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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2015 Jan 10;71(Pt 2):o90–o91. doi: 10.1107/S2056989014027790

Crystal structure of 3-[2-(4-methyl­phen­yl)ethyn­yl]-2H-chromen-2-one

Ignez Caracelli a,*, Stella H Maganhi a, Hélio A Stefani b, Karina Gueogjian b, Edward R T Tiekink c
PMCID: PMC4384545  PMID: 25878887

Abstract

The coumarin ring system in the title asymmetric alkyne, C18H12O2, is approximately planar (r.m.s. deviation of the 11 non-H atoms = 0.048 Å), and is inclined with respect to the methyl­benzene ring, forming a dihedral angle of 33.68 (4)°. In the crystal, supra­molecular zigzag chains along the c-axis direction are formed via weak C—H⋯O hydrogen bonds, and these are connected into double layers via weak C—H⋯π inter­actions; these stack along the a axis.

Keywords: crystal structure, coumarins, asymmetric alkyne, hydrogen bonding, C—H⋯π inter­actions

Related literature  

For the biological activity of coumarins, see: Wu et al. (2009). For background to previous work on coumarins, see: Stefani et al. (2012). For a related structure, see: Elangovan et al. (2004). For synthetic details, see: Gueogjian (2011).graphic file with name e-71-00o90-scheme1.jpg

Experimental  

Crystal data  

  • C18H12O2

  • M r = 260.28

  • Monoclinic, Inline graphic

  • a = 8.4695 (2) Å

  • b = 10.6759 (2) Å

  • c = 14.5208 (2) Å

  • β = 98.093 (2)°

  • V = 1299.89 (4) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 0.69 mm−1

  • T = 100 K

  • 0.30 × 0.25 × 0.20 mm

Data collection  

  • Agilent CCD diffratcometer diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) T min = 0.834, T max = 1.000

  • 5023 measured reflections

  • 2664 independent reflections

  • 2416 reflections with I > 2σ(I)

  • R int = 0.015

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.105

  • S = 1.04

  • 2664 reflections

  • 182 parameters

  • H-atom parameters constrained

  • Δρmax = 0.25 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: CrysAlis PRO (Agilent, 2011); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SIR2014 (Burla et al., 2015); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: MarvinSketch (ChemAxon, 2010) and publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S2056989014027790/hg5424sup1.cif

e-71-00o90-sup1.cif (189.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989014027790/hg5424Isup2.hkl

e-71-00o90-Isup2.hkl (146.4KB, hkl)

Supporting information file. DOI: 10.1107/S2056989014027790/hg5424Isup3.cml

. DOI: 10.1107/S2056989014027790/hg5424fig1.tif

The mol­ecular structure of the title compound showing the atom-labelling scheme and displacement ellipsoids at the 70% probability level.

c . DOI: 10.1107/S2056989014027790/hg5424fig2.tif

A view of the zigzag supra­molecular sustained by weak C—H⋯O hydrogen bonds (orange dashed lines) and aligned along the c axis in the crystal packing.

c . DOI: 10.1107/S2056989014027790/hg5424fig3.tif

A view in projection down the c axis of the unit-cell contents. The weak C—H⋯O and C—H⋯π inter­actions are shown as orange and purple dashed lines, respectively.

CCDC reference: 1040558

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

Table 1. Hydrogen-bond geometry (, ).

Cg1 and Cg2 are the centroids of the C4C9 and C12C17 rings, respectively.

DHA DH HA D A DHA
C7H7O2i 0.95 2.48 3.1425(14) 127
C13H13Cg1ii 0.95 2.94 3.4416(12) 115
C5H5Cg2iii 0.95 3.00 3.7780(13) 140

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

Acknowledgments

The Brazilian agencies CNPq (306121/2013–2 to IC and 308320/2010–7 to HAS), FAPESP and CAPES are acknowledged for financial support.

supplementary crystallographic information

S1. Introduction

Coumarins are heterocycles presenting a wide range of different biological activities (Wu et al., 2009). As part of our on-going inter­est in the synthesis of coumarin derivatives with biological activity (Stefani et al., 2012) the title compound was synthesized.

