Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802019839/lh6010sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536802019839/lh6010Isup2.hkl |
CCDC reference: 202319
The compound was prepared according to a method already described in the literature (Drewes et al., 1987). After evaporation of the solvent fine plates of crystals were obtained and analysed via X-ray analysis. Furthermore NMR spectra were recorded on a Bruker AMX 300. 1H NMR (300 MHz, CDCl3, p.p.m.): δ = 3.77 (s, 6H, 2 × OCH3), 4.55 (m, 4H, 2 × CH2), 5.90 and 6.33 (m, 4H, 2 × ═CH2); 13C NMR (75 MHz, CDCl3): δ = 51.67 (q, 2 × OCH3), 68.65 (t, 2 × CH2), 125.89 (t, 2 × CH2), 136.63 (s, 2 × ═C), 166.03 (s, 2 × C═O).
All H atoms were included in calculated positions, with C—H distances of 0.95 (for sp2 H atoms), 0.99 (for sp3 H atoms) and 0.98 Å (for methyl sp3 H atoms). The H atoms were then included in the refinement riding on their parent atoms, with Uiso = 1.2Ueq (or 1.5Ueq for methyl H atoms).
Data collection: SMART (Bruker, 1997); cell refinement: SMART; data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Bruker, 1998); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
C10H14O5 | Z = 2 |
Mr = 214.21 | F(000) = 228 |
Triclinic, P1 | Dx = 1.315 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 6.8104 (13) Å | Cell parameters from 1575 reflections |
b = 7.1777 (14) Å | θ = 3.1–28.2° |
c = 12.458 (3) Å | µ = 0.11 mm−1 |
α = 74.713 (3)° | T = 153 K |
β = 78.365 (4)° | Plate, colorless |
γ = 67.939 (3)° | 0.50 × 0.50 × 0.10 mm |
V = 540.84 (18) Å3 |
SMART APEX CCD area-detector diffractometer | 2342 independent reflections |
Radiation source: sealed tube | 1880 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.035 |
ϕ and ω scans | θmax = 28.3°, θmin = 1.7° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −7→8 |
Tmin = 0.889, Tmax = 0.931 | k = −9→9 |
3269 measured reflections | l = −14→15 |
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: difference Fourier map |
wR(F2) = 0.116 | H-atom parameters constrained |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0687P)2] where P = (Fo2 + 2Fc2)/3 |
2342 reflections | (Δ/σ)max = 0.001 |
138 parameters | Δρmax = 0.18 e Å−3 |
0 restraints | Δρmin = −0.24 e Å−3 |
C10H14O5 | γ = 67.939 (3)° |
Mr = 214.21 | V = 540.84 (18) Å3 |
Triclinic, P1 | Z = 2 |
a = 6.8104 (13) Å | Mo Kα radiation |
b = 7.1777 (14) Å | µ = 0.11 mm−1 |
c = 12.458 (3) Å | T = 153 K |
α = 74.713 (3)° | 0.50 × 0.50 × 0.10 mm |
β = 78.365 (4)° |
SMART APEX CCD area-detector diffractometer | 2342 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1880 reflections with I > 2σ(I) |
Tmin = 0.889, Tmax = 0.931 | Rint = 0.035 |
3269 measured reflections |
R[F2 > 2σ(F2)] = 0.039 | 0 restraints |
wR(F2) = 0.116 | H-atom parameters constrained |
S = 1.05 | Δρmax = 0.18 e Å−3 |
2342 reflections | Δρmin = −0.24 e Å−3 |
138 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 | ||
