


Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S2056989014027947/cv5480sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S2056989014027947/cv5480Isup2.hkl |
![]() | Chemical Markup Language (CML) file https://doi.org/10.1107/S2056989014027947/cv5480Isup3.cml |
CCDC reference: 1040655
Key indicators
- Single-crystal X-ray study
- T = 296 K
- Mean
(C-C) = 0.009 Å
- R factor = 0.057
- wR factor = 0.133
- Data-to-parameter ratio = 20.5
checkCIF/PLATON results
No syntax errors found
Alert level B PLAT026_ALERT_3_B Ratio Observed / Unique Reflections too Low .... 34 %
Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.968 Note PLAT242_ALERT_2_C Low Ueq as Compared to Neighbors for ..... C11 Check PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds ............... 0.0086 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H2 .. O2 .. 2.62 Ang. PLAT906_ALERT_3_C Large K value in the Analysis of Variance ...... 21.386 Check PLAT906_ALERT_3_C Large K value in the Analysis of Variance ...... 7.210 Check PLAT906_ALERT_3_C Large K value in the Analysis of Variance ...... 2.082 Check PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 70 Report
Alert level G PLAT005_ALERT_5_G No _iucr_refine_instructions_details in the CIF Please Do ! PLAT899_ALERT_4_G SHELXL97 is Deprecated and Succeeded by SHELXL 2014 Note PLAT912_ALERT_4_G Missing # of FCF Reflections Above STh/L= 0.600 118 Note
0 ALERT level A = Most likely a serious problem - resolve or explain 1 ALERT level B = A potentially serious problem, consider carefully 8 ALERT level C = Check. Ensure it is not caused by an omission or oversight 3 ALERT level G = General information/check it is not something unexpected 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 7 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
3-Acetyl-4-hydroxy-2H-chromen-2-one is one of the well-known 3-substituted-4-hydroxycoumarins, which form a class of fused-ring heterocycles and occur widely among natural products. Several natural products with the coumarinic moiety exhibit interesting biological properties such as anti-oxidant and antibacterial (Kayser & Kolodziej, 1997). They possess also pharmacological activities: anti-inflammatory (Mahidol et al., 2004), anticancer (Wang et al., 2002) and inhibition of platelet aggregation (Cravotto et al., 2001). These derivatives are very susceptible to electrophilic substitutions (Dou et al., 1969); their reaction with bromine can give rise to several compounds used as intermediate products susceptible to interesting substitutions (Takase et al., 1971) in a wide range of organic syntheses. The bromination of these compounds increases their anticonvulsant activity (Dimmock et al., 2000), which gives them pharmacological importance. Thus, as part of a study of the effects of substituents on the crystal structures of 3-acetyl-4-hydroxycoumarins (Traven et al., 2000), the structure of 3-(2,2-dibromoacetyl)-4-hydroxy-2H-chromen-2-one, (I), has been determined.
In the title compound (Fig. 1), the hydroxy group is involved in formation of an intramolecular O—H···O hydrogen bond (Table 1). In fact, the O3—H5 distance of 0.94 (7) Å has decreased from 1.02 (3) Å, observed in the starting reagent 3-acetyl-4-hydroxy-2H-chromen-2-one (Lyssenko & Antipin, 2001). The H5···O4 distance of 1.65 (7) Å is elongated compared with its value in the parent compound [1.45 (3) Å], and the O3—H5···O4 angle of 147 (6)° is significantly smaller than that found for the starting reagent [161 (2)°]. This trend has already been observed in the fluorinated compound 2-difluoroacetyl-1,3-cyclohexadione (Grieco et al., 2011), in which the O3—H5 and H5···O4 distances are even more affected (0.908 and 1.658 Å respectively). These observations can be easily understood from the point of view of the strong attractive effect of the halogen atoms due to their high electronegativities. All these geometrical parameters are in good agreement with the significant attractor effect of the halogen atoms, which affects the lone pairs of the oxygen atom O4, leading to a decrease of the attractor effect of O4 in the H5···O4 hydrogen bond and, consequently, an increase in the H5···O4 distance.
The C—C and C—O bond lengths in (I) correspond well to those observed in the parent compound, so they are not affected by the α-ketodibromation except for C10—C11 [1.523 (9) Å] which is elongated as compared to that in the starting reagent [1.485 (2) Å; Lyssenko & Antipin, 2001). This trend had previously been observed in the similar structure of 2-difluoroacetyl-1,3-cyclohexadione (Grieco et al., 2011), in which the difluoration reaction affects the C10—C11 distance [1.529 (2) Å].
