organic compounds
6,6′-Dimethoxy-2,2′-{[(E,E)-hydrazine-1,2-diylidene]bis(methanylylidene)}diphenol methanol disolvate
aDepartment of Chemistry, Memorial University of Newfoundland, St Johns, NL, Canada A1B 3X7, and bDepartment of Chemistry and C-CART X-Ray Diffraction Laboratory, Memorial University of Newfoundland, St Johns, NL, Canada A1B 3X7
*Correspondence e-mail: louise.dawe@mun.ca
The title compound, C16H16N2O4·2CH3OH, is a hydrazone in an E geometric arrangement, with an inversion centre at the mid-point of the N—N bond. A symmetry-related pair of six-membered hydrogen-bonded rings [graph-set motif S11(6)] are present for the terminal vanillin–imine moieties. Two lattice methanol solvent molecules are present per formula unit (Z′ = 1/2), which form hydrogen-bonded chains along [010] with two orientations due to disorder of the methanol H-atom.
Related literature
The synthesis of the title compound was originally reported by Lin et al. (2009); however, in this study, it was obtained from (2Z,6Z,N′2E,N′6E)-N′2,N′6-bis(2-hydroxy-3-methoxybenzylidene)pyridine-2,6-bis(carbohydrazonic) acid (Vadavi et al. 2011). The title compound has been used in the synthesis of first-row transition metal complexes (Zou et al. 2011) and in the synthesis of lanthanide complexes (Davidson et al. 2006). A solvent-free structure of the title compound has been previously reported (Lu et al. 2011) and contains a similar intramolecular hydrogen-bonding motif (Bernstein et al. 1995, Etter et al. 1990) to that reported herein.
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear-SM Expert (Rigaku, 2009); cell CrystalClear-SM Expert; data reduction: CrystalClear-SM Expert; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2.
Supporting information
10.1107/S1600536812034940/hg5235sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812034940/hg5235Isup2.hkl
DyCl3.H2O (0.06 g; 0.2 mmol) was dissolved in methanol (20 mL). (2Z,6Z,N'2E,N'6E)-N'2,N'6-bis(2-hydroxy-3-methoxybenzylidene)pyridine-2,6-bis(carbohydrazonic) acid (Vadavi et al. 2011) (0.05 g; 0.1 mmol) was added and the solution was refluxed for 3 h. Upon cooling, the resulting solution was gravity filtered and left for slow evaporation at room temperature to yield yellow-orange crystals of the title compound.
With the exception of H3A, H3B and H2, all hydrogen positions were calculated after each cycle of
using a riding model, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for aromatic H atoms, and with C—H = 0.96 Å and Uiso(H) = 1.5Ueq(C) for methyl H atoms. H2 was allowed to refine positionally, with Uiso(H) = 1.5Ueq(O2). The disordered H atoms, H3A and H3B were refined with distance (O3—H) and angle (C5—O3—H) restraints of 0.87 Å and 110° respectively, and with Uiso(H) = 1.5Ueq(O3). H3A and H3B were both assigned an occupancy of 0.5 based on similar residual peak height from examination of difference maps, prior to their introduction.Data collection: CrystalClear-SM Expert (Rigaku, 2009); cell
CrystalClear-SM Expert (Rigaku, 2009); data reduction: CrystalClear-SM Expert (Rigaku, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).Molecular structure of the title compound at 50% probability ellipsoid level. Symmetry operator i = 1 - x, 2 - y, 1 - z; iv = 1 - x, 1 - y, 1 - z. Packed of the title compound, highlighting the hydrogen bonding chains which propagate along [0 1 0]. One of the disordered H-atoms is omitted from each methanol molecule. |
