Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807029777/dn2193sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807029777/dn2193Isup2.hkl |
CCDC reference: 655036
A une solution de 3-hydroxy-5,6,7,8 - tétrahydronaphtalène-2-carboxylate d'éthyle (2 mmol) dans 2 ml d'acide acétique est ajoutée goutte-à -goutte une solution de brome (2 mmol) dans 2 ml d'acide acétique sous agitation magnétique, à température ambiante. Après deux heures, le mélange résultant a été dilué dans l'eau et extrait avec du dichlorométhane. La phase organique a été lavée avec de l'eau jusqu'á neutralité. Le résidu a été purifié sur une colonne de chromatographie (éther de pétrole) pour obtenir á l'état très pur le 4-bromo-3-hydroxy-5,6,7,8 - tétrahydronaphtalène-2-carboxylate d'éthyle.
L'ensemble des atomes d'hydrogène ont été fixés géométriquement et traités en utilisant un `riding model' avec des distances C—H = 0.93 Å (Caromatique), 0.97 Å (Cmethylène), 0.96 Å (CH3) et O—H = 0.82 Å avec des facteurs de température Uiso(H) = 1.2Ueq(Caromatique, Cmethylène, O) et Uiso(H) = 1.5Ueq(CH3).
Les esters du 4-bromo-3-hydroxynaphtalène ont été rarement étudiés bien qu'ils soient à la base de composés à intérêt biologique (Kasibhatla et al., 2001).
La molécule C13H15BrO3 est caracterisée par la présence d'un noyau 5,6,7,8 - tétrahydronaphtalène ayant le groupe phényle trisubstitué en C2, C3 et C4 portant respectivement une fonction ester, un groupe hydroxyle et un atome de brome (Fig. 1). Ces trois derniers substituants et le noyau phényle sont situés dans un plan miroir. Les atomes de carbone C5, C8, C9 et C10 sont situés dans ce plan miroir. Les atomes de carbone C6 et C7 sont statistiquement distribués par rapport à ce plan cristallographique. Les valeurs des longueurs des liaisions C4—Br1 (1,908 (5) Å), C11═O1 (1,217 (6) Å) et la valeur moyenne des distances C—O (1,381 (7) Å) sont en accord avec celles des composés possédant des liaisons de ce type (Ben Amor & Jouini, 1999; Canty et al., 2004; Béji et al., 2005).
Pour le contexte général du travail, voir: Kasibhatla et al. (2001). Pour structures associées, voir: Ben Amor & Jouini, 1999; Canty et al., 2004; Béji et al., 2005.
Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 1998); software used to prepare material for publication: SHELXL97.
Fig. 1. Représentation de la molécule C13H15BrO3. Les ellipsoides d'agitation thermique représentent 30% de probabilité de présence. |
C13H15BrO3 | F(000) = 608 |
Mr = 299.16 | Dx = 1.570 Mg m−3 |
Monoclinic, C2/m | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2y | Cell parameters from 25 reflections |
a = 20.840 (6) Å | θ = 10.5–14.7° |
b = 7.141 (3) Å | µ = 3.24 mm−1 |
c = 9.364 (3) Å | T = 298 K |
β = 114.77 (3)° | Plate, colourless |
V = 1265.3 (8) Å3 | 0.40 × 0.10 × 0.10 mm |
Z = 4 |
