Abstract
In the title compound, C6H6N2O·C8H8O3, an equimolar co-crystal of nicotinamide and vanillin, the aromatic ring and the amide fragment of the nicotinamide molecule make a dihedral angle of 32.6 (2)°. The vanillin molecule is almost planar, with an r.m.s. deviation for all non-H atoms of 0.0094 Å. The vaniline and nicotinamide aromatic rings are nearly coplanar, the dihedral angle between them being 3.20 (9)°. In the crystal, the two components are linked through N—H⋯O and O—H⋯N hydrogen bonds into chains along the a axis. The chains are connected via C—H⋯O interactions, forming a three-dimensional polymeric structure.
Related literature
For the crystal structure of nicotinamide, see: Miwa et al. (1999 ▶); Li et al. (2011 ▶). For the structure of vanillin, see: Velavan et al. (1995 ▶).
Experimental
Crystal data
C6H6N2O·C8H8O3
M r = 274.27
Triclinic,
a = 4.8979 (1) Å
b = 8.5440 (2) Å
c = 15.4713 (4) Å
α = 98.108 (1)°
β = 92.810 (2)°
γ = 94.784 (2)°
V = 637.52 (3) Å3
Z = 2
Mo Kα radiation
μ = 0.11 mm−1
T = 100 K
0.22 × 0.14 × 0.04 mm
Data collection
Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.977, T max = 0.996
3432 measured reflections
2243 independent reflections
1862 reflections with I > 2σ(I)
R int = 0.019
Refinement
R[F 2 > 2σ(F 2)] = 0.045
wR(F 2) = 0.112
S = 1.05
2243 reflections
191 parameters
4 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.66 e Å−3
Δρmin = −0.28 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: X-SEED (Barbour, 2001 ▶); software used to prepare material for publication: SHELXL97 and publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811045648/pv2471sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811045648/pv2471Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811045648/pv2471Isup3.cml
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 |
|---|---|---|---|---|
| N1—H1A⋯O4i | 0.87 (2) | 2.05 (2) | 2.900 (2) | 167 (2) |
| N1—H1B⋯O2ii | 0.87 (2) | 2.42 (2) | 3.085 (2) | 134 (2) |
| N1—H1B⋯O3ii | 0.87 (2) | 2.20 (2) | 3.019 (2) | 156 (2) |
| O2—H2⋯N2iii | 0.85 (2) | 1.80 (2) | 2.634 (2) | 164 (2) |
| C8—H8A⋯O1iv | 0.98 | 2.59 | 3.381 (3) | 137 |
| C8—H8C⋯O2i | 0.98 | 2.55 | 3.337 (2) | 138 |
| C13—H13⋯O1v | 0.95 | 2.49 | 3.185 (3) | 130 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
.
Acknowledgments
IIUM is acknowledged for funding this study (Endowment fund A No. EDWA10–150–0697).
supplementary crystallographic information
Comment
The crystal structures of nicotinamide (Miwa et al.,1999; Li et al., 2011) and 4-hydroxy-3-methoxybenzaldehyde, vanillin, (Velavan et al.,1995) have been previously reported. The title compound is an equimolar cocrystal of nicotinamide and vanillin (Fig. 1). The nicotinamide aromatic ring and the plane of the amide fragment, N1—C9—O4, are twisted with respect to each other, making a dihedral angle of 32.6 (2)°. The vanillin molecule is essentially planar, the highest deviation from the best plane passing through all non-H atoms being 0.0156 (13) Å for O3 atom. In the crystal, the molecules of nicotinamide and vanillin are linked through N—H···O and O—H···N hydrogen bonds into infinite chains along the a axis (Fig. 2). The chains are connected via C—H···O interactions (Table 1 and Fig. 2) to form a three-dimensional polymeric structure.
Experimental
A mixture of vanillin (1.52 g, 0.1 mol) and nicotinamide (1.22 g, 0.1 mol) in ethanol (30 ml) was heated for 1 hr. The solvent was then evaporated partially and the solution was left at room temperature. The colorless crystals of the title compound were obtained in a day.
Refinement
The C-bound H atoms were placed at calculated positions and were treated as riding on their parent C atoms with C—H distances of 0.95 (aryl) and 0.98 (methyl) Å. The N– and O-bound H atoms were located in a difference Fourier map, and refined with distance restraints of O—H = 0.84 (2) Å and N—H = 0.88 (2) Å. For all H atoms, Uiso(H) was set to 1.2–1.5eq(carrier atom). An additional rigid-bond type restraint (DELU in SHELXL97) was placed on the displacement parameters of C1 and C2.
Figures
Fig. 1.