O1 | 0.71444 (12) | 0.17269 (14) | 1.29153 (6) | 0.0327 (2) | |
O2 | 0.95015 (11) | 0.15845 (13) | 1.13605 (6) | 0.0348 (2) | |
O3 | 0.47136 (11) | 0.27161 (12) | 0.94051 (6) | 0.0276 (2) | |
O4 | 0.57704 (13) | 0.22754 (15) | 0.60466 (7) | 0.0445 (3) | |
O5 | 0.22465 (12) | 0.32825 (13) | 0.59753 (7) | 0.0354 (2) | |
C1 | 0.88874 (19) | 0.1302 (2) | 1.35511 (10) | 0.0390 (3) | |
H1A | 0.9927 | −0.0067 | 1.3506 | 0.059* | |
H1B | 0.8329 | 0.1353 | 1.4336 | 0.059* | |
H1C | 0.9582 | 0.2334 | 1.3241 | 0.059* | |
C2 | 0.76908 (17) | 0.18184 (16) | 1.18083 (9) | 0.0244 (3) | |
C3 | 0.58714 (16) | 0.22190 (15) | 1.11852 (9) | 0.0227 (2) | |
C4 | 0.38952 (17) | 0.24803 (17) | 1.16838 (9) | 0.0280 (3) | |
H4A | 0.3597 | 0.2415 | 1.2469 | 0.034* | |
H4B | 0.2781 | 0.2733 | 1.1255 | 0.034* | |
C5 | 0.65277 (16) | 0.22592 (18) | 0.99564 (9) | 0.0266 (3) | |
H5A | 0.7211 | 0.3313 | 0.9628 | 0.032* | |
H5B | 0.7579 | 0.0908 | 0.9849 | 0.032* | |
C6 | 0.53389 (17) | 0.26234 (17) | 0.82555 (9) | 0.0252 (3) | |
H6A | 0.6425 | 0.1266 | 0.8188 | 0.030* | |
H6B | 0.5978 | 0.3694 | 0.7876 | 0.030* | |
C7 | 0.34295 (17) | 0.29528 (16) | 0.77066 (9) | 0.0250 (3) | |
C8 | 0.14597 (18) | 0.32978 (19) | 0.82317 (10) | 0.0333 (3) | |
H8A | 0.0328 | 0.3454 | 0.7840 | 0.040* | |
H8B | 0.1185 | 0.3388 | 0.8998 | 0.040* | |
C9 | 0.39622 (18) | 0.27957 (17) | 0.65022 (9) | 0.0278 (3) | |
C10 | 0.2706 (2) | 0.3134 (2) | 0.48025 (10) | 0.0431 (3) | |
H10A | 0.3513 | 0.4036 | 0.4392 | 0.065* | |
H10B | 0.1365 | 0.3556 | 0.4482 | 0.065* | |
H10C | 0.3551 | 0.1712 | 0.4743 | 0.065* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0230 (4) | 0.0513 (5) | 0.0235 (4) | −0.0126 (4) | −0.0027 (3) | −0.0073 (4) |
O2 | 0.0202 (4) | 0.0519 (6) | 0.0331 (5) | −0.0114 (4) | 0.0006 (3) | −0.0142 (4) |
O3 | 0.0201 (4) | 0.0392 (5) | 0.0229 (4) | −0.0081 (3) | −0.0021 (3) | −0.0088 (3) |
O4 | 0.0266 (5) | 0.0721 (7) | 0.0307 (5) | −0.0109 (4) | 0.0016 (4) | −0.0163 (4) |
O5 | 0.0283 (5) | 0.0479 (5) | 0.0285 (5) | −0.0060 (4) | −0.0076 (3) | −0.0122 (4) |
C1 | 0.0295 (7) | 0.0600 (9) | 0.0279 (6) | −0.0133 (6) | −0.0080 (5) | −0.0090 (6) |
C2 | 0.0214 (6) | 0.0251 (6) | 0.0260 (6) | −0.0074 (4) | 0.0003 (4) | −0.0072 (4) |
C3 | 0.0204 (6) | 0.0217 (5) | 0.0254 (6) | −0.0065 (4) | −0.0017 (4) | −0.0052 (4) |
C4 | 0.0226 (6) | 0.0332 (6) | 0.0277 (6) | −0.0100 (5) | −0.0016 (4) | −0.0060 (5) |
C5 | 0.0177 (5) | 0.0332 (6) | 0.0268 (6) | −0.0066 (4) | −0.0012 (4) | −0.0070 (5) |
C6 | 0.0211 (6) | 0.0296 (6) | 0.0242 (6) | −0.0081 (4) | 0.0012 (4) | −0.0080 (4) |
C7 | 0.0233 (6) | 0.0235 (5) | 0.0262 (6) | −0.0058 (4) | −0.0033 (4) | −0.0045 (4) |
C8 | 0.0249 (6) | 0.0415 (7) | 0.0309 (6) | −0.0078 (5) | −0.0032 (5) | −0.0087 (5) |
C9 | 0.0250 (6) | 0.0295 (6) | 0.0268 (6) | −0.0073 (5) | −0.0036 (5) | −0.0053 (5) |
C10 | 0.0413 (8) | 0.0589 (9) | 0.0290 (7) | −0.0104 (6) | −0.0101 (5) | −0.0140 (6) |
O1—C2 | 1.3447 (13) | C1—H1A | 0.9800 |
