organic compounds
Redetermination of 3-methylbenzoic acid
aDepartamento de Química - Facultad de Ciencias, Universidad del Valle, Apartado 25360, Santiago de Cali, Colombia, bInstituto de Química, IQSC, Universidade de São Paulo, São Carlos, Brazil, and cWestCHEM, Department of Pure and Applied Chemistry, University of Strathclyde, 295 Cathedral Street, Glasgow G1 1XL, Scotland
*Correspondence e-mail: rodimo26@yahoo.es
The 8H8O2, contains two crystallographically independent molecules, which form dimers linked by O⋯H—O hydrogen bonds. The benzene rings in the dimers are inclined at a dihedral angle of 7.30 (8)° and both methyl groups display rotational disorder. This redetermination results in a with significantly higher precision than the original determination [Ellas & García-Blanco (1963). Acta Cryst. 16, 434], in which the authors reported only the unit-cell parameters and without any detailed information on the atomic arrangement. In the crystal, dimers are connected by weak C—H⋯O interactions, forming R22(10) and R44(18) rings along [110] and an infinite zigzag chain of dimers along the [001] direction also occurs.
of the title compound, CRelated literature
For a report of the unit-cell dimensions and ). For comparisons with other hydrogen-bond donors, see: Moreno-Fuquen et al. (1997, 2009, 2011). For related structures, see: Barcon et al. (1997). For bond-length data, see: Allen et al. (1987). For a structural discussion of hydrogen bonding, see: Desiraju & Steiner (1999). For general analysis of intermolecular interactions, see: Nardelli (1995) and for graph-set notation of hydrogen-bond patterns, see: Etter (1990).
of the title compound, see: Ellas & García-Blanco (1963Experimental
Crystal data
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Data collection
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Refinement
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Data collection: CrysAlis RED (Oxford Diffraction, 2009); cell CrysAlis RED; data reduction: CrysAlis CCD (Oxford Diffraction, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536811003849/sj5096sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811003849/sj5096Isup2.hkl
3-Methylbenzoic acid (0.545 g, 4 mmol) (Aldrich) was disssolved in ethanol (200 ml). The solution was left to evaporate slowly at room temperature. After three days, colourless crystals of a good quality suitable for X-ray analysis were obtained. M. p. 383 (1) K
All non-hydrogen atoms were identified by
All H atoms were observed in a difference Fourier map. The H-atoms in (I) were placed geometrically [C—H= 0.95 Å for aromatic, C—H= 0.98 Å for methyl, Uiso(H) (1.2 and 1.5 times Ueq of the parent atom respectivelly]. The coordinates of the H1H and H2H hydroxyl H atoms were refined.Data collection: CrysAlis RED (Oxford Diffraction, 2009); cell
