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2H-Benzopyrans (chromenes) and their analogues are the subject of considerable current inter­est due to their highly desirable photochromic properties. In the title compound, C23H19BrO, the pyran ring displays a half-chair conformation. Crystal stability is governed only by van der Waals inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807030796/dn3054sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807030796/dn3054Isup2.hkl
Contains datablock I

CCDC reference: 655060

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.046
  • wR factor = 0.115
  • Data-to-parameter ratio = 20.3

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.98 PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 1.08 PLAT128_ALERT_4_C Non-standard setting of Space group P21/c .... P21/a
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 1.076 Tmax scaled 0.570 Tmin scaled 0.516 PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 3 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

This type of compounds (Gemert et al., 1999; Vol. 1, Chapter 3.) has many useful applications in the marketplace (Pozzo et al., 1996; Pozzo et al., 1997; Crano et al., 1996), for example they are used to construct ophthalmic glasses (Crano et al., 1996). Functionalization of chromenes with halogen units greatly enlarges their field of applications. Bromine-substituted 2H-benzopyrans are very convenient starting material for the synthesis of a wide range of modified chromenes (Shilova, Perevalov et al., 2007). The structure of this class of compounds has been well documented by UV and NMR spectroscopy (Kodaman et al., 2000; Bougdid et al., 2007). However no X-ray crystallographic analysis for halogen-substituted 2H-benzopyrans were presented to date. The aim of the current study is to identify more exactly the structure of these key chromenes.

As observed in compound (I) (Shilova, Bougdid et al., 2007) the pyran ring displays half-chair conformation with puckering amplitude (Q) = 0.446 (2) Å, θ = 112.1 (4)°, φ = 214.7 (4)° (Cremer & Pople, 1975) (Fig. 1). Except for the C7 atom which is out of the mean plane defined by the benzopyran ring, by 0.492 Å, this fragment is roughly planar. The crystal stability is only assumed by van der Waals interactions.

Figure 2, where the pyran rings have been superimposed, shows light geometry differences at the benzene rings level. They correspond to rotations around the bonds linking these rings to the pyran one, as it appears in the values of the torsion angles O14—C7—C8—C9; O14—C7—C6—C5, respectively 142.9 (2); 161.2 (2) for compound (I) and 134.5 (2); 171.6 (2) for compound (II). These rotations around σ bonds are not significative in terms of strain energy.

Related literature top

For related literature, see: Bougdid et al. (2007); Crano et al. (1996); Cremer & Pople (1975); Gemert (1999); Kodaman et al. (2000); Pozzo et al. (1996, 1997); Shilova, Bougdid et al. (2007); Shilova, Perevalov et al. (2007).

Experimental top

6-Bromo-5,8-dimethyl-2,2-diphenyl-2H-1-benzopyran. 3,3-diphenylprop-1-yn-3-ol (11 mmol), 4-bromo-2,5-dimethylphenol (Bougdid et al., 2007) (10 mmol), a catalytic amount of p-toluene sulfonic acid (PTSA) and dry dichloromethane (20 ml) purged with argon and stirred at room temperature for 6–10 h. The progress of the reaction was monitored by TLC (pentane/Et2O, 1:1). After complete disappearance of the bromophenol, the reaction mixture was washed with brine (3x20 ml). The organic layer was dried with MgSO4, filtered and concentrated to dryness under reduced pressure. Purification by column chromatography (SiO2; cyclohexane/dichloromethane gradient 100:0 to 50:50) afforded pure compound as a white solid (yield 85%). Light yellow crystals appropriate for data collection were obtained by slow evaporation from acetonitrile solution at 277 K. M.p. 153–154 oC. FT—IR (KBr): ν = 3060, 3024, 2952, 2921, 2853, 1625, 1593, 1493, 1450, 1380, 1364, 1236, 1230, 1203, 1168, 1095, 1062, 1031, 970, 907, 864, 770, 754, 700, 573 cm-1 . 1H NMR (250 MHz, CDCl3): δ = 2.25 (s, 3 H), 2.35 (s, 3 H), 6.21 (d, J = 10.0 Hz, 1 H), 6.84 (d, J = 10.0 Hz, 1 H), 7.18 (br s, 1 H), 7.21–7.46 (m, 10 H). 13C NMR (62.5 MHz, CDCl3): δ = 15.5 (CH3), 18.1 (CH3), 81.6 (OC), 116.2 (C), 120.9 (C), 121.4 (CH=), 125.2 (C), 126.7 (4 x CH=), 127.5 (2 x CH=), 128.1 (4 x CH=), 129.3 (CH=), 130.8 (C), 133.7 (CH=), 144.9 (2 x C), 149.8 (C). Anal. Calcd. for C23H19BrO: C, 70.59; H, 4.89; Br, 20.42. Found: C, 70.56; H, 4.79; Br, 20.48.