O1—C1 | 1.4524 (13) | C1—H1B | 0.9800 |
O2—C2 | 1.2151 (13) | C1—H1C | 0.9800 |
O3—C6 | 1.4212 (13) | C4—H4A | 0.9500 |
O3—C5 | 1.4230 (13) | C4—H4B | 0.9500 |
O4—C9 | 1.2093 (14) | C5—H5A | 0.9900 |
O5—C9 | 1.3416 (13) | C5—H5B | 0.9900 |
O5—C10 | 1.4549 (14) | C6—H6A | 0.9900 |
C2—C3 | 1.4911 (14) | C6—H6B | 0.9900 |
C3—C4 | 1.3293 (15) | C8—H8A | 0.9500 |
C3—C5 | 1.5016 (15) | C8—H8B | 0.9500 |
C6—C7 | 1.5023 (15) | C10—H10A | 0.9800 |
C7—C8 | 1.3308 (16) | C10—H10B | 0.9800 |
C7—C9 | 1.4949 (15) | C10—H10C | 0.9800 |
C2—O1—C1 | 115.15 (9) | C3—C4—H4A | 120.0 |
C6—O3—C5 | 110.40 (8) | C3—C4—H4B | 120.0 |
C9—O5—C10 | 115.18 (9) | H4A—C4—H4B | 120.0 |
O2—C2—O1 | 123.04 (10) | O3—C5—H5A | 109.7 |
O2—C2—C3 | 123.25 (10) | C3—C5—H5A | 109.7 |
O1—C2—C3 | 113.71 (9) | O3—C5—H5B | 109.7 |
C4—C3—C2 | 122.70 (10) | C3—C5—H5B | 109.7 |
C4—C3—C5 | 124.47 (10) | H5A—C5—H5B | 108.2 |
C2—C3—C5 | 112.82 (9) | O3—C6—H6A | 109.7 |
O3—C5—C3 | 110.04 (8) | C7—C6—H6A | 109.7 |
O3—C6—C7 | 109.70 (8) | O3—C6—H6B | 109.7 |
C8—C7—C9 | 122.51 (10) | C7—C6—H6B | 109.7 |
C8—C7—C6 | 124.25 (10) | H6A—C6—H6B | 108.2 |
C9—C7—C6 | 113.22 (9) | C7—C8—H8A | 120.0 |
O4—C9—O5 | 123.20 (10) | C7—C8—H8B | 120.0 |
O4—C9—C7 | 123.12 (10) | H8A—C8—H8B | 120.0 |
O5—C9—C7 | 113.68 (9) | O5—C10—H10A | 109.5 |
O1—C1—H1A | 109.5 | O5—C10—H10B | 109.5 |
O1—C1—H1B | 109.5 | H10A—C10—H10B | 109.5 |
H1A—C1—H1B | 109.5 | O5—C10—H10C | 109.5 |
O1—C1—H1C | 109.5 | H10A—C10—H10C | 109.5 |
H1A—C1—H1C | 109.5 | H10B—C10—H10C | 109.5 |
H1B—C1—H1C | 109.5 | ||
C1—O1—C2—O2 | −0.65 (16) | C5—O3—C6—C7 | 175.78 (8) |
C1—O1—C2—C3 | 178.96 (9) | O3—C6—C7—C8 | 0.63 (15) |
O2—C2—C3—C4 | −179.73 (11) | O3—C6—C7—C9 | −177.70 (8) |
O1—C2—C3—C4 | 0.66 (15) | C10—O5—C9—O4 | 0.25 (17) |
O2—C2—C3—C5 | 1.14 (15) | C10—O5—C9—C7 | −179.64 (9) |
O1—C2—C3—C5 | −178.47 (8) | C8—C7—C9—O4 | −172.14 (12) |
C6—O3—C5—C3 | −176.15 (8) | C6—C7—C9—O4 | 6.22 (16) |
C4—C3—C5—O3 | 2.85 (15) | C8—C7—C9—O5 | 7.74 (16) |
C2—C3—C5—O3 | −178.03 (8) | C6—C7—C9—O5 | −173.89 (9) |
Experimental details
Crystal data | |
Chemical formula | C10H14O5 |
Mr | 214.21 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 153 |
a, b, c (Å) | 6.8104 (13), 7.1777 (14), 12.458 (3) |
α, β, γ (°) | 74.713 (3), 78.365 (4), 67.939 (3) |
V (Å3) | 540.84 (18) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.11 |
Crystal size (mm) | 0.50 × 0.50 × 0.10 |
Data collection | |
Diffractometer | SMART APEX CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.889, 0.931 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3269, 2342, 1880 |
Rint | 0.035 |
(sin θ/λ)max (Å−1) | 0.667 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.039, 0.116, 1.05 |
No. of reflections | 2342 |
No. of parameters | 138 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.18, −0.24 |
Computer programs: SMART (Bruker, 1997), SMART, SAINT (Bruker, 2000), SHELXTL (Bruker, 1998), SHELXTL.
