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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 Aug 1;70(Pt 9):o968–o969. doi: 10.1107/S1600536814017188

Crystal structure of 2-(2-bromo­phen­yl)-4-(1H-indol-3-yl)-6-(thio­phen-2-yl)pyridine-3-carbo­nitrile

R Vishnupriya a, J Suresh a, Shanmugavel Bharkavi b, Subbu Perumal b, P L Nilantha Lakshman c,*
PMCID: PMC4186133  PMID: 25309284

Abstract

In the title compound, C24H14BrN3S, the dihedral angles between the planes of the pyridine ring and the pendant thio­phene ring, the indole ring system (r.m.s. deviation = 0.022 Å) and the bromo­benzene ring are 9.37 (17), 21.90 (12) and 69.01 (15)°, respectively. The approximate coplanarity of the central ring and the indole ring system is supported by two intra­molecular C—H⋯N inter­actions. In the crystal, inversion dimers linked by pairs of N—H⋯N hydrogen bonds generate R 2 2(16) loops and the dimers are linked by C—H⋯π and aromatic π–π stacking [shortest centroid–centroid separation = 3.729 (3) Å] into a three-dimensional network.

Keywords: crystal structure, pyridine-3-carbo­nitrile, hydrogen bonding, π–π stacking

Related literature  

For the biological activity of pyridine-3-carbo­nitrile derivatives, see: Kim et al. (2005); Ji et al. (2007); Brandt et al. (2010); El-Sayed et al. (2011).graphic file with name e-70-0o968-scheme1.jpg

Experimental  

Crystal data  

  • C24H14BrN3S

  • M r = 456.35

  • Monoclinic, Inline graphic

  • a = 10.470 (5) Å

  • b = 21.353 (5) Å

  • c = 9.292 (5) Å

  • β = 107.710 (5)°

  • V = 1978.9 (15) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 2.20 mm−1

  • T = 293 K

  • 0.52 × 0.23 × 0.17 mm

Data collection  

  • Bruker Kappa APEXII diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.958, T max = 0.986

  • 17079 measured reflections

  • 4305 independent reflections

  • 2837 reflections with I > 2σ(I)

  • R int = 0.041

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.046

  • wR(F 2) = 0.121

  • S = 1.02

  • 4305 reflections

  • 262 parameters

  • H-atom parameters constrained

  • Δρmax = 0.48 e Å−3

  • Δρmin = −0.35 e Å−3

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814017188/hb7260sup1.cif

e-70-0o968-sup1.cif (27.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814017188/hb7260Isup2.hkl

e-70-0o968-Isup2.hkl (206.7KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814017188/hb7260Isup3.cml

. DOI: 10.1107/S1600536814017188/hb7260fig1.tif

The mol­ecular structure of compound showing 30% probability displacement ellipsoids.

x y z . DOI: 10.1107/S1600536814017188/hb7260fig2.tif

Partial packing view of the compound showing mol­ecules inter­connected through a C—H⋯π stacking inter­action (dotted lines; symmetry code: (i) Inline graphic − x, Inline graphic + y, Inline graphic − z)

CCDC reference: 1015962

Additional supporting information: crystallographic information; 3D view; checkCIF report

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

Cg1 is the centroid of the benzene ring of the indole moiety.

D—H⋯A D—H H⋯A DA D—H⋯A
C53—H53⋯N1 0.93 2.58 3.069 (4) 114
C58—H58⋯N2 0.93 2.55 3.278 (4) 135
N3—H3⋯N2i 0.86 2.17 3.008 (4) 165
C32—H32⋯Cg1ii 0.93 2.89 3.761 (4) 157

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

Acknowledgments

JS and RV thank the management of the Madura College for their encouragement and support. SP thanks the Department of Science and Technology, New Delhi, for a major research project (SR/S1/OC/-50/2011) and the University Grants Commission, New Delhi, for the award of a BSR Faculty Fellowship

supplementary crystallographic information

S1. Comment

3-Cyanopyridine derivatives have been reported for their wide range of applications such as in antimicrobial, analgesic, anti-hyperglycemic, antiproliferative and antitumor activities (Brandt et al., 2010; El-Sayed et al., 2011; Ji et al., 2007; Kim et al., 2005). As part of our studies in this area, the title compound was investigated.

