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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Oct 20;68(Pt 11):o3169–o3170. doi: 10.1107/S1600536812042250

2-(Prop-2-enyloxy)benzamide

Bernhard Bugenhagen a, Yosef Al Jasem b, Farah Barkhad c, Bassam al Hindawi d, Thies Thiemann d,*
PMCID: PMC3515263  PMID: 23284483

Abstract

In the title mol­ecule, C10H11NO2, the benzene ring forms dihedral angles of 33.15 (2) and 6.20 (2)° with the mean planes of the amide and propen­oxy groups, respectively. The amide –NH2 group is oriented toward the propen­oxy substituent and forms a weak intra­molecular N—H⋯O hydrogen bond to the propen­oxy O atom. The conformation of the propen­oxy group at the Csp 2—Csp 3 and Csp 3—O bonds is synperiplanar and anti­periplanar, respectively. In the crystal, N—H⋯O hydrogen bonds involving the amide groups generate C(4) and R 2 3(7) motifs that organize the mol­ecules into tapes along the a-axis direction. There are C—H⋯π inter­actions between the propen­oxy –CH2 group and the aromatic system of neighboring mol­ecules within the tape. The mean planes of the aromatic ring and the propen­oxy group belonging to mol­ecules located on opposite sites of the tape form an angle of 83.16 (2)°.

Related literature  

For crystal structures of similar compounds, see: Al Jasem et al. (2012); Pagola & Stephens (2009); Johnstone et al. (2010); Pertlik (1990); Sasada et al. (1964). For uses of 2-alk­oxy­benzamides, see: van de Waterbeemd & Testa (1983); Kusunoki & Harada (1984). For the preparation of a related 2-alk­oxy­benzamide, see: Al Jasem et al. (2012).graphic file with name e-68-o3169-scheme1.jpg

Experimental  

Crystal data  

  • C10H11NO2

  • M r = 177.20

  • Orthorhombic, Inline graphic

  • a = 5.08891 (17) Å

  • b = 11.2542 (4) Å

  • c = 15.8802 (6) Å

  • V = 909.48 (5) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 0.74 mm−1

  • T = 100 K

  • 0.30 × 0.09 × 0.08 mm

Data collection  

  • Agilent SuperNova Atlas diffractometer

  • Absorption correction: Gaussian (CrysAlis PRO; Agilent, 2012) T min = 0.862, T max = 0.951

  • 4718 measured reflections

  • 1079 independent reflections

  • 1016 reflections with I > 2σ(I)

  • R int = 0.025

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.033

  • wR(F 2) = 0.087

  • S = 1.03

  • 1079 reflections

  • 126 parameters

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

  • Δρmax = 0.17 e Å−3

  • Δρmin = −0.18 e Å−3

Data collection: CrysAlis PRO (Agilent, 2012); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008) within OLEX2 (Dolomanov et al., 2009); molecular graphics: PLATON (Spek, 2009); Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97, PLATON.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812042250/gk2521sup1.cif

e-68-o3169-sup1.cif (19.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812042250/gk2521Isup2.hkl

e-68-o3169-Isup2.hkl (53.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812042250/gk2521Isup3.cml

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

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

Cg is the centroid of the C1–C6 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯O1i 0.90 (2) 2.01 (2) 2.905 (2) 178 (17)
N1—H1B⋯O1ii 0.89 (3) 2.12 (3) 2.863 (2) 140 (2)
N1—H1B⋯O2 0.89 (3) 2.31 (2) 2.754 (2) 110.8 (18)
C8—H8BCg ii 0.99 2.68 3.461 (2) 137

