Abstract
Molecules of the title compound, C11H15NO2, are essentially planar (r.m.s. deviation = 0.035 Å) and are linked into a chain along the a axis by weak C—H⋯O hydrogen bonds.
Related literature
Benzoic acid and its derivatives are good inhibitors of influenza viruses, see: Luo et al. (1995 ▶). For the use of benzoic acid derivatives such as 4-aminobenzoic acid as bifunctional organic ligands due to the variety of their coordination modes, see: Amiraslanov et al. (1979 ▶); Chen & Chen (2002 ▶); Hauptmann et al. (2000 ▶). For the use of the title compound as a part of a self-curing two-part system comprising degradable copolymers with applications in medicine and dentistry as root-canal sealants, root-canal filling materials, dental restorative materials, implant materials, bone cements and pulp-capping materials, see: Jia & Jin (2004 ▶).
Experimental
Crystal data
C11H15NO2
M r = 193.24
Monoclinic,
a = 12.6949 (8) Å
b = 6.6596 (4) Å
c = 12.8529 (9) Å
β = 98.672 (11)°
V = 1074.20 (12) Å3
Z = 4
Mo Kα radiation
μ = 0.08 mm−1
T = 293 K
0.18 × 0.15 × 0.13 mm
Data collection
Nonius MACH-3 diffractometer
Absorption correction: ψ scan (North et al., 1968 ▶) T min = 0.985, T max = 0.989
4088 measured reflections
1873 independent reflections
1424 reflections with I > 2σ(I)
R int = 0.051
3 standard reflections every 60 min intensity decay: none
Refinement
R[F 2 > 2σ(F 2)] = 0.043
wR(F 2) = 0.134
S = 1.05
1873 reflections
131 parameters
H-atom parameters constrained
Δρmax = 0.16 e Å−3
Δρmin = −0.14 e Å−3
Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994 ▶); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1996 ▶); 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 datablocks global, I. DOI: 10.1107/S160053680905541X/ci2998sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053680905541X/ci2998Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C2—H2⋯O2i | 0.93 | 2.55 | 3.4682 (19) | 168 |
Symmetry code: (i)
.
Acknowledgments
The authors thank the DST for the FIST programme.
supplementary crystallographic information
Comment
Benzoic acid and its derivatives are good inhibitors of influenza viruses (Luo et al., 1995). Some benzoic acid derivatives such as 4-aminobenzoic acid have been extensively reported in coordination chemistry as bifunctional organic ligands due to the varieties of their coordination modes (Chen & Chen, 2002; Amiraslanov et al., 1979; Hauptmann et al., 2000). The title compound, a tertiary amine, is used as a part of self-curing two part system for dental/ medical compositions comprising degradable copolymers which are suitable for use as root canal sealants, root canal filling materials, dental restorative materials, implant materials, bone cements and pulp capping materials (Jia et al., 2004).
The molecule of the title compound, C11H15N O2, is essentially planar (r.m.s. deviation 0.035 Å). The molecules are linked into a chain along the a axis by weak C—H···O hydrogen bonds.
Experimental
Ethyl 4-(dimethylamino)benzoate (EDMAB) obtained from Sigma–Aldrich, India, was dissolved in ethanol. The saturated solution was transferred to a crystallizer and covered by a perforated polyethylene sheet for controlled evaporation at room temperature. Colourless crystals were harvested, after five days
Refinement
H atoms were placed at calculated positions and allowed to ride on their carrier atoms, with C-H = 0.93–0.97 Å and Uiso = 1.2Ueq(C) for CH2 and CH groups and Uiso = 1.5Ueq(C) for CH3 group.
Figures
Fig. 1.
The molecular structure of the title compound, showing 30% probability displacement ellipsoids and the atom-numbering scheme.