The deviation of the nitrile atoms (C41,N2) from the mean plane of the pyridine ring system is -0.013 (1) Å and -0.020 (5) Å. The shortening of the C—N distances [1.346 (3) and 1.345 (3) Å] and the opening of the N1–C11–C10 angle [122.83 (2)°] may be attributed to the size of the substituent at C1, correlating well with the values observed in the ortho-substituted derivative.

The crystal structure features a intermolecular N—H···N interaction between inverse related molecules generating a graph set ring motif R22 (16) which are linked into chains through C—H···Cg1 interation (Cg1 is the centroid of the benzene ring of the indole moiety) and by π···π stacking interaction involving adjacent pyridine and pyrrole rings of the symmetry related molecule at (-x, -y, -z), with a centroid-to-centroid distance of 3.729 (3) Å·(Fig 2).

S2. Experimental

A mixture of 3-(1H-indol-3-yl)-3-oxopropanenitrile 1 (1 mmol), 4,4,4-trifluoro-1-(thiophen-2-yl)butane-1,3-dione 2 (1 mmol) and 2-bromo benzaldehyde 3 (1 mmol) in the presence of ammonium acetate (400 mmol) under solvent-free condition was heated at 110 °C for 7 h. After completion of the reaction (TLC), the reaction mixture was poured into water and extracted with dichloromethane. After removal of the solvent, the residue was chromatographed over silica gel (230–400 mesh) using petroleum ether-ethyl acetate mixture (7:3 v/v), which afforded the pure compound. Melting point 282°C, yield: 67%.

S3. Refinement

H atoms were placed at calculated positions and allowed to ride on their carrier atoms with C—H = 0.93–0.98 Å and with Uiso = 1.2Ueq(C, N) for N, CH2 and CH atoms and Uiso = 1.5Ueq(C) for CH3 atoms.

Figures

Fig. 1.

Fig. 1.

The molecular structure of compound showing 30% probability displacement ellipsoids.

Fig. 2.

Fig. 2.

Partial packing view of the compound showing molecules interconnected through a C—H···π stacking interaction (dotted lines; symmetry code: (i) 1/2 - x, 1/2 + y, 1/2 - z)

Crystal data

C24H14BrN3S F(000) = 920
Mr = 456.35 Dx = 1.532 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 2000 reflections
a = 10.470 (5) Å θ = 2–27°
b = 21.353 (5) Å µ = 2.20 mm1
c = 9.292 (5) Å T = 293 K
β = 107.710 (5)° Block, colourless
V = 1978.9 (15) Å3 0.52 × 0.23 × 0.17 mm
Z = 4