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

supplementary crystallographic information

Comment

In 2-propenoxybenzamide (2-allyloxybenzamide) (Figure 1), the O1—C7—C1—C6 torsion angle characterizing the twist of the benzene ring relative to the amide group is -30.3 (2)° and the corresponding C8—O2—C2—C3 torsion angle for the propoxy group is 5.9 (2)°. There is an intramolecular N1—H1B···O2 bond within each molecule (Table 1). When compared to the structurally comparable 2-propoxybenzamide (Al Jasem et al., 2012), the torsion angle O1—C7—C1—C6 is much larger in the title compound. The amide groups generate C(4) and R23(7) hydrogen-bond motifs that organize the molecules into tapes along the a axis. The title compound exhibits a C10—H10A···O2 and a C8—H8··· π (Table 1) close contact, absent in 2-propoxybenzamide (Figure 2). The C4—H4···O1 intermolecular interaction in 2-propenoxybenzamide links the neighboring tapes of molecules along the a axis with each other (Figure 3). However, in 2-propoxybenzamide, where also a C–H···O intermolecular interaction is found, the interaction proceeds from the carbon ortho to the propoxy group, while in the present case, it proceeds from the carbon meta to the propenoxy group. As a result of more close intermolecular contacts in 2-propenoxybenzamide as compared to 2-propoxybenzamide, the difference in the packing between the two compounds is large. The main difference is that while in the 2-propoxybenzamide molecules are arranged into pairs by close contacts, where the pairs in one layer are not associated through close contacts, in the title compound all neighboring molecules form close contacts to each other. Nevertheless, both compounds exhibit particular molecular tapes, each compound with two different directions of tape propagation. In the title compound, the average plane (0 1 - 1) of a tape propagation has an angle of 68.78 (2)° with the corresponding plane (0 1 1) of the neighboring tape propagation. Due to the large dihedral angle between the benzene ring and the amide group in 2-propenoxybenzamide, the average plane (-1 2 2) of the benzene ring and the propenoxy group of a molecule in one stack makes an angle of 83.16 (2)° with the corresponding plane (1 2 2) of a molecule in the opposing motif within one tape.

Experimental

To powdered KOH (1.12 g, 20.0 mmol) in DMSO (18 ml) was added salicylamide (2.74 g, 20.0 mmol), and the resulting mixture was stirred for 10 min. at rt. Thereafter, n-propenyl bromide (4.2 g, mmol, 34.7 mmol) was added dropwise. The solution was stirred for 12 h at rt. Then, it was poured into water (200 ml) and extracted with chloroform (3 x 75 ml). The organic phase was dried over anhydrous MgSO4, concentrated in vacuo, and the residue was subjected to column chromatography on silica gel (CHCl3/MtBE/hexane v/v/v 1:1:1) to give 2-propenoxybenzamide (2.76 g, 78%) as colorless crystals (m.p. 377 K). The crystal was grown from CHCl3/ MtBE/hexane (v/v/v 1:1:1).IR (KBr) νmax 3406, 3190, 1631, 1600, 1399, 1243, 996, 921, 757, 643, 627 cm-1; δH (400 MHz, CDCl3) 4.67 (2H, d, 3J = 5.6 Hz), 5.36 (1H, dd, 3J = 10.4 Hz, 2J = 1.2 Hz), 5.44 (1H, dd, 3J = 17.2 Hz, 2J = 1.2 Hz), 6.03 – 6.13 (1H, dt, 3J = 17.2 Hz, 3J = 10.4 Hz, 3J = 5.6 Hz), 6.25 (1H, bs, NH), 6.96 (1H, d, 3J = 8.0 Hz), 7.07 (1H, dd, 3J = 8.0 Hz, 3J = 8.0 Hz), 7.80 (1H, bs, NH), 8.20 (1H, dd, 3J = 8.0 Hz, 4J = 1.6 Hz); δC (100.5 MHz, CDCl3) 69.9, 112.6, 119.4, 121.1, 121.4, 132.0, 132.6, 133.3, 156.9, 167.2.

Refinement

All carbon-bound hydrogen atoms were placed in calculated positions with C—H

distances of 0.95 - 0.99 Å and refined as riding with Uiso(H)

=xUeq(C), where x = 1.5 for methyl and x = 1.2 for all other H-atoms.

The N-bound H atom positions were determined from difference electron

density map and refined freely. In the absence of significant anomalous

scattering effects Friedel pairs have been merged.

Figures

Fig. 1.

Fig. 1.

A view of the title compound molecule with the atom-numbering scheme and the intramolecular interaction within the molecule. Displacement ellipsoids are shown at the 50% probability level.

Fig. 2.

Fig. 2.

Intermolecular attractions between molecules of the title compound. [Symmetry codes: i: 1+x,y,z; ii: x,y,z; iii: -1/2 + x,1/2 - y,1 - z; iiii: 1/2 + x, 1/2 - y,1 - z]

Fig. 3.

Fig. 3.

The crystal packing diagram showing the C—H···O intermolecular interactions between tapes formed via amide group interactions.

