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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Feb 13;69(Pt 3):o378–o379. doi: 10.1107/S1600536813003656

Fluconazole–malonic acid (1/1)

Jože Kastelic a, Danijel Kikelj b, Ivan Leban c, Nina Lah c,*
PMCID: PMC3588488  PMID: 23476565

Abstract

Co-crystallizaton of the anti­fungal drug fluconazole [2-(2,4-difluoro­phen­yl)-1,3-bis­(1H-1,2,4-triazol-1-yl)propan-2-ol] with malonic acid in acetonitrile solution resulted in the formation of the title 1:1 co-crystal, C13H12F2N6O·C3H4O4. The geometry around the central fluconazole atom is distorted tetrahedral. The dihedral angles between the triazole rings and the fluorinated phenyl ring are 30.64 (7) and 61.91 (5)°. In the crystal, the basic packing motif may be envisioned as a cyclic aggregate formed of two fluconazole mol­ecules linked by two malonic acid mol­ecules through O—H⋯N and O—H⋯O hydrogen bonds. Such aggregates are further connected into (001) layers by further O—H⋯N hydrogen bonds. The structure also features weak non-classical C—H⋯O and C—H⋯N inter­actions.

Related literature  

For general aspects of pharmaceutical co-crystals, see, for example: Brittain et al. (2012a ,b ). For known fluconazole co-crystals, see: Kastelic et al. (2010, 2011). For regulatory classification of pharmaceutical co-crystals, see: US Food and Drug Administration (2011).graphic file with name e-69-0o378-scheme1.jpg

Experimental  

Crystal data  

  • C13H12F2N6O·C3H4O4

  • M r = 410.35

  • Orthorhombic, Inline graphic

  • a = 14.7196 (2) Å

  • b = 8.4891 (1) Å

  • c = 28.1096 (4) Å

  • V = 3512.47 (8) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.13 mm−1

  • T = 150 K

  • 0.18 × 0.18 × 0.12 mm

Data collection  

  • Nonius Kappa CCD diffractometer

  • 7522 measured reflections

  • 4012 independent reflections

  • 3069 reflections with I > 2σ(I)

  • R int = 0.024

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.100

  • S = 1.03

  • 4012 reflections

  • 274 parameters

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

  • Δρmax = 0.32 e Å−3

  • Δρmin = −0.29 e Å−3

Data collection: COLLECT (Nonius, 1998); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813003656/gk2552sup1.cif

e-69-0o378-sup1.cif (24.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813003656/gk2552Isup2.hkl

e-69-0o378-Isup2.hkl (192.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813003656/gk2552Isup3.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
O1—H1⋯O11M 0.89 (2) 1.94 (2) 2.8057 (14) 166.2 (18)
O12M—H11⋯N14i 0.88 (2) 1.86 (2) 2.6830 (17) 156 (2)
O21M—H12⋯N24ii 0.88 (3) 1.89 (3) 2.7606 (17) 171 (2)
C6—H6⋯N14i 0.93 2.61 3.484 (2) 156
C12M—H12B⋯O11M iii 0.97 2.44 3.3880 (18) 165
C13—H13⋯O12M iv 0.93 2.54 3.3144 (19) 141
C25—H25⋯O11M 0.93 2.40 3.2018 (18) 144
C25—H25⋯O22M iii 0.93 2.37 3.0032 (19) 125

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

Acknowledgments

The financial support of the Slovenian Ministry of Education, Science, Culture and Sport through grant P1–175–103 is gratefully acknowledged. JK thanks ARRS for funding through the Innovative Scheme supported financially by the European Social Fund.

supplementary crystallographic information

Comment

There has been an intense interest in the preparation and characterization of pharmaceutical cocrystals which is evident from the increasing number of research publications on this topic in the past decade (Brittain, 2012a,b and references therein). Pharmaceutical cocrystals present a sub-set of multicomponent crystal solid forms of the active pharmaceutical ingredient (API) with the ability to modulate API's physicochemical properties and to provide intellectual property implications. Until now no cocrystal drug substances have received regulatory approval yet. The relevance of cocrystals in drug formulation research and development has been confirmed with the publication of new U.S. Food and Drug Administration's (FDA) draft guidance for the regulatory classification of pharmaceutical cocrystals in December 2011 (US Food and Drug Administration, 2011).