Data collection

Bruker Kappa APEXII diffractometer 4305 independent reflections
Radiation source: fine-focus sealed tube 2837 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.041
Detector resolution: 0 pixels mm-1 θmax = 27.0°, θmin = 1.9°
ω and φ scans h = −12→13
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) k = −27→27
Tmin = 0.958, Tmax = 0.986 l = −11→11
17079 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)] = 0.046 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.121 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0618P)2 + 0.4334P] where P = (Fo2 + 2Fc2)/3
4305 reflections (Δ/σ)max < 0.001
262 parameters Δρmax = 0.48 e Å3
0 restraints Δρmin = −0.35 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
C1 0.2640 (3) 0.50193 (12) 0.7417 (3) 0.0386 (7)
C2 0.3077 (3) 0.44165 (13) 0.7289 (3) 0.0425 (7)
H2 0.3543 0.4194 0.8149 0.051*
C3 0.2818 (3) 0.41458 (12) 0.5880 (3) 0.0390 (7)
C4 0.2078 (3) 0.45002 (12) 0.4630 (3) 0.0368 (6)
C5 0.1664 (3) 0.51133 (12) 0.4822 (3) 0.0371 (6)
C11 0.2890 (3) 0.53182 (14) 0.8898 (3) 0.0432 (7)
C12 0.3376 (3) 0.50426 (15) 1.0315 (3) 0.0481 (8)
H12 0.3625 0.4624 1.0484 0.058*
C13 0.3439 (4) 0.54874 (19) 1.1471 (3) 0.0622 (9)
H13 0.3745 0.5393 1.2496 0.075*
C14 0.3011 (4) 0.60608 (18) 1.0930 (4) 0.0651 (10)
H14 0.2995 0.6405 1.1538 0.078*
C31 0.3330 (3) 0.35097 (13) 0.5742 (3) 0.0402 (7)
C32 0.2810 (4) 0.30034 (14) 0.6331 (3) 0.0555 (8)
H32 0.2108 0.3068 0.6733 0.067*
C33 0.3322 (4) 0.24105 (16) 0.6326 (4) 0.0697 (11)
H33 0.2958 0.2078 0.6716 0.084*
C34 0.4351 (5) 0.23060 (17) 0.5759 (4) 0.0736 (11)
H34 0.4695 0.1904 0.5774 0.088*
C35 0.4892 (4) 0.27918 (16) 0.5159 (4) 0.0650 (10)
H35 0.5597 0.2721 0.4766 0.078*
C36 0.4366 (3) 0.33884 (13) 0.5151 (3) 0.0466 (7)
C41 0.1792 (3) 0.42163 (13) 0.3172 (3) 0.0451 (7)
C51 0.0943 (3) 0.55225 (13) 0.3593 (3) 0.0380 (6)
C52 0.0877 (3) 0.61968 (13) 0.3648 (3) 0.0404 (7)
C53 0.1419 (3) 0.66595 (14) 0.4726 (3) 0.0497 (8)
H53 0.1932 0.6550 0.5699 0.060*
C54 0.1186 (4) 0.72736 (15) 0.4329 (4) 0.0614 (9)
H54 0.1561 0.7581 0.5041 0.074*
C55 0.0405 (4) 0.74537 (17) 0.2892 (4) 0.0657 (10)
H55 0.0253 0.7877 0.2669 0.079*
C56 −0.0136 (4) 0.70208 (16) 0.1814 (4) 0.0581 (9)
H56 −0.0650 0.7140 0.0849 0.070*
C57 0.0104 (3) 0.63913 (14) 0.2198 (3) 0.0451 (7)
C58 0.0214 (3) 0.53562 (14) 0.2152 (3) 0.0452 (7)
H58 0.0082 0.4948 0.1791 0.054*
N1 0.1961 (2) 0.53636 (10) 0.6215 (2) 0.0386 (6)
