Abstract
In the crystal structure of the title compound, C18H18O4, the full molecule is generated by the application of an inversion centre. The molecule is essentially planar, with an r.m.s. deviation of 0.017 (1) Å for all non-H atoms. The molecules are linked through intermolecular C—H⋯O interactions to form a molecular sheet parallel to the (
02) plane.
Related literature
For the synthesis and related structures, see: Hu et al. (2005 ▶); Aravindan et al. (2003 ▶). For related literature on Schiff bases and their transition metal complexes, see: Ilhan et al. (2009 ▶, 2010 ▶); Yilmaz et al. (2009 ▶).
Experimental
Crystal data
C18H18O4
M r = 298.34
Monoclinic,
a = 8.0624 (7) Å
b = 14.5896 (7) Å
c = 6.8003 (4) Å
β = 108.549 (4)°
V = 758.35 (8) Å3
Z = 2
Mo Kα radiation
μ = 0.09 mm−1
T = 190 K
0.30 × 0.24 × 0.15 mm
Data collection
Rigaku R-AXIS RAPID II diffractometer
Absorption correction: numerical (NUMABS; Higashi, 1999 ▶) T min = 0.980, T max = 0.986
12149 measured reflections
2210 independent reflections
1243 reflections with I > 2σ(I)
R int = 0.041
Refinement
R[F 2 > 2σ(F 2)] = 0.044
wR(F 2) = 0.132
S = 1.13
2210 reflections
100 parameters
H-atom parameters constrained
Δρmax = 0.29 e Å−3
Δρmin = −0.24 e Å−3
Data collection: PROCESS-AUTO (Rigaku/MSC, 2004 ▶); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2004 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: CrystalStructure and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811034210/tk2783sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811034210/tk2783Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811034210/tk2783Isup3.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 |
|---|---|---|---|---|
| C3—H3⋯O1i | 0.95 | 2.53 | 3.397 (2) | 152 |
Symmetry code: (i)
.
Acknowledgments
This work was partly supported by a Grant-in-Aid for Scientific Research (C) (No. 22550013) from the Japan Society for the Promotion of Science. We also acknowledge Golestan University for partial support of this work.
supplementary crystallographic information
Comment
In recent years, much attention has been paid to the synthesis and coordination chemistry of salicylaldehyde, its Schiff base derivatives and transition metal complexes (Hu et al., 2005; Aravindan et al., 2003; Ilhan et al., 2009, 2010; Yilmaz et al., 2009). The two-arm aldehydes can be condensed with primary diamines to form macrocyclic Schiff base ligands (Ilhan et al., 2009, 2010; Yilmaz et al., 2009).
In the crystal structure, the title molecule, 2,2'-[butane-1,4-diylbis(oxy)]dibenzaldehyde (Fig. 1), lies on a crystallographic inversion center, thus indicating that one half the molecule comprises the asymmetric unit. The molecules are linked through intermolecular C3—H3···O1ii contacts (Table 1), resulting in a molecular sheet parallel to the (102) plane (Fig. 2).
Experimental
The title compound was isolated from the reaction between salicylaldehyde and butane-1,4-diamine in the presence of K2CO3 at 85 °C for about 48 h according to the literature (Hu et al., 2005). A small amount of the precipitate was dissolved in a mixture of methanol-chloroform (1:1 v/v) to make a clear solution and kept at room temperature for 3 days to give single crystals suitable for X-ray diffraction.
Refinement
All H atoms were positioned geometrically (C—H = 0.95 or 0.99 Å) and were refined as riding, with Uiso(H) = 1.2Ueq(C).
Figures
Fig. 1.
The molecular structure of the title compound, showing the atom-numbering scheme. Displacement ellipsoids of non-H atoms are drawn at the 50% probability level.
Fig. 2.
A packing diagram of the title compound, showing a molecular sheet formed by C—H···O hydrogen bonds (dashed lines).
