Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807040020/wn2191sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807040020/wn2191Isup2.hkl |
CCDC reference: 660299
Key indicators
- Single-crystal X-ray study
- T = 100 K
- Mean (C-C) = 0.002 Å
- R factor = 0.042
- wR factor = 0.140
- Data-to-parameter ratio = 58.4
checkCIF/PLATON results
No syntax errors found
Alert level B PLAT431_ALERT_2_B Short Inter HL..A Contact Br1 .. Br1 .. 3.38 Ang.
Alert level C PLAT061_ALERT_3_C Tmax/Tmin Range Test RR' too Large ............. 0.82 PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.59
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 0.590 Tmax scaled 0.145 Tmin scaled 0.063
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 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 2 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
To prepare the title compound, a mixture of 9,9-diethylfluorene (1.11 g, 5 mmol), paraformaldehyde (0.33 g, 11.0 mmol) and 33% HBr solution in acetic acid (10 ml) was heated at 333–343 K for 20 h. The precipitate obtained after cooling the reaction mixture was collected by filtration and washed with water and dried in vacuo. The crude product was recrystallized from hexane.
H atoms were positioned geometrically and allowed to ride on their parent atoms, with C—H = 0.95–0.99 Å and Uiso(H) = xUeq(carrier atom), where x = 1.5 for methyl C and 1.2 for all other C atoms. The highest residual electron density peak is located 0.70 Å from atom Br1 and the deepest hole is located 0.17 Å from atom Br1.
Fluorene and its polymeric derivatives have been used as laser-generating (Bazyl, 1986) or photo-active fluorescent materials (Johansson et al., 2001). Homopolymers and copolymers of fluorene derivatives have emerged as the most attractive blue-emitting materials due to their high effiency and excellent thermal stability (Lee & Tsuysui, 2000). Fluorene derivatives can also be used as potential anti-HIV and anticancer drugs (Abdel-Rahman et al., 1994). In view of this wide range of activities associated with fluorene derivatives, the X-ray crystal structure determination of 2,7-bis(bromomethyl)-9,9-diethylfluorene was undertaken.
The asymmetric unit of the title compound contains one half-molecule (Fig.1). The other half is generated by a crystallographic twofold axis of symmetry; this axis passes through the atom C8 and the mid-point of the C6—C6A bond [symmetry code: (A) -x, y, 1/2 - z] and is parallel to the b axis of the unit cell.
The C—C distances in the benzene ring lie in the range 1.388 (2)–1.403 (2) Å. The C6—C6A distance of 1.459 (3) Å is longer than the normal Csp2—Csp2 bond distance, but comparable to that observed in similar structures (McFarlane et al., 2005, 2006; Leclerc et al., 1998; Hu et al., 2005, 2006). The angles subtended at C8 lie in the range 100.9 (2)–112.46 (8)°, deviating significantly from the ideal tetrahedral angle of ca 109.5°.
The three fused rings are essentially coplanar, the dihedral angles formed by the five-membered ring with the two benzene rings being 0.46 (7)°. The non-hydrogen atoms of the two symmetry-related ethyl groups are coplanar, and this plane is perpendicular to the plane of the fused-ring system [dihedral angle 89.8 (1)°].
In the crystal structure the molecules are linked by C4—H4···Br1i [symmetry code: (i) 1/2 - x, 1/2 + y, z] hydrogen bonds into zigzag layers parallel to the ab plane. Such a layer, viewed approximately along the c axis, is shown in Fig.2. The adjacent layers are cross-linked by C—H···π hydrogen bonds (Table 1) involving the C1—C6 benzene ring (centroid Cg1) and Br1···Br1(1 - x, 1 - y, 1 - z) short contacts [3.3774 (3) Å] into a three-dimensional framework (Fig.3).
For general background, see: Abdel-Rahman et al. (1994); Bazyl (1986); Johansson et al. (2001); Lee & Tsuysui (2000). For related structures, see: Hu et al. (2005, 2006); Leclerc et al. (1998); McFarlane et al. (2005, 2006). Cg1 is the centroid of the C1–C6 benzene ring.
Data collection: APEX2 (Bruker, 2005); cell refinement: APEX2 (Bruker, 2005); data reduction: SAINT (Bruker, 2005); program(s) used to solve structure: SHELXTL (Sheldrick, 1998); program(s) used to refine structure: SHELXTL (Sheldrick, 1998); molecular graphics: SHELXTL (Sheldrick, 1998); software used to prepare material for publication: SHELXTL (Sheldrick, 1998) and PLATON (Spek, 2003).