Refinement top

All H atoms were fixed geometrically and treated as riding with C—H = 0.93 Å (aromatic) or 0.96 Å (methyl) with Uiso(H) = xUeq(C) where x = 1.2 for H aromatic and 1.5 for H methyl.

Structure description top

This type of compounds (Gemert et al., 1999; Vol. 1, Chapter 3.) has many useful applications in the marketplace (Pozzo et al., 1996; Pozzo et al., 1997; Crano et al., 1996), for example they are used to construct ophthalmic glasses (Crano et al., 1996). Functionalization of chromenes with halogen units greatly enlarges their field of applications. Bromine-substituted 2H-benzopyrans are very convenient starting material for the synthesis of a wide range of modified chromenes (Shilova, Perevalov et al., 2007). The structure of this class of compounds has been well documented by UV and NMR spectroscopy (Kodaman et al., 2000; Bougdid et al., 2007). However no X-ray crystallographic analysis for halogen-substituted 2H-benzopyrans were presented to date. The aim of the current study is to identify more exactly the structure of these key chromenes.

As observed in compound (I) (Shilova, Bougdid et al., 2007) the pyran ring displays half-chair conformation with puckering amplitude (Q) = 0.446 (2) Å, θ = 112.1 (4)°, φ = 214.7 (4)° (Cremer & Pople, 1975) (Fig. 1). Except for the C7 atom which is out of the mean plane defined by the benzopyran ring, by 0.492 Å, this fragment is roughly planar. The crystal stability is only assumed by van der Waals interactions.

Figure 2, where the pyran rings have been superimposed, shows light geometry differences at the benzene rings level. They correspond to rotations around the bonds linking these rings to the pyran one, as it appears in the values of the torsion angles O14—C7—C8—C9; O14—C7—C6—C5, respectively 142.9 (2); 161.2 (2) for compound (I) and 134.5 (2); 171.6 (2) for compound (II). These rotations around σ bonds are not significative in terms of strain energy.

For related literature, see: Bougdid et al. (2007); Crano et al. (1996); Cremer & Pople (1975); Gemert (1999); Kodaman et al. (2000); Pozzo et al. (1996, 1997); Shilova, Bougdid et al. (2007); Shilova, Perevalov et al. (2007).

