Abstract
The molecule of the title compund, C30H28N2O2, a Schiff base synthesised via a condensation reaction between 4-methoxybenzaldehyde and 3,3′-dimethylbenzidine, a crystallographic twofold rotation axis passes through the mid-point of the C—C bond of the biphenyl unit. Thus, the asymmetric unit comprises one half-molecule. In the biphenyl unit, the aromatic rings are twisted by 13.49 (7)° with respect to one another. The dihedral angles between the biphenyl and methoxybenzene rings are 49.95 (12) and 50.06 (12)°. In the crystal, weak intermolecular C—H⋯ O hydrogen bonds contribute to the stabilization of the packing.
Related literature
For the biological properties of Schiff base ligands, see: Bedia et al. (2006 ▶). For related structures, see: Harada et al. (2004 ▶); Nesterov (2004 ▶). For reference bond-length values, see: Allen et al. (1987 ▶).
Experimental
Crystal data
C30H28N2O2
M r = 448.54
Monoclinic,
a = 11.644 (2) Å
b = 16.228 (3) Å
c = 12.431 (3) Å
β = 91.75 (3)°
V = 2347.9 (8) Å3
Z = 4
Mo Kα radiation
μ = 0.08 mm−1
T = 93 K
0.38 × 0.34 × 0.22 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.703, T max = 0.786
11279 measured reflections
2667 independent reflections
2350 reflections with I > 2σ(I)
R int = 0.033
Refinement
R[F 2 > 2σ(F 2)] = 0.039
wR(F 2) = 0.111
S = 1.05
2667 reflections
210 parameters
All H-atom parameters refined
Δρmax = 0.40 e Å−3
Δρmin = −0.19 e Å−3
Data collection: RAPID-AUTO (Rigaku, 1998 ▶); cell refinement: RAPID-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: XP in SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811023749/kp2337sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811023749/kp2337Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811023749/kp2337Isup3.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 |
|---|---|---|---|---|
| C6—H6A⋯O1i | 0.960 (13) | 2.688 (13) | 3.4462 (15) | 136.32 (su?) |
Symmetry code: (i)
.
Acknowledgments
Financial support from Huaibei Normal University is gratefully acknowledged.
supplementary crystallographic information
Comment
Schiff base ligands have received considerable attention during the last decades, mainly because of their structures or their biological properties (Bedia et al., 2006). We report here the crystal structure of the title compound, (I), a novel Schiff base (Fig. 1). The bond lengths (Allen et al., 1987) and angles are normal and comparable to the values observed in similar compounds (Harada et al., 2004; Nesterov et al., 2004). In the biphenyl moiety, the aromatic rings are inclined by 13.49 (7)°. The dihedral angles between the biphenyl and methoxybenzal rings are 49.95 (12)° and 50.06 (12)°, respectively. In the crystal, weak intermolecular C—H··· O hydrogen bonds contribute to the stabilisation of the packing (Table 1).
Experimental
4-Methoxybenzaldehyde (0.272 g,2 mmol), 3,3'-Dimethylbenzidine (0.212 g,1 mmol) and 20 mL toluene were placed in a round-bottom flask equipped with a magnetic stirring bar. The reaction mixture was stirred at reflux for 4 h and then cooled.The solid that precipitated was filtered off and washed with methanol. This compound (0.224 g, 0.5 mmol) was dissolved in ethylacetate and left to crystallise. Crystals obtained were suitable for data collection.
Figures
Fig. 1.
The molecular structure of the title compound, drawn with 30% probability displacement ellipsoids. The molecule has the crystallographic twofold rotation axes through the mid of C12-C12A. To generate the whole molecule symmetry operation A: -x,y, 1/2-z was used.
