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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 23;68(Pt 6):o1863. doi: 10.1107/S1600536812022192

Ethyl 2-(4-chloro­phen­yl)-1-phenyl-1H-benzimidazole-5-carboxyl­ate

Yeong Keng Yoon a, Elumalai Manogaran b, Tan Soo Choon a, Suhana Arshad c, Ibrahim Abdul Razak c,*,
PMCID: PMC3379429  PMID: 22719627

Abstract

In the title compound, C22H17ClN2O2, the essentially planar benzimidazole ring system [maximum deviation = 0.012 (2) Å] forms dihedral angles of 28.69 (6) and 63.65 (7)°, respectively, with the phenyl and chloro-substituted benzene rings. The dihedral angle between the phenyl and benzene rings is 64.23 (8)°. In the crystal, mol­ecules are linked into a zigzag chain along the a axis by inter­molecular C—H⋯O hydrogen bonds. C—H⋯π inter­actions are also present.

Related literature  

For applications of benzimidazoles, see: Tanious et al. (2004); Townsend & Revankar (1970). For related structures, see: Yoon et al. (2011, 2012); Kassim et al. (2012). For stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).graphic file with name e-68-o1863-scheme1.jpg

Experimental  

Crystal data  

  • C22H17ClN2O2

  • M r = 376.83

  • Triclinic, Inline graphic

  • a = 9.3357 (2) Å

  • b = 9.7982 (2) Å

  • c = 11.7718 (4) Å

  • α = 107.502 (2)°

  • β = 102.106 (2)°

  • γ = 109.539 (1)°

  • V = 908.31 (4) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.23 mm−1

  • T = 100 K

  • 0.38 × 0.29 × 0.24 mm

Data collection  

  • Bruker SMART APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2009) T min = 0.917, T max = 0.946

  • 18472 measured reflections

  • 5326 independent reflections

  • 4233 reflections with I > 2σ(I)

  • R int = 0.033

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.048

  • wR(F 2) = 0.127

  • S = 1.04

  • 5326 reflections

  • 245 parameters

  • H-atom parameters constrained

  • Δρmax = 0.57 e Å−3

  • Δρmin = −0.31 e Å−3

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812022192/is5137sup1.cif

e-68-o1863-sup1.cif (27.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812022192/is5137Isup2.hkl

e-68-o1863-Isup2.hkl (260.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812022192/is5137Isup3.cml

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

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

Cg1, Cg2 and Cg3 are the centroids of the N1/C7/N2/C1/C6, C1–C6 and C8–C13 rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
C15—H15A⋯O2i 0.95 2.39 3.324 (2) 166
C21—H21ACg1ii 0.99 2.63 3.5183 (16) 149
C12—H12ACg2iii 0.95 2.96 3.5940 (16) 125
C19—H19ACg3iii 0.95 2.60 3.4770 (18) 153

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

Acknowledgments

The authors thank the Malaysian Government and Universiti Sains Malaysia (USM) for the Research University Grant Nos.1001/PFIZIK/811151 and 1001/PSK/8620012. The authors also wish to express their thanks to the Pharmacogenetic and Novel Therapeutic Research, Institute for Research in Mol­ecular Medicine, Universiti Sains Malaysia. SA also thanks the Malaysian Government and USM for an Academic Staff Training Scheme (ASTS) fellowship.

supplementary crystallographic information

Comment

Substituted benzimidazoles are proven important drug leads. Substituted benzimidazole is the key building block for numerous compounds which plays crucial roles in the function of biologically important molecules (Tanious et al., 2004). In particular, 2-substituted benzimidazoles are recognized as potential anticancer agents (Townsend & Revankar, 1970). As part of our ongoing structural studies of benzimidazole derivatives (Yoon et al., 2011), we now report the structure of the title compound.

In the molecular structure (Fig. 1), The benzimidazole ring system (N1/N2/C1—C7) is essentially planar with a maximum deviation of 0.012 (2) Å at atom C1 and forms dihedral angles of 28.69 (6) and 63.65 (7)°, respectively, with the phenyl (C8–C13) and chloro-substituted benzene (C14–C19) ring. The dihedral angle between the phenyl ring and the chloro-substituted benzene ring is 64.23 (8)°. Bond lengths and angles are within normal ranges and are comparable to related structures (Yoon et al., 2011; Kassim et al., 2012; Yoon et al., 2012).