C16H16N2O4·2CH4O | F(000) = 388 |
Mr = 364.39 | Dx = 1.282 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71075 Å |
Hall symbol: -P 2ybc | Cell parameters from 9154 reflections |
a = 20.517 (2) Å | θ = 3.4–27.6° |
b = 4.8374 (5) Å | µ = 0.10 mm−1 |
c = 21.366 (3) Å | T = 163 K |
β = 153.566 (7)° | Irregular, yellow |
V = 944.0 (3) Å3 | 0.59 × 0.14 × 0.13 mm |
Z = 2 |
Rigaku Saturn70 CCD diffractometer | 1941 independent reflections |
Radiation source: fine-focus sealed tube | 1651 reflections with I > 2σ(I) |
Graphite - Rigaku SHINE monochromator | Rint = 0.036 |
Detector resolution: 14.63 pixels mm-1 | θmax = 26.5°, θmin = 3.4° |
ω scans | h = −25→25 |
Absorption correction: multi-scan (REQAB; Jacobson, 1998) | k = −5→6 |
Tmin = 0.725, Tmax = 1.000 | l = −26→26 |
12068 measured reflections |
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)] = 0.062 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.194 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | w = 1/[σ2(Fo2) + (0.118P)2 + 0.3328P] where P = (Fo2 + 2Fc2)/3 |
1941 reflections | (Δ/σ)max < 0.001 |
129 parameters | Δρmax = 0.32 e Å−3 |
4 restraints | Δρmin = −0.41 e Å−3 |
C16H16N2O4·2CH4O | V = 944.0 (3) Å3 |
Mr = 364.39 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 20.517 (2) Å | µ = 0.10 mm−1 |
b = 4.8374 (5) Å | T = 163 K |
c = 21.366 (3) Å | 0.59 × 0.14 × 0.13 mm |
β = 153.566 (7)° |
Rigaku Saturn70 CCD diffractometer | 1941 independent reflections |
Absorption correction: multi-scan (REQAB; Jacobson, 1998) | 1651 reflections with I > 2σ(I) |
Tmin = 0.725, Tmax = 1.000 | Rint = 0.036 |
12068 measured reflections |
R[F2 > 2σ(F2)] = 0.062 | 4 restraints |
wR(F2) = 0.194 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | Δρmax = 0.32 e Å−3 |
1941 reflections | Δρmin = −0.41 e Å−3 |
129 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 | Occ. (<1) | |
O2 | 0.26395 (15) | 0.6929 (3) | 0.38898 (14) | 0.0446 (4) | |
H2 | 0.318 (3) | 0.797 (6) | 0.411 (3) | 0.067* | |
C3 | 0.51958 (19) | 0.5637 (4) | 0.61567 (19) | 0.0321 (4) | |
C4 | 0.6264 (2) | 0.3959 (4) | 0.73588 (19) | 0.0360 (5) | |
H4 | 0.7240 | 0.4131 | 0.8082 | 0.043* | |
C2 | 0.37270 (19) | 0.5380 (4) | 0.50753 (18) | 0.0341 (5) | |
C1 | 0.3337 (2) | 0.3422 (4) | 0.52005 (19) | 0.0357 (5) | |
C6 | 0.4408 (2) | 0.1796 (4) | 0.6393 (2) | 0.0367 (5) | |
H6 | 0.4151 | 0.0514 | 0.6478 | 0.044* | |
C5 | 0.5869 (2) | 0.2059 (4) | 0.74696 (19) | 0.0381 (5) | |
H5 | 0.6580 | 0.0949 | 0.8265 | 0.046* | |
O1 | 0.18781 (15) | 0.3354 (3) | 0.40867 (15) | 0.0490 (5) | |
N1 | 0.46904 (17) | 0.9117 (3) | 0.49594 (16) | 0.0353 (4) | |
C8 | 0.5634 (2) | 0.7607 (4) | 0.60529 (19) | 0.0347 (4) | |
H8 | 0.6619 | 0.7772 | 0.6796 | 0.042* | |
C7 | 0.1407 (2) | 0.1307 (5) | 0.4117 (2) | 0.0498 (6) | |
H7A | 0.0360 | 0.1364 | 0.3253 | 0.075* | |
H7B | 0.1839 | 0.1667 | 0.4890 | 0.075* | |
H7C | 0.1704 | −0.0487 | 0.4229 | 0.075* | |
O3 | 0.0380 (3) | 0.2477 (5) | 0.0577 (3) | 0.0813 (7) | |
H3A | 0.032 (10) | 0.428 (5) | 0.044 (9) | 0.122* | 0.50 |
