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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Apr 21;68(Pt 5):o1482. doi: 10.1107/S1600536812016510

(E)-Ethyl 2-cyano-3-(furan-2-yl)acrylate

Rajesh G Kalkhambkar a, D Gayathri b, Vivek K Gupta c, Rajni Kant c, Yeon Tae Jeong d,*
PMCID: PMC3344592  PMID: 22590354

Abstract

There are two independent mol­ecules in the asymmetric unit of the title compound, C10H9NO3, in both of which, all non-H atoms except for the methyl C atom lie nearly in the same plane [maximum deviations = 0.094 (3) and 0.043 (2) Å]. In the crystal, each independent mol­ecules is linked by pairs of C—H⋯O inter­actions, generating inversion dimers with R 2 2(10) ring motifs.

Related literature  

For the synthesis of related compounds, see: Yadav et al. (2004). For related structures, see: Wang & Jian (2008); Zhang et al. (2009); Ye et al. (2009); Yuvaraj et al. (2011).graphic file with name e-68-o1482-scheme1.jpg

Experimental  

Crystal data  

  • C10H9NO3

  • M r = 191.18

  • Monoclinic, Inline graphic

  • a = 4.6611 (2) Å

  • b = 19.8907 (9) Å

  • c = 20.9081 (9) Å

  • β = 91.988 (4)°

  • V = 1937.28 (15) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 293 K

  • 0.30 × 0.20 × 0.10 mm

Data collection  

  • Oxford Diffraction Xcalibur Sapphire3 diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) T min = 0.933, T max = 0.990

  • 12870 measured reflections

  • 4568 independent reflections

  • 2407 reflections with I > 2σ(I)

  • R int = 0.034

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.066

  • wR(F 2) = 0.209

  • S = 1.04

  • 4568 reflections

  • 253 parameters

  • H-atom parameters constrained

  • Δρmax = 0.26 e Å−3

  • Δρmin = −0.24 e Å−3

Data collection: CrysAlis PRO (Oxford Diffraction, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis RED (Oxford Diffraction, 2010); 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: PLATON.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812016510/is5119sup1.cif

e-68-o1482-sup1.cif (20.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016510/is5119Isup2.hkl

e-68-o1482-Isup2.hkl (219.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812016510/is5119Isup3.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
C5A—H5A⋯O2Ai 0.93 2.40 3.242 (3) 151
C5B—H5B⋯O2Bii 0.93 2.46 3.320 (3) 153

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

Acknowledgments

YTJ is thankful for the support provided by the second stage of the BK-21 program. The authors thank the Director, USIC University of Jammu, Jammu Tawi, India, for the X-ray data collection.

supplementary crystallographic information

Comment

Knoevenagel condensation is an important carbon-carbon bond forming reaction in organic synthesis (Yadav et al., 2004). In continuation of our work on nitrogen and oxygen based heterocycles, we herein report the crystal structure of the title compound.

The title compound crystallizes in monoclinic system with two molecules in the asymmetric unit. Bond lengths and bond angles are comparable with the similar crystal structures solved earlier (Zhang et al., 2009; Wang & Jian, 2008; Ye et al., 2009; Yuvaraj et al., 2011). All the non-hydrogen atoms, except the methyl group, lie nearly in the same plane with a maximum out-of-plane deviation of 0.094 (3) and 0.043 (2) Å (r.m.s deviation = 0.04 and 0.024 Å), respectively, for molecules A and B. Difference in the torsion angles C7A—O3A—C8A—C9A [-167.4 (3)°] and C7B—O3B—C8B—C9B [125.3 (4)°] has been observed, indicating the flexibility of the methyl group. The crystal packing is stabilized by C—H···O intermolecular interactions generating the centrosymmetric dimer of R22(10) ring motif.

Experimental

A solution of furan-2-aldehyde (1 mol), ethyl cyanoacetate (1.2 mol) and piperidine (0.1 ml) in ethanol (20 ml) was stirred at room temperature for 8 h. After removal of the volatiles in vacuo, orange solid was obtained in quantitative yield. A sample for analysis was obtained by recrystallization from EtOAc as pale yellow needles: 1H NMR (300 MHz, CDCl3) δ p.p.m.: 1.42 (t, 3H, CH3), 4.40 (q, 2H, CH2), 6.61 (m, 1H, CH), 6.80 (m, 1H, CH), 7.28 (m, 1H, CH), 7.98 (s, 1H, HC=C).