O1—C2 | 1.3447 (13) | O5—C10 | 1.4549 (14) |
O1—C1 | 1.4524 (13) | C2—C3 | 1.4911 (14) |
O2—C2 | 1.2151 (13) | C3—C4 | 1.3293 (15) |
O3—C6 | 1.4212 (13) | C3—C5 | 1.5016 (15) |
O3—C5 | 1.4230 (13) | C6—C7 | 1.5023 (15) |
O4—C9 | 1.2093 (14) | C7—C8 | 1.3308 (16) |
O5—C9 | 1.3416 (13) | C7—C9 | 1.4949 (15) |
C2—O1—C1 | 115.15 (9) | O3—C5—C3 | 110.04 (8) |
C6—O3—C5 | 110.40 (8) | O3—C6—C7 | 109.70 (8) |
C9—O5—C10 | 115.18 (9) | C8—C7—C9 | 122.51 (10) |
O2—C2—O1 | 123.04 (10) | C8—C7—C6 | 124.25 (10) |
O2—C2—C3 | 123.25 (10) | C9—C7—C6 | 113.22 (9) |
O1—C2—C3 | 113.71 (9) | O4—C9—O5 | 123.20 (10) |
C4—C3—C2 | 122.70 (10) | O4—C9—C7 | 123.12 (10) |
C4—C3—C5 | 124.47 (10) | O5—C9—C7 | 113.68 (9) |
C2—C3—C5 | 112.82 (9) |
The title compound, (I), is interesting due to its high functionality. It can be used as a polymerizing agent not only on its own but also as a crosslinker. Although (I) has been well known for several years (Drewes et al., 1987), this is the first crystallographic determination.
The molecular structure of (I) shows non-crystallographic C2v symmetry with atom O3 as its centre. The molecule is almost planar, with maximum deviations of −0.158 (1) Å for O4 and 0.120 (1) Å for O3 from the mean plane for all the atoms. The torsion angles C4—C3—C7—C8 and O2—C2—C9—O4 have values of 2.6 (1) and 9.4 (1)°, respectively. Bond lengths and angles are in good agreement with those reported for related structures, such as CIFYIZ10 or CUMYUE (Rohrer et al., 1984), and LIQHAU or LIQHIC (Steurer & Podlech, 1999). The crystal structure shows complex weak hydrogen-bonding patterns (Fig. 2). The C1—H1B···O4(x, y, z + 1) bridges of 2.44 Å (angle at H of 160°) lead to infinite chains of molecules along [001]. Additional C4—H4B···O2(x − 1, y, z) bridges of 2.53 Å (angle at H of 138°) in the [100] direction link these chains to sheets which are then stacked parallel along [010] with C5—H5B···O2(-x + 2, −y, −z + 2) and C10—H10B···O5(-x, −y + 1, −z + 1) contacts of 2.56 Å (angle at H of 152°) and 2.60 Å (angle at H of 142°), respectively. All these geometric parameters are normalized for C—H = 1.08 Å.