N2 0.1568 (3) 0.39821 (12) 0.2015 (3) 0.0630 (8)
N3 −0.0283 (3) 0.58711 (12) 0.1335 (3) 0.0500 (7)
H3 −0.0773 0.5870 0.0405 0.060*
S 0.25060 (12) 0.60852 (4) 0.90204 (10) 0.0706 (3)
Br 0.51614 (4) 0.404354 (16) 0.43368 (4) 0.06285 (16)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0378 (18) 0.0460 (16) 0.0330 (14) −0.0027 (13) 0.0123 (13) 0.0018 (13)
C2 0.049 (2) 0.0473 (17) 0.0288 (14) 0.0025 (14) 0.0084 (13) 0.0054 (12)
C3 0.0397 (18) 0.0415 (15) 0.0365 (15) −0.0016 (13) 0.0128 (13) 0.0067 (12)
C4 0.0403 (18) 0.0393 (14) 0.0298 (14) −0.0037 (13) 0.0094 (12) 0.0000 (12)
C5 0.0362 (17) 0.0420 (15) 0.0330 (14) −0.0041 (13) 0.0103 (12) 0.0019 (12)
C11 0.0382 (18) 0.0517 (17) 0.0380 (16) −0.0058 (14) 0.0093 (13) −0.0024 (13)
C12 0.054 (2) 0.0600 (18) 0.0271 (14) −0.0014 (15) 0.0083 (14) −0.0045 (14)
C13 0.059 (2) 0.088 (3) 0.0347 (17) −0.005 (2) 0.0078 (16) −0.0043 (17)
C14 0.076 (3) 0.075 (2) 0.0419 (18) −0.001 (2) 0.0139 (18) −0.0232 (17)
C31 0.0467 (19) 0.0402 (15) 0.0285 (14) 0.0000 (13) 0.0038 (13) 0.0009 (12)
C32 0.062 (2) 0.0500 (19) 0.0537 (19) −0.0032 (16) 0.0163 (17) 0.0094 (15)
C33 0.087 (3) 0.0421 (19) 0.071 (2) −0.0048 (19) 0.012 (2) 0.0172 (17)
C34 0.086 (3) 0.046 (2) 0.080 (3) 0.011 (2) 0.013 (2) 0.0019 (18)
C35 0.070 (3) 0.057 (2) 0.066 (2) 0.0158 (18) 0.0176 (19) −0.0031 (18)
C36 0.051 (2) 0.0464 (17) 0.0392 (16) −0.0005 (15) 0.0082 (15) 0.0002 (13)
C41 0.054 (2) 0.0375 (15) 0.0383 (17) 0.0044 (14) 0.0051 (14) 0.0058 (14)
C51 0.0384 (18) 0.0446 (15) 0.0318 (14) −0.0001 (13) 0.0119 (13) 0.0035 (12)
C52 0.0407 (18) 0.0457 (15) 0.0389 (16) 0.0046 (14) 0.0182 (14) 0.0090 (13)
C53 0.056 (2) 0.0463 (17) 0.0477 (18) 0.0001 (15) 0.0179 (16) 0.0005 (14)
C54 0.072 (3) 0.0451 (18) 0.073 (2) −0.0003 (17) 0.031 (2) 0.0008 (17)
C55 0.076 (3) 0.0490 (19) 0.078 (3) 0.0099 (18) 0.032 (2) 0.0204 (19)
C56 0.057 (2) 0.061 (2) 0.058 (2) 0.0113 (18) 0.0199 (17) 0.0262 (18)
C57 0.0436 (19) 0.0540 (18) 0.0409 (16) 0.0052 (15) 0.0177 (14) 0.0119 (14)
C58 0.045 (2) 0.0494 (17) 0.0402 (16) 0.0037 (14) 0.0111 (14) 0.0024 (14)
N1 0.0424 (15) 0.0416 (13) 0.0316 (12) −0.0021 (11) 0.0107 (11) 0.0006 (10)
N2 0.089 (2) 0.0508 (16) 0.0405 (15) 0.0127 (14) 0.0065 (15) −0.0049 (12)
N3 0.0488 (18) 0.0617 (17) 0.0330 (13) 0.0058 (13) 0.0024 (12) 0.0085 (12)
S 0.0982 (9) 0.0602 (5) 0.0497 (5) 0.0089 (5) 0.0167 (5) −0.0073 (4)
Br 0.0616 (3) 0.0661 (3) 0.0687 (3) −0.00767 (17) 0.0314 (2) 0.00167 (16)