Refinement

All H-atoms were refined using a riding model [C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for aromatic, C—H = 0.97 Å and Uiso = 1.2Ueq (C) for CH2, and C—H = 0.96 Å and Uiso = 1.5Ueq(C) for CH3].

Figures

Fig. 1.

Fig. 1.

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

Fig. 2.

Fig. 2.

A molecular packing view of the title compound, showing intermolecular interactions. For clarity, hydrogen atoms not involved in the hydrogen bonding have been omitted.

Crystal data

C10H9NO3 F(000) = 800
Mr = 191.18 Dx = 1.311 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 4295 reflections
a = 4.6611 (2) Å θ = 3.6–29.1°
b = 19.8907 (9) Å µ = 0.10 mm1
c = 20.9081 (9) Å T = 293 K
β = 91.988 (4)° Needle, pale yellow
V = 1937.28 (15) Å3 0.30 × 0.20 × 0.10 mm
Z = 8

Data collection

Oxford Diffraction Xcalibur Sapphire3 diffractometer 4568 independent reflections
Radiation source: fine-focus sealed tube 2407 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.034
Detector resolution: 16.1049 pixels mm-1 θmax = 29.2°, θmin = 3.6°
ω scans h = −6→6
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) k = −26→24
Tmin = 0.933, Tmax = 0.990 l = −27→27
12870 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)] = 0.066 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.209 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0908P)2 + 0.185P] where P = (Fo2 + 2Fc2)/3
4568 reflections (Δ/σ)max < 0.001
253 parameters Δρmax = 0.26 e Å3
0 restraints Δρmin = −0.24 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
O1A 1.1671 (4) 0.14995 (9) 0.41737 (9) 0.0642 (5)
O2A 0.5561 (4) 0.03506 (10) 0.58448 (9) 0.0724 (6)
O3A 0.8013 (4) 0.10818 (9) 0.64695 (8) 0.0617 (5)
N1A 1.2730 (5) 0.19852 (12) 0.56530 (12) 0.0695 (7)
C1A 0.9635 (5) 0.10093 (13) 0.41935 (12) 0.0524 (6)
C2A 0.9058 (6) 0.07717 (15) 0.35931 (13) 0.0658 (8)
H2A 0.7747 0.0437 0.3478 0.079*
C3A 1.0809 (7) 0.11270 (15) 0.31803 (14) 0.0709 (8)
H3A 1.0900 0.1074 0.2740 0.085*
C4A 1.2328 (7) 0.15591 (16) 0.35497 (14) 0.0747 (9)
H4A 1.3663 0.1861 0.3397 0.090*
C5A 0.8457 (5) 0.08207 (13) 0.47874 (12) 0.0520 (6)
H5A 0.7104 0.0477 0.4761 0.062*
C6A 0.9001 (5) 0.10636 (12) 0.53795 (11) 0.0468 (6)
C7A 0.7339 (6) 0.07857 (13) 0.59153 (12) 0.0516 (6)
C8A 0.6382 (7) 0.08504 (17) 0.70119 (14) 0.0781 (9)
H8A1 0.4352 0.0835 0.6894 0.094*
H8A2 0.6995 0.0402 0.7137 0.094*
C9A 0.6886 (10) 0.13165 (19) 0.75412 (17) 0.1063 (13)
H9A1 0.5820 0.1173 0.7902 0.159*
H9A2 0.6274 0.1759 0.7413 0.159*
H9A3 0.8896 0.1324 0.7658 0.159*
C10A 1.1070 (6) 0.15760 (13) 0.55250 (12) 0.0511 (6)
O1B 1.1874 (4) 0.12570 (9) 0.88858 (9) 0.0650 (5)
O2B 0.5452 (4) −0.07433 (10) 0.94337 (10) 0.0763 (6)
O3B 0.7859 (4) −0.11775 (9) 0.86263 (10) 0.0737 (6)
N1B 1.2343 (6) −0.00911 (12) 0.79884 (12) 0.0752 (8)
C1B 0.9833 (5) 0.11024 (13) 0.93153 (12) 0.0526 (6)
C2B 0.9368 (6) 0.16376 (14) 0.96945 (14) 0.0654 (8)