Fluconazole is a wide spectrum triazole antifungal agent which is only slightly soluble in water. It is a weak base (pKa value of 1.76 for its conjugated acid). Therefore, the formation of a salt as a mean to improve solubility properties, could only be expected with very strong acids. On the other hand, cocrystallization offers possibilities to influence the solubility with numerous coformers. Along these lines, we have focused our research on the preparation of new fluconazole cocrystals. The results of our systematic cocrystallization screening are the cocrystals of fluconazole with three dicarboxylic acids, namely maleic, glutaric and fumaric (Kastelic et al., 2010) and a cocrystal with salicylic acid (Kastelic et al., 2011). As a continuation of our work we present here the crystal structure of a 1:1 cocrystal of fluconazole with malonic acid.

The asymmetric unit consists of one fluconazole and one malonic acid molecule, both in their neutral forms (Fig. 1). Both crystal formers can act as donors and/or acceptors in hydrogen bonding. As expected, the packing arrangement of the two molecules in the crystal is governed by hydrogen-bond interactions. A basic packing motif may be envisioned as a ring in which two fluconazole molecules (related by a two fold axis; symmetry code: +1-x, y, +1.5-z) are bridged by two malonic acid molecules by hydrogen bond interactions including fluconazole OH group as a donor to carboxylic O atom of malonic acid (for hydrgen bond geometry see Table 1). Additionally, the same carboxylic group acts as a donor to one of the triazole N atoms of the fluconazole moiety (Fig. 2). Such rings are further connected into two-dimensional layers through the interaction of the second carboxylic group of malonic acid with another fluconazole triazole nitrogen atom (N24) of the adjacent building unit . The layers are oriented perpendicular to the z axis (Fig. 3). Additionally, the structure is stabilized by non-classical H-bond interactions (for details see Table 1).

The packing in the title compound does not resemble the structures of other known fluconazole cocrystals with carboxylic acids where the formation of zigzag coloumns or sheets were observed. The generation of a flat-layered structure provides the possibilities for the improved mechanical properties relevant to the tablet formulation. Their investigations are underway.

Experimental

Fluconazole was obtained from Krka d.d., Novo mesto, malonic acid was obtained from Merck and both were used without further purification. Equimolar amounts of fluconazole (100 mg, 0.33 mmol) and malonic acid (34.3 mg, 0.33 mmol) were dissolved in 3 ml of acetonitrile by heating at 50°C. The clear solution was slowly cooled to ambient temperature and solvent was then allowed to evaporate to form a transparent film from which crystals grew in 72 h. Crystals suitable for single-crystal X-ray diffraction analysis were prepared by dissolving fluconazole (100.0 mg, 0.33 mmol) and malonic acid (34.3 mg, 0.33 mmol) in 3 ml of acetonitrile by heating at 50°C. Seeds from screening experiment described above were added to clear solution. The mixture was slowly cooled to ambient temperature and allowed to evaporate slowly until the crystals of suitable size and quality appeared.

Refinement

All H atoms were initially found in a Fourier-difference map, but they were repositioned to their calculated positions and were refined using a riding model. Aromatic H atoms were permitted to ride with C—H = 0.93 Å and Ueq(H) = 1.2Uiso(C). H atoms of the CH2 group were constrained with C—H = 0.97 Å and Ueq(H)=1.2Uiso(C). H atoms of hydroxyl groups involved in the formation of hydrogen bonds were freely refined.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title compound, showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.

Fig. 2.

Fig. 2.

Part of the crystal structure showing the formation of a cyclic hydrogen bonded heterotetramer built from two fluconazole and two malonic acid molecules (projection down the b axis). Symmetry code for generation of the tetramer: -x+1, y, -z+1.5.

Fig. 3.

Fig. 3.

Two-dimensional (001) layers viewed down the b axis. The tetrameric buliding units are alternately coloured red and blue to emphasize their linkage. Hydrogen bonds are indicated as dashed lines.

Crystal data

C13H12F2N6O·C3H4O4 Dx = 1.552 Mg m3
Mr = 410.35 Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pbcn Cell parameters from 4524 reflections
a = 14.7196 (2) Å θ = 1.0–27.5°
b = 8.4891 (1) Å µ = 0.13 mm1
c = 28.1096 (4) Å T = 150 K
V = 3512.47 (8) Å3 Hexagonal plates, colourless
Z = 8 0.18 × 0.18 × 0.12 mm
F(000) = 1696

Data collection

Nonius Kappa CCD diffractometer 3069 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.024
Graphite monochromator θmax = 27.5°, θmin = 2.0°
ω–scans at κ=55° h = −19→19
7522 measured reflections k = −11→11
4012 independent reflections l = −36→36

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)] = 0.038 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.100 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0504P)2 + 1.0478P] where P = (Fo2 + 2Fc2)/3
4012 reflections (Δ/σ)max = 0.001
274 parameters Δρmax = 0.32 e Å3
0 restraints Δρmin = −0.29 e Å3