Crystal data
| C11H15NO2 | F(000) = 416 |
| Mr = 193.24 | Dx = 1.195 Mg m−3 |
| Monoclinic, P21/a | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yab | Cell parameters from 25 reflections |
| a = 12.6949 (8) Å | θ = 2–25° |
| b = 6.6596 (4) Å | µ = 0.08 mm−1 |
| c = 12.8529 (9) Å | T = 293 K |
| β = 98.672 (11)° | Block, colourless |
| V = 1074.20 (12) Å3 | 0.18 × 0.15 × 0.13 mm |
| Z = 4 |
Data collection
| Nonius MACH-3 diffractometer | 1424 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.051 |
| graphite | θmax = 25.0°, θmin = 3.2° |
| ω–2θ scans | h = −1→15 |
| Absorption correction: ψ scan (North et al., 1968) | k = −7→7 |
| Tmin = 0.985, Tmax = 0.989 | l = −15→15 |
| 4088 measured reflections | 3 standard reflections every 60 min |
| 1873 independent reflections | intensity decay: none |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.043 | H-atom parameters constrained |
| wR(F2) = 0.134 | w = 1/[σ2(Fo2) + (0.0618P)2 + 0.2249P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max = 0.001 |
| 1873 reflections | Δρmax = 0.16 e Å−3 |
| 131 parameters | Δρmin = −0.13 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.018 (3) |
Special details
| Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 | ||
| O1 | 0.40072 (9) | 0.08183 (18) | 0.88044 (9) | 0.0572 (4) | |
| O2 | 0.54776 (10) | 0.0855 (2) | 0.80386 (11) | 0.0707 (4) | |
| C1 | 0.34843 (11) | −0.5441 (3) | 0.66547 (12) | 0.0469 (4) | |
| C4 | 0.42325 (12) | −0.1813 (3) | 0.76552 (12) | 0.0461 (4) | |
| N1 | 0.31326 (11) | −0.7203 (3) | 0.61807 (13) | 0.0627 (5) | |
| C7 | 0.46496 (12) | 0.0065 (3) | 0.81690 (12) | 0.0497 (4) | |
| C3 | 0.32462 (12) | −0.2619 (3) | 0.77847 (12) | 0.0479 (4) | |
| H3 | 0.2828 | −0.1950 | 0.8208 | 0.057* | |
| C6 | 0.44776 (12) | −0.4608 (3) | 0.65238 (13) | 0.0528 (5) | |
| H6 | 0.4900 | −0.5262 | 0.6098 | 0.063* | |
| C2 | 0.28788 (12) | −0.4375 (3) | 0.73023 (13) | 0.0491 (4) | |
| H2 | 0.2217 | −0.4869 | 0.7405 | 0.059* | |
| C5 | 0.48322 (12) | −0.2852 (3) | 0.70133 (13) | 0.0531 (5) | |
| H5 | 0.5492 | −0.2343 | 0.6913 | 0.064* | |
| C8 | 0.43523 (14) | 0.2641 (3) | 0.93720 (13) | 0.0574 (5) | |
| H8A | 0.4448 | 0.3713 | 0.8884 | 0.069* | |
| H8B | 0.5023 | 0.2419 | 0.9829 | 0.069* | |
| C1A | 0.37347 (16) | −0.8242 (3) | 0.54815 (15) | 0.0685 (5) | |
| H1A1 | 0.3762 | −0.7437 | 0.4867 | 0.103* | |
| H1A2 | 0.3397 | −0.9501 | 0.5277 | 0.103* | |
| H1A3 | 0.4445 | −0.8481 | 0.5835 | 0.103* | |