Enraf–Nonius CAD-4 diffractometer | 1070 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.013 |
Graphite monochromator | θmax = 27.0°, θmin = 2.2° |
ω/2θ scans | h = −26→24 |
Absorption correction: ψ scan (North et al., 1968) | k = −1→9 |
Tmin = 0.567, Tmax = 1.000 | l = 0→11 |
3614 measured reflections | 2 standard reflections every 120 min |
1483 independent reflections | intensity decay: 4% |
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)] = 0.047 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.120 | H-atom parameters constrained |
S = 1.15 | w = 1/[σ2(Fo2) + (0.051P)2 + 1.9759P] where P = (Fo2 + 2Fc2)/3 |
1483 reflections | (Δ/σ)max = 0.002 |
109 parameters | Δρmax = 0.59 e Å−3 |
0 restraints | Δρmin = −0.31 e Å−3 |
C13H15BrO3 | V = 1265.3 (8) Å3 |
Mr = 299.16 | Z = 4 |
Monoclinic, C2/m | Mo Kα radiation |
a = 20.840 (6) Å | µ = 3.24 mm−1 |
b = 7.141 (3) Å | T = 298 K |
c = 9.364 (3) Å | 0.40 × 0.10 × 0.10 mm |
β = 114.77 (3)° |
Enraf–Nonius CAD-4 diffractometer | 1070 reflections with I > 2σ(I) |
Absorption correction: ψ scan (North et al., 1968) | Rint = 0.013 |
Tmin = 0.567, Tmax = 1.000 | 2 standard reflections every 120 min |
3614 measured reflections | intensity decay: 4% |
1483 independent reflections |
R[F2 > 2σ(F2)] = 0.047 | 0 restraints |
wR(F2) = 0.120 | H-atom parameters constrained |
S = 1.15 | Δρmax = 0.59 e Å−3 |
1483 reflections | Δρmin = −0.31 e Å−3 |
109 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) | |
Br1 | 0.59010 (3) | 0.5000 | 0.98075 (8) | 0.0748 (3) | |
O1 | 0.8758 (2) | 0.5000 | 1.3330 (4) | 0.0636 (10) | |
O2 | 0.92499 (17) | 0.5000 | 1.1618 (4) | 0.0572 (9) | |
O3 | 0.7377 (2) | 0.5000 | 1.2234 (4) | 0.0630 (10) | |
H3 | 0.7785 | 0.5000 | 1.2911 | 0.076* | |
C1 | 0.7968 (2) | 0.5000 | 0.9059 (5) | 0.0468 (11) | |
H1 | 0.8385 | 0.5000 | 0.8924 | 0.056* | |
C2 | 0.8008 (2) | 0.5000 | 1.0587 (5) | 0.0417 (10) | |
C3 | 0.7380 (3) | 0.5000 | 1.0790 (5) | 0.0449 (11) | |
C4 | 0.6740 (2) | 0.5000 | 0.9467 (6) | 0.0445 (11) | |
C5 | 0.5989 (2) | 0.5000 | 0.6514 (6) | 0.0544 (12) | |
H5A | 0.5761 | 0.3798 | 0.6447 | 0.065* | 0.50 |
H5B | 0.5689 | 0.5955 | 0.6655 | 0.065* | 0.50 |
C6 | 0.6056 (4) | 0.536 (5) | 0.4988 (8) | 0.084 (10) | 0.50 |
H6A | 0.5871 | 0.4255 | 0.4348 | 0.101* | 0.50 |
H6B | 0.5726 | 0.6367 | 0.4470 | 0.101* | 0.50 |
C7 | 0.6621 (3) | 0.5774 (12) | 0.4855 (7) | 0.062 (2) | 0.50 |
H7A | 0.6656 | 0.7128 | 0.4853 | 0.074* | 0.50 |
H7B | 0.6572 | 0.5338 | 0.3834 | 0.074* | 0.50 |
C8 | 0.7335 (3) | 0.5000 | 0.6118 (6) | 0.0624 (15) | |
H8A | 0.7408 | 0.3734 | 0.5841 | 0.075* | 0.50 |
H8B | 0.7722 | 0.5770 | 0.6136 | 0.075* | 0.50 |
C9 | 0.7332 (2) | 0.5000 | 0.7743 (5) | 0.0432 (10) | |
C10 | 0.6699 (2) | 0.5000 | 0.7937 (5) | 0.0422 (10) | |
C11 | 0.8699 (3) | 0.5000 | 1.1980 (6) | 0.0492 (11) | |
C12 | 0.9947 (3) | 0.5000 | 1.2930 (6) | 0.0611 (14) | |