CrysAlis RED (Oxford Diffraction, 2009); data reduction: CrysAlis CCD (Oxford Diffraction, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).Fig. 1. The asymmetric unit of the title compound with the atomic labelling scheme and displacement ellipsoids drawn at the 50% probability level. H bonds are drawn as open dashed lines and only one component of the disordered methyl groups is shown. | |
Fig. 2. Part of the crystal structure of (I), showing the formation of R22(10) and R44(18) rings, running along [110]. H bonds are drawn as dashed lines. Symmetry codes: (i) -x + 1, -y + 1,-z; (ii) -x + 2,-y + 2,-z. | |
Fig. 3. Part of the crystal structure of (I), showing the formation of an infinite zigzag chain of dimers along the [001] direction. H bonds are drawn as dashed lines. Symmetry code: (iii) x,-y + 1/2 + 1,+z - 1/2. |
C8H8O2 | F(000) = 576 |
Mr = 136.14 | Dx = 1.295 Mg m−3 |
Monoclinic, P21/c | Melting point: 383(1) K |
Hall symbol: -P 2ybc | Mo Kα radiation, λ = 0.71073 Å |
a = 10.3693 (9) Å | Cell parameters from 2724 reflections |
b = 8.1844 (7) Å | θ = 2.5–31.0° |
c = 16.4715 (17) Å | µ = 0.09 mm−1 |
β = 92.836 (9)° | T = 123 K |
V = 1396.2 (2) Å3 | Tablet, colourless |
Z = 8 | 0.22 × 0.18 × 0.06 mm |
Oxford Diffraction Gemini S diffractometer | 1898 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.055 |
Graphite monochromator | θmax = 29.0°, θmin = 2.8° |
ω scans | h = −12→14 |
13219 measured reflections | k = −11→11 |
3705 independent reflections | l = −22→21 |
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)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.104 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.83 | w = 1/[σ2(Fo2) + (0.0487P)2] where P = (Fo2 + 2Fc2)/3 |
3705 reflections | (Δ/σ)max < 0.001 |
187 parameters | Δρmax = 0.23 e Å−3 |
0 restraints | Δρmin = −0.26 e Å−3 |
C8H8O2 | V = 1396.2 (2) Å3 |
Mr = 136.14 | Z = 8 |
Monoclinic, P21/c | Mo Kα radiation |
a = 10.3693 (9) Å | µ = 0.09 mm−1 |
b = 8.1844 (7) Å | T = 123 K |
c = 16.4715 (17) Å | 0.22 × 0.18 × 0.06 mm |
β = 92.836 (9)° |
Oxford Diffraction Gemini S diffractometer | 1898 reflections with I > 2σ(I) |
13219 measured reflections | Rint = 0.055 |
3705 independent reflections |
R[F2 > 2σ(F2)] = 0.045 | 0 restraints |
wR(F2) = 0.104 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.83 | Δρmax = 0.23 e Å−3 |
3705 reflections | Δρmin = −0.26 e Å−3 |
187 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
O1 | 0.71126 (10) | 0.51712 (14) | 0.01320 (7) | 0.0292 (3) | |
H1H | 0.7709 (16) | 0.584 (2) | −0.0173 (11) | 0.044* | |
O2 | 0.86464 (10) | 0.53282 (13) | 0.11340 (7) | 0.0282 (3) | |
O3 | 1.01280 (11) | 0.71203 (14) | 0.02472 (7) | 0.0305 (3) | |
H2H | 0.9547 (16) | 0.646 (2) | 0.0585 (11) | 0.046* | |