The crystal packing is shown in Fig. 2. The molecules are linked into a zigzag chain along the a-axis via intermolecular C15—H15A···O2 (Table 1) hydrogen bonds. The crystal structure is further stabilized by intermolecular C21—H21A···Cg1, C1—H12A···Cg2 and C19—H19A···Cg3 (Table 1) interactions (Cg1, Cg2 and Cg3 are the centroids of N1/N2/C1/C6/C7, C1–C6 and C8–C13 rings, respectively).

Experimental

Ethyl 3-amino-4-(phenyl amino) benzoate (0.84 mmol) and sodium metabisulfite adduct of chlorobenzaldehyde (1.68 mmol) were dissolved in DMF. The reaction mixture was reflux at 130 °C for 2 h. After completion, the reaction mixture was diluted in ethyl acetate (20 ml) and washed with water (20 ml). The organic layer was collected, dried over Na2SO4 and the evaporated in-vacuo to yield the product. The product was recrystallized from ethyl acetate.

Refinement

All H atoms were positioned geometrically (C—H = 0.95–0.99 Å) and refined using a riding model with Uiso(H) = 1.2 and 1.5Ueq(C). A rotating group model was applied to the methyl group.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, showing 50% probability displacement ellipsoids and the atom-numbering scheme.

Fig. 2.

Fig. 2.

A crystal packing diagram of the title compound viewed along the b axis. The H atoms not involved in the intermolecular interactions (dashed lines) have been omitted for clarity.

Crystal data

C22H17ClN2O2 Z = 2
Mr = 376.83 F(000) = 392
Triclinic, P1 Dx = 1.378 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.3357 (2) Å Cell parameters from 7225 reflections
b = 9.7982 (2) Å θ = 2.6–30.2°
c = 11.7718 (4) Å µ = 0.23 mm1
α = 107.502 (2)° T = 100 K
β = 102.106 (2)° Block, colourless
γ = 109.539 (1)° 0.38 × 0.29 × 0.24 mm
V = 908.31 (4) Å3

Data collection

Bruker SMART APEXII CCD area-detector diffractometer 5326 independent reflections
Radiation source: fine-focus sealed tube 4233 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.033
φ and ω scans θmax = 30.2°, θmin = 1.9°
Absorption correction: multi-scan (SADABS; Bruker, 2009) h = −13→13
Tmin = 0.917, Tmax = 0.946 k = −13→13
18472 measured reflections l = −14→16

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)] = 0.048 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.127 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0648P)2 + 0.3753P] where P = (Fo2 + 2Fc2)/3
5326 reflections (Δ/σ)max < 0.001
245 parameters Δρmax = 0.57 e Å3
0 restraints Δρmin = −0.31 e Å3

