supplementary materials


Acta Cryst. (2007). E63, o2795    [ doi:10.1107/S1600536807020983 ]

4-Hydroxy-3-iodo-5-methoxybenzaldehyde

Q.-L. Zhou, C.-L. Wang and Z.-L. Jing

Abstract top

The title compound, C8H7IO3, contains two independent molecules, each lying on a mirror plane. The two molecules differ in the orientation of the -CHO group by a 180° rotation around its bond with the benzene ring. In the mirror plane, each independent molecule is linked to a symmetry-equivalent molecule by intermolecular O-H...O hydrogen bonds, forming a chain along the b axis. Short intermolecular I...O contacts are observed between adjacent chains.

Comment top

In order to establish control over the preparation of crystalline solid materials so that their architecture and properties are predictable (Belloni et al., 2005; Tynan et al., 2005; Parashar et al., 1988), the synthesis of new and designed crystal structures has become a major strand of modern chemistry. Metal complexes based on Schiff bases have attracted much attention because they can be utilized as model compounds of the active centres

in various proteins and enzymes (Kahwa et al., 1986; Santos et al., 2001). As part of an investigation of the coordination properties of Shiff bases functioning as ligands, we report the synthesis and crystal structure of the title compound, (I).

The asymmetric unit of (I) comprises two independent molecules (Fig. 1), lying on the mirror planes, one at z = 0 and the other at z = 1/2. The two molecules differ in the orientation of the –CHO group by a 180° rotation around its bond with the benzene ring. In both molecules the geometric parameters are normal.

Each independent molecule is linked to a symmetry-equivalent molecule by intermolecular O—H···O hydrogen bonds, forming a chain along the b axis, in the mirror plane. The chains formed by each independent molecule are shown in Fig.2 and Fig.3. Short intermolecular I1···O3(x - 1/2, 1/2 - y, 1 - z) [3.099 (3) Å] and I2···O6(x - 1/2, 1/2 - y, -z) [3.388 (3) Å] contacts are observed between the adjacent chains.]

Related literature top

For general background, see: Belloni et al. (2005); Kahwa et al. (1986); Parashar et al. (1988); Santos et al. (2001); Tynan et al. (2005).

Experimental top

4-Hydroxy-3-iodo-5-methoxy-benzaldehyde (1 g) was added to an anhydrous ethanol (50 ml), with stirring at 350 K. The resulting yellow solution was filtered and the filtrate was allowed to stand in air at room temperature for 10 d, yielding yellow crystals of (I)

Refinement top

H atoms were placed in calculated positions [O—H = 0.82 Å and C—H = 0.93 (aromatic) or 0.96 Å (methyl)] and refined using a riding model, with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(O).

Computing details top

Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The asymmetric unit of (I). Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. Hydrogen-bonded (dashed lines) chains formed by one of the independent molecules, viewed down the c axis.
[Figure 3] Fig. 3. Hydrogen-bonded (dashed lines) chains formed by other independent molecules, viewed down the c axis.
4-Hydroxy-3-iodo-5-methoxybenzaldehyde top
Crystal data top
C8H7IO3F(000) = 1056
Mr = 278.04Dx = 2.098 Mg m3
Orthorhombic, PbamMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2 2abCell parameters from 4592 reflections
a = 16.332 (2) Åθ = 2.5–26.4°
b = 16.344 (2) ŵ = 3.60 mm1
c = 6.5957 (12) ÅT = 293 K
V = 1760.6 (4) Å3Block, yellow
Z = 80.20 × 0.16 × 0.12 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1974 independent reflections
Radiation source: fine-focus sealed tube1654 reflections with I > 2σ(I)
graphiteRint = 0.037
φ and ω scansθmax = 26.4°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1620
Tmin = 0.533, Tmax = 0.672k = 2019
9744 measured reflectionsl = 58
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.022Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.053H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.025P)2 + 0.749P]
where P = (Fo2 + 2Fc2)/3
1974 reflections(Δ/σ)max = 0.001
145 parametersΔρmax = 0.47 e Å3
0 restraintsΔρmin = 0.47 e Å3
Crystal data top
C8H7IO3V = 1760.6 (4) Å3
Mr = 278.04Z = 8
Orthorhombic, PbamMo Kα radiation
a = 16.332 (2) ŵ = 3.60 mm1
b = 16.344 (2) ÅT = 293 K
c = 6.5957 (12) Å0.20 × 0.16 × 0.12 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1974 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1654 reflections with I > 2σ(I)
Tmin = 0.533, Tmax = 0.672Rint = 0.037
9744 measured reflectionsθmax = 26.4°
Refinement top
R[F2 > 2σ(F2)] = 0.022H-atom parameters constrained
wR(F2) = 0.053Δρmax = 0.47 e Å3
S = 1.03Δρmin = 0.47 e Å3
1974 reflectionsAbsolute structure: ?
145 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