Molecular structure of the title compound with displacement ellipsoids drawn at 50% probability level. Hydrogen atoms are drawn as spheres of arbitrary radii.
Fig. 2.
A chain along the a axis formed by N—H···O and O—H···N hydrogen bonds.
Crystal data
| C6H6N2O·C8H8O3 | Z = 2 |
| Mr = 274.27 | F(000) = 288 |
| Triclinic, P1 | Dx = 1.429 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 4.8979 (1) Å | Cell parameters from 1226 reflections |
| b = 8.5440 (2) Å | θ = 2.6–29.7° |
| c = 15.4713 (4) Å | µ = 0.11 mm−1 |
| α = 98.108 (1)° | T = 100 K |
| β = 92.810 (2)° | Lath, colorless |
| γ = 94.784 (2)° | 0.22 × 0.14 × 0.04 mm |
| V = 637.52 (3) Å3 |
Data collection
| Bruker APEXII CCD diffractometer | 2243 independent reflections |
| Radiation source: fine-focus sealed tube | 1862 reflections with I > 2σ(I) |
| graphite | Rint = 0.019 |
| φ and ω scans | θmax = 25.3°, θmin = 2.4° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −5→5 |
| Tmin = 0.977, Tmax = 0.996 | k = −10→10 |
| 3432 measured reflections | l = −18→18 |
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)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.112 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0439P)2 + 0.4685P] where P = (Fo2 + 2Fc2)/3 |
| 2243 reflections | (Δ/σ)max < 0.001 |
| 191 parameters | Δρmax = 0.66 e Å−3 |
| 4 restraints | Δρmin = −0.28 e Å−3 |
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 | ||
| O1 | 0.3651 (3) | 0.83011 (19) | 0.61085 (10) | 0.0359 (4) | |
| O2 | 0.8107 (3) | 0.63328 (16) | 0.23075 (9) | 0.0195 (3) | |
| H2 | 0.949 (4) | 0.698 (2) | 0.2250 (15) | 0.029* | |
| O3 | 0.4028 (3) | 0.44026 (16) | 0.25734 (9) | 0.0218 (3) | |
| C1 | 0.3070 (5) | 0.7306 (3) | 0.54863 (14) | 0.0286 (5) | |
| H1 | 0.1529 | 0.6570 | 0.5522 | 0.034* | |
| C2 | 0.4516 (4) | 0.7113 (2) | 0.46701 (13) | 0.0210 (4) | |
| C3 | 0.6726 (4) | 0.8148 (2) | 0.45164 (13) | 0.0221 (5) | |
| H3 | 0.7380 | 0.9016 | 0.4951 | 0.026* | |
| C4 | 0.7972 (4) | 0.7912 (2) | 0.37307 (13) | 0.0204 (4) | |
| H4 | 0.9482 | 0.8620 | 0.3629 | 0.024* | |
| C5 | 0.7035 (4) | 0.6648 (2) | 0.30888 (12) | 0.0166 (4) | |
| C6 | 0.4793 (4) | 0.5600 (2) | 0.32443 (12) | 0.0176 (4) | |
| C7 | 0.3561 (4) | 0.5847 (2) | 0.40255 (13) | 0.0208 (5) | |
| H7 | 0.2040 | 0.5146 | 0.4128 | 0.025* | |
| C8 | 0.1709 (4) | 0.3323 (2) | 0.26827 (14) | 0.0217 (5) | |
| H8A | 0.2110 | 0.2765 | 0.3179 | 0.033* | |
| H8B | 0.1328 | 0.2551 | 0.2150 | 0.033* | |
| H8C | 0.0103 | 0.3917 | 0.2793 | 0.033* | |
| O4 | 0.8254 (3) | 0.71964 (19) | −0.04761 (9) | 0.0299 (4) | |
| N1 | 0.3766 (4) | 0.6341 (2) | −0.07875 (11) | 0.0205 (4) | |
| H1A | 0.207 (3) | 0.645 (3) | −0.0672 (14) | 0.025* | |
| H1B | 0.415 (4) | 0.586 (2) | −0.1293 (11) | 0.025* | |
| N2 | 0.2385 (3) | 0.80224 (19) | 0.18395 (10) | 0.0170 (4) | |
| C9 | 0.5840 (4) | 0.7129 (2) | −0.02755 (13) | 0.0197 (4) | |