O4 | 0.85611 (10) | 0.70355 (14) | −0.07354 (7) | 0.0331 (3) | |
C1 | 0.75522 (14) | 0.48677 (17) | 0.08633 (9) | 0.0210 (3) | |
C2 | 0.66970 (14) | 0.39351 (17) | 0.13857 (9) | 0.0206 (3) | |
C3 | 0.71441 (14) | 0.34920 (18) | 0.21672 (9) | 0.0224 (4) | |
H3 | 0.7986 | 0.3812 | 0.2357 | 0.027* | |
C4 | 0.63808 (15) | 0.25912 (19) | 0.26726 (10) | 0.0261 (4) | |
C5 | 0.51487 (15) | 0.2154 (2) | 0.23776 (10) | 0.0285 (4) | |
H5 | 0.4613 | 0.1529 | 0.2711 | 0.034* | |
C6 | 0.46861 (15) | 0.2611 (2) | 0.16069 (10) | 0.0290 (4) | |
H6 | 0.3836 | 0.2314 | 0.1422 | 0.035* | |
C7 | 0.54596 (14) | 0.35009 (18) | 0.11062 (10) | 0.0247 (4) | |
H7 | 0.5146 | 0.3811 | 0.0577 | 0.030* | |
C8 | 0.68850 (17) | 0.2078 (2) | 0.35071 (10) | 0.0404 (5) | |
H8A | 0.6218 | 0.1456 | 0.3774 | 0.061* | 0.50 |
H8B | 0.7111 | 0.3050 | 0.3831 | 0.061* | 0.50 |
H8C | 0.7653 | 0.1394 | 0.3460 | 0.061* | 0.50 |
H8D | 0.7770 | 0.2478 | 0.3602 | 0.061* | 0.50 |
H8E | 0.6877 | 0.0883 | 0.3545 | 0.061* | 0.50 |
H8F | 0.6335 | 0.2539 | 0.3917 | 0.061* | 0.50 |
C9 | 0.96396 (14) | 0.75391 (18) | −0.04584 (10) | 0.0229 (4) | |
C10 | 1.04204 (14) | 0.86537 (18) | −0.09412 (10) | 0.0217 (3) | |
C11 | 1.15930 (14) | 0.92586 (18) | −0.06163 (10) | 0.0236 (4) | |
H11 | 1.1880 | 0.8960 | −0.0080 | 0.028* | |
C12 | 1.23462 (14) | 1.02899 (18) | −0.10643 (10) | 0.0244 (4) | |
C13 | 1.19025 (15) | 1.07092 (19) | −0.18470 (10) | 0.0284 (4) | |
H13 | 1.2408 | 1.1415 | −0.2161 | 0.034* | |
C14 | 1.07403 (15) | 1.01207 (19) | −0.21794 (10) | 0.0287 (4) | |
H14 | 1.0454 | 1.0425 | −0.2715 | 0.034* | |
C15 | 0.99964 (14) | 0.90856 (19) | −0.17276 (10) | 0.0256 (4) | |
H15 | 0.9201 | 0.8673 | −0.1954 | 0.031* | |
C16 | 1.36251 (15) | 1.0906 (2) | −0.07154 (11) | 0.0331 (4) | |
H16A | 1.4020 | 1.1616 | −0.1112 | 0.050* | 0.50 |
H16B | 1.4197 | 0.9977 | −0.0589 | 0.050* | 0.50 |
H16C | 1.3491 | 1.1525 | −0.0217 | 0.050* | 0.50 |
H16D | 1.3785 | 1.0462 | −0.0167 | 0.050* | 0.50 |
H16E | 1.3608 | 1.2102 | −0.0690 | 0.050* | 0.50 |
H16F | 1.4315 | 1.0554 | −0.1062 | 0.050* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0287 (6) | 0.0374 (7) | 0.0211 (6) | −0.0020 (5) | −0.0018 (5) | 0.0040 (6) |
O2 | 0.0249 (6) | 0.0303 (6) | 0.0290 (7) | −0.0045 (5) | −0.0046 (5) | 0.0047 (5) |
O3 | 0.0291 (6) | 0.0339 (6) | 0.0284 (7) | −0.0014 (5) | 0.0009 (5) | 0.0092 (6) |
O4 | 0.0247 (6) | 0.0380 (7) | 0.0361 (7) | −0.0051 (5) | −0.0029 (5) | 0.0029 (6) |
C1 | 0.0227 (8) | 0.0188 (7) | 0.0215 (9) | 0.0042 (7) | 0.0000 (7) | −0.0023 (7) |
C2 | 0.0220 (8) | 0.0183 (7) | 0.0217 (9) | 0.0024 (6) | 0.0012 (7) | −0.0023 (7) |
C3 | 0.0185 (8) | 0.0257 (8) | 0.0227 (9) | 0.0011 (6) | −0.0023 (7) | −0.0022 (7) |
C4 | 0.0267 (8) | 0.0276 (9) | 0.0240 (9) | 0.0012 (7) | 0.0004 (7) | 0.0004 (7) |