In the crystal structure of (I), the molecules are assembled in a head-to-tail overlapping manner as a result of the π–π interactions between the benzene and lactone rings of neighbouring molecules (Table 2) into stacks along the b-axis direction (Fig. 2). The observed stacking arrangement can be considered as a balance between van der Waals dispersion and repulsion interactions, and electrostatic interactions between two rings of opposed polarity – the benzene ring (high electron density) and the lactone ring (low electron density) (Hunter & Sanders, 1990). Weak intermolecular C—H···O hydrogen bonds (Table 2) further link these stacks into layers parallel to the ab plane (Fig. 3).
An excess amount of bromine dissolved in acetic acid was added dropwise to a solution of 3-acetyl-4-hydroxy-2H-chromen-2-one in acetic acid (Fig. 4). During the reaction, the drop addition was made after every disappearance of the brown colour of the bromine. The reaction mixture was maintained under stirring at 373 K until the bromine colour persisted. The resulting solution was left to crystallize at room temperature to obtain transparent crystals of a light-yellow colour. Yield: 70%; m.p. = 375 K.
Data collection: SMART (Bruker, 2001); cell refinement: SMART (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: WinGX (Farrugia, 2012).
C11H6Br2O4 | Z = 4 |
Mr = 361.98 | F(000) = 696 |
Monoclinic, P21/n | Dx = 2.076 Mg m−3 |
Hall symbol: -P 2yn | Melting point: 375 K |
a = 9.399 (4) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 6.916 (3) Å | µ = 7.00 mm−1 |
c = 17.967 (7) Å | T = 296 K |
β = 97.37 (3)° | Needle, yellow |
V = 1158.4 (8) Å3 | 0.15 × 0.12 × 0.10 mm |
Bruker SMART CCD area-detector diffractometer | 3234 independent reflections |
Radiation source: fine-focus sealed tube | 1094 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.089 |
ϕ and ω scans | θmax = 30.4°, θmin = 2.3° |
Absorption correction: for a sphere (WinGX; Farrugia, 2012) | h = −10→13 |
Tmin = 0.58, Tmax = 0.75 | k = −6→8 |
11685 measured reflections | l = −25→25 |
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)] = 0.057 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.133 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.96 | w = 1/[σ2(Fo2) + (0.0409P)2 + 0.259P] where P = (Fo2 + 2Fc2)/3 |
3234 reflections | (Δ/σ)max < 0.001 |
158 parameters | Δρmax = 0.43 e Å−3 |
0 restraints | Δρmin = −0.48 e Å−3 |
C11H6Br2O4 | V = 1158.4 (8) Å3 |
Mr = 361.98 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 9.399 (4) Å | µ = 7.00 mm−1 |
b = 6.916 (3) Å | T = 296 K |
c = 17.967 (7) Å | 0.15 × 0.12 × 0.10 mm |
β = 97.37 (3)° |
Bruker SMART CCD area-detector diffractometer | 3234 independent reflections |
Absorption correction: for a sphere (WinGX; Farrugia, 2012) | 1094 reflections with I > 2σ(I) |
Tmin = 0.58, Tmax = 0.75 | Rint = 0.089 |
11685 measured reflections |
R[F2 > 2σ(F2)] = 0.057 | 0 restraints |