Geometric parameters (Å, º)

C1—N1 1.345 (3) C33—H33 0.9300
C1—C2 1.383 (4) C34—C35 1.378 (5)
C1—C11 1.466 (4) C34—H34 0.9300
C2—C3 1.380 (4) C35—C36 1.387 (4)
C2—H2 0.9300 C35—H35 0.9300
C3—C4 1.405 (4) C36—Br 1.899 (3)
C3—C31 1.480 (4) C41—N2 1.143 (4)
C4—C5 1.408 (4) C51—C58 1.371 (4)
C4—C41 1.431 (4) C51—C52 1.443 (4)
C5—N1 1.346 (3) C52—C53 1.399 (4)
C5—C51 1.454 (4) C52—C57 1.407 (4)
C11—C12 1.390 (4) C53—C54 1.364 (4)
C11—S 1.698 (3) C53—H53 0.9300
C12—C13 1.420 (4) C54—C55 1.391 (5)
C12—H12 0.9300 C54—H54 0.9300
C13—C14 1.347 (5) C55—C56 1.354 (5)
C13—H13 0.9300 C55—H55 0.9300
C14—S 1.691 (4) C56—C57 1.394 (4)
C14—H14 0.9300 C56—H56 0.9300
C31—C36 1.381 (4) C57—N3 1.358 (4)
C31—C32 1.395 (4) C58—N3 1.347 (4)
C32—C33 1.376 (5) C58—H58 0.9300
C32—H32 0.9300 N3—H3 0.8600
C33—C34 1.354 (6)
N1—C1—C2 122.8 (2) C35—C34—H34 119.8
N1—C1—C11 116.1 (2) C34—C35—C36 118.8 (4)
C2—C1—C11 121.1 (2) C34—C35—H35 120.6
C3—C2—C1 119.8 (3) C36—C35—H35 120.6
C3—C2—H2 120.1 C31—C36—C35 121.9 (3)
C1—C2—H2 120.1 C31—C36—Br 120.9 (2)
C2—C3—C4 117.3 (3) C35—C36—Br 117.2 (3)
C2—C3—C31 119.7 (2) N2—C41—C4 179.1 (3)
C4—C3—C31 123.1 (2) C58—C51—C52 105.9 (2)
C3—C4—C5 120.6 (2) C58—C51—C5 127.8 (3)
C3—C4—C41 117.3 (2) C52—C51—C5 126.2 (2)
C5—C4—C41 122.0 (2) C53—C52—C57 117.9 (3)
N1—C5—C4 120.1 (2) C53—C52—C51 135.8 (3)
N1—C5—C51 115.4 (2) C57—C52—C51 106.3 (2)
C4—C5—C51 124.5 (2) C54—C53—C52 119.0 (3)
C12—C11—C1 127.9 (3) C54—C53—H53 120.5
C12—C11—S 111.8 (2) C52—C53—H53 120.5
C1—C11—S 120.3 (2) C53—C54—C55 122.0 (3)
C11—C12—C13 110.6 (3) C53—C54—H54 119.0
C11—C12—H12 124.7 C55—C54—H54 119.0
C13—C12—H12 124.7 C56—C55—C54 120.9 (3)
C14—C13—C12 113.1 (3) C56—C55—H55 119.6
C14—C13—H13 123.5 C54—C55—H55 119.6
C12—C13—H13 123.5 C55—C56—C57 117.8 (3)
C13—C14—S 112.5 (3) C55—C56—H56 121.1
C13—C14—H14 123.8 C57—C56—H56 121.1
S—C14—H14 123.8 N3—C57—C56 129.7 (3)
C36—C31—C32 117.3 (3) N3—C57—C52 107.8 (3)
C36—C31—C3 123.8 (3) C56—C57—C52 122.4 (3)
C32—C31—C3 118.8 (3) N3—C58—C51 110.1 (3)
C33—C32—C31 120.8 (3) N3—C58—H58 124.9
C33—C32—H32 119.6 C51—C58—H58 124.9
C31—C32—H32 119.6 C1—N1—C5 119.4 (2)
C34—C33—C32 120.7 (3) C58—N3—C57 109.9 (3)
C34—C33—H33 119.7 C58—N3—H3 125.1
C32—C33—H33 119.7 C57—N3—H3 125.1
C33—C34—C35 120.5 (3) C14—S—C11 92.04 (16)
C33—C34—H34 119.8
N1—C1—C2—C3 0.0 (5) C34—C35—C36—C31 0.8 (5)
C11—C1—C2—C3 179.6 (3) C34—C35—C36—Br 179.2 (3)
C1—C2—C3—C4 −1.7 (4) N1—C5—C51—C58 −161.3 (3)
C1—C2—C3—C31 177.8 (3) C4—C5—C51—C58 20.3 (5)
C2—C3—C4—C5 2.1 (4) N1—C5—C51—C52 20.1 (4)
C31—C3—C4—C5 −177.3 (3) C4—C5—C51—C52 −158.3 (3)