C5 | 0.0257 (9) | 0.0313 (9) | 0.0287 (10) | −0.0030 (7) | 0.0042 (8) | 0.0013 (8) |
C6 | 0.0221 (8) | 0.0331 (9) | 0.0314 (10) | −0.0015 (7) | −0.0032 (7) | −0.0025 (8) |
C7 | 0.0247 (8) | 0.0262 (8) | 0.0228 (9) | 0.0023 (7) | −0.0030 (7) | −0.0006 (7) |
C8 | 0.0397 (11) | 0.0515 (12) | 0.0292 (10) | −0.0039 (9) | −0.0047 (9) | 0.0111 (9) |
C9 | 0.0223 (8) | 0.0219 (8) | 0.0242 (9) | 0.0032 (7) | −0.0020 (7) | −0.0007 (7) |
C10 | 0.0212 (8) | 0.0188 (7) | 0.0251 (9) | 0.0033 (6) | 0.0015 (7) | 0.0002 (7) |
C11 | 0.0242 (8) | 0.0231 (8) | 0.0233 (9) | 0.0057 (7) | −0.0015 (7) | −0.0004 (7) |
C12 | 0.0227 (8) | 0.0221 (8) | 0.0283 (9) | 0.0034 (7) | 0.0005 (7) | −0.0029 (7) |
C13 | 0.0285 (9) | 0.0240 (8) | 0.0331 (10) | −0.0019 (7) | 0.0038 (8) | 0.0044 (8) |
C14 | 0.0301 (9) | 0.0295 (9) | 0.0261 (9) | 0.0030 (7) | −0.0025 (8) | 0.0049 (8) |
C15 | 0.0216 (8) | 0.0246 (8) | 0.0300 (10) | 0.0005 (7) | −0.0040 (7) | 0.0008 (7) |
C16 | 0.0280 (9) | 0.0316 (9) | 0.0396 (11) | −0.0023 (8) | −0.0012 (8) | −0.0030 (8) |
O1—C1 | 1.2909 (17) | C8—H8D | 0.9800 |
O1—H1H | 0.984 (18) | C8—H8E | 0.9800 |
O2—C1 | 1.2562 (17) | C8—H8F | 0.9800 |
O3—C9 | 1.2911 (18) | C9—C10 | 1.478 (2) |
O3—H2H | 0.998 (19) | C10—C15 | 1.393 (2) |
O4—C9 | 1.2563 (16) | C10—C11 | 1.395 (2) |
C1—C2 | 1.478 (2) | C11—C12 | 1.387 (2) |
C2—C7 | 1.3878 (19) | C11—H11 | 0.9500 |
C2—C3 | 1.394 (2) | C12—C13 | 1.390 (2) |
C3—C4 | 1.389 (2) | C12—C16 | 1.506 (2) |
C3—H3 | 0.9500 | C13—C14 | 1.385 (2) |
C4—C5 | 1.391 (2) | C13—H13 | 0.9500 |
C4—C8 | 1.506 (2) | C14—C15 | 1.387 (2) |
C5—C6 | 1.386 (2) | C14—H14 | 0.9500 |
C5—H5 | 0.9500 | C15—H15 | 0.9500 |
C6—C7 | 1.385 (2) | C16—H16A | 0.9800 |
C6—H6 | 0.9500 | C16—H16B | 0.9800 |
C7—H7 | 0.9500 | C16—H16C | 0.9800 |
C8—H8A | 0.9800 | C16—H16D | 0.9800 |
C8—H8B | 0.9800 | C16—H16E | 0.9800 |
C8—H8C | 0.9800 | C16—H16F | 0.9800 |
C1—O1—H1H | 112.5 (10) | H8E—C8—H8F | 109.5 |
C9—O3—H2H | 115.1 (10) | O4—C9—O3 | 122.84 (15) |
O2—C1—O1 | 122.99 (14) | O4—C9—C10 | 120.58 (14) |
O2—C1—C2 | 120.38 (13) | O3—C9—C10 | 116.58 (13) |
O1—C1—C2 | 116.63 (13) | C15—C10—C11 | 119.73 (14) |
C7—C2—C3 | 119.96 (14) | C15—C10—C9 | 120.06 (14) |
C7—C2—C1 | 120.70 (13) | C11—C10—C9 | 120.20 (14) |
C3—C2—C1 | 119.34 (13) | C12—C11—C10 | 121.00 (14) |
C4—C3—C2 | 121.21 (14) | C12—C11—H11 | 119.5 |
C4—C3—H3 | 119.4 | C10—C11—H11 | 119.5 |
C2—C3—H3 | 119.4 | C11—C12—C13 | 118.31 (14) |
C3—C4—C5 | 117.90 (14) | C11—C12—C16 | 120.61 (14) |
C3—C4—C8 | 120.86 (14) | C13—C12—C16 | 121.07 (15) |
C5—C4—C8 | 121.23 (15) | C14—C13—C12 | 121.48 (15) |
C6—C5—C4 | 121.38 (16) | C14—C13—H13 | 119.3 |
C6—C5—H5 | 119.3 | C12—C13—H13 | 119.3 |
C4—C5—H5 | 119.3 | C13—C14—C15 | 119.76 (15) |
C7—C6—C5 | 120.18 (15) | C13—C14—H14 | 120.1 |
C7—C6—H6 | 119.9 | C15—C14—H14 | 120.1 |
C5—C6—H6 | 119.9 | C14—C15—C10 | 119.71 (14) |
