organic compounds
1,4-Bis(pyridin-3-ylmethoxy)benzene
aCollege of Chemistry and Materials Science, Heilongjiang University, Harbin 150080, People's Republic of China
*Correspondence e-mail: hgf1000@163.com
The 18H16N2O2, contains one half-molecule. The central benzene ring forms a dihedral angle of 66.8 (1)° with two outer aromatic rings. In the weak intermolecular C—H⋯N hydrogen bonds link molecules into sheets parallel to (104).
of the centrosymmetric title compound, CRelated literature
For general background to bridging molecules with pyridyl substituents at the terminal positions, see: McMorran & Steel (1998); Zaman et al. (2005). For details of the synthesis, see: Gao et al. (2004). For a related structure, see: Gao et al. (2006).
Experimental
Crystal data
|
Refinement
|
Data collection: RAPID-AUTO (Rigaku, 1998); cell RAPID-AUTO; data reduction: CrystalClear (Rigaku/MSC, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536809036265/cv2613sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809036265/cv2613Isup2.hkl
The 1,4-bis(3-pyridylmethoxy)benzene was synthesized by the reaction of p-benzenediol and 3-chloromethylpyridine hydrochloride under nitrogen atmosphere and alkaline condition (Gao et al., 2004; Gao et al., 2006). Colourless block-shaped crystals of title compound were obtained by slow evaporation of an methanol solution after three days.
All H atoms were placed in calculated positions with C—H = 0.93 Å (aromatic), C—H = 0.97 Å (methylene), and treated as riding on their parent atoms, with Uiso(H) = 1.2Ueq(C).
Data collection: RAPID-AUTO (Rigaku, 1998); cell
RAPID-AUTO (Rigaku, 1998); data reduction: CrystalClear (Rigaku/MSC, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).C18H16N2O2 | F(000) = 308 |
Mr = 292.33 | Dx = 1.321 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 4889 reflections |
a = 6.852 (5) Å | θ = 3.7–27.5° |
b = 5.688 (3) Å | µ = 0.09 mm−1 |
c = 18.861 (12) Å | T = 291 K |
β = 90.60 (3)° | Block, colourless |
V = 735.0 (8) Å3 | 0.22 × 0.20 × 0.19 mm |
Z = 2 |
Rigaku RAXIS-RAPID diffractometer | 1684 independent reflections |
Radiation source: fine-focus sealed tube | 1213 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.030 |
ω scan | θmax = 27.5°, θmin = 3.7° |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | h = −8→8 |
Tmin = 0.981, Tmax = 0.984 | k = −6→7 |
6855 measured reflections | l = −24→24 |
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)] = 0.041 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.118 | H-atom parameters constrained |
S = 1.09 | w = 1/[σ2(Fo2) + (0.0606P)2 + 0.0635P] where P = (Fo2 + 2Fc2)/3 |
1684 reflections | (Δ/σ)max < 0.001 |
100 parameters | Δρmax = 0.24 e Å−3 |
0 restraints | Δρmin = −0.14 e Å−3 |
C18H16N2O2 | V = 735.0 (8) Å3 |
Mr = 292.33 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 6.852 (5) Å | µ = 0.09 mm−1 |
b = 5.688 (3) Å | T = 291 K |
c = 18.861 (12) Å | 0.22 × 0.20 × 0.19 mm |
β = 90.60 (3)° |
Rigaku RAXIS-RAPID diffractometer | 1684 independent reflections |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | 1213 reflections with I > 2σ(I) |
Tmin = 0.981, Tmax = 0.984 | Rint = 0.030 |
6855 measured reflections |
R[F2 > 2σ(F2)] = 0.041 | 0 restraints |
wR(F2) = 0.118 | H-atom parameters constrained |
S = 1.09 | Δρmax = 0.24 e Å−3 |
1684 reflections | Δρmin = −0.14 e Å−3 |