S2. Experimental

S2.1. Synthesis and crystallization

The title compound was prepared as per Gueogjian (2011). 3-Bromo coumarin (112.5 mg, 0.5 mmol), potassium tri­fluoro­borate salt (0.55 mmol), PdCl2(dppf).CH2Cl2 (41 mg, 10 mol%), i-Pr2NEt (0.3 mL, 1.5 mmol)and 1,4-dioxane/H2O (2/1, 3 mL), in aceto­nitrile (20 mL) were added to a two-necked round-bottomed flask equipped with a reflux condenser under N2. The reaction mixture was heated under reflux at 353 K, and was monitored by TLC and GC analysis. After the consumption of the 3-bromo­coumarin, the mixture was extracted twice with ethyl acetate (50 mL). The organic phase was separated, dried over MgSO4 and concentrated under vacuum. The residue was purified by flash chromatography (ethyl acetate/hexane 10:90). The title compound was obtained as a brown solid in 70% yield. Suitable crystals were obtained by slow evaporation from ethyl acetate/hexane.

S2.2. Refinement

Carbon-bound H-atoms were placed in calculated positions (C—H = 0.95 to 0.98 Å) and were included in the refinement in the riding model approximation, with Uiso(H) = 1.2–1.5Ueq(C).

S3. Results and discussion

The title compound, Fig. 1, is an asymmetric alkyne. The coumarin residue is approximately planar with the r.m.s. deviation of the 11 non-hydrogen atoms being 0.048 Å; the maximum deviations from their least-squares plane are 0.078 (1) and -0.066 (1) Å for the C2 and O2 atoms, respectively. Overall, the molecule is non-planar as seen in the dihedral between the fused ring system and the methyl­benzene ring of 33.68 (4)°.

The most closely related structure in the literature is of the derivative where the methyl group of the title compound has been replaced by an isoprop­oxy group (Elangovan et al., 2004). In this case, with the exception of the terminal methyl groups, the molecule is planar with the dihedral angle between the 11 non-hydrogen atoms of the courmarin residue the benzene ring being 0.88 (6)°.

Weak coumarin-C6—C—H···O(exocyclic) hydrogen bonding gives rise to a supra­molecular chain aligned along the c axis, Table 1 and Fig. 2. The chains are connected into double layers, sustained by weak C—H···π inter­actions, that stack along the a axis with no specific inter­actions between them, Table 2 and Fig. 3.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound showing the atom-labelling scheme and displacement ellipsoids at the 70% probability level.

Fig. 2.

Fig. 2.

A view of the zigzag supramolecular sustained by weak C—H···O hydrogen bonds (orange dashed lines) and aligned along the c axis in the crystal packing.

Fig. 3.

Fig. 3.

A view in projection down the c axis of the unit-cell contents. The weak C—H···O and C—H···π interactions are shown as orange and purple dashed lines, respectively.

Crystal data

C18H12O2 F(000) = 544
Mr = 260.28 Dx = 1.330 Mg m3
Monoclinic, P21/c Cu Kα radiation, λ = 1.54184 Å
a = 8.4695 (2) Å Cell parameters from 3107 reflections
b = 10.6759 (2) Å θ = 3.1–76.1°
c = 14.5208 (2) Å µ = 0.69 mm1
β = 98.093 (2)° T = 100 K
V = 1299.89 (4) Å3 Prism, dark orange
Z = 4 0.30 × 0.25 × 0.20 mm

Data collection

Agilent CCD diffratcometer diffractometer 2416 reflections with I > 2σ(I)
Radiation source: SuperNova (Cu) X-ray Source Rint = 0.015
ω scans θmax = 76.3°, θmin = 5.2°
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) h = −9→10
Tmin = 0.834, Tmax = 1.000 k = −6→13
5023 measured reflections l = −17→18
2664 independent reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038 H-atom parameters constrained
wR(F2) = 0.105 w = 1/[σ2(Fo2) + (0.0605P)2 + 0.3358P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max < 0.001
2664 reflections Δρmax = 0.25 e Å3
182 parameters Δρmin = −0.21 e Å3
0 restraints

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.