C2—C3—C4—C41 −179.0 (3) C58—C51—C52—C53 −177.4 (3)
C31—C3—C4—C41 1.6 (4) C5—C51—C52—C53 1.5 (5)
C3—C4—C5—N1 −0.8 (4) C58—C51—C52—C57 −0.4 (3)
C41—C4—C5—N1 −179.7 (3) C5—C51—C52—C57 178.4 (3)
C3—C4—C5—C51 177.5 (3) C57—C52—C53—C54 −0.4 (4)
C41—C4—C5—C51 −1.4 (4) C51—C52—C53—C54 176.3 (3)
N1—C1—C11—C12 169.4 (3) C52—C53—C54—C55 1.2 (5)
C2—C1—C11—C12 −10.2 (5) C53—C54—C55—C56 −1.3 (5)
N1—C1—C11—S −7.5 (4) C54—C55—C56—C57 0.7 (5)
C2—C1—C11—S 172.9 (2) C55—C56—C57—N3 −178.0 (3)
C1—C11—C12—C13 −178.3 (3) C55—C56—C57—C52 0.0 (5)
S—C11—C12—C13 −1.2 (4) C53—C52—C57—N3 178.3 (3)
C11—C12—C13—C14 0.5 (4) C51—C52—C57—N3 0.7 (3)
C12—C13—C14—S 0.5 (4) C53—C52—C57—C56 −0.2 (4)
C2—C3—C31—C36 −108.6 (3) C51—C52—C57—C56 −177.8 (3)
C4—C3—C31—C36 70.8 (4) C52—C51—C58—N3 0.1 (3)
C2—C3—C31—C32 66.9 (4) C5—C51—C58—N3 −178.8 (3)
C4—C3—C31—C32 −113.7 (3) C2—C1—N1—C5 1.3 (4)
C36—C31—C32—C33 0.4 (5) C11—C1—N1—C5 −178.3 (2)
C3—C31—C32—C33 −175.3 (3) C4—C5—N1—C1 −0.9 (4)
C31—C32—C33—C34 0.5 (5) C51—C5—N1—C1 −179.3 (2)
C32—C33—C34—C35 −0.8 (6) C51—C58—N3—C57 0.4 (4)
C33—C34—C35—C36 0.2 (6) C56—C57—N3—C58 177.6 (3)
C32—C31—C36—C35 −1.1 (4) C52—C57—N3—C58 −0.6 (4)
C3—C31—C36—C35 174.4 (3) C13—C14—S—C11 −1.0 (3)
C32—C31—C36—Br −179.4 (2) C12—C11—S—C14 1.3 (3)
C3—C31—C36—Br −3.9 (4) C1—C11—S—C14 178.6 (3)

Hydrogen-bond geometry (Å, º)

Cg1 is the centroid of the benzene ring of the indole moiety.

D—H···A D—H H···A D···A D—H···A
C53—H53···N1 0.93 2.58 3.069 (4) 114
C58—H58···N2 0.93 2.55 3.278 (4) 135
N3—H3···N2i 0.86 2.17 3.008 (4) 165
C32—H32···Cg1ii 0.93 2.89 3.761 (4) 157

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

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: HB7260).

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/S1600536814017188/hb7260sup1.cif

e-70-0o968-sup1.cif (27.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814017188/hb7260Isup2.hkl

e-70-0o968-Isup2.hkl (206.7KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814017188/hb7260Isup3.cml

. DOI: 10.1107/S1600536814017188/hb7260fig1.tif

The mol­ecular structure of compound showing 30% probability displacement ellipsoids.

x y z . DOI: 10.1107/S1600536814017188/hb7260fig2.tif

Partial packing view of the compound showing mol­ecules inter­connected through a C—H⋯π stacking inter­action (dotted lines; symmetry code: (i) Inline graphic − x, Inline graphic + y, Inline graphic − z)

CCDC reference: 1015962

Additional supporting information: 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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