H2B 0.8081 0.1659 1.0024 0.078*
C3B 1.1182 (7) 0.21538 (15) 0.95001 (15) 0.0717 (8)
H3B 1.1340 0.2584 0.9672 0.086*
C4B 1.2645 (7) 0.19017 (15) 0.90153 (17) 0.0732 (8)
H4B 1.4018 0.2139 0.8795 0.088*
C5B 0.8538 (5) 0.04531 (13) 0.93108 (12) 0.0545 (7)
H5B 0.7222 0.0384 0.9629 0.065*
C6B 0.8908 (5) −0.00742 (13) 0.89236 (11) 0.0492 (6)
C7B 0.7208 (6) −0.06891 (14) 0.90287 (13) 0.0571 (7)
C8B 0.6333 (9) −0.18142 (18) 0.86891 (18) 0.0999 (12)
H8B1 0.7679 −0.2160 0.8829 0.120*
H8B2 0.4903 −0.1769 0.9013 0.120*
C9B 0.4999 (11) −0.2007 (2) 0.8116 (2) 0.1386 (19)
H9B1 0.4030 −0.2428 0.8173 0.208*
H9B2 0.6412 −0.2057 0.7796 0.208*
H9B3 0.3631 −0.1671 0.7981 0.208*
C10B 1.0847 (6) −0.00751 (13) 0.84084 (12) 0.0541 (7)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1A 0.0780 (12) 0.0690 (13) 0.0461 (11) −0.0191 (10) 0.0102 (9) −0.0059 (9)
O2A 0.0919 (14) 0.0708 (13) 0.0550 (12) −0.0275 (11) 0.0091 (10) 0.0000 (10)
O3A 0.0759 (12) 0.0698 (12) 0.0399 (10) −0.0140 (10) 0.0093 (8) −0.0011 (8)
N1A 0.0813 (16) 0.0642 (16) 0.0636 (16) −0.0126 (14) 0.0113 (13) −0.0078 (12)
C1A 0.0597 (15) 0.0511 (15) 0.0467 (15) 0.0011 (12) 0.0061 (11) −0.0023 (11)
C2A 0.0812 (19) 0.0655 (18) 0.0510 (16) −0.0147 (15) 0.0053 (14) −0.0076 (13)
C3A 0.091 (2) 0.079 (2) 0.0434 (16) −0.0073 (17) 0.0117 (15) −0.0046 (14)
C4A 0.095 (2) 0.081 (2) 0.0499 (17) −0.0172 (17) 0.0225 (16) −0.0014 (15)
C5A 0.0601 (15) 0.0480 (15) 0.0480 (15) −0.0011 (12) 0.0049 (11) −0.0014 (11)
C6A 0.0537 (14) 0.0419 (14) 0.0450 (14) 0.0002 (11) 0.0042 (11) −0.0007 (10)
C7A 0.0632 (16) 0.0495 (15) 0.0421 (14) −0.0021 (13) 0.0044 (11) 0.0029 (11)
C8A 0.098 (2) 0.091 (2) 0.0464 (17) −0.0161 (18) 0.0209 (15) 0.0028 (15)
C9A 0.150 (4) 0.111 (3) 0.060 (2) −0.021 (3) 0.036 (2) −0.0106 (19)
C10A 0.0634 (15) 0.0515 (16) 0.0390 (13) 0.0055 (13) 0.0098 (11) 0.0003 (11)
O1B 0.0693 (12) 0.0633 (13) 0.0633 (13) −0.0045 (10) 0.0132 (9) −0.0107 (9)
O2B 0.0828 (14) 0.0810 (14) 0.0665 (14) −0.0095 (11) 0.0257 (11) 0.0105 (11)
O3B 0.1015 (15) 0.0592 (12) 0.0617 (13) −0.0246 (11) 0.0199 (11) −0.0061 (10)
N1B 0.0915 (18) 0.0755 (18) 0.0601 (16) −0.0159 (14) 0.0255 (14) −0.0079 (13)
C1B 0.0568 (15) 0.0572 (17) 0.0438 (14) 0.0064 (13) 0.0024 (11) −0.0014 (11)
C2B 0.0736 (18) 0.0630 (19) 0.0596 (18) 0.0083 (15) 0.0041 (14) −0.0094 (14)
C3B 0.085 (2) 0.0586 (18) 0.071 (2) 0.0061 (16) −0.0049 (16) −0.0118 (15)
C4B 0.0759 (19) 0.0613 (19) 0.083 (2) −0.0098 (16) 0.0064 (16) −0.0059 (16)
C5B 0.0578 (15) 0.0630 (18) 0.0429 (15) 0.0028 (13) 0.0027 (11) 0.0000 (12)
C6B 0.0553 (14) 0.0531 (15) 0.0392 (13) −0.0010 (12) 0.0028 (10) 0.0030 (11)
C7B 0.0659 (17) 0.0623 (17) 0.0433 (15) −0.0005 (14) 0.0016 (12) 0.0049 (13)
C8B 0.151 (3) 0.075 (2) 0.074 (2) −0.051 (2) 0.011 (2) 0.0059 (18)
C9B 0.220 (5) 0.098 (3) 0.096 (3) −0.083 (3) −0.014 (3) 0.009 (2)
C10B 0.0702 (17) 0.0485 (15) 0.0438 (15) −0.0059 (12) 0.0039 (12) −0.0017 (11)