Crystal data
| C30H28N2O2 | F(000) = 952 |
| Mr = 448.54 | Dx = 1.269 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 9010 reflections |
| a = 11.644 (2) Å | θ = 3.0–27.5° |
| b = 16.228 (3) Å | µ = 0.08 mm−1 |
| c = 12.431 (3) Å | T = 93 K |
| β = 91.75 (3)° | Block, yellow |
| V = 2347.9 (8) Å3 | 0.38 × 0.34 × 0.22 mm |
| Z = 4 |
Data collection
| Rigaku R-AXIS RAPID diffractometer | 2667 independent reflections |
| Radiation source: fine-focus sealed tube | 2350 reflections with I > 2σ(I) |
| graphite | Rint = 0.033 |
| ω scans | θmax = 27.5°, θmin = 3.0° |
| Absorption correction: multi-scan (ABSCOR ;Higashi, 1995) | h = −15→15 |
| Tmin = 0.703, Tmax = 0.786 | k = −20→20 |
| 11279 measured reflections | l = −14→16 |
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)] = 0.039 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.111 | All H-atom parameters refined |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0658P)2 + 1.0766P] where P = (Fo2 + 2Fc2)/3 |
| 2667 reflections | (Δ/σ)max = 0.001 |
| 210 parameters | Δρmax = 0.40 e Å−3 |
| 0 restraints | Δρmin = −0.19 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 | 0.14801 (6) | 0.07986 (5) | 1.08572 (5) | 0.01981 (19) | |
| N1 | 0.36979 (7) | 0.15477 (5) | 0.62842 (7) | 0.0176 (2) | |
| C1 | 0.20415 (11) | 0.12644 (8) | 1.16991 (9) | 0.0262 (3) | |
| H1A | 0.2839 (14) | 0.1056 (10) | 1.1839 (12) | 0.034 (4)* | |
| H1C | 0.2050 (14) | 0.1847 (10) | 1.1522 (12) | 0.038 (4)* | |
| H1B | 0.1570 (13) | 0.1177 (10) | 1.2330 (12) | 0.037 (4)* | |
| C2 | 0.18777 (9) | 0.08948 (6) | 0.98408 (8) | 0.0165 (2) | |
| C3 | 0.28693 (9) | 0.13363 (6) | 0.96025 (8) | 0.0183 (2) | |
| H3A | 0.3342 (12) | 0.1589 (8) | 1.0165 (11) | 0.025 (3)* | |
| C4 | 0.31999 (9) | 0.13940 (6) | 0.85410 (8) | 0.0179 (2) | |
| H4A | 0.3903 (12) | 0.1681 (8) | 0.8377 (10) | 0.022 (3)* | |
| C5 | 0.25488 (8) | 0.10280 (6) | 0.77062 (8) | 0.0163 (2) | |
| C6 | 0.15643 (9) | 0.05837 (6) | 0.79627 (8) | 0.0179 (2) | |
| H6A | 0.1119 (11) | 0.0334 (8) | 0.7388 (10) | 0.021 (3)* | |
| C7 | 0.12313 (9) | 0.05104 (6) | 0.90185 (8) | 0.0179 (2) | |
| H7A | 0.0561 (12) | 0.0194 (8) | 0.9196 (10) | 0.024 (3)* | |
| C8 | 0.28718 (8) | 0.10911 (6) | 0.65788 (8) | 0.0176 (2) | |
| H8A | 0.2396 (11) | 0.0762 (8) | 0.6043 (10) | 0.020 (3)* | |
| C9 | 0.40025 (8) | 0.15379 (6) | 0.51899 (8) | 0.0162 (2) | |
| C10 | 0.43005 (8) | 0.22903 (6) | 0.47132 (8) | 0.0159 (2) | |
| C11 | 0.46879 (8) | 0.22851 (6) | 0.36602 (8) | 0.0165 (2) | |
| H11A | 0.4919 (11) | 0.2820 (9) | 0.3346 (10) | 0.023 (3)* | |
| C12 | 0.47841 (8) | 0.15556 (6) | 0.30593 (7) | 0.0160 (2) | |