100 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 | ||
C1 | 0.8460 (2) | −0.0288 (3) | 0.20865 (8) | 0.0485 (4) | |
H1 | 0.9650 | −0.0611 | 0.2307 | 0.058* | |
C2 | 0.7721 (2) | −0.1906 (3) | 0.16191 (8) | 0.0530 (4) | |
H2 | 0.8404 | −0.3281 | 0.1524 | 0.064* | |
C3 | 0.5951 (2) | −0.1469 (3) | 0.12921 (8) | 0.0484 (4) | |
H3 | 0.5422 | −0.2545 | 0.0972 | 0.058* | |
C4 | 0.49744 (18) | 0.0588 (2) | 0.14460 (7) | 0.0367 (3) | |
C5 | 0.5857 (2) | 0.2119 (3) | 0.19208 (7) | 0.0428 (4) | |
H5 | 0.5213 | 0.3517 | 0.2022 | 0.051* | |
C6 | 0.30072 (19) | 0.1158 (3) | 0.11378 (7) | 0.0433 (4) | |
H6A | 0.2437 | −0.0233 | 0.0922 | 0.052* | |
H6B | 0.2144 | 0.1704 | 0.1507 | 0.052* | |
C7 | 0.15874 (17) | 0.3913 (2) | 0.03246 (7) | 0.0368 (3) | |
C8 | −0.02824 (18) | 0.3034 (3) | 0.04198 (7) | 0.0408 (3) | |
H8 | −0.0477 | 0.1710 | 0.0700 | 0.049* | |
C9 | −0.18583 (18) | 0.4142 (3) | 0.00955 (7) | 0.0408 (3) | |
H9 | −0.3112 | 0.3563 | 0.0163 | 0.049* | |
N1 | 0.75686 (17) | 0.1729 (2) | 0.22431 (7) | 0.0510 (4) | |
O1 | 0.32526 (13) | 0.29466 (19) | 0.06180 (5) | 0.0509 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0308 (7) | 0.0572 (9) | 0.0571 (9) | 0.0002 (6) | −0.0101 (6) | 0.0171 (7) |
C2 | 0.0439 (9) | 0.0449 (8) | 0.0700 (10) | 0.0117 (7) | −0.0063 (7) | 0.0064 (8) |
C3 | 0.0487 (8) | 0.0432 (8) | 0.0532 (8) | 0.0035 (7) | −0.0108 (6) | −0.0038 (7) |
C4 | 0.0308 (6) | 0.0395 (7) | 0.0396 (7) | −0.0005 (5) | −0.0056 (5) | 0.0083 (6) |
C5 | 0.0371 (7) | 0.0388 (7) | 0.0525 (8) | 0.0016 (6) | −0.0069 (6) | 0.0008 (6) |
C6 | 0.0334 (7) | 0.0482 (8) | 0.0482 (8) | −0.0010 (6) | −0.0093 (6) | 0.0109 (6) |
C7 | 0.0264 (6) | 0.0465 (8) | 0.0374 (6) | 0.0056 (5) | −0.0046 (5) | 0.0038 (6) |
C8 | 0.0308 (7) | 0.0475 (8) | 0.0438 (7) | −0.0007 (6) | −0.0045 (5) | 0.0111 (6) |
C9 | 0.0250 (6) | 0.0530 (8) | 0.0444 (7) | −0.0016 (6) | −0.0030 (5) | 0.0073 (6) |
N1 | 0.0394 (7) | 0.0538 (8) | 0.0596 (8) | −0.0056 (6) | −0.0145 (6) | 0.0004 (6) |
O1 | 0.0269 (5) | 0.0683 (7) | 0.0573 (6) | 0.0058 (4) | −0.0048 (4) | 0.0267 (5) |
C1—N1 | 1.334 (2) | C6—O1 | 1.4239 (17) |
C1—C2 | 1.368 (2) | C6—H6A | 0.9700 |
C1—H1 | 0.9300 | C6—H6B | 0.9700 |
C2—C3 | 1.378 (2) | C7—C9i | 1.374 (2) |
C2—H2 | 0.9300 | C7—O1 | 1.3773 (17) |
C3—C4 | 1.380 (2) | C7—C8 | 1.389 (2) |
C3—H3 | 0.9300 | C8—C9 | 1.3869 (19) |
C4—C5 | 1.3839 (19) | C8—H8 | 0.9300 |
C4—C6 | 1.4979 (19) | C9—C7i | 1.374 (2) |
C5—N1 | 1.3336 (19) | C9—H9 | 0.9300 |
C5—H5 | 0.9300 | ||
N1—C1—C2 | 123.64 (13) | O1—C6—H6A | 110.1 |
N1—C1—H1 | 118.2 | C4—C6—H6A | 110.1 |
C2—C1—H1 | 118.2 | O1—C6—H6B | 110.1 |
C1—C2—C3 | 119.03 (14) | C4—C6—H6B | 110.1 |
C1—C2—H2 | 120.5 | H6A—C6—H6B | 108.4 |
C3—C2—H2 | 120.5 | C9i—C7—O1 | 115.88 (11) |
C2—C3—C4 | 119.04 (14) | C9i—C7—C8 | 119.64 (12) |
C2—C3—H3 | 120.5 | O1—C7—C8 | 124.47 (13) |
C4—C3—H3 | 120.5 | C9—C8—C7 | 119.64 (14) |
C3—C4—C5 | 117.37 (13) | C9—C8—H8 | 120.2 |
C3—C4—C6 | 122.56 (13) | C7—C8—H8 | 120.2 |
C5—C4—C6 | 120.04 (13) | C7i—C9—C8 | 120.71 (12) |
N1—C5—C4 | 124.50 (14) | C7i—C9—H9 | 119.6 |
N1—C5—H5 | 117.7 | C8—C9—H9 | 119.6 |
C4—C5—H5 | 117.7 | C5—N1—C1 | 116.41 (13) |
O1—C6—C4 | 108.04 (11) | C7—O1—C6 | 117.28 (10) |
Symmetry code: (i) −x, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···N1ii | 0.93 | 2.57 | 3.437 (3) | 155 |