Special details

Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K.
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
Cl1 −0.66895 (5) −0.31206 (5) −0.07003 (4) 0.02705 (11)
O1 0.66316 (12) −0.10624 (12) 0.40052 (10) 0.0196 (2)
O2 0.84606 (13) 0.14573 (13) 0.46871 (11) 0.0229 (2)
N1 0.11793 (15) −0.10887 (14) 0.20878 (12) 0.0173 (2)
N2 0.16095 (14) 0.14100 (14) 0.23348 (12) 0.0158 (2)
C1 0.31182 (17) 0.14553 (17) 0.28366 (14) 0.0165 (3)
C2 0.46660 (18) 0.26942 (17) 0.34187 (14) 0.0190 (3)
H2A 0.4848 0.3744 0.3520 0.023*
C3 0.59248 (18) 0.23218 (18) 0.38427 (15) 0.0201 (3)
H3A 0.6997 0.3136 0.4249 0.024*
C4 0.56507 (17) 0.07571 (17) 0.36849 (14) 0.0179 (3)
C5 0.41041 (18) −0.04706 (17) 0.31022 (14) 0.0180 (3)
H5A 0.3924 −0.1521 0.2997 0.022*
C6 0.28203 (17) −0.01073 (17) 0.26755 (13) 0.0165 (3)
C7 0.04967 (17) −0.01571 (16) 0.19011 (13) 0.0159 (3)
C8 −0.12637 (17) −0.07740 (17) 0.12872 (13) 0.0158 (3)
C9 −0.22379 (18) −0.21369 (17) 0.13982 (14) 0.0178 (3)
H9A −0.1746 −0.2585 0.1881 0.021*
C10 −0.39041 (19) −0.28384 (18) 0.08158 (14) 0.0199 (3)
H10A −0.4559 −0.3739 0.0919 0.024*
C11 −0.46027 (18) −0.21990 (18) 0.00743 (14) 0.0192 (3)
C12 −0.36672 (18) −0.08703 (18) −0.00704 (14) 0.0186 (3)
H12A −0.4161 −0.0458 −0.0588 0.022*
C13 −0.19981 (18) −0.01465 (17) 0.05489 (13) 0.0171 (3)
H13A −0.1354 0.0779 0.0470 0.021*
C14 0.13273 (17) 0.27784 (17) 0.23909 (13) 0.0163 (3)
C15 0.04178 (18) 0.32176 (18) 0.31023 (14) 0.0188 (3)
H15A −0.0040 0.2607 0.3534 0.023*
C16 0.01898 (19) 0.45680 (19) 0.31695 (15) 0.0223 (3)
H16A −0.0417 0.4888 0.3661 0.027*
C17 0.0840 (2) 0.54544 (18) 0.25259 (16) 0.0242 (3)
H17A 0.0675 0.6374 0.2577 0.029*
C18 0.1728 (2) 0.49899 (19) 0.18094 (16) 0.0246 (3)
H18A 0.2161 0.5586 0.1360 0.029*
C19 0.19904 (19) 0.36522 (18) 0.17450 (14) 0.0204 (3)
H19A 0.2614 0.3343 0.1266 0.024*
C20 0.70739 (18) 0.04619 (17) 0.41852 (14) 0.0171 (3)
C21 0.79321 (18) −0.14740 (18) 0.44432 (14) 0.0188 (3)
H21A 0.8447 −0.0928 0.5378 0.023*
H21B 0.8767 −0.1165 0.4056 0.023*
C22 0.7175 (2) −0.32370 (19) 0.40427 (16) 0.0254 (3)
H22A 0.8013 −0.3578 0.4317 0.038*
H22B 0.6667 −0.3759 0.3117 0.038*
H22C 0.6354 −0.3523 0.4433 0.038*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.01444 (18) 0.0278 (2) 0.0327 (2) 0.00672 (15) 0.00290 (15) 0.01040 (16)
O1 0.0137 (5) 0.0191 (5) 0.0244 (5) 0.0072 (4) 0.0042 (4) 0.0082 (4)
O2 0.0151 (5) 0.0228 (5) 0.0280 (6) 0.0061 (5) 0.0055 (4) 0.0100 (5)
N1 0.0149 (6) 0.0164 (6) 0.0196 (6) 0.0061 (5) 0.0041 (5) 0.0077 (5)
N2 0.0141 (6) 0.0151 (5) 0.0192 (6) 0.0060 (5) 0.0063 (5) 0.0079 (5)
C1 0.0151 (6) 0.0175 (6) 0.0181 (6) 0.0073 (6) 0.0064 (5) 0.0081 (5)
C2 0.0180 (7) 0.0154 (6) 0.0228 (7) 0.0060 (6) 0.0073 (6) 0.0078 (6)
C3 0.0152 (7) 0.0189 (7) 0.0237 (7) 0.0049 (6) 0.0067 (6) 0.0082 (6)
C4 0.0152 (7) 0.0201 (7) 0.0187 (7) 0.0073 (6) 0.0056 (5) 0.0084 (6)
C5 0.0169 (7) 0.0170 (6) 0.0206 (7) 0.0074 (6) 0.0064 (6) 0.0080 (5)
C6 0.0155 (6) 0.0163 (6) 0.0173 (6) 0.0062 (6) 0.0059 (5) 0.0067 (5)
C7 0.0163 (6) 0.0150 (6) 0.0156 (6) 0.0057 (6) 0.0053 (5) 0.0064 (5)
C8 0.0144 (6) 0.0159 (6) 0.0152 (6) 0.0062 (5) 0.0042 (5) 0.0045 (5)
C9 0.0177 (7) 0.0179 (6) 0.0172 (6) 0.0069 (6) 0.0057 (5) 0.0073 (5)
C10 0.0190 (7) 0.0202 (7) 0.0194 (7) 0.0066 (6) 0.0076 (6) 0.0080 (6)
C11 0.0140 (6) 0.0224 (7) 0.0180 (7) 0.0076 (6) 0.0047 (5) 0.0048 (6)
C12 0.0182 (7) 0.0217 (7) 0.0177 (7) 0.0114 (6) 0.0058 (5) 0.0071 (5)
C13 0.0183 (7) 0.0170 (6) 0.0176 (7) 0.0082 (6) 0.0072 (5) 0.0075 (5)
C14 0.0161 (6) 0.0151 (6) 0.0169 (6) 0.0065 (6) 0.0040 (5) 0.0066 (5)
C15 0.0172 (7) 0.0196 (7) 0.0190 (7) 0.0074 (6) 0.0058 (6) 0.0076 (6)
C16 0.0189 (7) 0.0221 (7) 0.0254 (8) 0.0111 (6) 0.0068 (6) 0.0067 (6)
C17 0.0225 (8) 0.0173 (7) 0.0295 (8) 0.0094 (6) 0.0027 (6) 0.0086 (6)
C18 0.0305 (8) 0.0183 (7) 0.0253 (8) 0.0089 (7) 0.0084 (7) 0.0119 (6)
C19 0.0240 (8) 0.0191 (7) 0.0202 (7) 0.0092 (6) 0.0099 (6) 0.0090 (6)
C20 0.0154 (6) 0.0198 (7) 0.0181 (7) 0.0078 (6) 0.0081 (5) 0.0083 (5)
C21 0.0154 (7) 0.0219 (7) 0.0198 (7) 0.0097 (6) 0.0049 (5) 0.0081 (6)
C22 0.0282 (8) 0.0247 (8) 0.0256 (8) 0.0139 (7) 0.0083 (7) 0.0110 (6)