| C10 | 0.5123 (4) | 0.7959 (2) | 0.05932 (12) | 0.0169 (4) | |
| C11 | 0.6653 (4) | 0.9350 (2) | 0.09779 (13) | 0.0201 (4) | |
| H11 | 0.8121 | 0.9801 | 0.0687 | 0.024* | |
| C12 | 0.5998 (4) | 1.0066 (2) | 0.17913 (13) | 0.0220 (5) | |
| H12 | 0.6997 | 1.1023 | 0.2066 | 0.026* | |
| C13 | 0.3864 (4) | 0.9363 (2) | 0.21971 (13) | 0.0192 (4) | |
| H13 | 0.3429 | 0.9856 | 0.2757 | 0.023* | |
| C14 | 0.3015 (4) | 0.7346 (2) | 0.10499 (12) | 0.0162 (4) | |
| H14 | 0.1966 | 0.6397 | 0.0788 | 0.019* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0440 (10) | 0.0363 (9) | 0.0266 (9) | 0.0056 (8) | 0.0038 (7) | 0.0006 (7) |
| O2 | 0.0182 (8) | 0.0217 (7) | 0.0174 (7) | −0.0031 (6) | 0.0053 (6) | 0.0004 (6) |
| O3 | 0.0223 (8) | 0.0214 (7) | 0.0198 (7) | −0.0045 (6) | 0.0064 (6) | −0.0016 (6) |
| C1 | 0.0356 (13) | 0.0308 (12) | 0.0189 (10) | 0.0104 (10) | −0.0028 (9) | −0.0012 (9) |
| C2 | 0.0226 (11) | 0.0246 (11) | 0.0170 (10) | 0.0074 (8) | 0.0004 (8) | 0.0045 (8) |
| C3 | 0.0270 (11) | 0.0214 (10) | 0.0165 (10) | 0.0060 (9) | −0.0036 (8) | −0.0020 (8) |
| C4 | 0.0187 (10) | 0.0193 (10) | 0.0218 (11) | −0.0018 (8) | −0.0001 (8) | 0.0014 (8) |
| C5 | 0.0157 (10) | 0.0209 (10) | 0.0145 (9) | 0.0054 (8) | 0.0026 (8) | 0.0043 (8) |
| C6 | 0.0193 (10) | 0.0176 (10) | 0.0157 (10) | 0.0033 (8) | 0.0002 (8) | 0.0007 (8) |
| C7 | 0.0193 (11) | 0.0242 (11) | 0.0199 (10) | 0.0020 (8) | 0.0046 (8) | 0.0055 (8) |
| C8 | 0.0185 (11) | 0.0198 (10) | 0.0259 (11) | −0.0031 (8) | 0.0035 (8) | 0.0021 (8) |
| O4 | 0.0144 (8) | 0.0516 (10) | 0.0228 (8) | 0.0064 (7) | 0.0038 (6) | −0.0003 (7) |
| N1 | 0.0172 (9) | 0.0279 (9) | 0.0153 (9) | 0.0046 (7) | 0.0035 (7) | −0.0030 (7) |
| N2 | 0.0171 (9) | 0.0194 (8) | 0.0148 (8) | 0.0031 (7) | 0.0012 (6) | 0.0027 (6) |
| C9 | 0.0178 (11) | 0.0255 (11) | 0.0168 (10) | 0.0055 (8) | 0.0018 (8) | 0.0042 (8) |
| C10 | 0.0144 (10) | 0.0210 (10) | 0.0156 (10) | 0.0038 (8) | −0.0008 (7) | 0.0030 (8) |
| C11 | 0.0149 (10) | 0.0240 (10) | 0.0221 (10) | 0.0003 (8) | 0.0020 (8) | 0.0058 (8) |
| C12 | 0.0227 (11) | 0.0180 (10) | 0.0234 (11) | −0.0030 (8) | −0.0011 (8) | −0.0002 (8) |
| C13 | 0.0217 (11) | 0.0192 (10) | 0.0160 (10) | 0.0031 (8) | 0.0002 (8) | 0.0001 (8) |
| C14 | 0.0157 (10) | 0.0162 (9) | 0.0161 (10) | 0.0009 (7) | −0.0013 (8) | 0.0012 (7) |
Geometric parameters (Å, °)
| O1—C1 | 1.197 (3) | C8—H8B | 0.9800 |
| O2—C5 | 1.343 (2) | C8—H8C | 0.9800 |
| O2—H2 | 0.854 (16) | O4—C9 | 1.236 (2) |
| O3—C6 | 1.365 (2) | N1—C9 | 1.330 (3) |
| O3—C8 | 1.435 (2) | N1—H1A | 0.868 (16) |
| C1—C2 | 1.474 (3) | N1—H1B | 0.869 (16) |
| C1—H1 | 0.9500 | N2—C13 | 1.336 (2) |
| C2—C3 | 1.391 (3) | N2—C14 | 1.338 (2) |
| C2—C7 | 1.396 (3) | C9—C10 | 1.500 (3) |
| C3—C4 | 1.384 (3) | C10—C14 | 1.388 (3) |
| C3—H3 | 0.9500 | C10—C11 | 1.392 (3) |
| C4—C5 | 1.391 (3) | C11—C12 | 1.384 (3) |