Geometric parameters (Å, º)

O1A—C4A 1.356 (3) O1B—C4B 1.357 (3)
O1A—C1A 1.362 (3) O1B—C1B 1.366 (3)
O2A—C7A 1.204 (3) O2B—C7B 1.203 (3)
O3A—C7A 1.328 (3) O3B—C7B 1.327 (3)
O3A—C8A 1.461 (3) O3B—C8B 1.461 (4)
N1A—C10A 1.148 (3) N1B—C10B 1.140 (3)
C1A—C2A 1.360 (3) C1B—C2B 1.349 (4)
C1A—C5A 1.425 (3) C1B—C5B 1.425 (4)
C2A—C3A 1.400 (4) C2B—C3B 1.399 (4)
C2A—H2A 0.9300 C2B—H2B 0.9300
C3A—C4A 1.341 (4) C3B—C4B 1.338 (4)
C3A—H3A 0.9300 C3B—H3B 0.9300
C4A—H4A 0.9300 C4B—H4B 0.9300
C5A—C6A 1.345 (3) C5B—C6B 1.340 (3)
C5A—H5A 0.9300 C5B—H5B 0.9300
C6A—C10A 1.429 (4) C6B—C10B 1.430 (3)
C6A—C7A 1.490 (3) C6B—C7B 1.478 (4)
C8A—C9A 1.457 (4) C8B—C9B 1.385 (5)
C8A—H8A1 0.9700 C8B—H8B1 0.9700
C8A—H8A2 0.9700 C8B—H8B2 0.9700
C9A—H9A1 0.9600 C9B—H9B1 0.9600
C9A—H9A2 0.9600 C9B—H9B2 0.9600
C9A—H9A3 0.9600 C9B—H9B3 0.9600
C4A—O1A—C1A 105.8 (2) C4B—O1B—C1B 105.5 (2)
C7A—O3A—C8A 115.1 (2) C7B—O3B—C8B 117.1 (2)
C2A—C1A—O1A 109.7 (2) C2B—C1B—O1B 109.8 (2)
C2A—C1A—C5A 130.0 (3) C2B—C1B—C5B 130.0 (3)
O1A—C1A—C5A 120.3 (2) O1B—C1B—C5B 120.3 (2)
C1A—C2A—C3A 107.0 (3) C1B—C2B—C3B 107.3 (3)
C1A—C2A—H2A 126.5 C1B—C2B—H2B 126.4
C3A—C2A—H2A 126.5 C3B—C2B—H2B 126.4
C4A—C3A—C2A 106.0 (3) C4B—C3B—C2B 105.9 (3)
C4A—C3A—H3A 127.0 C4B—C3B—H3B 127.1
C2A—C3A—H3A 127.0 C2B—C3B—H3B 127.1
C3A—C4A—O1A 111.5 (3) C3B—C4B—O1B 111.5 (3)
C3A—C4A—H4A 124.3 C3B—C4B—H4B 124.2
O1A—C4A—H4A 124.3 O1B—C4B—H4B 124.2
C6A—C5A—C1A 129.9 (2) C6B—C5B—C1B 130.5 (2)
C6A—C5A—H5A 115.1 C6B—C5B—H5B 114.7
C1A—C5A—H5A 115.1 C1B—C5B—H5B 114.7
C5A—C6A—C10A 123.8 (2) C5B—C6B—C10B 123.7 (2)
C5A—C6A—C7A 118.2 (2) C5B—C6B—C7B 118.5 (2)
C10A—C6A—C7A 118.0 (2) C10B—C6B—C7B 117.9 (2)
O2A—C7A—O3A 124.5 (2) O2B—C7B—O3B 123.8 (3)
O2A—C7A—C6A 123.2 (2) O2B—C7B—C6B 124.1 (3)
O3A—C7A—C6A 112.2 (2) O3B—C7B—C6B 112.1 (2)
C9A—C8A—O3A 108.3 (3) C9B—C8B—O3B 111.6 (3)
C9A—C8A—H8A1 110.0 C9B—C8B—H8B1 109.3
O3A—C8A—H8A1 110.0 O3B—C8B—H8B1 109.3
C9A—C8A—H8A2 110.0 C9B—C8B—H8B2 109.3
