 (4)
N2—C2—C3—C4 0.1 (2) N1—C11—C12—C13 178.1 (2)
C1—C2—C3—C4 −178.6 (2) C11—C12—C13—C14 −1.0 (4)
N2—N1—C4—C3 0.4 (2) C12—C13—C14—C15 1.8 (4)
C11—N1—C4—C3 −173.52 (19) C12—C13—C14—S1 −177.8 (2)
N2—N1—C4—C5 179.93 (17) O2—S1—C14—C13 158.1 (2)
C11—N1—C4—C5 6.0 (3) O1—S1—C14—C13 28.8 (2)
C2—C3—C4—N1 −0.3 (2) N3—S1—C14—C13 −85.5 (2)
C2—C3—C4—C5 −179.8 (2) O2—S1—C14—C15 −21.5 (2)
N1—C4—C5—C6 −149.8 (2) O1—S1—C14—C15 −150.81 (17)
C3—C4—C5—C6 29.6 (3) N3—S1—C14—C15 94.88 (19)
N1—C4—C5—C10 30.2 (3) C13—C14—C15—C16 −0.7 (3)
C3—C4—C5—C10 −150.4 (2) S1—C14—C15—C16 178.87 (16)
C10—C5—C6—C7 −1.8 (3) C12—C11—C16—C15 1.9 (3)
C4—C5—C6—C7 178.14 (19) N1—C11—C16—C15 −176.98 (18)
C5—C6—C7—C8 −0.1 (3) C14—C15—C16—C11 −1.1 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N3—H1···O1i 0.84 (3) 2.14 (3) 2.911 (2) 153 (2)
N3—H2···N2ii 0.87 (2) 2.21 (3) 3.049 (3) 164 (2)
C9—H9···O2iii 0.95 2.49 3.376 (3) 155
C16—H16···O2iv 0.95 2.55 3.137 (2) 120

Symmetry codes: (i) x, y−1, z; (ii) −x+1, −y+1, −z+1; (iii) −x+1, y+1/2, −z+1/2; (iv) −x+1, y−1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5083).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811033435/hg5083sup1.cif

e-67-o2424-sup1.cif (19.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811033435/hg5083Isup2.hkl

e-67-o2424-Isup2.hkl (174.6KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811033435/hg5083Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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