| C4—H4 | 0.9500 | C11—H11 | 0.9500 |
| C5—C6 | 1.410 (3) | C12—C13 | 1.384 (3) |
| C6—C7 | 1.375 (3) | C12—H12 | 0.9500 |
| C7—H7 | 0.9500 | C13—H13 | 0.9500 |
| C8—H8A | 0.9800 | C14—H14 | 0.9500 |
| C5—O2—H2 | 112.6 (16) | O3—C8—H8C | 109.5 |
| C6—O3—C8 | 117.44 (15) | H8A—C8—H8C | 109.5 |
| O1—C1—C2 | 126.2 (2) | H8B—C8—H8C | 109.5 |
| O1—C1—H1 | 116.9 | C9—N1—H1A | 121.6 (15) |
| C2—C1—H1 | 116.9 | C9—N1—H1B | 117.5 (15) |
| C3—C2—C7 | 119.56 (18) | H1A—N1—H1B | 120 (2) |
| C3—C2—C1 | 122.83 (19) | C13—N2—C14 | 117.72 (17) |
| C7—C2—C1 | 117.59 (19) | O4—C9—N1 | 123.82 (19) |
| C4—C3—C2 | 119.93 (19) | O4—C9—C10 | 119.84 (18) |
| C4—C3—H3 | 120.0 | N1—C9—C10 | 116.34 (17) |
| C2—C3—H3 | 120.0 | C14—C10—C11 | 118.15 (18) |
| C3—C4—C5 | 120.68 (18) | C14—C10—C9 | 121.73 (18) |
| C3—C4—H4 | 119.7 | C11—C10—C9 | 120.07 (18) |
| C5—C4—H4 | 119.7 | C12—C11—C10 | 118.88 (18) |
| O2—C5—C4 | 124.72 (18) | C12—C11—H11 | 120.6 |
| O2—C5—C6 | 115.90 (17) | C10—C11—H11 | 120.6 |
| C4—C5—C6 | 119.38 (18) | C13—C12—C11 | 118.77 (19) |
| O3—C6—C7 | 125.62 (18) | C13—C12—H12 | 120.6 |
| O3—C6—C5 | 114.82 (17) | C11—C12—H12 | 120.6 |
| C7—C6—C5 | 119.56 (18) | N2—C13—C12 | 123.12 (18) |
| C6—C7—C2 | 120.88 (19) | N2—C13—H13 | 118.4 |
| C6—C7—H7 | 119.6 | C12—C13—H13 | 118.4 |
| C2—C7—H7 | 119.6 | N2—C14—C10 | 123.34 (18) |
| O3—C8—H8A | 109.5 | N2—C14—H14 | 118.3 |
| O3—C8—H8B | 109.5 | C10—C14—H14 | 118.3 |
| H8A—C8—H8B | 109.5 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···O4i | 0.87 (2) | 2.05 (2) | 2.900 (2) | 167 (2) |
| N1—H1B···O2ii | 0.87 (2) | 2.42 (2) | 3.085 (2) | 134.(2) |
| N1—H1B···O3ii | 0.87 (2) | 2.20 (2) | 3.019 (2) | 156 (2) |
| O2—H2···N2iii | 0.85 (2) | 1.80 (2) | 2.634 (2) | 164 (2) |
| C8—H8A···O1iv | 0.98 | 2.59 | 3.381 (3) | 137. |
| C8—H8C···O2i | 0.98 | 2.55 | 3.337 (2) | 138. |
| C13—H13···O1v | 0.95 | 2.49 | 3.185 (3) | 130. |
Symmetry codes: (i) x−1, y, z; (ii) −x+1, −y+1, −z; (iii) x+1, y, z; (iv) −x+1, −y+1, −z+1; (v) −x+1, −y+2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2471).
References
- Barbour, L. J. (2001). J. Supramol. Chem, 1, 189–191.
- Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
- Li, J., Bourne, S. A. & Caira, M. R. (2011). Chem. Commun. 47, 1530–1532. [DOI] [PubMed]
- Miwa, Y., Mizuno, T., Tsuchida, K., Taga, T. & Iwata, Y. (1999). Acta Cryst. B55, 78–84. [DOI] [PubMed]
- Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Velavan, R., Sureshkumar, P., Sivakumar, K. & Natarajan, S. (1995). Acta Cryst. C51, 1131–1133.
- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
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/S1600536811045648/pv2471sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811045648/pv2471Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811045648/pv2471Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