wR(F2) = 0.133 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.96 | Δρmax = 0.43 e Å−3 |
3234 reflections | Δρmin = −0.48 e Å−3 |
158 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 | ||
Br1 | 0.56249 (8) | 0.89000 (12) | 0.15244 (5) | 0.0906 (3) | |
Br2 | 0.58984 (10) | 0.45607 (13) | 0.21230 (4) | 0.1029 (4) | |
O1 | 0.1772 (4) | 0.7341 (5) | −0.05777 (19) | 0.0525 (10) | |
O2 | 0.4010 (5) | 0.6891 (6) | −0.0136 (2) | 0.0637 (12) | |
O3 | 0.0411 (5) | 0.6852 (6) | 0.1484 (2) | 0.0639 (12) | |
O4 | 0.2923 (5) | 0.6171 (7) | 0.2042 (2) | 0.0782 (14) | |
C1 | −0.1597 (7) | 0.7718 (8) | 0.0249 (3) | 0.0552 (16) | |
H1 | −0.1941 | 0.7656 | 0.0711 | 0.066* | |
C2 | −0.2515 (7) | 0.8099 (8) | −0.0390 (4) | 0.0609 (17) | |
H2 | −0.3490 | 0.8267 | −0.0365 | 0.073* | |
C3 | −0.1981 (8) | 0.8233 (8) | −0.1075 (3) | 0.0590 (17) | |
H3 | −0.2612 | 0.8507 | −0.1504 | 0.071* | |
C4 | −0.0559 (7) | 0.7973 (8) | −0.1138 (3) | 0.0533 (16) | |
H4 | −0.0219 | 0.8061 | −0.1601 | 0.064* | |
C5 | 0.0358 (7) | 0.7576 (7) | −0.0489 (3) | 0.0453 (15) | |
C6 | −0.0123 (6) | 0.7421 (7) | 0.0202 (3) | 0.0426 (14) | |
C7 | 0.0922 (7) | 0.7009 (8) | 0.0839 (3) | 0.0476 (15) | |
C8 | 0.2351 (7) | 0.6807 (8) | 0.0762 (3) | 0.0448 (14) | |
C9 | 0.2804 (8) | 0.7008 (8) | 0.0022 (3) | 0.0489 (15) | |
C10 | 0.3352 (7) | 0.6382 (8) | 0.1427 (3) | 0.0576 (17) | |
C11 | 0.4958 (7) | 0.6271 (9) | 0.1383 (3) | 0.0637 (18) | |
H11 | 0.5117 | 0.5825 | 0.0883 | 0.076* | |
H5 | 0.117 (8) | 0.628 (9) | 0.180 (3) | 0.08 (2)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0551 (5) | 0.1001 (6) | 0.1139 (7) | −0.0050 (4) | 0.0000 (4) | −0.0223 (5) |
Br2 | 0.1112 (8) | 0.1317 (8) | 0.0614 (5) | 0.0584 (6) | −0.0057 (4) | 0.0091 (4) |
O1 | 0.044 (3) | 0.071 (3) | 0.042 (2) | 0.005 (2) | 0.004 (2) | 0.0054 (18) |
O2 | 0.044 (3) | 0.093 (3) | 0.055 (3) | 0.010 (2) | 0.008 (2) | 0.006 (2) |
O3 | 0.061 (3) | 0.088 (3) | 0.044 (3) | 0.006 (3) | 0.012 (2) | −0.003 (2) |
O4 | 0.066 (3) | 0.130 (4) | 0.037 (2) | 0.005 (3) | 0.003 (2) | 0.001 (2) |
C1 | 0.052 (5) | 0.054 (4) | 0.062 (4) | −0.001 (3) | 0.017 (4) | −0.007 (3) |
C2 | 0.048 (4) | 0.054 (4) | 0.078 (5) | 0.003 (3) | −0.005 (4) | −0.002 (3) |
C3 | 0.062 (5) | 0.053 (4) | 0.058 (4) | 0.002 (3) | −0.006 (4) | 0.006 (3) |
C4 | 0.046 (5) | 0.054 (4) | 0.058 (4) | 0.000 (3) | 0.001 (3) | 0.004 (3) |
C5 | 0.045 (4) | 0.035 (4) | 0.055 (4) | 0.001 (3) | 0.003 (3) | 0.004 (3) |
C6 | 0.048 (4) | 0.036 (4) | 0.043 (4) | −0.003 (3) | 0.006 (3) | −0.003 (2) |
C7 | 0.059 (5) | 0.046 (4) | 0.040 (4) | −0.008 (3) | 0.016 (3) | −0.004 (3) |
C8 | 0.050 (4) | 0.054 (4) | 0.031 (3) | 0.001 (3) | 0.007 (3) | 0.000 (3) |
C9 | 0.054 (5) | 0.045 (4) | 0.048 (4) | 0.005 (3) | 0.007 (4) | 0.000 (3) |
C10 | 0.062 (5) | 0.064 (4) | 0.045 (4) | 0.005 (3) | 0.002 (4) | −0.001 (3) |
C11 | 0.058 (5) | 0.086 (5) | 0.044 (4) | 0.011 (4) | −0.006 (3) | −0.004 (3) |
Br1—C11 | 1.930 (6) | C2—H2 | 0.9300 |
Br2—C11 | 1.910 (6) | C3—C4 | 1.368 (8) |