Geometric parameters (Å, º)

Cl1—C11 1.7393 (15) C10—C11 1.394 (2)
O1—C20 1.3440 (17) C10—H10A 0.9500
O1—C21 1.4466 (17) C11—C12 1.386 (2)
O2—C20 1.2101 (18) C12—C13 1.391 (2)
N1—C7 1.3186 (18) C12—H12A 0.9500
N1—C6 1.3858 (19) C13—H13A 0.9500
N2—C1 1.3885 (17) C14—C19 1.389 (2)
N2—C7 1.3916 (18) C14—C15 1.390 (2)
N2—C14 1.4359 (17) C15—C16 1.391 (2)
C1—C2 1.394 (2) C15—H15A 0.9500
C1—C6 1.4057 (19) C16—C17 1.390 (2)
C2—C3 1.383 (2) C16—H16A 0.9500
C2—H2A 0.9500 C17—C18 1.386 (2)
C3—C4 1.413 (2) C17—H17A 0.9500
C3—H3A 0.9500 C18—C19 1.395 (2)
C4—C5 1.389 (2) C18—H18A 0.9500
C4—C20 1.4923 (19) C19—H19A 0.9500
C5—C6 1.3985 (19) C21—C22 1.503 (2)
C5—H5A 0.9500 C21—H21A 0.9900
C7—C8 1.471 (2) C21—H21B 0.9900
C8—C13 1.3990 (19) C22—H22A 0.9800
C8—C9 1.403 (2) C22—H22B 0.9800
C9—C10 1.384 (2) C22—H22C 0.9800
C9—H9A 0.9500
C20—O1—C21 115.83 (11) C11—C12—H12A 120.3
C7—N1—C6 105.12 (12) C13—C12—H12A 120.3
C1—N2—C7 106.08 (11) C12—C13—C8 120.38 (14)
C1—N2—C14 124.39 (12) C12—C13—H13A 119.8
C7—N2—C14 129.30 (12) C8—C13—H13A 119.8
N2—C1—C2 131.98 (13) C19—C14—C15 121.23 (13)
N2—C1—C6 105.41 (12) C19—C14—N2 119.15 (13)
C2—C1—C6 122.60 (13) C15—C14—N2 119.61 (13)
C3—C2—C1 116.80 (13) C14—C15—C16 118.77 (14)
C3—C2—H2A 121.6 C14—C15—H15A 120.6
C1—C2—H2A 121.6 C16—C15—H15A 120.6
C2—C3—C4 121.44 (14) C17—C16—C15 120.81 (14)
C2—C3—H3A 119.3 C17—C16—H16A 119.6
C4—C3—H3A 119.3 C15—C16—H16A 119.6
C5—C4—C3 121.36 (13) C18—C17—C16 119.67 (14)
C5—C4—C20 120.65 (13) C18—C17—H17A 120.2
C3—C4—C20 117.98 (13) C16—C17—H17A 120.2
C4—C5—C6 117.73 (13) C17—C18—C19 120.38 (15)
C4—C5—H5A 121.1 C17—C18—H18A 119.8
C6—C5—H5A 121.1 C19—C18—H18A 119.8
N1—C6—C5 129.46 (13) C14—C19—C18 119.13 (14)
N1—C6—C1 110.46 (12) C14—C19—H19A 120.4
C5—C6—C1 120.07 (13) C18—C19—H19A 120.4
N1—C7—N2 112.93 (12) O2—C20—O1 123.55 (13)
N1—C7—C8 121.50 (13) O2—C20—C4 124.85 (13)
N2—C7—C8 125.57 (12) O1—C20—C4 111.60 (12)
C13—C8—C9 118.95 (13) O1—C21—C22 106.27 (12)
C13—C8—C7 124.14 (13) O1—C21—H21A 110.5
C9—C8—C7 116.79 (12) C22—C21—H21A 110.5
C10—C9—C8 121.07 (13) O1—C21—H21B 110.5
C10—C9—H9A 119.5 C22—C21—H21B 110.5
C8—C9—H9A 119.5 H21A—C21—H21B 108.7
C9—C10—C11 118.76 (14) C21—C22—H22A 109.5
C9—C10—H10A 120.6 C21—C22—H22B 109.5
C11—C10—H10A 120.6 H22A—C22—H22B 109.5
C12—C11—C10 121.37 (14) C21—C22—H22C 109.5