Special details

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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
C1 0.54177 (9) 0.13534 (17) 0.64550 (5) 0.0206 (3)
C2 0.58200 (10) −0.00574 (18) 0.63211 (5) 0.0244 (3)
C3 0.55741 (11) −0.15059 (19) 0.64974 (6) 0.0293 (3)
H3 0.5863 −0.2425 0.6400 0.035*
C4 0.48774 (11) −0.15328 (19) 0.68268 (6) 0.0288 (3)
C5 0.44513 (11) −0.01972 (19) 0.69784 (6) 0.0286 (3)
H5 0.3987 −0.0248 0.7202 0.034*
C6 0.47258 (10) 0.12392 (18) 0.67916 (5) 0.0241 (3)
H6 0.4439 0.2154 0.6894 0.029*
F2 0.65063 (6) −0.00225 (11) 0.59954 (3) 0.0341 (2)
F4 0.46114 (7) −0.29475 (11) 0.70033 (4) 0.0425 (3)
C10 0.57056 (9) 0.29636 (17) 0.62593 (5) 0.0200 (3)
O1 0.51652 (7) 0.41828 (12) 0.64549 (3) 0.0222 (2)
C21 0.56338 (10) 0.29942 (17) 0.57093 (5) 0.0230 (3)
H21A 0.6091 0.2302 0.5575 0.028*
H21B 0.5042 0.2604 0.5614 0.028*
N21 0.57605 (8) 0.45798 (15) 0.55235 (4) 0.0225 (3)
N22 0.65894 (9) 0.51379 (18) 0.53827 (5) 0.0319 (3)
C23 0.64032 (11) 0.6622 (2) 0.52823 (6) 0.0322 (4)
H23 0.6843 0.7322 0.5174 0.039*
N24 0.55240 (8) 0.70550 (15) 0.53487 (4) 0.0262 (3)
C25 0.51475 (10) 0.57304 (18) 0.55025 (5) 0.0233 (3)
H25 0.4539 0.5620 0.5585 0.028*
C11 0.66769 (9) 0.33814 (19) 0.64058 (5) 0.0224 (3)
H11A 0.7095 0.2650 0.6256 0.027*
H11B 0.6820 0.4431 0.6292 0.027*
N11 0.68076 (8) 0.33275 (14) 0.69205 (4) 0.0206 (3)
C15 0.64684 (10) 0.42420 (18) 0.72607 (5) 0.0231 (3)
H15 0.6054 0.5053 0.7212 0.028*
N14 0.68090 (9) 0.38273 (15) 0.76801 (4) 0.0260 (3)
C13 0.73709 (11) 0.26218 (19) 0.75655 (5) 0.0292 (3)
H13 0.7714 0.2088 0.7792 0.035*
N12 0.73963 (9) 0.22619 (15) 0.71109 (4) 0.0288 (3)
O11M 0.34684 (6) 0.39993 (12) 0.60035 (4) 0.0233 (2)
O12M 0.25373 (8) 0.51564 (13) 0.65244 (4) 0.0285 (2)
C11M 0.27804 (9) 0.47413 (16) 0.60930 (5) 0.0195 (3)
C12M 0.21064 (9) 0.52498 (17) 0.57209 (5) 0.0209 (3)
H12A 0.2418 0.5411 0.5421 0.025*
H12B 0.1833 0.6242 0.5815 0.025*
C13M 0.13749 (10) 0.40240 (17) 0.56589 (5) 0.0219 (3)
O21M 0.06834 (7) 0.45375 (13) 0.54002 (4) 0.0286 (3)
O22M 0.14215 (8) 0.27195 (13) 0.58274 (5) 0.0389 (3)
H1 0.4594 (14) 0.409 (2) 0.6360 (7) 0.039 (5)*
H11 0.2895 (15) 0.474 (3) 0.6739 (8) 0.050 (6)*