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

x y z Uiso*/Ueq
O1 0.13803 (10) 0.67272 (7) 0.66818 (5) 0.0210 (2)
O2 0.15964 (12) 0.72775 (8) 0.52430 (6) 0.0313 (2)
C1 0.16397 (14) 0.64322 (11) 0.57962 (7) 0.0211 (2)
C2 0.19557 (13) 0.51127 (11) 0.56003 (7) 0.0199 (2)
C3 0.18389 (13) 0.42253 (10) 0.62585 (7) 0.0199 (2)
H3 0.1980 0.3368 0.6115 0.024*
C4 0.15055 (13) 0.45668 (10) 0.71666 (7) 0.0184 (2)
C5 0.14038 (13) 0.36959 (11) 0.78810 (8) 0.0206 (2)
H5 0.1504 0.2826 0.7763 0.025*
C6 0.11585 (13) 0.40976 (11) 0.87544 (8) 0.0217 (2)
H6 0.1078 0.3504 0.9233 0.026*
C7 0.10299 (13) 0.53744 (11) 0.89331 (7) 0.0213 (2)
H7 0.0880 0.5645 0.9538 0.026*
C8 0.11176 (13) 0.62546 (11) 0.82380 (7) 0.0204 (2)
H8 0.1033 0.7124 0.8360 0.025*
C9 0.13313 (13) 0.58337 (10) 0.73620 (7) 0.0181 (2)
C10 0.24056 (14) 0.48424 (11) 0.47093 (8) 0.0219 (2)
C11 0.28627 (14) 0.46381 (11) 0.39787 (8) 0.0213 (2)
C12 0.34093 (13) 0.43519 (11) 0.31108 (7) 0.0191 (2)
C13 0.28464 (13) 0.50208 (11) 0.23036 (8) 0.0214 (2)
H13 0.2132 0.5701 0.2333 0.026*
C14 0.33248 (14) 0.46968 (12) 0.14599 (8) 0.0227 (3)
H14 0.2941 0.5166 0.0919 0.027*
C15 0.43582 (13) 0.36949 (11) 0.13914 (8) 0.0215 (2)
C16 0.49343 (14) 0.30434 (11) 0.22028 (8) 0.0229 (2)
H16 0.5653 0.2366 0.2172 0.027*
C17 0.44814 (14) 0.33623 (11) 0.30511 (8) 0.0218 (2)
H17 0.4897 0.2910 0.3595 0.026*
C18 0.48231 (15) 0.32959 (13) 0.04694 (8) 0.0286 (3)
H18A 0.4267 0.3821 −0.0027 0.043*
H18B 0.4526 0.2417 0.0351 0.043*
H18C 0.5978 0.3390 0.0486 0.043*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0288 (4) 0.0177 (4) 0.0170 (4) 0.0023 (3) 0.0054 (3) 0.0017 (3)
O2 0.0459 (6) 0.0265 (5) 0.0239 (4) 0.0070 (4) 0.0132 (4) 0.0074 (3)
C1 0.0237 (6) 0.0236 (6) 0.0164 (5) 0.0020 (4) 0.0046 (4) 0.0019 (4)
C2 0.0189 (5) 0.0235 (6) 0.0170 (5) 0.0023 (4) 0.0016 (4) −0.0011 (4)
C3 0.0198 (5) 0.0201 (5) 0.0195 (5) 0.0020 (4) 0.0018 (4) −0.0012 (4)
C4 0.0168 (5) 0.0201 (5) 0.0179 (5) 0.0009 (4) 0.0009 (4) 0.0001 (4)
C5 0.0202 (5) 0.0193 (5) 0.0217 (5) 0.0006 (4) 0.0008 (4) 0.0021 (4)
C6 0.0211 (5) 0.0252 (6) 0.0182 (5) −0.0015 (4) 0.0003 (4) 0.0051 (4)
C7 0.0205 (5) 0.0282 (6) 0.0148 (5) −0.0019 (4) 0.0007 (4) −0.0009 (4)
C8 0.0216 (5) 0.0207 (5) 0.0187 (5) −0.0006 (4) 0.0018 (4) −0.0017 (4)
C9 0.0183 (5) 0.0194 (5) 0.0163 (5) 0.0001 (4) 0.0013 (4) 0.0023 (4)
C10 0.0223 (5) 0.0241 (5) 0.0189 (5) 0.0014 (4) 0.0018 (4) −0.0002 (4)
C11 0.0213 (5) 0.0226 (5) 0.0197 (5) −0.0006 (4) 0.0013 (4) −0.0009 (4)
C12 0.0191 (5) 0.0214 (5) 0.0169 (5) −0.0036 (4) 0.0027 (4) −0.0027 (4)
C13 0.0196 (5) 0.0231 (6) 0.0209 (5) 0.0012 (4) 0.0013 (4) −0.0014 (4)
C14 0.0218 (5) 0.0292 (6) 0.0164 (5) −0.0008 (5) −0.0006 (4) 0.0012 (4)
C15 0.0191 (5) 0.0278 (6) 0.0178 (5) −0.0054 (4) 0.0030 (4) −0.0048 (4)
C16 0.0211 (5) 0.0231 (6) 0.0250 (6) 0.0013 (4) 0.0053 (4) −0.0022 (4)
C17 0.0229 (5) 0.0238 (6) 0.0184 (5) −0.0002 (4) 0.0021 (4) 0.0023 (4)
C18 0.0274 (6) 0.0394 (7) 0.0200 (6) −0.0036 (5) 0.0062 (5) −0.0074 (5)

