Abstract
The title compound, C22H30N4O2, has a crystallographic inversion center located at the mid-point of the N—N single bond. Apart from the four ethyl C atoms, the non-H atoms are nearly coplanar with a mean deviation of 0.0596 (2) Å. An intramolecular O—H⋯N hydrogen bond occurs. In the crystal, weak intermolecular C—H⋯O hydrogen bonds link the molecules into layers parallel to (100).
Related literature
For the synthesis, see Tang et al. (2009 ▶). For a related structure, see Gil et al. (2010 ▶). For applications of photochromic aromatic Schiff base molecules as molecular memories and switches, see Sliwa et al. (2005 ▶).
Experimental
Crystal data
C22H30N4O2
M r = 382.50
Monoclinic,
a = 8.736 (5) Å
b = 7.809 (5) Å
c = 16.122 (10) Å
β = 103.57 (2)°
V = 1069.1 (11) Å3
Z = 2
Mo Kα radiation
μ = 0.08 mm−1
T = 290 K
0.15 × 0.14 × 0.12 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.988, T max = 0.991
9903 measured reflections
2431 independent reflections
1227 reflections with I > 2σ(I)
R int = 0.046
Refinement
R[F 2 > 2σ(F 2)] = 0.074
wR(F 2) = 0.228
S = 1.10
2431 reflections
129 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.45 e Å−3
Δρmin = −0.25 e Å−3
Data collection: RAPID-AUTO (Rigaku Corporation, 1998 ▶); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC and Rigaku Corporation, 2002 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811013237/ng5147sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013237/ng5147Isup2.hkl
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 |
---|---|---|---|---|
C8—H8B⋯O1i | 0.97 | 2.64 | 3.481 (5) | 145 |
O1—H1⋯N1 | 0.85 | 1.88 | 2.640 (3) | 149 |
Symmetry code: (i) .
Acknowledgments
The authors acknowledge financial support from the National Natural Science Foundation of China (grant No. 21062022) and the Open Project of the State Key Laboratory of Supramolecular Structure and Materials, Jilin University.
supplementary crystallographic information
Comment
Salicylaldehyde azine belongs to the photochromic aromatic schiff base molecules with two intramolecular hydrogen bonds (Gil et al., 2010). The photochromism of the molecules, owing to enol-keto intramolecular tautomerism, attracts much interest because of possible applications, for example, in molecular memories and switches (Sliwa et al., 2005). Herein, we report the crystal structure of the title compound.
The title compound, as shown in Fig. 1, all bond lengths and angles are in the normal ranges. Except for four carbon atoms, all the other non-hydrogen atoms nearly lie on the same plane. The intramolecular O—H···N and intermolecular C—H···O hydrogen bonds (Table 1) link the molecules into layers prallel to (100).
Experimental
The title compound was prepared according to the literature (Tang et al., 2009). Single crystals suitable for X-ray diffraction were prepared by slow evaporation a mixture of dichloromethane and petroleum (60–90 °C) at room temperature.
Refinement
Carbon-bound H-atoms were placed in calculated positions (C—H 0.93 to 0.97 Å) and were included in the refinement in the riding model with Uiso(H) = 1.2 or 1.5 Ueq(C). The hydroxy H atom was located in a difference Fourier map and treated as riding on its parent O atom with Uiso(H) = 1.5 Ueq(O). The distance of O1 and H1 was restricted to 0.85 Å with DFIX command.
Figures
Fig. 1.