Crystal data

C10H11NO2 Dx = 1.294 Mg m3
Mr = 177.20 Melting point: 377 K
Orthorhombic, P212121 Cu Kα radiation, λ = 1.5418 Å
a = 5.08891 (17) Å Cell parameters from 2824 reflections
b = 11.2542 (4) Å θ = 3.9–72.6°
c = 15.8802 (6) Å µ = 0.74 mm1
V = 909.48 (5) Å3 T = 100 K
Z = 4 Needle, colourless
F(000) = 376 0.30 × 0.09 × 0.08 mm

Data collection

Agilent SuperNova Atlas diffractometer 1079 independent reflections
Radiation source: SuperNova (Cu) X-ray Source 1016 reflections with I > 2σ(I)
Mirror monochromator Rint = 0.025
Detector resolution: 10.4127 pixels mm-1 θmax = 72.7°, θmin = 4.8°
ω scans h = −6→3
Absorption correction: gaussian (CrysAlis PRO; Agilent, 2012) k = −12→13
Tmin = 0.862, Tmax = 0.951 l = −19→19
4718 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)] = 0.033 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.087 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0609P)2 + 0.1267P] where P = (Fo2 + 2Fc2)/3
1079 reflections (Δ/σ)max < 0.001
126 parameters Δρmax = 0.17 e Å3
0 restraints Δρmin = −0.18 e Å3

Special details

Experimental. Numerical absorption correction based on gaussian integration over a multifaceted crystal model
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 0.2397 (4) 0.43317 (15) 0.31664 (10) 0.0181 (4)
C10 0.9389 (4) 0.59453 (19) 0.49447 (12) 0.0289 (4)
C2 0.4129 (3) 0.52840 (15) 0.30222 (11) 0.0188 (4)
C3 0.3949 (4) 0.59415 (17) 0.22777 (12) 0.0238 (4)
C4 0.2055 (4) 0.56545 (18) 0.16826 (11) 0.0262 (4)
C5 0.0314 (4) 0.47271 (17) 0.18190 (11) 0.0244 (4)
C6 0.0478 (4) 0.40808 (16) 0.25658 (11) 0.0208 (4)
C7 0.2401 (3) 0.35748 (15) 0.39466 (11) 0.0181 (4)
C8 0.7520 (4) 0.65550 (15) 0.35506 (12) 0.0231 (4)
C9 0.9255 (4) 0.66806 (17) 0.43007 (12) 0.0268 (4)
H10A 0.8310 0.5257 0.4958 0.035*
H10B 1.0565 0.6104 0.5396 0.035*
H1A 0.484 (5) 0.288 (2) 0.4772 (13) 0.028 (6)*
H1B 0.623 (5) 0.358 (2) 0.4113 (16) 0.040 (7)*
H3 0.5120 0.6584 0.2179 0.029*
H4 0.1950 0.6099 0.1175 0.031*
H5 −0.0975 0.4534 0.1408 0.029*
H6 −0.0741 0.3458 0.2667 0.025*
H8A 0.6389 0.7267 0.3496 0.028*
H8B 0.8604 0.6488 0.3035 0.028*
H9 1.0373 0.7356 0.4316 0.032*
N1 0.4686 (3) 0.33298 (15) 0.43084 (10) 0.0218 (3)
O1 0.0291 (2) 0.31561 (12) 0.42082 (8) 0.0224 (3)
O2 0.5922 (2) 0.55184 (11) 0.36411 (7) 0.0217 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0162 (8) 0.0185 (8) 0.0197 (8) 0.0023 (7) 0.0017 (7) −0.0006 (6)
C2 0.0149 (8) 0.0194 (8) 0.0221 (8) 0.0015 (7) 0.0019 (7) 0.0001 (7)
C3 0.0226 (9) 0.0230 (8) 0.0259 (9) 0.0029 (8) 0.0040 (7) 0.0037 (7)
C4 0.0309 (10) 0.0275 (10) 0.0202 (8) 0.0076 (9) 0.0018 (8) 0.0044 (7)
C5 0.0245 (9) 0.0280 (9) 0.0207 (8) 0.0049 (8) −0.0038 (7) −0.0032 (7)
C6 0.0180 (8) 0.0205 (8) 0.0239 (8) 0.0014 (7) −0.0004 (8) −0.0028 (7)
C7 0.0159 (8) 0.0173 (8) 0.0210 (8) 0.0005 (7) 0.0006 (7) −0.0019 (6)
C8 0.0213 (9) 0.0177 (8) 0.0304 (9) −0.0038 (8) 0.0011 (8) 0.0008 (7)
C9 0.0211 (9) 0.0240 (9) 0.0353 (10) −0.0040 (8) 0.0013 (8) −0.0066 (8)
C10 0.0270 (10) 0.0315 (9) 0.0283 (9) 0.0002 (9) −0.0022 (9) −0.0070 (8)
N1 0.0153 (7) 0.0260 (8) 0.0240 (7) −0.0007 (6) 0.0000 (6) 0.0071 (6)
O1 0.0153 (6) 0.0243 (6) 0.0276 (6) −0.0017 (5) 0.0006 (5) 0.0053 (5)
O2 0.0195 (6) 0.0210 (6) 0.0246 (6) −0.0045 (5) −0.0015 (5) 0.0033 (5)