H12 0.0268 (17) 0.380 (3) 0.5357 (9) 0.068 (8)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0193 (7) 0.0243 (7) 0.0182 (6) 0.0026 (6) −0.0046 (5) −0.0010 (6)
C2 0.0215 (7) 0.0309 (8) 0.0208 (7) 0.0057 (6) −0.0003 (6) −0.0017 (6)
C3 0.0352 (8) 0.0239 (8) 0.0288 (8) 0.0076 (7) −0.0042 (7) −0.0020 (6)
C4 0.0347 (8) 0.0235 (8) 0.0281 (8) −0.0023 (7) −0.0050 (7) 0.0044 (6)
C5 0.0267 (8) 0.0319 (9) 0.0273 (8) −0.0005 (7) 0.0019 (6) 0.0018 (6)
C6 0.0231 (7) 0.0241 (8) 0.0250 (7) 0.0042 (6) −0.0001 (6) −0.0018 (6)
F2 0.0322 (5) 0.0348 (5) 0.0351 (5) 0.0114 (4) 0.0111 (4) 0.0001 (4)
F4 0.0563 (6) 0.0244 (5) 0.0468 (6) −0.0023 (5) 0.0060 (5) 0.0071 (4)
C10 0.0182 (6) 0.0231 (7) 0.0188 (7) 0.0048 (6) −0.0018 (5) −0.0028 (6)
O1 0.0202 (5) 0.0232 (5) 0.0233 (5) 0.0050 (4) −0.0017 (4) −0.0039 (4)
C21 0.0264 (7) 0.0240 (8) 0.0185 (7) 0.0038 (6) −0.0034 (6) −0.0002 (6)
N21 0.0206 (6) 0.0281 (7) 0.0188 (6) 0.0021 (5) −0.0007 (5) 0.0014 (5)
N22 0.0226 (6) 0.0449 (9) 0.0282 (7) 0.0032 (6) 0.0054 (5) 0.0101 (6)
C23 0.0271 (8) 0.0390 (10) 0.0306 (8) −0.0031 (7) 0.0039 (7) 0.0110 (7)
N24 0.0267 (6) 0.0296 (7) 0.0223 (6) 0.0001 (6) 0.0016 (5) 0.0028 (5)
C25 0.0215 (7) 0.0269 (8) 0.0215 (7) 0.0018 (6) −0.0006 (6) 0.0007 (6)
C11 0.0202 (7) 0.0291 (8) 0.0180 (7) 0.0003 (6) 0.0002 (5) 0.0014 (6)
N11 0.0186 (5) 0.0232 (6) 0.0201 (6) −0.0005 (5) −0.0033 (5) 0.0020 (5)
C15 0.0226 (7) 0.0237 (8) 0.0230 (7) −0.0001 (6) −0.0024 (6) 0.0001 (6)
N14 0.0293 (7) 0.0272 (7) 0.0214 (6) −0.0056 (5) −0.0025 (5) 0.0015 (5)
C13 0.0334 (8) 0.0286 (8) 0.0255 (8) 0.0013 (7) −0.0073 (6) 0.0054 (6)
N12 0.0309 (7) 0.0297 (7) 0.0260 (6) 0.0079 (6) −0.0067 (5) 0.0028 (5)
O11M 0.0208 (5) 0.0226 (5) 0.0265 (5) 0.0019 (4) −0.0007 (4) −0.0007 (4)
O12M 0.0301 (5) 0.0361 (6) 0.0193 (5) 0.0079 (5) −0.0008 (5) −0.0002 (5)
C11M 0.0203 (7) 0.0157 (7) 0.0227 (7) −0.0030 (6) 0.0015 (5) 0.0008 (5)
C12M 0.0217 (7) 0.0199 (7) 0.0211 (7) 0.0010 (6) −0.0001 (5) 0.0018 (5)
C13M 0.0214 (7) 0.0213 (8) 0.0229 (7) 0.0025 (6) −0.0023 (6) −0.0019 (6)
O21M 0.0254 (6) 0.0267 (6) 0.0338 (6) −0.0024 (5) −0.0108 (5) 0.0061 (5)
O22M 0.0306 (6) 0.0216 (6) 0.0646 (8) −0.0022 (5) −0.0169 (6) 0.0094 (6)