| C2A | 0.21248 (14) | −0.8068 (3) | 0.63395 (17) | 0.0690 (6) | |
| H2A1 | 0.2090 | −0.8138 | 0.7080 | 0.103* | |
| H2A2 | 0.2062 | −0.9395 | 0.6044 | 0.103* | |
| H2A3 | 0.1553 | −0.7247 | 0.6000 | 0.103* | |
| C9 | 0.34993 (18) | 0.3176 (3) | 1.00051 (16) | 0.0767 (6) | |
| H9A | 0.2835 | 0.3340 | 0.9545 | 0.115* | |
| H9B | 0.3683 | 0.4409 | 1.0376 | 0.115* | |
| H9C | 0.3431 | 0.2125 | 1.0502 | 0.115* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0615 (7) | 0.0553 (8) | 0.0586 (7) | −0.0047 (6) | 0.0215 (6) | −0.0083 (6) |
| O2 | 0.0583 (7) | 0.0663 (9) | 0.0929 (10) | −0.0141 (7) | 0.0289 (7) | −0.0111 (7) |
| C1 | 0.0436 (8) | 0.0519 (10) | 0.0451 (8) | 0.0024 (7) | 0.0062 (6) | 0.0041 (7) |
| C4 | 0.0448 (8) | 0.0495 (10) | 0.0459 (8) | 0.0027 (7) | 0.0129 (7) | 0.0052 (7) |
| N1 | 0.0543 (8) | 0.0650 (11) | 0.0710 (10) | −0.0081 (7) | 0.0163 (7) | −0.0160 (8) |
| C7 | 0.0481 (8) | 0.0529 (10) | 0.0500 (9) | 0.0034 (8) | 0.0132 (7) | 0.0061 (8) |
| C3 | 0.0465 (8) | 0.0507 (10) | 0.0500 (9) | 0.0056 (7) | 0.0186 (7) | 0.0041 (7) |
| C6 | 0.0470 (8) | 0.0591 (11) | 0.0560 (10) | 0.0024 (8) | 0.0200 (7) | −0.0052 (8) |
| C2 | 0.0399 (8) | 0.0560 (11) | 0.0535 (9) | 0.0010 (7) | 0.0139 (7) | 0.0055 (8) |
| C5 | 0.0431 (8) | 0.0622 (12) | 0.0578 (10) | −0.0045 (8) | 0.0198 (7) | −0.0025 (8) |
| C8 | 0.0711 (11) | 0.0483 (10) | 0.0526 (10) | −0.0032 (9) | 0.0089 (8) | −0.0005 (8) |
| C1A | 0.0794 (13) | 0.0657 (13) | 0.0612 (11) | 0.0003 (11) | 0.0133 (9) | −0.0123 (10) |
| C2A | 0.0613 (11) | 0.0597 (12) | 0.0851 (13) | −0.0125 (10) | 0.0083 (9) | −0.0028 (10) |
| C9 | 0.0951 (15) | 0.0653 (13) | 0.0750 (13) | 0.0003 (12) | 0.0296 (11) | −0.0139 (11) |
Geometric parameters (Å, °)
| O1—C7 | 1.3361 (19) | C2—H2 | 0.9300 |
| O1—C8 | 1.449 (2) | C5—H5 | 0.9300 |
| O2—C7 | 1.2095 (19) | C8—C9 | 1.493 (2) |
| C1—N1 | 1.365 (2) | C8—H8A | 0.9700 |
| C1—C2 | 1.408 (2) | C8—H8B | 0.9700 |
| C1—C6 | 1.411 (2) | C1A—H1A1 | 0.9600 |
| C4—C5 | 1.389 (2) | C1A—H1A2 | 0.9600 |
| C4—C3 | 1.395 (2) | C1A—H1A3 | 0.9600 |
| C4—C7 | 1.475 (3) | C2A—H2A1 | 0.9600 |
| N1—C1A | 1.442 (2) | C2A—H2A2 | 0.9600 |
| N1—C2A | 1.446 (2) | C2A—H2A3 | 0.9600 |
| C3—C2 | 1.372 (2) | C9—H9A | 0.9600 |
| C3—H3 | 0.9300 | C9—H9B | 0.9600 |
| C6—C5 | 1.372 (3) | C9—H9C | 0.9600 |
| C6—H6 | 0.9300 | ||
| C7—O1—C8 | 117.15 (13) | O1—C8—C9 | 106.59 (14) |
| N1—C1—C2 | 121.76 (14) | O1—C8—H8A | 110.4 |