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) top
xyzUiso*/Ueq
I10.024919 (16)0.352244 (16)0.50000.03520 (9)
O10.13388 (17)0.45773 (15)0.50000.0385 (7)
H1O0.17440.48730.50000.058*
O20.29270 (16)0.42133 (16)0.50000.0419 (7)
O30.29135 (17)0.10050 (16)0.50000.0374 (7)
C10.0976 (2)0.3182 (2)0.50000.0271 (8)
C20.1575 (2)0.3788 (2)0.50000.0266 (8)
C30.2406 (2)0.3558 (2)0.50000.0269 (8)
C40.2620 (2)0.2753 (2)0.50000.0292 (8)
H40.31700.26040.50000.035*
C50.2013 (2)0.2148 (2)0.50000.0263 (8)
C60.1193 (2)0.2362 (2)0.50000.0287 (8)
H60.07910.19590.50000.034*
C70.2227 (3)0.1278 (2)0.50000.0321 (9)
H70.17970.09040.50000.038*
C80.3785 (2)0.4039 (3)0.50000.0474 (12)
H8A0.40870.45420.50000.071*
H8B0.39210.37280.38120.071*
I20.049445 (18)0.127572 (19)0.00000.04574 (11)
O40.15122 (18)0.03449 (17)0.00000.0434 (7)
H4O0.17630.07790.00000.065*
O50.30938 (17)0.06768 (16)0.00000.0411 (7)
O60.3560 (2)0.29765 (18)0.00000.0586 (9)
C90.1756 (2)0.1081 (2)0.00000.0311 (9)
C100.2044 (2)0.0276 (2)0.00000.0311 (9)
C110.2889 (2)0.0137 (2)0.00000.0294 (8)
C120.3422 (2)0.0785 (2)0.00000.0329 (9)
H120.39840.06900.00000.039*
C130.3128 (3)0.1583 (2)0.00000.0318 (9)
C140.2296 (3)0.1732 (2)0.00000.0352 (10)
H140.21010.22660.00000.042*
C150.3720 (3)0.2257 (3)0.00000.0402 (10)
H150.42710.21150.00000.048*
C160.3938 (3)0.0866 (3)0.00000.0475 (11)
H16A0.40080.14490.00000.071*
H16B0.41900.06380.11880.071*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.02010 (14)0.03288 (15)0.05262 (19)0.00134 (10)0.0000.000
O10.0261 (15)0.0192 (13)0.070 (2)0.0014 (11)0.0000.000
O20.0207 (14)0.0257 (14)0.079 (2)0.0031 (11)0.0000.000
O30.0319 (16)0.0232 (14)0.0570 (19)0.0058 (12)0.0000.000
C10.0181 (19)0.0271 (18)0.036 (2)0.0006 (15)0.0000.000
C20.025 (2)0.0206 (17)0.034 (2)0.0020 (14)0.0000.000
C30.022 (2)0.0205 (18)0.038 (2)0.0034 (14)0.0000.000
C40.023 (2)0.0285 (19)0.036 (2)0.0047 (15)0.0000.000
C50.028 (2)0.0206 (17)0.030 (2)0.0040 (15)0.0000.000
C60.028 (2)0.0242 (19)0.034 (2)0.0050 (15)0.0000.000
C70.035 (2)0.0199 (18)0.042 (2)0.0007 (16)0.0000.000
C80.020 (2)0.045 (3)0.077 (3)0.0009 (19)0.0000.000
I20.02894 (17)0.05050 (19)0.0578 (2)0.00543 (12)0.0000.000
O40.0333 (16)0.0306 (15)0.066 (2)0.0051 (12)0.0000.000
O50.0323 (16)0.0268 (14)0.064 (2)0.0049 (12)0.0000.000
O60.067 (2)0.0269 (16)0.082 (2)0.0079 (15)0.0000.000
C90.025 (2)0.034 (2)0.034 (2)0.0051 (17)0.0000.000
C100.031 (2)0.0284 (19)0.034 (2)0.0059 (16)0.0000.000