Computing details top

Data collection: KappaCCD Reference Manual (Nonius, 1998); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK; program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEPIII (Burnett & Johnson, 1996) and ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. Molecular view of compound (I) with the atom-labelling scheme. Ellipsoids are drawn at the 50% propability level. H atoms are represented as small sphers of arbitrary radii.
[Figure 2] Fig. 2. Compounds (I) and compound (II) with the pyran rings superimposed.
6-Bromo-5,8-dimethyl-2,2-diphenyl-2H-1-benzopyran top
Crystal data top
C23H19BrODx = 1.417 Mg m3
Mr = 391.29Melting point: 427(1) K
Monoclinic, P21/aMo Kα radiation, λ = 0.71073 Å
a = 8.8953 (2) ÅCell parameters from 17209 reflections
b = 22.4365 (5) Åθ = 0.9–28.7°
c = 9.2114 (1) ŵ = 2.25 mm1
β = 93.921 (2)°T = 293 K
V = 1834.10 (6) Å3Cube, light yellow
Z = 40.30 × 0.25 × 0.25 mm
F(000) = 800
Data collection top
Nonius KappaCCD area-detector
diffractometer
4630 independent reflections
Radiation source: fine-focus sealed tube3552 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
φ scansθmax = 28.7°, θmin = 3.2°
Absorption correction: multi-scan
(Blessing & Langs, 1987)
h = 119
Tmin = 0.48, Tmax = 0.53k = 3027
17209 measured reflectionsl = 1012
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)] = 0.046Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.115H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0381P)2 + 1.5124P]
where P = (Fo2 + 2Fc2)/3
4630 reflections(Δ/σ)max = 0.014
228 parametersΔρmax = 0.75 e Å3
0 restraintsΔρmin = 0.89 e Å3
Crystal data top
C23H19BrOV = 1834.10 (6) Å3
Mr = 391.29Z = 4
Monoclinic, P21/aMo Kα radiation
a = 8.8953 (2) ŵ = 2.25 mm1
b = 22.4365 (5) ÅT = 293 K
c = 9.2114 (1) Å0.30 × 0.25 × 0.25 mm
β = 93.921 (2)°
Data collection top
Nonius KappaCCD area-detector
diffractometer
4630 independent reflections
Absorption correction: multi-scan
(Blessing & Langs, 1987)
3552 reflections with I > 2σ(I)
Tmin = 0.48, Tmax = 0.53Rint = 0.038
17209 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0460 restraints
wR(F2) = 0.115H-atom parameters constrained
S = 1.03Δρmax = 0.75 e Å3
4630 reflectionsΔρmin = 0.89 e Å3
228 parameters
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
C10.1988 (3)0.46171 (12)0.1181 (3)0.0500 (6)
H10.19560.45880.01720.060*
C20.1233 (3)0.50778 (13)0.1826 (4)0.0607 (7)
H20.07060.53570.12440.073*
C30.1255 (3)0.51266 (14)0.3307 (4)0.0655 (8)
H30.07490.54370.37310.079*
C40.2032 (4)0.47115 (16)0.4163 (4)0.0692 (8)
H40.20480.47410.51710.083*
C50.2789 (3)0.42512 (14)0.3535 (3)0.0578 (7)
H50.33060.39720.41240.069*
C60.2786 (3)0.42021 (11)0.2033 (3)0.0421 (5)
C70.3662 (3)0.36977 (10)0.1367 (2)0.0384 (5)
C80.5311 (3)0.37212 (10)0.1974 (2)0.0385 (5)
C90.5947 (3)0.32934 (11)0.2914 (3)0.0456 (5)
H90.53740.29690.31770.055*
C100.7431 (3)0.33457 (14)0.3465 (3)0.0551 (7)
H100.78450.30590.41030.066*
C110.8296 (3)0.38209 (15)0.3073 (3)0.0605 (7)
H110.92920.38550.34400.073*
C120.7673 (3)0.42461 (15)0.2131 (3)0.0636 (8)
H120.82560.45650.18550.076*
C130.6186 (3)0.42003 (12)0.1595 (3)0.0530 (6)
H130.57710.44930.09750.064*
O140.36250 (18)0.38213 (7)0.01785 (16)0.0401 (4)
C150.4191 (2)0.33737 (10)0.1008 (2)0.0383 (5)
C160.3976 (3)0.27765 (11)0.0641 (3)0.0416 (5)
C170.3108 (3)0.26690 (11)0.0623 (3)0.0469 (6)
H170.26820.22960.07590.056*
C180.2926 (3)0.30986 (11)0.1574 (3)0.0460 (5)
H180.23490.30340.23650.055*
C190.4881 (3)0.35455 (11)0.2249 (3)0.0439 (5)
C200.5425 (3)0.30952 (12)0.3095 (3)0.0503 (6)
H200.59110.31920.39260.060*
C210.5256 (3)0.25056 (12)0.2724 (3)0.0499 (6)
C220.4524 (3)0.23218 (11)0.1512 (3)0.0472 (6)
C230.5019 (4)0.41928 (13)0.2651 (3)0.0616 (7)
H23A0.54820.42250.35600.092*
H23B0.56270.43960.19060.092*
H23C0.40350.43700.27450.092*
Br240.60679 (4)0.192806 (16)0.39843 (4)0.07243 (14)
C250.4343 (4)0.16768 (13)0.1121 (4)0.0683 (8)
H25A0.36490.14900.18240.102*
H25B0.39630.16480.01730.102*