H3B | −0.024 (7) | 0.138 (13) | −0.015 (5) | 0.122* | 0.50 |
C9 | 0.0339 (3) | 0.2220 (7) | 0.1198 (3) | 0.0704 (8) | |
H9A | −0.0661 | 0.2228 | 0.0478 | 0.106* | |
H9B | 0.0853 | 0.3742 | 0.1827 | 0.106* | |
H9C | 0.0796 | 0.0516 | 0.1713 | 0.106* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O2 | 0.0338 (7) | 0.0509 (9) | 0.0391 (8) | 0.0011 (6) | 0.0315 (7) | 0.0087 (6) |
C3 | 0.0351 (9) | 0.0337 (10) | 0.0352 (9) | −0.0036 (7) | 0.0323 (8) | −0.0044 (7) |
C4 | 0.0330 (9) | 0.0410 (10) | 0.0353 (9) | −0.0003 (7) | 0.0308 (9) | −0.0011 (8) |
C2 | 0.0345 (9) | 0.0356 (10) | 0.0340 (9) | 0.0001 (7) | 0.0309 (9) | 0.0006 (7) |
C1 | 0.0339 (9) | 0.0396 (10) | 0.0364 (9) | −0.0047 (8) | 0.0318 (9) | −0.0036 (8) |
C6 | 0.0442 (10) | 0.0364 (10) | 0.0427 (10) | −0.0035 (8) | 0.0404 (10) | −0.0019 (8) |
C5 | 0.0406 (10) | 0.0400 (10) | 0.0367 (9) | 0.0033 (8) | 0.0349 (9) | 0.0035 (8) |
O1 | 0.0352 (7) | 0.0593 (10) | 0.0456 (8) | −0.0025 (6) | 0.0354 (7) | 0.0066 (7) |
N1 | 0.0399 (8) | 0.0368 (9) | 0.0410 (9) | −0.0055 (7) | 0.0376 (8) | −0.0037 (7) |
C8 | 0.0370 (9) | 0.0376 (10) | 0.0389 (9) | −0.0043 (7) | 0.0351 (9) | −0.0050 (8) |
C7 | 0.0427 (11) | 0.0598 (14) | 0.0506 (12) | −0.0086 (10) | 0.0422 (11) | −0.0013 (10) |
O3 | 0.0841 (14) | 0.0932 (16) | 0.0861 (14) | −0.0099 (12) | 0.0783 (14) | −0.0147 (13) |
C9 | 0.0518 (13) | 0.098 (2) | 0.0550 (14) | 0.0091 (14) | 0.0472 (13) | 0.0002 (14) |
O2—C2 | 1.354 (2) | O1—C7 | 1.425 (3) |
O2—H2 | 0.88 (3) | N1—C8 | 1.281 (3) |
C3—C2 | 1.402 (3) | N1—N1i | 1.407 (3) |
C3—C4 | 1.407 (3) | C8—H8 | 0.9300 |
C3—C8 | 1.456 (3) | C7—H7A | 0.9600 |
C4—C5 | 1.378 (3) | C7—H7B | 0.9600 |
C4—H4 | 0.9300 | C7—H7C | 0.9600 |
C2—C1 | 1.412 (3) | O3—C9 | 1.409 (4) |
C1—O1 | 1.367 (2) | O3—H3A | 0.89 (2) |
C1—C6 | 1.383 (3) | O3—H3B | 0.88 (2) |
C6—C5 | 1.395 (3) | C9—H9A | 0.9600 |
C6—H6 | 0.9300 | C9—H9B | 0.9600 |
C5—H5 | 0.9300 | C9—H9C | 0.9600 |
C2—O2—H2 | 98.1 (19) | C8—N1—N1i | 113.50 (19) |
C2—C3—C4 | 119.54 (17) | N1—C8—C3 | 121.36 (17) |
C2—C3—C8 | 121.05 (17) | N1—C8—H8 | 119.3 |
C4—C3—C8 | 119.41 (16) | C3—C8—H8 | 119.3 |
C5—C4—C3 | 120.29 (17) | O1—C7—H7A | 109.5 |
C5—C4—H4 | 119.9 | O1—C7—H7B | 109.5 |
C3—C4—H4 | 119.9 | H7A—C7—H7B | 109.5 |
O2—C2—C3 | 122.92 (17) | O1—C7—H7C | 109.5 |
O2—C2—C1 | 117.48 (16) | H7A—C7—H7C | 109.5 |
C3—C2—C1 | 119.59 (17) | H7B—C7—H7C | 109.5 |
O1—C1—C6 | 125.69 (17) | C9—O3—H3A | 106 (3) |
O1—C1—C2 | 114.56 (16) | C9—O3—H3B | 113 (4) |
C6—C1—C2 | 119.74 (17) | H3A—O3—H3B | 118 (7) |
C1—C6—C5 | 120.61 (17) | O3—C9—H9A | 109.5 |
C1—C6—H6 | 119.7 | O3—C9—H9B | 109.5 |
C5—C6—H6 | 119.7 | H9A—C9—H9B | 109.5 |
C4—C5—C6 | 120.23 (17) | O3—C9—H9C | 109.5 |
C4—C5—H5 | 119.9 | H9A—C9—H9C | 109.5 |
C6—C5—H5 | 119.9 | H9B—C9—H9C | 109.5 |
C1—O1—C7 | 117.07 (16) |
Symmetry code: (i) −x+1, −y+2, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H2···N1 | 0.88 (3) | 1.77 (7) | 2.613 (5) | 160 (3) |
O3—H3A···O3ii | 0.89 (8) | 1.91 (7) | 2.754 (4) | 157 (9) |
O3—H3B···O3iii | 0.88 (7) | 1.98 (7) | 2.715 (4) | 140 (5) |
Symmetry codes: (ii) −x, −y+1, −z; (iii) −x, −y, −z. |
Experimental details
Crystal data | |
Chemical formula | C16H16N2O4·2CH4O |
Mr | 364.39 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 163 |