Geometric parameters (Å, º)

O1—C1 1.3713 (13) C8—H8 0.9500
O1—C9 1.3780 (13) C10—C11 1.1995 (16)
O2—C1 1.2053 (14) C11—C12 1.4353 (15)
C1—C2 1.4691 (16) C12—C13 1.3978 (16)
C2—C3 1.3592 (15) C12—C17 1.4036 (16)
C2—C10 1.4287 (15) C13—C14 1.3873 (15)
C3—C4 1.4339 (14) C13—H13 0.9500
C3—H3 0.9500 C14—C15 1.3945 (17)
C4—C9 1.3941 (15) C14—H14 0.9500
C4—C5 1.4048 (15) C15—C16 1.3958 (16)
C5—C6 1.3820 (15) C15—C18 1.5090 (14)
C5—H5 0.9500 C16—C17 1.3833 (15)
C6—C7 1.3946 (17) C16—H16 0.9500
C6—H6 0.9500 C17—H17 0.9500
C7—C8 1.3887 (16) C18—H18A 0.9800
C7—H7 0.9500 C18—H18B 0.9800
C8—C9 1.3847 (15) C18—H18C 0.9800
C1—O1—C9 122.56 (9) C8—C9—C4 122.22 (10)
O2—C1—O1 117.33 (10) C11—C10—C2 176.53 (12)
O2—C1—C2 125.32 (10) C10—C11—C12 178.19 (12)
O1—C1—C2 117.35 (9) C13—C12—C17 118.68 (10)
C3—C2—C10 123.44 (11) C13—C12—C11 120.89 (10)
C3—C2—C1 119.92 (10) C17—C12—C11 120.39 (10)
C10—C2—C1 116.62 (10) C14—C13—C12 120.37 (11)
C2—C3—C4 120.84 (10) C14—C13—H13 119.8
C2—C3—H3 119.6 C12—C13—H13 119.8
C4—C3—H3 119.6 C13—C14—C15 121.24 (10)
C9—C4—C5 118.20 (10) C13—C14—H14 119.4
C9—C4—C3 118.30 (10) C15—C14—H14 119.4
C5—C4—C3 123.46 (10) C14—C15—C16 118.05 (10)
C6—C5—C4 120.34 (11) C14—C15—C18 121.64 (11)
C6—C5—H5 119.8 C16—C15—C18 120.29 (11)
C4—C5—H5 119.8 C17—C16—C15 121.42 (11)
C5—C6—C7 119.99 (10) C17—C16—H16 119.3
C5—C6—H6 120.0 C15—C16—H16 119.3
C7—C6—H6 120.0 C16—C17—C12 120.21 (10)
C8—C7—C6 120.84 (10) C16—C17—H17 119.9
C8—C7—H7 119.6 C12—C17—H17 119.9
C6—C7—H7 119.6 C15—C18—H18A 109.5
C9—C8—C7 118.38 (10) C15—C18—H18B 109.5
C9—C8—H8 120.8 H18A—C18—H18B 109.5
C7—C8—H8 120.8 C15—C18—H18C 109.5
O1—C9—C8 117.06 (10) H18A—C18—H18C 109.5
O1—C9—C4 120.72 (9) H18B—C18—H18C 109.5
C9—O1—C1—O2 177.09 (10) C7—C8—C9—O1 178.68 (9)
C9—O1—C1—C2 −3.21 (15) C7—C8—C9—C4 −1.88 (17)
O2—C1—C2—C3 −174.34 (12) C5—C4—C9—O1 −178.37 (9)
O1—C1—C2—C3 5.98 (16) C3—C4—C9—O1 3.95 (16)
O2—C1—C2—C10 6.73 (18) C5—C4—C9—C8 2.21 (16)
O1—C1—C2—C10 −172.95 (10) C3—C4—C9—C8 −175.47 (10)
C10—C2—C3—C4 175.00 (10) C17—C12—C13—C14 0.91 (16)
C1—C2—C3—C4 −3.86 (17) C11—C12—C13—C14 −176.91 (10)