H25C0.53030.14810.11160.102*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0454 (14)0.0468 (14)0.0574 (15)0.0011 (11)0.0006 (11)0.0021 (11)
C20.0478 (15)0.0481 (15)0.086 (2)0.0045 (12)0.0019 (14)0.0048 (14)
C30.0476 (16)0.0611 (18)0.089 (2)0.0034 (13)0.0184 (15)0.0213 (16)
C40.0638 (19)0.085 (2)0.0607 (18)0.0075 (17)0.0183 (14)0.0171 (16)
C50.0547 (16)0.0704 (18)0.0491 (15)0.0091 (14)0.0096 (12)0.0023 (13)
C60.0344 (11)0.0439 (12)0.0484 (13)0.0035 (10)0.0049 (9)0.0023 (10)
C70.0397 (11)0.0400 (12)0.0357 (11)0.0021 (9)0.0033 (8)0.0023 (8)
C80.0408 (12)0.0410 (12)0.0340 (11)0.0014 (9)0.0049 (8)0.0027 (8)
C90.0468 (13)0.0483 (13)0.0419 (13)0.0031 (11)0.0039 (10)0.0013 (10)
C100.0487 (15)0.0694 (18)0.0464 (14)0.0136 (13)0.0024 (11)0.0011 (12)
C110.0398 (14)0.083 (2)0.0573 (16)0.0015 (14)0.0031 (11)0.0092 (14)
C120.0490 (16)0.0716 (19)0.0696 (19)0.0171 (14)0.0012 (13)0.0048 (15)
C130.0495 (15)0.0527 (15)0.0562 (15)0.0075 (12)0.0019 (11)0.0081 (12)
O140.0463 (9)0.0382 (8)0.0359 (8)0.0003 (7)0.0021 (6)0.0026 (6)
C150.0357 (11)0.0401 (12)0.0382 (11)0.0025 (9)0.0038 (8)0.0027 (9)
C160.0406 (12)0.0404 (12)0.0430 (12)0.0065 (10)0.0027 (9)0.0005 (9)
C170.0483 (14)0.0391 (13)0.0531 (14)0.0122 (11)0.0013 (10)0.0057 (10)
C180.0457 (13)0.0470 (14)0.0458 (13)0.0086 (11)0.0071 (10)0.0070 (10)
C190.0420 (12)0.0495 (13)0.0396 (12)0.0082 (10)0.0013 (9)0.0006 (10)
C200.0472 (14)0.0657 (17)0.0379 (12)0.0065 (12)0.0017 (10)0.0054 (11)
C210.0426 (13)0.0581 (15)0.0478 (14)0.0030 (11)0.0063 (10)0.0148 (11)
C220.0450 (13)0.0417 (13)0.0531 (14)0.0021 (10)0.0092 (10)0.0059 (10)
C230.079 (2)0.0568 (17)0.0496 (15)0.0152 (15)0.0081 (13)0.0084 (12)
Br240.0667 (2)0.0817 (3)0.0678 (2)0.01434 (16)0.00321 (14)0.03119 (16)
C250.081 (2)0.0399 (15)0.083 (2)0.0024 (14)0.0017 (17)0.0063 (14)
Geometric parameters (Å, º) top
C1—C61.383 (4)C12—H120.9300
C1—C21.388 (4)C13—H130.9300
C1—H10.9300O14—C151.378 (3)
C2—C31.367 (5)C15—C191.389 (3)
C2—H20.9300C15—C161.398 (3)
C3—C41.376 (5)C16—C221.406 (3)
C3—H30.9300C16—C171.460 (3)
C4—C51.381 (4)C17—C181.320 (4)
C4—H40.9300C17—H170.9300
C5—C61.388 (4)C18—H180.9300
C5—H50.9300C19—C201.383 (4)
C6—C71.526 (3)C19—C231.506 (4)
C7—O141.449 (3)C20—C211.377 (4)
C7—C181.513 (3)C20—H200.9300
C7—C81.534 (3)C21—C221.393 (4)
C8—C131.386 (3)C21—Br241.914 (3)
C8—C91.388 (3)C22—C251.503 (4)
C9—C101.387 (4)C23—H23A0.9600
C9—H90.9300C23—H23B0.9600
C10—C111.377 (4)C23—H23C0.9600
C10—H100.9300C25—H25A0.9600
C11—C121.380 (4)C25—H25B0.9600
C11—H110.9300C25—H25C0.9600
C12—C131.384 (4)
C6—C1—C2120.2 (3)C12—C13—H13119.7
C6—C1—H1119.9C8—C13—H13119.7
C2—C1—H1119.9C15—O14—C7114.90 (17)
C3—C2—C1120.8 (3)O14—C15—C19117.0 (2)
C3—C2—H2119.6O14—C15—C16120.2 (2)
C1—C2—H2119.6C19—C15—C16122.7 (2)
C2—C3—C4119.3 (3)C15—C16—C22119.9 (2)
C2—C3—H3120.3C15—C16—C17116.1 (2)
C4—C3—H3120.3C22—C16—C17123.9 (2)
C3—C4—C5120.4 (3)C18—C17—C16120.3 (2)
C3—C4—H4119.8C18—C17—H17119.9
C5—C4—H4119.8C16—C17—H17119.9
C4—C5—C6120.6 (3)C17—C18—C7119.4 (2)
C4—C5—H5119.7C17—C18—H18120.3
C6—C5—H5119.7C7—C18—H18120.3
C1—C6—C5118.6 (2)C20—C19—C15116.9 (2)
C1—C6—C7121.9 (2)C20—C19—C23121.9 (2)
C5—C6—C7119.6 (2)C15—C19—C23121.2 (2)
O14—C7—C18108.25 (18)C21—C20—C19120.9 (2)
O14—C7—C6105.95 (18)C21—C20—H20119.6
C18—C7—C6111.76 (19)C19—C20—H20119.6
O14—C7—C8107.96 (17)C20—C21—C22123.3 (2)
C18—C7—C8113.33 (19)C20—C21—Br24116.6 (2)
C6—C7—C8109.25 (18)C22—C21—Br24120.2 (2)
C13—C8—C9118.8 (2)C21—C22—C16116.3 (2)
C13—C8—C7118.3 (2)C21—C22—C25122.7 (3)
C9—C8—C7122.9 (2)C16—C22—C25121.0 (3)
C10—C9—C8120.5 (2)C19—C23—H23A109.5
C10—C9—H9119.7C19—C23—H23B109.5
C8—C9—H9119.7H23A—C23—H23B109.5
C11—C10—C9120.3 (3)C19—C23—H23C109.5
C11—C10—H10119.9H23A—C23—H23C109.5
C9—C10—H10119.9H23B—C23—H23C109.5
C10—C11—C12119.5 (3)C22—C25—H25A109.5
C10—C11—H11120.2C22—C25—H25B109.5
C12—C11—H11120.2H25A—C25—H25B109.5
C11—C12—C13120.4 (3)C22—C25—H25C109.5
C11—C12—H12119.8H25A—C25—H25C109.5
C13—C12—H12119.8H25B—C25—H25C109.5
C12—C13—C8120.5 (3)
O14—C7—C8—C9134.5 (2)O14—C7—C6—C5171.6 (2)