The crystal structure of the title compound, with the atom numbering. Displacement ellipsoids of non-H atoms are drawn at the 30% probalility level. [Symmetry code: A: 1 - x, 1 - y, 1 - z]
Crystal data
C22H30N4O2 | F(000) = 412 |
Mr = 382.50 | Dx = 1.188 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 5162 reflections |
a = 8.736 (5) Å | θ = 3.1–27.7° |
b = 7.809 (5) Å | µ = 0.08 mm−1 |
c = 16.122 (10) Å | T = 290 K |
β = 103.57 (2)° | Block, yellow |
V = 1069.1 (11) Å3 | 0.15 × 0.14 × 0.12 mm |
Z = 2 |
Data collection
Rigaku R-AXIS RAPID diffractometer | 2431 independent reflections |
Radiation source: fine-focus sealed tube | 1227 reflections with I > 2σ(I) |
graphite | Rint = 0.046 |
ω scans | θmax = 27.5°, θmin = 3.1° |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | h = −11→11 |
Tmin = 0.988, Tmax = 0.991 | k = −10→10 |
9903 measured reflections | l = −20→20 |
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)] = 0.074 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.228 | H-atom parameters constrained |
S = 1.10 | w = 1/[σ2(Fo2) + (0.0919P)2 + 0.3133P] where P = (Fo2 + 2Fc2)/3 |
2431 reflections | (Δ/σ)max = 0.003 |
129 parameters | Δρmax = 0.45 e Å−3 |
1 restraint | Δρmin = −0.25 e Å−3 |
Special details
Experimental. (See detailed section in the paper) |
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 | 0.2021 (2) | 0.6394 (3) | 0.57469 (13) | 0.0809 (8) | |
H1 | 0.2663 | 0.6244 | 0.5433 | 0.121* | |
C1 | 0.4983 (3) | 0.4599 (4) | 0.60317 (18) | 0.0556 (7) | |
H1A | 0.5914 | 0.3972 | 0.6165 | 0.067* | |
C2 | 0.4129 (3) | 0.4858 (3) | 0.66828 (16) | 0.0489 (7) | |
C3 | 0.4698 (3) | 0.4235 (4) | 0.75059 (18) | 0.0602 (8) | |
H3 | 0.5638 | 0.3624 | 0.7625 | 0.072* | |
C4 | 0.3937 (3) | 0.4480 (4) | 0.81492 (18) | 0.0653 (9) | |
H4 | 0.4360 | 0.4031 | 0.8688 | 0.078* | |
C5 | 0.2503 (3) | 0.5418 (4) | 0.79966 (18) | 0.0575 (7) | |
C6 | 0.1898 (3) | 0.5998 (4) | 0.71712 (17) | 0.0558 (7) | |
H6 | 0.0939 | 0.6573 | 0.7048 | 0.067* | |
C7 | 0.2678 (3) | 0.5745 (4) | 0.65257 (17) | 0.0537 (7) | |
C8 | 0.2343 (5) | 0.5030 (6) | 0.9510 (2) | 0.0878 (11) | |
H8A | 0.3481 | 0.5128 | 0.9679 | 0.105* | |
H8B | 0.1906 | 0.5672 | 0.9915 | 0.105* | |
C9 | 0.1893 (5) | 0.3226 (6) | 0.9530 (3) | 0.1028 (14) | |
H9A | 0.0770 | 0.3142 | 0.9441 | 0.154* | |
H9B | 0.2387 | 0.2742 | 1.0074 | 0.154* | |
H9C | 0.2226 | 0.2614 | 0.9086 | 0.154* | |
C10 | 0.0357 (4) | 0.6857 (5) | 0.8511 (2) | 0.0735 (9) | |
H10A | 0.0461 | 0.7776 | 0.8123 | 0.088* | |
H10B | 0.0312 | 0.7373 | 0.9052 | 0.088* | |
C11 | −0.1157 (4) | 0.5939 (5) | 0.8161 (2) | 0.0858 (11) | |
H11A | −0.1144 | 0.5460 | 0.7615 | 0.129* | |
H11B | −0.2018 | 0.6729 | 0.8100 | 0.129* | |
H11C | −0.1283 | 0.5038 | 0.8545 | 0.129* | |
N1 | 0.4511 (3) | 0.5198 (3) | 0.52728 (15) | 0.0589 (7) | |
N2 | 0.1766 (3) | 0.5765 (4) | 0.86429 (15) | 0.0752 (8) |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0839 (14) | 0.1066 (19) | 0.0616 (13) | 0.0420 (13) | 0.0362 (11) | 0.0333 (12) |
C1 | 0.0554 (15) | 0.0532 (17) | 0.0651 (18) | 0.0019 (13) | 0.0280 (13) | 0.0001 (13) |
C2 | 0.0482 (14) | 0.0504 (16) | 0.0521 (15) | −0.0016 (12) | 0.0197 (11) | 0.0012 (12) |