Geometric parameters (Å, º)

C1—C2 1.406 (2) C7—N1 1.326 (2)
C1—C6 1.394 (2) C7—O1 1.244 (2)
C1—C7 1.504 (2) C8—H8A 0.9900
C2—C3 1.398 (2) C8—H8B 0.9900
C2—O2 1.367 (2) C8—C9 1.489 (3)
C3—H3 0.9500 C8—O2 1.429 (2)
C3—C4 1.388 (3) C9—H9 0.9500
C4—H4 0.9500 C9—C10 1.317 (3)
C4—C5 1.386 (3) C10—H10A 0.9500
C5—H5 0.9500 C10—H10B 0.9500
C5—C6 1.394 (2) N1—H1A 0.90 (2)
C6—H6 0.9500 N1—H1B 0.89 (3)
C1—C6—H6 119.4 C7—N1—H1A 123.2 (16)
C10—C9—C8 126.30 (18) C7—N1—H1B 124.0 (16)
C10—C9—H9 116.9 C8—C9—H9 116.9
C2—C1—C7 124.39 (15) C9—C10—H10A 120.0
C2—C3—H3 120.1 C9—C10—H10B 120.0
C2—O2—C8 117.72 (13) C9—C8—H8A 109.8
C3—C2—C1 120.00 (16) C9—C8—H8B 109.8
C3—C4—H4 119.6 H10A—C10—H10B 120.0
C4—C3—C2 119.89 (18) H1A—N1—H1B 113 (2)
C4—C3—H3 120.1 H8A—C8—H8B 108.2
C4—C5—H5 120.4 N1—C7—C1 118.44 (16)
C4—C5—C6 119.20 (17) O1—C7—C1 119.23 (15)
C5—C4—C3 120.84 (17) O1—C7—N1 122.25 (16)
C5—C4—H4 119.6 O2—C2—C1 116.64 (14)
C5—C6—C1 121.22 (17) O2—C2—C3 123.36 (16)
C5—C6—H6 119.4 O2—C8—H8A 109.8
C6—C1—C2 118.81 (15) O2—C8—H8B 109.8
C6—C1—C7 116.76 (16) O2—C8—C9 109.54 (15)
C6—C5—H5 120.4

Hydrogen-bond geometry (Å, º)

Cg is the centroid of the C1–C6 ring.

D—H···A D—H H···A D···A D—H···A
N1—H1A···O1i 0.90 (2) 2.01 (2) 2.905 (2) 178 (17)
N1—H1B···O1ii 0.89 (3) 2.12 (3) 2.863 (2) 140 (2)
N1—H1B···O2 0.89 (3) 2.31 (2) 2.754 (2) 110.8 (18)
C8—H8B···Cgii 0.99 2.68 3.461 (2) 137

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: GK2521).

References

  1. Agilent (2012). CrysAlis PRO. Agilent Technologies, Yarnton, England.
  2. Al Jasem, Y., Hindawi, B. al, Thiemann, T. & White, F. (2012). Acta Cryst. E68, o2639–o2640. [DOI] [PMC free article] [PubMed]
  3. Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.
  4. Johnstone, R. D. L., Lennie, A. R., Parker, S. F., Parsons, S., Pidcock, E., Richardson, P. R., Warren, J. E. & Wood, P. A. (2010). CrystEngComm, 12, 1065–1078.
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  6. Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470.
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  8. Pertlik, F. (1990). Monatsh. Chem. 121, 129–139.
  9. Sasada, Y., Takano, T. & Kakudo, M. (1964). Bull. Chem. Soc. Jpn, 37, 940–946.
  10. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
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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/S1600536812042250/gk2521sup1.cif

e-68-o3169-sup1.cif (19.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812042250/gk2521Isup2.hkl

e-68-o3169-Isup2.hkl (53.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812042250/gk2521Isup3.cml

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


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