H12A | 1.0005 | 0.3897 | 1.3578 | 0.073* | 0.50 |
H12B | 1.0005 | 0.6103 | 1.3578 | 0.073* | 0.50 |
C13 | 1.0479 (3) | 0.5000 | 1.2249 (7) | 0.085 (2) | |
H13A | 1.0946 | 0.5000 | 1.3084 | 0.127* | |
H13B | 1.0416 | 0.6098 | 1.1613 | 0.127* | 0.50 |
H13C | 1.0416 | 0.3902 | 1.1613 | 0.127* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0585 (4) | 0.0930 (5) | 0.0924 (5) | 0.000 | 0.0507 (3) | 0.000 |
O1 | 0.066 (2) | 0.083 (3) | 0.0402 (18) | 0.000 | 0.0209 (17) | 0.000 |
O2 | 0.0413 (17) | 0.083 (3) | 0.0418 (18) | 0.000 | 0.0119 (14) | 0.000 |
O3 | 0.067 (2) | 0.080 (3) | 0.054 (2) | 0.000 | 0.0383 (18) | 0.000 |
C1 | 0.041 (2) | 0.055 (3) | 0.047 (2) | 0.000 | 0.020 (2) | 0.000 |
C2 | 0.047 (2) | 0.038 (2) | 0.042 (2) | 0.000 | 0.021 (2) | 0.000 |
C3 | 0.056 (3) | 0.034 (2) | 0.054 (3) | 0.000 | 0.032 (2) | 0.000 |
C4 | 0.043 (2) | 0.038 (2) | 0.061 (3) | 0.000 | 0.031 (2) | 0.000 |
C5 | 0.035 (2) | 0.060 (3) | 0.066 (3) | 0.000 | 0.018 (2) | 0.000 |
C6 | 0.049 (4) | 0.13 (3) | 0.054 (4) | 0.023 (9) | 0.006 (3) | 0.021 (9) |
C7 | 0.051 (4) | 0.085 (6) | 0.042 (3) | 0.000 (4) | 0.013 (3) | 0.002 (3) |
C8 | 0.048 (3) | 0.099 (4) | 0.040 (2) | 0.000 | 0.018 (2) | 0.000 |
C9 | 0.040 (2) | 0.049 (3) | 0.043 (2) | 0.000 | 0.020 (2) | 0.000 |
C10 | 0.040 (2) | 0.034 (2) | 0.054 (3) | 0.000 | 0.021 (2) | 0.000 |
C11 | 0.054 (3) | 0.047 (3) | 0.045 (3) | 0.000 | 0.019 (2) | 0.000 |
C12 | 0.048 (3) | 0.082 (4) | 0.042 (3) | 0.000 | 0.008 (2) | 0.000 |
C13 | 0.045 (3) | 0.140 (7) | 0.058 (3) | 0.000 | 0.011 (3) | 0.000 |
Br1—C4 | 1.905 (4) | C6—C7 | 1.268 (12) |
O1—C11 | 1.218 (6) | C6—H6A | 0.9700 |
O2—C11 | 1.327 (6) | C6—H6B | 0.9700 |
O2—C12 | 1.457 (6) | C7—C8 | 1.563 (8) |
O3—C3 | 1.356 (5) | C7—H7A | 0.9700 |
O3—H3 | 0.8200 | C7—H7B | 0.9700 |
C1—C9 | 1.380 (7) | C8—C9 | 1.525 (6) |
C1—C2 | 1.397 (6) | C8—C7i | 1.563 (8) |
C1—H1 | 0.9300 | C8—H8A | 0.9700 |
C2—C3 | 1.399 (6) | C8—H8B | 0.9700 |
C2—C11 | 1.483 (7) | C9—C10 | 1.405 (6) |
C3—C4 | 1.388 (7) | C12—C13 | 1.492 (8) |
C4—C10 | 1.399 (6) | C12—H12A | 0.9700 |
C5—C6i | 1.516 (10) | C12—H12B | 0.9700 |
C5—C6 | 1.516 (10) | C13—H13A | 0.9600 |
C5—C10 | 1.520 (7) | C13—H13B | 0.9600 |
C5—H5A | 0.9700 | C13—H13C | 0.9600 |
C5—H5B | 0.9700 | ||
C11—O2—C12 | 116.7 (4) | C8—C7—H7B | 107.8 |
C3—O3—H3 | 109.5 | H7A—C7—H7B | 107.1 |
C9—C1—C2 | 122.6 (4) | C9—C8—C7i | 110.7 (4) |
C9—C1—H1 | 118.7 | C9—C8—C7 | 110.7 (4) |
C2—C1—H1 | 118.7 | C7i—C8—C7 | 41.4 (6) |
C1—C2—C3 | 118.7 (4) | C9—C8—H8A | 109.5 |
C1—C2—C11 | 121.4 (4) | C7i—C8—H8A | 71.0 |
C3—C2—C11 | 119.9 (4) | C7—C8—H8A | 109.5 |
O3—C3—C4 | 119.0 (4) | C9—C8—H8B | 109.5 |
O3—C3—C2 | 122.1 (4) | C7i—C8—H8B | 137.3 |
C4—C3—C2 | 118.8 (4) | C7—C8—H8B | 109.5 |
C3—C4—C10 | 122.5 (4) | H8A—C8—H8B | 108.1 |
C3—C4—Br1 | 117.2 (3) | C1—C9—C10 | 119.1 (4) |
C10—C4—Br1 | 120.3 (3) | C1—C9—C8 | 119.2 (4) |