Experimental details

Crystal data
Chemical formulaC23H19BrO
Mr391.29
Crystal system, space groupMonoclinic, P21/a
Temperature (K)293
a, b, c (Å)8.8953 (2), 22.4365 (5), 9.2114 (1)
β (°) 93.921 (2)
V3)1834.10 (6)
Z4
Radiation typeMo Kα
µ (mm1)2.25
Crystal size (mm)0.30 × 0.25 × 0.25
Data collection
DiffractometerNonius KappaCCD area-detector
Absorption correctionMulti-scan
(Blessing & Langs, 1987)
Tmin, Tmax0.48, 0.53
No. of measured, independent and
observed [I > 2σ(I)] reflections
17209, 4630, 3552
Rint0.038
(sin θ/λ)max1)0.676
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.046, 0.115, 1.03
No. of reflections4630
No. of parameters228
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.75, 0.89

Computer programs: KappaCCD Reference Manual (Nonius, 1998), DENZO and SCALEPACK (Otwinowski & Minor, 1997), DENZO and SCALEPACK, SIR97 (Altomare et al., 1999), SHELXL97 (Sheldrick, 1997), ORTEPIII (Burnett & Johnson, 1996) and ORTEP-3 for Windows (Farrugia, 1997), PLATON (Spek, 2003).

 

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