C3 | 0.0454 (14) | 0.076 (2) | 0.0619 (18) | 0.0117 (13) | 0.0182 (13) | 0.0085 (15) |
C4 | 0.0519 (15) | 0.097 (2) | 0.0484 (16) | 0.0105 (16) | 0.0142 (12) | 0.0101 (15) |
C5 | 0.0505 (14) | 0.0707 (19) | 0.0569 (17) | 0.0039 (13) | 0.0242 (13) | 0.0042 (14) |
C6 | 0.0525 (14) | 0.0620 (18) | 0.0581 (16) | 0.0110 (13) | 0.0235 (13) | 0.0091 (14) |
C7 | 0.0560 (15) | 0.0550 (17) | 0.0549 (16) | 0.0075 (13) | 0.0227 (13) | 0.0111 (13) |
C8 | 0.084 (2) | 0.115 (3) | 0.074 (2) | 0.002 (2) | 0.0365 (19) | −0.009 (2) |
C9 | 0.101 (3) | 0.114 (4) | 0.103 (3) | 0.019 (3) | 0.043 (2) | 0.009 (2) |
C10 | 0.075 (2) | 0.083 (2) | 0.072 (2) | 0.0104 (18) | 0.0374 (17) | −0.0018 (17) |
C11 | 0.079 (2) | 0.091 (3) | 0.094 (3) | 0.009 (2) | 0.0336 (19) | 0.007 (2) |
N1 | 0.0643 (14) | 0.0606 (15) | 0.0616 (15) | 0.0027 (12) | 0.0345 (11) | 0.0032 (12) |
N2 | 0.0708 (16) | 0.108 (2) | 0.0548 (15) | 0.0222 (15) | 0.0301 (12) | 0.0097 (14) |
Geometric parameters (Å, °)
O1—C7 | 1.351 (3) | C8—C9 | 1.465 (6) |
O1—H1 | 0.8461 | C8—N2 | 1.486 (4) |
C1—N1 | 1.284 (4) | C8—H8A | 0.9700 |
C1—C2 | 1.438 (4) | C8—H8B | 0.9700 |
C1—H1A | 0.9300 | C9—H9A | 0.9600 |
C2—C3 | 1.391 (4) | C9—H9B | 0.9600 |
C2—C7 | 1.414 (4) | C9—H9C | 0.9600 |
C3—C4 | 1.371 (4) | C10—N2 | 1.471 (4) |
C3—H3 | 0.9300 | C10—C11 | 1.494 (5) |
C4—C5 | 1.422 (4) | C10—H10A | 0.9700 |
C4—H4 | 0.9300 | C10—H10B | 0.9700 |
C5—N2 | 1.374 (3) | C11—H11A | 0.9600 |
C5—C6 | 1.387 (4) | C11—H11B | 0.9600 |
C6—C7 | 1.386 (3) | C11—H11C | 0.9600 |
C6—H6 | 0.9300 | N1—N1i | 1.397 (4) |
C7—O1—H1 | 107.9 | C9—C8—H8B | 109.4 |
N1—C1—C2 | 122.6 (3) | N2—C8—H8B | 109.4 |
N1—C1—H1A | 118.7 | H8A—C8—H8B | 108.0 |
C2—C1—H1A | 118.7 | C8—C9—H9A | 109.5 |
C3—C2—C7 | 116.6 (2) | C8—C9—H9B | 109.5 |
C3—C2—C1 | 121.1 (2) | H9A—C9—H9B | 109.5 |
C7—C2—C1 | 122.3 (2) | C8—C9—H9C | 109.5 |
C4—C3—C2 | 123.0 (3) | H9A—C9—H9C | 109.5 |
C4—C3—H3 | 118.5 | H9B—C9—H9C | 109.5 |
C2—C3—H3 | 118.5 | N2—C10—C11 | 114.4 (3) |
C3—C4—C5 | 120.3 (3) | N2—C10—H10A | 108.7 |
C3—C4—H4 | 119.8 | C11—C10—H10A | 108.7 |
C5—C4—H4 | 119.8 | N2—C10—H10B | 108.7 |
N2—C5—C6 | 121.5 (2) | C11—C10—H10B | 108.7 |
N2—C5—C4 | 121.4 (3) | H10A—C10—H10B | 107.6 |
C6—C5—C4 | 117.1 (2) | C10—C11—H11A | 109.5 |
C7—C6—C5 | 122.0 (2) | C10—C11—H11B | 109.5 |
C7—C6—H6 | 119.0 | H11A—C11—H11B | 109.5 |
C5—C6—H6 | 119.0 | C10—C11—H11C | 109.5 |
O1—C7—C6 | 117.9 (2) | H11A—C11—H11C | 109.5 |
O1—C7—C2 | 121.2 (2) | H11B—C11—H11C | 109.5 |
C6—C7—C2 | 120.9 (2) | C1—N1—N1i | 114.3 (3) |
C9—C8—N2 | 111.0 (3) | C5—N2—C10 | 122.0 (2) |
C9—C8—H8A | 109.4 | C5—N2—C8 | 121.4 (3) |
N2—C8—H8A | 109.4 | C10—N2—C8 | 116.6 (2) |
Symmetry codes: (i) −x+1, −y+1, −z+1.
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
C8—H8B···O1ii | 0.97 | 2.64 | 3.481 (5) | 145 |
O1—H1···N1 | 0.85 | 1.88 | 2.640 (3) | 149 |
Symmetry codes: (ii) x, −y+3/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5147).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811013237/ng5147sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013237/ng5147Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report