| N1—C1—C6 | 121.51 (14) | C9—C8—H8A | 110.4 |
| C2—C1—C6 | 116.73 (16) | O1—C8—H8B | 110.4 |
| C5—C4—C3 | 117.49 (16) | C9—C8—H8B | 110.4 |
| C5—C4—C7 | 119.76 (14) | H8A—C8—H8B | 108.6 |
| C3—C4—C7 | 122.75 (14) | N1—C1A—H1A1 | 109.5 |
| C1—N1—C1A | 121.48 (15) | N1—C1A—H1A2 | 109.5 |
| C1—N1—C2A | 121.10 (15) | H1A1—C1A—H1A2 | 109.5 |
| C1A—N1—C2A | 117.40 (16) | N1—C1A—H1A3 | 109.5 |
| O2—C7—O1 | 123.00 (17) | H1A1—C1A—H1A3 | 109.5 |
| O2—C7—C4 | 124.59 (15) | H1A2—C1A—H1A3 | 109.5 |
| O1—C7—C4 | 112.41 (13) | N1—C2A—H2A1 | 109.5 |
| C2—C3—C4 | 121.61 (15) | N1—C2A—H2A2 | 109.5 |
| C2—C3—H3 | 119.2 | H2A1—C2A—H2A2 | 109.5 |
| C4—C3—H3 | 119.2 | N1—C2A—H2A3 | 109.5 |
| C5—C6—C1 | 121.20 (14) | H2A1—C2A—H2A3 | 109.5 |
| C5—C6—H6 | 119.4 | H2A2—C2A—H2A3 | 109.5 |
| C1—C6—H6 | 119.4 | C8—C9—H9A | 109.5 |
| C3—C2—C1 | 121.24 (15) | C8—C9—H9B | 109.5 |
| C3—C2—H2 | 119.4 | H9A—C9—H9B | 109.5 |
| C1—C2—H2 | 119.4 | C8—C9—H9C | 109.5 |
| C6—C5—C4 | 121.73 (15) | H9A—C9—H9C | 109.5 |
| C6—C5—H5 | 119.1 | H9B—C9—H9C | 109.5 |
| C4—C5—H5 | 119.1 | ||
| C2—C1—N1—C1A | 177.23 (16) | C7—C4—C3—C2 | −179.64 (15) |
| C6—C1—N1—C1A | −3.2 (3) | N1—C1—C6—C5 | −179.15 (16) |
| C2—C1—N1—C2A | −1.0 (3) | C2—C1—C6—C5 | 0.5 (2) |
| C6—C1—N1—C2A | 178.53 (16) | C4—C3—C2—C1 | 0.1 (2) |
| C8—O1—C7—O2 | −1.5 (2) | N1—C1—C2—C3 | 179.19 (15) |
| C8—O1—C7—C4 | 178.51 (13) | C6—C1—C2—C3 | −0.4 (2) |
| C5—C4—C7—O2 | 3.6 (3) | C1—C6—C5—C4 | −0.2 (3) |
| C3—C4—C7—O2 | −176.55 (16) | C3—C4—C5—C6 | −0.2 (2) |
| C5—C4—C7—O1 | −176.49 (14) | C7—C4—C5—C6 | 179.69 (15) |
| C3—C4—C7—O1 | 3.4 (2) | C7—O1—C8—C9 | 179.26 (15) |
| C5—C4—C3—C2 | 0.3 (2) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C2—H2···O2i | 0.93 | 2.55 | 3.4682 (19) | 168 |
Symmetry codes: (i) x−1/2, −y−1/2, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI2998).
References
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- Chen, H. J. & Chen, X. M. (2002). Inorg. Chim. Acta, 329, 13–21.
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- Hauptmann, R., Kondo, M. & Kitagawa, S. (2000). Z. Kristallogr. New Cryst. Struct.215, 169–172.
- Jia, W.-T. & Jin, S.-H. (2004). US Patent No. 6787584.
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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 datablocks global, I. DOI: 10.1107/S160053680905541X/ci2998sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053680905541X/ci2998Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