| C13 | 0.44641 (9) | 0.08169 (6) | 0.35559 (8) | 0.0180 (2) | |
| H13A | 0.4501 (11) | 0.0292 (8) | 0.3175 (10) | 0.019 (3)* | |
| C14 | 0.40833 (9) | 0.08084 (6) | 0.46040 (8) | 0.0183 (2) | |
| H14A | 0.3897 (12) | 0.0279 (8) | 0.4927 (10) | 0.024 (3)* | |
| C15 | 0.41802 (9) | 0.30788 (7) | 0.53365 (8) | 0.0199 (2) | |
| H15C | 0.3378 (12) | 0.3186 (9) | 0.5538 (11) | 0.028 (3)* | |
| H15B | 0.4624 (13) | 0.3043 (9) | 0.6036 (12) | 0.032 (4)* | |
| H15A | 0.4450 (12) | 0.3550 (8) | 0.4925 (11) | 0.025 (3)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0209 (4) | 0.0261 (4) | 0.0126 (4) | −0.0009 (3) | 0.0023 (3) | 0.0020 (3) |
| N1 | 0.0179 (4) | 0.0209 (4) | 0.0141 (4) | 0.0005 (3) | 0.0020 (3) | 0.0021 (3) |
| C1 | 0.0341 (6) | 0.0295 (6) | 0.0151 (5) | −0.0047 (5) | 0.0020 (4) | −0.0012 (4) |
| C2 | 0.0178 (5) | 0.0179 (5) | 0.0140 (5) | 0.0039 (4) | 0.0024 (3) | 0.0029 (4) |
| C3 | 0.0184 (5) | 0.0198 (5) | 0.0166 (5) | −0.0003 (4) | −0.0011 (4) | 0.0006 (4) |
| C4 | 0.0163 (5) | 0.0192 (5) | 0.0181 (5) | −0.0012 (4) | 0.0012 (4) | 0.0023 (4) |
| C5 | 0.0166 (5) | 0.0171 (5) | 0.0153 (5) | 0.0021 (4) | 0.0018 (3) | 0.0019 (4) |
| C6 | 0.0171 (5) | 0.0201 (5) | 0.0166 (5) | −0.0001 (4) | 0.0005 (4) | −0.0009 (4) |
| C7 | 0.0160 (5) | 0.0195 (5) | 0.0185 (5) | −0.0010 (4) | 0.0032 (4) | 0.0010 (4) |
| C8 | 0.0168 (5) | 0.0200 (5) | 0.0160 (5) | 0.0009 (4) | 0.0003 (4) | 0.0014 (4) |
| C9 | 0.0130 (4) | 0.0224 (5) | 0.0132 (5) | −0.0003 (4) | 0.0003 (3) | 0.0011 (4) |
| C10 | 0.0129 (4) | 0.0197 (5) | 0.0150 (5) | −0.0008 (3) | 0.0000 (3) | −0.0005 (4) |
| C11 | 0.0161 (5) | 0.0184 (5) | 0.0152 (5) | −0.0007 (4) | 0.0008 (3) | 0.0015 (4) |
| C12 | 0.0151 (5) | 0.0191 (5) | 0.0138 (5) | 0.0002 (3) | 0.0003 (4) | 0.0004 (4) |
| C13 | 0.0195 (5) | 0.0179 (5) | 0.0167 (5) | −0.0003 (4) | 0.0009 (4) | −0.0012 (4) |
| C14 | 0.0186 (5) | 0.0187 (5) | 0.0176 (5) | −0.0014 (4) | 0.0016 (4) | 0.0032 (4) |
| C15 | 0.0223 (5) | 0.0203 (5) | 0.0172 (5) | −0.0017 (4) | 0.0040 (4) | −0.0021 (4) |
Geometric parameters (Å, °)
| O1—C2 | 1.3677 (12) | C7—H7A | 0.965 (14) |
| O1—C1 | 1.4325 (14) | C8—H8A | 1.006 (13) |
| N1—C8 | 1.2767 (13) | C9—C14 | 1.3946 (15) |
| N1—C9 | 1.4164 (12) | C9—C10 | 1.4054 (14) |
| C1—H1A | 0.999 (16) | C10—C11 | 1.3976 (14) |
| C1—H1C | 0.972 (17) | C10—C15 | 1.5046 (14) |
| C1—H1B | 0.981 (15) | C11—C12 | 1.4061 (14) |
| C2—C7 | 1.3978 (15) | C11—H11A | 0.992 (14) |
| C2—C3 | 1.3982 (14) | C12—C13 | 1.4039 (14) |
| C3—C4 | 1.3891 (14) | C12—C12i | 1.4930 (18) |
| C3—H3A | 0.968 (14) | C13—C14 | 1.3892 (14) |
| C4—C5 | 1.3987 (15) | C13—H13A | 0.975 (13) |
| C4—H4A | 0.969 (14) | C14—H14A | 0.976 (13) |