Symmetry code: (ii) −x+2, y−1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C18H16N2O2 |
Mr | 292.33 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 291 |
a, b, c (Å) | 6.852 (5), 5.688 (3), 18.861 (12) |
β (°) | 90.60 (3) |
V (Å3) | 735.0 (8) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.22 × 0.20 × 0.19 |
Data collection | |
Diffractometer | Rigaku RAXIS-RAPID diffractometer |
Absorption correction | Multi-scan (ABSCOR; Higashi, 1995) |
Tmin, Tmax | 0.981, 0.984 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6855, 1684, 1213 |
Rint | 0.030 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.041, 0.118, 1.09 |
No. of reflections | 1684 |
No. of parameters | 100 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.24, −0.14 |
Computer programs: RAPID-AUTO (Rigaku, 1998), CrystalClear (Rigaku/MSC, 2002), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···N1i | 0.93 | 2.57 | 3.437 (3) | 155.2 |
Symmetry code: (i) −x+2, y−1/2, −z+1/2. |
Acknowledgements
The authors thank the Specialized Research Funds for Technological Innovative Talent in Harbin (RC2009XK018007) and Heilongjiang University for supporting this study.
References
Gao, C.-M., Cao, D. & Zhu, L. (2004). Photogr. Sci. Photochem. 22, 103–107. CAS Google Scholar
Gao, J.-S., Liu, Y., Hou, G.-F., Yu, Y.-H. & Yan, P.-F. (2006). Acta Cryst. E62, o5645–o5646. Web of Science CSD CrossRef IUCr Journals Google Scholar
Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan. Google Scholar
McMorran, D. A. & Steel, P. J. (1998). Angew. Chem. Int. Ed. 37, 3295–3297. CrossRef CAS Google Scholar
Rigaku (1998). RAPID-AUTO. Rigaku Corporation, Tokyo, Japan. Google Scholar
Rigaku/MSC (2002). CrystalClear. Rigaku/MSC Inc., The Woodlands, Texas, USA. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Zaman, Md. B., Udachin, K., Ripmeester, J. A., Smith, M. D. & zur Loye, H.-C. (2005). Inorg. Chem. 44, 5047–5059. Web of Science CSD CrossRef PubMed CAS Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
The bridging molecules with pyridyl substituents at the terminal positions are hoped to construct interesting supramolecular architectures by intermolecular hydrogen bonding and coordination with metals. McMorran' group have reported the synthesis of a quadruply stranded helicate that encapsulates a hexafluorophosphate anion by the reaction of 1,4-bis(3-pyridylmethoxy)benzene with palladium chlorate (McMorran et al., 1998). Zaman's group have designed a long rigid organic ligand, 1,4-bis[(3-pyridyl)ethynyl]benzene, which reacted with metal salts to form interpenetrating two-dimensional and three-dimensional cross-zigzag chains and metallocyclic chain structures (Zaman et al., 2005). As an extension of our work about bipyridyl aromatic ligands, we report the crystal structure of the title compound here.
In the title compound (Fig. 1), all bond lengths and angles are normal and correpond to those observed in the related compound (Gao et al., 2006). The 1,4-bis(3-pyridylmethoxy)benzene molecule is centrosymmetric. The planes of two terminal pyridyl groups rotate drastically and make dihedral angles of 66.8 (1) ° with the plane of the central benzene ring.
In the crystal structure, the adjacent 1,4-bis(3-pyridylmethoxy)benzene molecules are linked into two-dimensional supramolecular sheets by intermolecular C—H···N hydrogen bonds (Table 1, Figure 2).