Crystal data
| C18H18O4 | F(000) = 316.00 |
| Mr = 298.34 | Dx = 1.306 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71075 Å |
| Hall symbol: -P 2ybc | Cell parameters from 7072 reflections |
| a = 8.0624 (7) Å | θ = 3.0–30.1° |
| b = 14.5896 (7) Å | µ = 0.09 mm−1 |
| c = 6.8003 (4) Å | T = 190 K |
| β = 108.549 (4)° | Block, pale-yellow |
| V = 758.35 (8) Å3 | 0.30 × 0.24 × 0.15 mm |
| Z = 2 |
Data collection
| Rigaku R-AXIS RAPID II diffractometer | 1243 reflections with I > 2σ(I) |
| Detector resolution: 10.00 pixels mm-1 | Rint = 0.041 |
| ω scans | θmax = 30.0° |
| Absorption correction: numerical (NUMABS; Higashi, 1999) | h = −11→11 |
| Tmin = 0.980, Tmax = 0.986 | k = −20→20 |
| 12149 measured reflections | l = −9→9 |
| 2210 independent 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)] = 0.044 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.132 | H-atom parameters constrained |
| S = 1.13 | w = 1/[σ2(Fo2) + (0.0563P)2 + 0.0806P] where P = (Fo2 + 2Fc2)/3 |
| 2210 reflections | (Δ/σ)max = 0.0001 |
| 100 parameters | Δρmax = 0.29 e Å−3 |
| 0 restraints | Δρmin = −0.24 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 | 0.18122 (15) | 0.33844 (8) | 0.1640 (2) | 0.0554 (4) | |
| O2 | 0.69626 (12) | 0.36790 (7) | 0.37956 (16) | 0.0343 (3) | |
| C1 | 0.45915 (17) | 0.26677 (9) | 0.2840 (2) | 0.0307 (3) | |
| C2 | 0.64045 (18) | 0.27981 (9) | 0.3598 (2) | 0.0297 (3) | |
| C3 | 0.75273 (18) | 0.20492 (10) | 0.4082 (2) | 0.0327 (3) | |
| H3 | 0.8758 | 0.2135 | 0.4596 | 0.039* | |
| C4 | 0.6825 (2) | 0.11807 (10) | 0.3803 (2) | 0.0380 (4) | |
| H4 | 0.7586 | 0.0666 | 0.4134 | 0.046* | |
| C5 | 0.5042 (2) | 0.10385 (11) | 0.3054 (3) | 0.0411 (4) | |
| H5 | 0.4582 | 0.0434 | 0.2868 | 0.049* | |
| C6 | 0.3940 (2) | 0.17801 (10) | 0.2582 (2) | 0.0380 (4) | |
| H6 | 0.2712 | 0.1684 | 0.2071 | 0.046* | |
| C7 | 0.3391 (2) | 0.34439 (11) | 0.2358 (3) | 0.0396 (4) | |
| H7 | 0.3882 | 0.4041 | 0.2625 | 0.047* | |
| C8 | 0.88087 (17) | 0.38476 (10) | 0.4570 (2) | 0.0333 (3) | |
| H8A | 0.9405 | 0.3547 | 0.3674 | 0.040* | |
| H8B | 0.9307 | 0.3604 | 0.5996 | 0.040* | |
| C9 | 0.90444 (18) | 0.48669 (10) | 0.4558 (2) | 0.0350 (4) | |
| H9A | 0.8379 | 0.5159 | 0.5387 | 0.042* | |
| H9B | 0.8568 | 0.5096 | 0.3117 | 0.042* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0243 (6) | 0.0575 (8) | 0.0782 (9) | 0.0011 (5) | 0.0074 (6) | −0.0063 (6) |
| O2 | 0.0210 (5) | 0.0285 (5) | 0.0497 (6) | −0.0040 (4) | 0.0060 (4) | −0.0021 (4) |
| C1 | 0.0234 (7) | 0.0324 (8) | 0.0352 (7) | −0.0038 (5) | 0.0077 (6) | −0.0030 (6) |
| C2 | 0.0268 (7) | 0.0287 (7) | 0.0333 (7) | −0.0051 (5) | 0.0092 (6) | −0.0032 (6) |
| C3 | 0.0244 (7) | 0.0320 (8) | 0.0391 (8) | −0.0013 (6) | 0.0065 (6) | −0.0020 (6) |
| C4 | 0.0358 (8) | 0.0316 (8) | 0.0447 (9) | 0.0011 (6) | 0.0102 (7) | 0.0001 (7) |
| C5 | 0.0363 (8) | 0.0317 (8) | 0.0521 (9) | −0.0074 (6) | 0.0095 (7) | −0.0039 (7) |
| C6 | 0.0286 (8) | 0.0388 (9) | 0.0441 (9) | −0.0085 (6) | 0.0081 (7) | −0.0055 (7) |
| C7 | 0.0265 (8) | 0.0372 (9) | 0.0529 (10) | −0.0018 (6) | 0.0095 (7) | −0.0027 (7) |
| C8 | 0.0206 (7) | 0.0313 (7) | 0.0453 (8) | −0.0026 (5) | 0.0068 (6) | −0.0035 (6) |