C12—C11—Cl1 119.89 (11) H22A—C22—H22C 109.5
C10—C11—Cl1 118.73 (12) H22B—C22—H22C 109.5
C11—C12—C13 119.42 (13)
C7—N2—C1—C2 −178.88 (15) C13—C8—C9—C10 −1.5 (2)
C14—N2—C1—C2 −4.0 (2) C7—C8—C9—C10 −177.72 (13)
C7—N2—C1—C6 −0.11 (15) C8—C9—C10—C11 2.2 (2)
C14—N2—C1—C6 174.80 (13) C9—C10—C11—C12 −1.1 (2)
N2—C1—C2—C3 178.50 (15) C9—C10—C11—Cl1 177.86 (11)
C6—C1—C2—C3 −0.1 (2) C10—C11—C12—C13 −0.8 (2)
C1—C2—C3—C4 0.3 (2) Cl1—C11—C12—C13 −179.71 (11)
C2—C3—C4—C5 −0.3 (2) C11—C12—C13—C8 1.5 (2)
C2—C3—C4—C20 −179.22 (14) C9—C8—C13—C12 −0.4 (2)
C3—C4—C5—C6 −0.1 (2) C7—C8—C13—C12 175.52 (13)
C20—C4—C5—C6 178.85 (13) C1—N2—C14—C19 65.11 (19)
C7—N1—C6—C5 179.06 (15) C7—N2—C14—C19 −121.21 (16)
C7—N1—C6—C1 −0.26 (16) C1—N2—C14—C15 −114.00 (16)
C4—C5—C6—N1 −178.95 (14) C7—N2—C14—C15 59.7 (2)
C4—C5—C6—C1 0.3 (2) C19—C14—C15—C16 −0.6 (2)
N2—C1—C6—N1 0.23 (16) N2—C14—C15—C16 178.49 (13)
C2—C1—C6—N1 179.15 (13) C14—C15—C16—C17 0.8 (2)
N2—C1—C6—C5 −179.16 (13) C15—C16—C17—C18 −0.1 (2)
C2—C1—C6—C5 −0.2 (2) C16—C17—C18—C19 −0.8 (2)
C6—N1—C7—N2 0.19 (16) C15—C14—C19—C18 −0.3 (2)
C6—N1—C7—C8 179.89 (13) N2—C14—C19—C18 −179.41 (14)
C1—N2—C7—N1 −0.05 (16) C17—C18—C19—C14 1.0 (2)
C14—N2—C7—N1 −174.62 (13) C21—O1—C20—O2 −0.5 (2)
C1—N2—C7—C8 −179.73 (13) C21—O1—C20—C4 179.16 (12)
C14—N2—C7—C8 5.7 (2) C5—C4—C20—O2 178.84 (15)
N1—C7—C8—C13 −149.37 (15) C3—C4—C20—O2 −2.2 (2)
N2—C7—C8—C13 30.3 (2) C5—C4—C20—O1 −0.83 (19)
N1—C7—C8—C9 26.6 (2) C3—C4—C20—O1 178.10 (13)
N2—C7—C8—C9 −153.74 (14) C20—O1—C21—C22 −175.16 (12)

Hydrogen-bond geometry (Å, º)

Cg1, Cg2 and Cg3 are the centroids of the N1/C7/N2/C1/C6, C1–C6 and C8–C13 rings, respectively.

D—H···A D—H H···A D···A D—H···A
C15—H15A···O2i 0.95 2.39 3.324 (2) 166
C21—H21A···Cg1ii 0.99 2.63 3.5183 (16) 149
C12—H12A···Cg2iii 0.95 2.96 3.5940 (16) 125
C19—H19A···Cg3iii 0.95 2.60 3.4770 (18) 153

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS5137).

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/S1600536812022192/is5137sup1.cif

e-68-o1863-sup1.cif (27.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812022192/is5137Isup2.hkl

e-68-o1863-Isup2.hkl (260.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812022192/is5137Isup3.cml

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


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