a, b, c (Å) | 20.517 (2), 4.8374 (5), 21.366 (3) |
β (°) | 153.566 (7) |
V (Å3) | 944.0 (3) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.10 |
Crystal size (mm) | 0.59 × 0.14 × 0.13 |
Data collection | |
Diffractometer | Rigaku Saturn70 CCD diffractometer |
Absorption correction | Multi-scan (REQAB; Jacobson, 1998) |
Tmin, Tmax | 0.725, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12068, 1941, 1651 |
Rint | 0.036 |
(sin θ/λ)max (Å−1) | 0.628 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.062, 0.194, 1.09 |
No. of reflections | 1941 |
No. of parameters | 129 |
No. of restraints | 4 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.32, −0.41 |
Computer programs: CrystalClear-SM Expert (Rigaku, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), OLEX2 (Dolomanov et al., 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H2···N1 | 0.88 (3) | 1.77 (7) | 2.613 (5) | 160 (3) |
O3—H3A···O3i | 0.89 (8) | 1.91 (7) | 2.754 (4) | 157 (9) |
O3—H3B···O3ii | 0.88 (7) | 1.98 (7) | 2.715 (4) | 140 (5) |
Symmetry codes: (i) −x, −y+1, −z; (ii) −x, −y, −z. |
Acknowledgements
We thank NSERC (Canada) for financial support for these studies.
References
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The synthesis of this compound was performed because of its intriguing interactions with both transition and lanthanide metals. The ability for the vanillin moieties to bridge multiple metal centers to form polymetallic clusters has potential applications in the fields of molecular magnetics and supramolecular chemistry.
While the previously reported solventless structure (Lu et al. 2011) and the title compound are comprised of two vanillin-imine moieties, in the title compound, these are related by an inversion centre about the N1i—N1 bond (i = 1 - x,2 - y,1 - z). There are two available geometries for the hydrazone functional group, the E and Z isomers. Both this report, and the previously reported structure, feature the E isomer (Figure 1).
There are multiple hydrogen bonding interactions, one intramolecular for the main molecule and one intermolecular hydrogen bonding chain, however, there are no discernable hydrogen bonding interaction between the main molecule and the solvent methanol molecules. The intramolecular hydrogen bond between N1 and H1 forms a stable six-membered hydrogen bound ring with graph set notation S11(6) (one hydrogen bond donor, and one acceptor enclosed in a six-membered ring; Figure 1) (Bernstein et al. 1995, Etter et al. 1990). This interaction was also present in the previous report (Lu et al. 2011). This structural motif would likely provide an energetic barrier to rotation about the C2—C3 bond, which would be required to maximize the number of metals that could be incorporated into a cluster for further study.
A second hydrogen bond interaction is present as a one-dimensional chain of solvent methanol molecules, with graph set notation of C11(2) (Figure 2.) The methanolic protons, H3A and H3B, are disordered, with occupancy of 1/2, and when extended packing diagrams are examined, it can be seen that the hydrogen bonded chains propagate along [0 1 0] (i.e. run parallel to the b axis), with the disorder representing a reversal in the D—H···A orientation.