| C9 | 0.0239 (7) | 0.0294 (7) | 0.0489 (9) | −0.0023 (6) | 0.0075 (6) | −0.0035 (6) |
Geometric parameters (Å, °)
| O1—C7 | 1.2128 (18) | C5—C6 | 1.372 (2) |
| O2—C2 | 1.3543 (16) | C5—H5 | 0.9500 |
| O2—C8 | 1.4333 (16) | C6—H6 | 0.9500 |
| C1—C6 | 1.3874 (19) | C7—H7 | 0.9500 |
| C1—C2 | 1.3997 (19) | C8—C9 | 1.500 (2) |
| C1—C7 | 1.458 (2) | C8—H8A | 0.9900 |
| C2—C3 | 1.390 (2) | C8—H8B | 0.9900 |
| C3—C4 | 1.376 (2) | C9—C9i | 1.516 (3) |
| C3—H3 | 0.9500 | C9—H9A | 0.9900 |
| C4—C5 | 1.379 (2) | C9—H9B | 0.9900 |
| C4—H4 | 0.9500 | ||
| C2—O2—C8 | 118.21 (11) | C5—C6—H6 | 119.5 |
| C6—C1—C2 | 118.83 (13) | C1—C6—H6 | 119.5 |
| C6—C1—C7 | 119.95 (13) | O1—C7—C1 | 124.87 (14) |
| C2—C1—C7 | 121.21 (12) | O1—C7—H7 | 117.6 |
| O2—C2—C3 | 123.48 (13) | C1—C7—H7 | 117.6 |
| O2—C2—C1 | 116.14 (12) | O2—C8—C9 | 106.66 (11) |
| C3—C2—C1 | 120.37 (12) | O2—C8—H8A | 110.4 |
| C4—C3—C2 | 118.85 (13) | C9—C8—H8A | 110.4 |
| C4—C3—H3 | 120.6 | O2—C8—H8B | 110.4 |
| C2—C3—H3 | 120.6 | C9—C8—H8B | 110.4 |
| C3—C4—C5 | 121.62 (14) | H8A—C8—H8B | 108.6 |
| C3—C4—H4 | 119.2 | C8—C9—C9i | 111.50 (15) |
| C5—C4—H4 | 119.2 | C8—C9—H9A | 109.3 |
| C6—C5—C4 | 119.28 (14) | C9i—C9—H9A | 109.3 |
| C6—C5—H5 | 120.4 | C8—C9—H9B | 109.3 |
| C4—C5—H5 | 120.4 | C9i—C9—H9B | 109.3 |
| C5—C6—C1 | 121.05 (14) | H9A—C9—H9B | 108.0 |
| C8—O2—C2—C3 | −0.8 (2) | C3—C4—C5—C6 | −0.2 (2) |
| C8—O2—C2—C1 | 179.88 (12) | C4—C5—C6—C1 | 0.2 (2) |
| C6—C1—C2—O2 | 179.34 (12) | C2—C1—C6—C5 | −0.1 (2) |
| C7—C1—C2—O2 | −1.8 (2) | C7—C1—C6—C5 | −179.02 (15) |
| C6—C1—C2—C3 | 0.0 (2) | C6—C1—C7—O1 | −3.4 (3) |
| C7—C1—C2—C3 | 178.91 (14) | C2—C1—C7—O1 | 177.73 (16) |
| O2—C2—C3—C4 | −179.30 (13) | C2—O2—C8—C9 | 178.18 (12) |
| C1—C2—C3—C4 | 0.0 (2) | O2—C8—C9—C9i | 177.46 (15) |
| C2—C3—C4—C5 | 0.1 (2) |
Symmetry codes: (i) −x+2, −y+1, −z+1.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C3—H3···O1ii | 0.95 | 2.53 | 3.397 (2) | 152 |
Symmetry codes: (ii) x+1, −y+1/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: TK2783).
References
- Aravindan, P. G., Yogavel, M., Thirumavalavan, M., Akilan, P., Velmurugan, D., Kandaswamy, M., Shanmuga Sundara Raj, S. & Fun, H.-K. (2003). Acta Cryst. E59, o806–o807. [DOI] [PubMed]
- Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
- Higashi, T. (1999). NUMABS Rigaku Corporation, Tokyo, Japan.
- Hu, P.-Z., Ma, L.-F., Wang, J.-G., Zhao, B.-T. & Wang, L.-Y. (2005). Acta Cryst. E61, o2775–o2777.
- Ilhan, S., Temel, H. & Pasa, S. (2009). Chin. Chem. Lett. 20, 339–343.
- Ilhan, S., Temel, H., Pasa, S. & Tegin, I. (2010). Russ. J. Coord. Chem. 55, 1402–1409.
- Rigaku/MSC (2004). PROCESS-AUTO and CrystalStructure Rigaku/MSC Inc., The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
- Yilmaz, I., Ilhan, S., Temel, H. & Kilic, A. (2009). J. Incl. Phenom. Macrocycl. Chem. 63, 163–169.
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/S1600536811034210/tk2783sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811034210/tk2783Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811034210/tk2783Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