| C5—C6 | 1.3993 (14) | C15—H15C | 0.990 (14) |
| C5—C8 | 1.4657 (13) | C15—H15B | 1.000 (15) |
| C6—C7 | 1.3851 (14) | C15—H15A | 0.977 (14) |
| C6—H6A | 0.960 (13) | ||
| C2—O1—C1 | 117.07 (8) | N1—C8—H8A | 121.5 (7) |
| C8—N1—C9 | 118.82 (9) | C5—C8—H8A | 116.3 (7) |
| O1—C1—H1A | 110.5 (9) | C14—C9—C10 | 119.73 (9) |
| O1—C1—H1C | 110.8 (9) | C14—C9—N1 | 122.27 (9) |
| H1A—C1—H1C | 110.7 (13) | C10—C9—N1 | 117.87 (9) |
| O1—C1—H1B | 104.7 (9) | C11—C10—C9 | 118.72 (9) |
| H1A—C1—H1B | 110.6 (12) | C11—C10—C15 | 121.69 (9) |
| H1C—C1—H1B | 109.4 (13) | C9—C10—C15 | 119.58 (9) |
| O1—C2—C7 | 115.77 (9) | C10—C11—C12 | 122.41 (9) |
| O1—C2—C3 | 124.00 (9) | C10—C11—H11A | 117.6 (7) |
| C7—C2—C3 | 120.23 (9) | C12—C11—H11A | 120.0 (7) |
| C4—C3—C2 | 119.37 (10) | C13—C12—C11 | 117.30 (9) |
| C4—C3—H3A | 119.3 (8) | C13—C12—C12i | 120.73 (6) |
| C2—C3—H3A | 121.3 (8) | C11—C12—C12i | 121.96 (6) |
| C3—C4—C5 | 121.10 (9) | C14—C13—C12 | 121.17 (9) |
| C3—C4—H4A | 119.5 (8) | C14—C13—H13A | 117.8 (7) |
| C5—C4—H4A | 119.4 (8) | C12—C13—H13A | 121.1 (7) |
| C4—C5—C6 | 118.62 (9) | C13—C14—C9 | 120.66 (9) |
| C4—C5—C8 | 122.06 (9) | C13—C14—H14A | 118.4 (7) |
| C6—C5—C8 | 119.33 (9) | C9—C14—H14A | 120.9 (7) |
| C7—C6—C5 | 121.02 (10) | C10—C15—H15C | 112.6 (8) |
| C7—C6—H6A | 120.6 (8) | C10—C15—H15B | 110.1 (9) |
| C5—C6—H6A | 118.4 (8) | H15C—C15—H15B | 104.9 (11) |
| C6—C7—C2 | 119.64 (9) | C10—C15—H15A | 111.0 (8) |
| C6—C7—H7A | 120.9 (8) | H15C—C15—H15A | 108.4 (11) |
| C2—C7—H7A | 119.4 (8) | H15B—C15—H15A | 109.6 (12) |
| N1—C8—C5 | 122.17 (9) |
Symmetry codes: (i) −x+1, y, −z+1/2.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C6—H6A···O1ii | 0.960 (13) | 2.688 (13) | 3.4462 (15) | 136.32 |
Symmetry codes: (ii) x, −y, z−1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2337).
References
- Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
- Bedia, K. K., Elcin, O., Seda, U., Fatma, K., Nathaly, S., Sevim, R. & Dimoglo, A. (2006). Eur. J. Med. Chem. 41, 1253–1261. [DOI] [PubMed]
- Harada, J., Harakawa, M. & Ogawa, K. (2004). Acta Cryst. B60, 578–588. [DOI] [PubMed]
- Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
- Nesterov, V. N. (2004). Acta Cryst. C60, o806–o809. [DOI] [PubMed]
- Rigaku (1998). RAPID-AUTO Rigaku Corporation, Tokyo, Japan.
- Rigaku/MSC (2004). CrystalStructure Rigaku/MSC Inc., The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
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/S1600536811023749/kp2337sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811023749/kp2337Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811023749/kp2337Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