C6i—C5—C6 | 20 (3) | C10—C9—C8 | 121.7 (4) |
C6i—C5—C10 | 112.7 (4) | C4—C10—C9 | 118.3 (4) |
C6—C5—C10 | 112.7 (4) | C4—C10—C5 | 121.2 (4) |
C6i—C5—H5A | 91.3 | C9—C10—C5 | 120.6 (4) |
C6—C5—H5A | 109.1 | O1—C11—O2 | 122.9 (5) |
C10—C5—H5A | 109.1 | O1—C11—C2 | 123.5 (5) |
C6i—C5—H5B | 124.6 | O2—C11—C2 | 113.6 (4) |
C6—C5—H5B | 109.1 | O2—C12—C13 | 107.2 (4) |
C10—C5—H5B | 109.1 | O2—C12—H12A | 110.3 |
H5A—C5—H5B | 107.8 | C13—C12—H12A | 110.3 |
C7—C6—C5 | 126.0 (6) | O2—C12—H12B | 110.3 |
C7—C6—H6A | 105.8 | C13—C12—H12B | 110.3 |
C5—C6—H6A | 105.8 | H12A—C12—H12B | 108.5 |
C7—C6—H6B | 105.8 | C12—C13—H13A | 109.5 |
C5—C6—H6B | 105.8 | C12—C13—H13B | 109.5 |
H6A—C6—H6B | 106.2 | H13A—C13—H13B | 109.5 |
C6—C7—C8 | 118.2 (11) | C12—C13—H13C | 109.5 |
C6—C7—H7A | 107.8 | H13A—C13—H13C | 109.5 |
C8—C7—H7A | 107.8 | H13B—C13—H13C | 109.5 |
C6—C7—H7B | 107.8 |
Symmetry code: (i) x, −y+1, z. |
Experimental details
Crystal data | |
Chemical formula | C13H15BrO3 |
Mr | 299.16 |
Crystal system, space group | Monoclinic, C2/m |
Temperature (K) | 298 |
a, b, c (Å) | 20.840 (6), 7.141 (3), 9.364 (3) |
β (°) | 114.77 (3) |
V (Å3) | 1265.3 (8) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 3.24 |
Crystal size (mm) | 0.40 × 0.10 × 0.10 |
Data collection | |
Diffractometer | Enraf–Nonius CAD-4 |
Absorption correction | ψ scan (North et al., 1968) |
Tmin, Tmax | 0.567, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3614, 1483, 1070 |
Rint | 0.013 |
(sin θ/λ)max (Å−1) | 0.638 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.047, 0.120, 1.15 |
No. of reflections | 1483 |
No. of parameters | 109 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.59, −0.31 |
Computer programs: CAD-4 EXPRESS (Enraf–Nonius, 1994), CAD-4 EXPRESS, XCAD4 (Harms & Wocadlo, 1995), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), DIAMOND (Brandenburg, 1998), SHELXL97.
Les esters du 4-bromo-3-hydroxynaphtalène ont été rarement étudiés bien qu'ils soient à la base de composés à intérêt biologique (Kasibhatla et al., 2001).
La molécule C13H15BrO3 est caracterisée par la présence d'un noyau 5,6,7,8 - tétrahydronaphtalène ayant le groupe phényle trisubstitué en C2, C3 et C4 portant respectivement une fonction ester, un groupe hydroxyle et un atome de brome (Fig. 1). Ces trois derniers substituants et le noyau phényle sont situés dans un plan miroir. Les atomes de carbone C5, C8, C9 et C10 sont situés dans ce plan miroir. Les atomes de carbone C6 et C7 sont statistiquement distribués par rapport à ce plan cristallographique. Les valeurs des longueurs des liaisions C4—Br1 (1,908 (5) Å), C11═O1 (1,217 (6) Å) et la valeur moyenne des distances C—O (1,381 (7) Å) sont en accord avec celles des composés possédant des liaisons de ce type (Ben Amor & Jouini, 1999; Canty et al., 2004; Béji et al., 2005).