O1—C5 | 1.368 (6) | C3—H3 | 0.9300 |
O1—C9 | 1.374 (6) | C4—C5 | 1.386 (7) |
O2—C9 | 1.206 (7) | C4—H4 | 0.9300 |
O3—C7 | 1.315 (6) | C5—C6 | 1.379 (7) |
O3—H5 | 0.94 (7) | C6—C7 | 1.438 (7) |
O4—C10 | 1.233 (7) | C7—C8 | 1.375 (8) |
C1—C2 | 1.370 (7) | C8—C10 | 1.453 (7) |
C1—C6 | 1.413 (8) | C8—C9 | 1.454 (8) |
C1—H1 | 0.9300 | C10—C11 | 1.523 (9) |
C2—C3 | 1.391 (8) | C11—H11 | 0.9800 |
C5—O1—C9 | 121.8 (5) | C1—C6—C7 | 123.8 (5) |
C7—O3—H5 | 103 (4) | O3—C7—C8 | 123.5 (5) |
C2—C1—C6 | 119.7 (6) | O3—C7—C6 | 115.4 (6) |
C2—C1—H1 | 120.2 | C8—C7—C6 | 121.1 (5) |
C6—C1—H1 | 120.2 | C7—C8—C10 | 118.4 (5) |
C1—C2—C3 | 119.6 (6) | C7—C8—C9 | 119.1 (5) |
C1—C2—H2 | 120.2 | C10—C8—C9 | 122.5 (6) |
C3—C2—H2 | 120.2 | O2—C9—O1 | 114.7 (5) |
C4—C3—C2 | 122.2 (6) | O2—C9—C8 | 127.1 (6) |
C4—C3—H3 | 118.9 | O1—C9—C8 | 118.2 (6) |
C2—C3—H3 | 118.9 | O4—C10—C8 | 120.7 (6) |
C3—C4—C5 | 117.7 (6) | O4—C10—C11 | 118.7 (5) |
C3—C4—H4 | 121.1 | C8—C10—C11 | 120.6 (6) |
C5—C4—H4 | 121.1 | C10—C11—Br2 | 111.6 (4) |
O1—C5—C6 | 122.1 (5) | C10—C11—Br1 | 104.7 (4) |
O1—C5—C4 | 115.7 (5) | Br2—C11—Br1 | 112.2 (3) |
C6—C5—C4 | 122.2 (6) | C10—C11—H11 | 109.4 |
C5—C6—C1 | 118.7 (5) | Br2—C11—H11 | 109.4 |
C5—C6—C7 | 117.5 (6) | Br1—C11—H11 | 109.4 |
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H5···O4 | 0.94 (7) | 1.65 (7) | 2.489 (6) | 147 (6) |
C11—H11···O2 | 0.98 | 2.12 | 2.793 (7) | 125 |
C11—H11···O2i | 0.98 | 2.51 | 3.362 (8) | 146 |
C2—H2···O2ii | 0.93 | 2.62 | 3.458 (8) | 151 |
Symmetry codes: (i) −x+1, −y+1, −z; (ii) x−1, y, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H5···O4 | 0.94 (7) | 1.65 (7) | 2.489 (6) | 147 (6) |
C11—H11···O2 | 0.98 | 2.12 | 2.793 (7) | 125 |
C11—H11···O2i | 0.98 | 2.51 | 3.362 (8) | 146 |
C2—H2···O2ii | 0.93 | 2.62 | 3.458 (8) | 151 |
Symmetry codes: (i) −x+1, −y+1, −z; (ii) x−1, y, z. |
Cg1 and Cg2 are centroids of the C1–C6 and O1/C5–C9 rings, respectively. |
Cg1···Cg2i | 3.498 (7) |
Cg1···Cg2ii | 3.539 (7) |
Symmetry codes: (i) -x, -y + 2, -z; (ii) -x, -y + 1, -z. |
Experimental details
Crystal data | |
Chemical formula | C11H6Br2O4 |
Mr | 361.98 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 296 |
a, b, c (Å) | 9.399 (4), 6.916 (3), 17.967 (7) |
β (°) | 97.37 (3) |
V (Å3) | 1158.4 (8) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 7.00 |
Crystal size (mm) | 0.15 × 0.12 × 0.10 |
Data collection | |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | For a sphere (WinGX; Farrugia, 2012) |
Tmin, Tmax | 0.58, 0.75 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 11685, 3234, 1094 |
Rint | 0.089 |
(sin θ/λ)max (Å−1) | 0.712 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.057, 0.133, 0.96 |
No. of reflections | 3234 |
No. of parameters | 158 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.43, −0.48 |
Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2001), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 2012), WinGX (Farrugia, 2012).