Geometric parameters (Å, º)

C1—C2 1.388 (2) C23—H23 0.9300
C1—C6 1.394 (2) N24—C25 1.326 (2)
C1—C10 1.533 (2) C25—H25 0.9300
C2—F2 1.3637 (17) C11—N11 1.4601 (17)
C2—C3 1.374 (2) C11—H11A 0.9700
C3—C4 1.382 (2) C11—H11B 0.9700
C3—H3 0.9300 N11—C15 1.3292 (19)
C4—F4 1.3570 (18) N11—N12 1.3623 (17)
C4—C5 1.364 (2) C15—N14 1.3285 (18)
C5—C6 1.388 (2) C15—H15 0.9300
C5—H5 0.9300 N14—C13 1.355 (2)
C6—H6 0.9300 C13—N12 1.314 (2)
C10—O1 1.4163 (16) C13—H13 0.9300
C10—C11 1.5296 (19) O11M—C11M 1.2190 (17)
C10—C21 1.5497 (18) O12M—C11M 1.3126 (17)
O1—H1 0.89 (2) O12M—H11 0.88 (2)
C21—N21 1.4558 (19) C11M—C12M 1.505 (2)
C21—H21A 0.9700 C12M—C13M 1.507 (2)
C21—H21B 0.9700 C12M—H12A 0.9700
N21—C25 1.3311 (19) C12M—H12B 0.9700
N21—N22 1.3674 (18) C13M—O22M 1.2063 (18)
N22—C23 1.320 (2) C13M—O21M 1.3247 (17)
C23—N24 1.358 (2) O21M—H12 0.88 (3)
C2—C1—C6 115.84 (14) N24—C23—H23 122.4
C2—C1—C10 123.64 (12) C25—N24—C23 102.34 (13)
C6—C1—C10 120.51 (13) N24—C25—N21 110.69 (13)
F2—C2—C3 117.17 (13) N24—C25—H25 124.7
F2—C2—C1 118.65 (13) N21—C25—H25 124.7
C3—C2—C1 124.18 (14) N11—C11—C10 112.50 (11)
C2—C3—C4 116.86 (14) N11—C11—H11A 109.1
C2—C3—H3 121.6 C10—C11—H11A 109.1
C4—C3—H3 121.6 N11—C11—H11B 109.1
F4—C4—C5 119.27 (14) C10—C11—H11B 109.1
F4—C4—C3 118.27 (14) H11A—C11—H11B 107.8
C5—C4—C3 122.46 (15) C15—N11—N12 110.12 (12)
C4—C5—C6 118.58 (14) C15—N11—C11 130.18 (12)
C4—C5—H5 120.7 N12—N11—C11 119.60 (11)
C6—C5—H5 120.7 N14—C15—N11 109.99 (13)
C5—C6—C1 122.06 (14) N14—C15—H15 125.0
C5—C6—H6 119.0 N11—C15—H15 125.0
C1—C6—H6 119.0 C15—N14—C13 102.69 (12)
O1—C10—C11 104.54 (11) N12—C13—N14 115.10 (13)
O1—C10—C1 110.91 (11) N12—C13—H13 122.5
C11—C10—C1 111.62 (11) N14—C13—H13 122.5
O1—C10—C21 109.67 (11) C13—N12—N11 102.10 (12)
C11—C10—C21 109.17 (11) C11M—O12M—H11 111.3 (14)
C1—C10—C21 110.74 (11) O11M—C11M—O12M 123.77 (13)
C10—O1—H1 110.4 (13) O11M—C11M—C12M 123.54 (13)
N21—C21—C10 111.39 (11) O12M—C11M—C12M 112.67 (12)
N21—C21—H21A 109.3 C11M—C12M—C13M 110.69 (12)
C10—C21—H21A 109.3 C11M—C12M—H12A 109.5
N21—C21—H21B 109.3 C13M—C12M—H12A 109.5
C10—C21—H21B 109.3 C11M—C12M—H12B 109.5
H21A—C21—H21B 108.0 C13M—C12M—H12B 109.5
C25—N21—N22 109.74 (13) H12A—C12M—H12B 108.1
C25—N21—C21 127.41 (13) O22M—C13M—O21M 124.14 (14)
N22—N21—C21 122.58 (12) O22M—C13M—C12M 123.20 (13)
C23—N22—N21 101.97 (12) O21M—C13M—C12M 112.65 (12)
N22—C23—N24 115.26 (14) C13M—O21M—H12 112.1 (16)
N22—C23—H23 122.4

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O1—H1···O11M 0.89 (2) 1.94 (2) 2.8057 (14) 166.2 (18)
O12M—H11···N14i 0.88 (2) 1.86 (2) 2.6830 (17) 156 (2)
O21M—H12···N24ii 0.88 (3) 1.89 (3) 2.7606 (17) 171 (2)
C6—H6···N14i 0.93 2.61 3.484 (2) 156
C12M—H12B···O11Miii 0.97 2.44 3.3880 (18) 165
C13—H13···O12Miv 0.93 2.54 3.3144 (19) 141
C25—H25···O11M 0.93 2.40 3.2018 (18) 144
C25—H25···O22Miii 0.93 2.37 3.0032 (19) 125

Symmetry codes: (i) −x+1, y, −z+3/2; (ii) −x+1/2, y−1/2, z; (iii) −x+1/2, y+1/2, z; (iv) x+1/2, y−1/2, −z+3/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: GK2552).

References

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  2. Brittain, H. G. (2012b). Cryst. Growth Des. 12, 5823–5832.
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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/S1600536813003656/gk2552sup1.cif

e-69-0o378-sup1.cif (24.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813003656/gk2552Isup2.hkl

e-69-0o378-Isup2.hkl (192.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813003656/gk2552Isup3.cml

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


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