C110.032 (2)0.0216 (19)0.035 (2)0.0016 (16)0.0000.000
C120.028 (2)0.036 (2)0.035 (2)0.0005 (17)0.0000.000
C130.040 (2)0.0248 (19)0.030 (2)0.0032 (17)0.0000.000
C140.041 (3)0.026 (2)0.038 (2)0.0044 (18)0.0000.000
C150.037 (3)0.038 (2)0.045 (3)0.0093 (19)0.0000.000
C160.039 (3)0.038 (2)0.065 (3)0.014 (2)0.0000.000
Geometric parameters (Å, °) top
I1—C12.077 (4)I2—C92.085 (4)
O1—C21.347 (4)O4—C101.336 (4)
O1—H1O0.8200O4—H4O0.82
O2—C31.368 (4)O5—C111.371 (4)
O2—C81.430 (5)O5—C161.413 (5)
O3—C71.207 (5)O6—C151.205 (5)
C1—C61.386 (5)C9—C141.382 (6)
C1—C21.392 (5)C9—C101.396 (5)
C2—C31.408 (5)C10—C111.399 (5)
C3—C41.363 (5)C11—C121.371 (5)
C4—C51.400 (5)C12—C131.390 (5)
C4—H40.93C12—H120.93
C5—C61.384 (5)C13—C141.379 (6)
C5—C71.464 (5)C13—C151.465 (5)
C6—H60.93C14—H140.93
C7—H70.93C15—H150.93
C8—H8A0.96C16—H16A0.96
C8—H8B0.96C16—H16B0.96
C2—O1—H1O109.5C10—O4—H4O109.5
C3—O2—C8117.0 (3)C11—O5—C16116.8 (3)
C6—C1—C2120.5 (3)C14—C9—C10120.7 (4)
C6—C1—I1120.4 (3)C14—C9—I2120.9 (3)
C2—C1—I1119.1 (3)C10—C9—I2118.4 (3)
O1—C2—C1118.7 (3)O4—C10—C9119.8 (4)
O1—C2—C3122.1 (3)O4—C10—C11121.1 (3)
C1—C2—C3119.2 (3)C9—C10—C11119.0 (3)
C4—C3—O2126.7 (3)C12—C11—O5126.4 (4)
C4—C3—C2120.3 (3)C12—C11—C10120.1 (3)
O2—C3—C2113.0 (3)O5—C11—C10113.5 (3)
C3—C4—C5120.1 (3)C11—C12—C13120.3 (4)
C3—C4—H4120.0C11—C12—H12119.8
C5—C4—H4120.0C13—C12—H12119.8
C6—C5—C4120.4 (3)C14—C13—C12120.4 (4)
C6—C5—C7118.5 (3)C14—C13—C15121.1 (4)
C4—C5—C7121.1 (3)C12—C13—C15118.5 (4)
C5—C6—C1119.5 (3)C13—C14—C9119.5 (4)
C5—C6—H6120.2C13—C14—H14120.2
C1—C6—H6120.2C9—C14—H14120.2
O3—C7—C5125.5 (4)O6—C15—C13126.2 (4)
O3—C7—H7117.3O6—C15—H15116.9
C5—C7—H7117.3C13—C15—H15116.9
O2—C8—H8A109.5O5—C16—H16A109.5
O2—C8—H8B109.5O5—C16—H16B109.5
H8A—C8—H8B109.5H16A—C16—H16B109.5
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1O···O20.822.212.661 (4)115
O1—H1O···O3i0.821.932.634 (4)143
O4—H4O···O50.822.182.639 (4)116
O4—H4O···O6ii0.822.102.746 (4)135
Symmetry codes: (i) −x+1/2, y+1/2, −z+1; (ii) −x+1/2, y−1/2, −z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1—H1O···O20.822.212.661 (4)115
O1—H1O···O3i0.821.932.634 (4)143
O4—H4O···O50.822.182.639 (4)116
O4—H4O···O6ii0.822.102.746 (4)135
Symmetry codes: (i) −x+1/2, y+1/2, −z+1; (ii) −x+1/2, y−1/2, −z.
Acknowledgements top

This work was supported by the National Natural Science Foundation of China (grant No. 20576066).

references
References top

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