O3A—C8A—H8A2 110.0 O3B—C8B—H8B2 109.3
H8A1—C8A—H8A2 108.4 H8B1—C8B—H8B2 108.0
C8A—C9A—H9A1 109.5 C8B—C9B—H9B1 109.5
C8A—C9A—H9A2 109.5 C8B—C9B—H9B2 109.5
H9A1—C9A—H9A2 109.5 H9B1—C9B—H9B2 109.5
C8A—C9A—H9A3 109.5 C8B—C9B—H9B3 109.5
H9A1—C9A—H9A3 109.5 H9B1—C9B—H9B3 109.5
H9A2—C9A—H9A3 109.5 H9B2—C9B—H9B3 109.5
N1A—C10A—C6A 178.8 (3) N1B—C10B—C6B 177.9 (3)
C4A—O1A—C1A—C2A 0.1 (3) C4B—O1B—C1B—C2B 0.1 (3)
C4A—O1A—C1A—C5A −179.9 (2) C4B—O1B—C1B—C5B 179.8 (2)
O1A—C1A—C2A—C3A 0.1 (3) O1B—C1B—C2B—C3B 0.0 (3)
C5A—C1A—C2A—C3A −179.9 (3) C5B—C1B—C2B—C3B −179.7 (3)
C1A—C2A—C3A—C4A −0.3 (3) C1B—C2B—C3B—C4B −0.1 (3)
C2A—C3A—C4A—O1A 0.4 (4) C2B—C3B—C4B—O1B 0.2 (4)
C1A—O1A—C4A—C3A −0.3 (4) C1B—O1B—C4B—C3B −0.2 (3)
C2A—C1A—C5A—C6A −178.9 (3) C2B—C1B—C5B—C6B 177.4 (3)
O1A—C1A—C5A—C6A 1.1 (4) O1B—C1B—C5B—C6B −2.2 (4)
C1A—C5A—C6A—C10A −2.1 (4) C1B—C5B—C6B—C10B 0.5 (4)
C1A—C5A—C6A—C7A 177.5 (2) C1B—C5B—C6B—C7B −179.0 (2)
C8A—O3A—C7A—O2A −1.0 (4) C8B—O3B—C7B—O2B −0.2 (4)
C8A—O3A—C7A—C6A 177.8 (2) C8B—O3B—C7B—C6B 179.4 (3)
C5A—C6A—C7A—O2A 0.8 (4) C5B—C6B—C7B—O2B 1.7 (4)
C10A—C6A—C7A—O2A −179.5 (2) C10B—C6B—C7B—O2B −177.8 (3)
C5A—C6A—C7A—O3A −178.0 (2) C5B—C6B—C7B—O3B −177.9 (2)
C10A—C6A—C7A—O3A 1.6 (3) C10B—C6B—C7B—O3B 2.6 (3)
C7A—O3A—C8A—C9A −167.4 (3) C7B—O3B—C8B—C9B 125.3 (4)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C5A—H5A···O2Ai 0.93 2.40 3.242 (3) 151
C5B—H5B···O2Bii 0.93 2.46 3.320 (3) 153

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS5119).

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) I, global. DOI: 10.1107/S1600536812016510/is5119sup1.cif

e-68-o1482-sup1.cif (20.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016510/is5119Isup2.hkl

e-68-o1482-Isup2.hkl (219.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812016510/is5119Isup3.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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