C6—C7—C2 | 119.35 (14) | C14—C15—H15 | 120.1 |
C6—C7—H7 | 120.3 | C10—C15—H15 | 120.1 |
C2—C7—H7 | 120.3 | C12—C16—H16A | 109.5 |
C4—C8—H8A | 109.5 | C12—C16—H16B | 109.5 |
C4—C8—H8B | 109.5 | H16A—C16—H16B | 109.5 |
H8A—C8—H8B | 109.5 | C12—C16—H16C | 109.5 |
C4—C8—H8C | 109.5 | H16A—C16—H16C | 109.5 |
H8A—C8—H8C | 109.5 | H16B—C16—H16C | 109.5 |
H8B—C8—H8C | 109.5 | C12—C16—H16D | 109.5 |
C4—C8—H8D | 109.5 | H16A—C16—H16D | 141.1 |
H8A—C8—H8D | 141.1 | H16B—C16—H16D | 56.3 |
H8B—C8—H8D | 56.3 | H16C—C16—H16D | 56.3 |
H8C—C8—H8D | 56.3 | C12—C16—H16E | 109.5 |
C4—C8—H8E | 109.5 | H16A—C16—H16E | 56.3 |
H8A—C8—H8E | 56.3 | H16B—C16—H16E | 141.1 |
H8B—C8—H8E | 141.1 | H16C—C16—H16E | 56.3 |
H8C—C8—H8E | 56.3 | H16D—C16—H16E | 109.5 |
H8D—C8—H8E | 109.5 | C12—C16—H16F | 109.5 |
C4—C8—H8F | 109.5 | H16A—C16—H16F | 56.3 |
H8A—C8—H8F | 56.3 | H16B—C16—H16F | 56.3 |
H8B—C8—H8F | 56.3 | H16C—C16—H16F | 141.1 |
H8C—C8—H8F | 141.1 | H16D—C16—H16F | 109.5 |
H8D—C8—H8F | 109.5 | H16E—C16—H16F | 109.5 |
O2—C1—C2—C7 | 176.39 (14) | O4—C9—C10—C15 | −3.5 (2) |
O1—C1—C2—C7 | −3.5 (2) | O3—C9—C10—C15 | 176.20 (14) |
O2—C1—C2—C3 | −3.6 (2) | O4—C9—C10—C11 | 177.45 (14) |
O1—C1—C2—C3 | 176.54 (13) | O3—C9—C10—C11 | −2.9 (2) |
C7—C2—C3—C4 | 1.2 (2) | C15—C10—C11—C12 | 0.1 (2) |
C1—C2—C3—C4 | −178.85 (14) | C9—C10—C11—C12 | 179.20 (14) |
C2—C3—C4—C5 | −0.5 (2) | C10—C11—C12—C13 | 0.1 (2) |
C2—C3—C4—C8 | 178.29 (15) | C10—C11—C12—C16 | −178.59 (14) |
C3—C4—C5—C6 | −0.6 (2) | C11—C12—C13—C14 | 0.0 (2) |
C8—C4—C5—C6 | −179.39 (16) | C16—C12—C13—C14 | 178.60 (15) |
C4—C5—C6—C7 | 1.0 (2) | C12—C13—C14—C15 | −0.2 (2) |
C5—C6—C7—C2 | −0.3 (2) | C13—C14—C15—C10 | 0.4 (2) |
C3—C2—C7—C6 | −0.8 (2) | C11—C10—C15—C14 | −0.4 (2) |
C1—C2—C7—C6 | 179.30 (14) | C9—C10—C15—C14 | −179.42 (14) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1H···O4 | 0.984 (18) | 1.634 (19) | 2.6149 (16) | 173.7 (16) |
O3—H2H···O2 | 0.998 (19) | 1.623 (19) | 2.6205 (16) | 177.6 (16) |
C7—H7···O1i | 0.95 | 2.70 | 3.4520 (18) | 137 |
C16—H16E···O1ii | 0.98 | 2.54 | 3.448 (2) | 154 |
C14—H14···O2iii | 0.95 | 2.67 | 3.460 (2) | 141 |
Symmetry codes: (i) −x+1, −y+1, −z; (ii) −x+2, −y+2, −z; (iii) x, −y+3/2, z−1/2. |
Experimental details
Crystal data | |
Chemical formula | C8H8O2 |
Mr | 136.14 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 123 |
a, b, c (Å) | 10.3693 (9), 8.1844 (7), 16.4715 (17) |
β (°) | 92.836 (9) |
V (Å3) | 1396.2 (2) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.22 × 0.18 × 0.06 |
Data collection | |
Diffractometer | Oxford Diffraction Gemini S diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 13219, 3705, 1898 |
Rint | 0.055 |
(sin θ/λ)max (Å−1) | 0.682 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.045, 0.104, 0.83 |
No. of reflections | 3705 |