C2—C3—C4—C9 −1.08 (16) C12—C13—C14—C15 0.70 (17)
C2—C3—C4—C5 −178.62 (10) C13—C14—C15—C16 −1.63 (17)
C9—C4—C5—C6 −0.84 (16) C13—C14—C15—C18 177.00 (11)
C3—C4—C5—C6 176.70 (10) C14—C15—C16—C17 0.99 (17)
C4—C5—C6—C7 −0.77 (17) C18—C15—C16—C17 −177.67 (10)
C5—C6—C7—C8 1.12 (17) C15—C16—C17—C12 0.60 (18)
C6—C7—C8—C9 0.18 (17) C13—C12—C17—C16 −1.54 (17)
C1—O1—C9—C8 177.74 (10) C11—C12—C17—C16 176.28 (10)
C1—O1—C9—C4 −1.71 (16)

Hydrogen-bond geometry (Å, º)

Cg1 and Cg2 are the centroids of the C4–C9 and C12–C17 rings, respectively.

D—H···A D—H H···A D···A D—H···A
C7—H7···O2i 0.95 2.48 3.1425 (14) 127
C13—H13···Cg1ii 0.95 2.94 3.4416 (12) 115
C5—H5···Cg2iii 0.95 3.00 3.7780 (13) 140

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

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: HG5424).

References

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  6. Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
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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) I, New_Global_Publ_Block. DOI: 10.1107/S2056989014027790/hg5424sup1.cif

e-71-00o90-sup1.cif (189.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989014027790/hg5424Isup2.hkl

e-71-00o90-Isup2.hkl (146.4KB, hkl)

Supporting information file. DOI: 10.1107/S2056989014027790/hg5424Isup3.cml

. DOI: 10.1107/S2056989014027790/hg5424fig1.tif

The mol­ecular structure of the title compound showing the atom-labelling scheme and displacement ellipsoids at the 70% probability level.

c . DOI: 10.1107/S2056989014027790/hg5424fig2.tif

A view of the zigzag supra­molecular sustained by weak C—H⋯O hydrogen bonds (orange dashed lines) and aligned along the c axis in the crystal packing.

c . DOI: 10.1107/S2056989014027790/hg5424fig3.tif

A view in projection down the c axis of the unit-cell contents. The weak C—H⋯O and C—H⋯π inter­actions are shown as orange and purple dashed lines, respectively.

CCDC reference: 1040558

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


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