No. of parameters | 187 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.23, −0.26 |
Computer programs: CrysAlis RED (Oxford Diffraction, 2009), CrysAlis CCD (Oxford Diffraction, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 1997) and Mercury (Macrae et al., 2006).
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1H···O4 | 0.984 (18) | 1.634 (19) | 2.6149 (16) | 173.7 (16) |
O3—H2H···O2 | 0.998 (19) | 1.623 (19) | 2.6205 (16) | 177.6 (16) |
C7—H7···O1i | 0.95 | 2.70 | 3.4520 (18) | 137 |
C16—H16E···O1ii | 0.98 | 2.54 | 3.448 (2) | 154 |
C14—H14···O2iii | 0.95 | 2.67 | 3.460 (2) | 141 |
Symmetry codes: (i) −x+1, −y+1, −z; (ii) −x+2, −y+2, −z; (iii) x, −y+3/2, z−1/2. |
Acknowledgements
RMF is grateful to the Spanish Research Council (CSIC) for the use of a free-of-charge licence to the Cambridge Structural Database. RMF also thanks the Universidad del Valle, Colombia, and the Instituto de Química de São Carlos, USP, Brazil for partial financial support.
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The title compound (I) was investigated in a continuation of our studies on the formation of molecular complexes from N-oxide derivatives with different hydrogen bond donors (Moreno-Fuquen et al., 1997, 2009, 2011). The structure of a similar molecule was taken to compare with the title molecule (Barcon et al., 1997). A perspective view of the dimeric hydrogen-bonding in (I), showing the atomic numbering scheme, is given in Figure 1. Both molecules of m-toluic acid are held together by intermolecular O···H—O hydrogen bonds of moderate character (Desiraju & Steiner, 1999). Indeed, carbonylic O4 and O2 atoms are linked to O1 and O3 atoms with O···O distances of 2.6149 (16) and 2.6205 (16)Å respectively. The two aromatic rings in (I) form a dihedral angle of 7.30 (8)°. Both methyl groups display rotational disorder. The rotamer ratio found in this modeling was 50:50. In (I), Fig. 1, bond lengths and bond angles are in normal ranges (Allen et al., 1987). The title crystal structure also exhibits other weak C—H···O interactions (see Table 1, Nardelli, 1995). Indeed, in a first substructure, atom C7 acts as hydrogen bond donor to O1i in the molecule at (-x + 1,-y + 1,-z) and the C16 atom acts as hydrogen bond donor to O1ii in the molecule at (-x + 2,-y + 2,-z). The propagation of these interactions generates rings with graph-set notation R22(10) and R44(18) (Etter, 1990), running along the [110] direction (see Fig. 2). In a second substructure, atom C14 acts as a hydrogen bond donor to O2iii in the molecule at (x,-y + 1/2 + 1,+z - 1/2). The propagation of this interaction forms an infinite zigzag chain of dimers along the [001] direction (see Fig. 3). All of these interactions in the [110] and [001] directions define the bulk structure of the crystal.