C19H20Br2 | F(000) = 816 |
Mr = 408.17 | Dx = 1.617 Mg m−3 |
Orthorhombic, Pbcn | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2n 2ab | Cell parameters from 6378 reflections |
a = 10.9244 (2) Å | θ = 2.3–35.8° |
b = 8.8066 (2) Å | µ = 4.83 mm−1 |
c = 17.4316 (4) Å | T = 100 K |
V = 1677.04 (6) Å3 | Block, yellow |
Z = 4 | 0.58 × 0.49 × 0.40 mm |
Bruker SMART APEX II CCD area-detector diffractometer | 5609 independent reflections |
Radiation source: fine-focus sealed tube | 3854 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.045 |
Detector resolution: 8.33 pixels mm-1 | θmax = 41.3°, θmin = 3.0° |
ω scans | h = −20→20 |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | k = −15→16 |
Tmin = 0.106, Tmax = 0.246 | l = −32→32 |
69232 measured reflections |
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)] = 0.042 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.140 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0752P)2 + 0.7685P] where P = (Fo2 + 2Fc2)/3 |
5609 reflections | (Δ/σ)max = 0.001 |
96 parameters | Δρmax = 1.23 e Å−3 |
0 restraints | Δρmin = −1.42 e Å−3 |
C19H20Br2 | V = 1677.04 (6) Å3 |
Mr = 408.17 | Z = 4 |
Orthorhombic, Pbcn | Mo Kα radiation |
a = 10.9244 (2) Å | µ = 4.83 mm−1 |
b = 8.8066 (2) Å | T = 100 K |
c = 17.4316 (4) Å | 0.58 × 0.49 × 0.40 mm |
Bruker SMART APEX II CCD area-detector diffractometer | 5609 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | 3854 reflections with I > 2σ(I) |
Tmin = 0.106, Tmax = 0.246 | Rint = 0.045 |
69232 measured reflections |
R[F2 > 2σ(F2)] = 0.042 | 0 restraints |
wR(F2) = 0.140 | H-atom parameters constrained |
S = 1.06 | Δρmax = 1.23 e Å−3 |
5609 reflections | Δρmin = −1.42 e Å−3 |
96 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 | 0.348167 (16) | 0.49225 (2) | 0.517755 (10) | 0.02468 (6) | |
C1 | 0.04152 (13) | 0.38455 (16) | 0.31212 (8) | 0.0172 (2) | |
C2 | 0.09122 (14) | 0.35223 (17) | 0.38370 (8) | 0.0189 (2) | |
H2 | 0.1030 | 0.2499 | 0.3993 | 0.023* | |
C3 | 0.12362 (15) | 0.47126 (18) | 0.43244 (9) | 0.0196 (2) | |
C4 | 0.10699 (15) | 0.62203 (18) | 0.40870 (9) | 0.0220 (3) | |
H4 | 0.1294 | 0.7025 | 0.4422 | 0.026* | |
C5 | 0.05831 (15) | 0.65573 (17) | 0.33714 (9) | 0.0218 (3) | |
H5 | 0.0474 | 0.7581 | 0.3214 | 0.026* | |
C6 | 0.02571 (13) | 0.53575 (17) | 0.28861 (9) | 0.0180 (2) | |
C7 | 0.17355 (15) | 0.4393 (2) | 0.51043 (9) | 0.0224 (3) | |
H7A | 0.1629 | 0.3302 | 0.5223 | 0.027* | |
H7B | 0.1269 | 0.4983 | 0.5489 | 0.027* | |
C8 | 0.0000 | 0.2745 (2) | 0.2500 | 0.0177 (3) | |
C9 | 0.10677 (16) | 0.17259 (18) | 0.22344 (9) | 0.0219 (3) | |
H9A | 0.1343 | 0.1105 | 0.2675 | 0.026* | |
H9B | 0.0759 | 0.1021 | 0.1837 | 0.026* | |
C10 | 0.21637 (17) | 0.2570 (2) | 0.19130 (10) | 0.0278 (3) | |
H10A | 0.2821 | 0.1845 | 0.1800 | 0.042* | |
H10B | 0.2453 | 0.3312 | 0.2290 | 0.042* | |
H10C | 0.1926 | 0.3096 | 0.1441 | 0.042* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.02126 (9) | 0.02858 (10) | 0.02421 (9) | 0.00002 (5) | −0.00302 (5) | −0.00119 (5) |
C1 | 0.0166 (5) | 0.0190 (5) | 0.0158 (5) | 0.0002 (4) | −0.0003 (4) | 0.0001 (4) |
C2 | 0.0199 (6) | 0.0211 (6) | 0.0159 (5) | 0.0000 (4) | −0.0009 (4) | 0.0002 (4) |
C3 | 0.0177 (5) | 0.0247 (6) | 0.0165 (5) | −0.0014 (5) | −0.0005 (4) | −0.0021 (4) |
C4 | 0.0223 (6) | 0.0223 (6) | 0.0214 (6) | −0.0019 (5) | −0.0023 (5) | −0.0039 (5) |
C5 | 0.0231 (6) | 0.0189 (5) | 0.0234 (6) | −0.0014 (5) | −0.0028 (5) | −0.0015 (5) |
C6 | 0.0175 (5) | 0.0184 (5) | 0.0180 (5) | 0.0000 (4) | −0.0011 (4) | −0.0010 (4) |
C7 | 0.0205 (6) | 0.0288 (7) | 0.0179 (6) | −0.0027 (5) | −0.0012 (5) | −0.0016 (5) |
C8 | 0.0204 (8) | 0.0184 (7) | 0.0144 (7) | 0.000 | 0.0005 (6) | 0.000 |
C9 | 0.0266 (7) | 0.0224 (6) | 0.0167 (6) | 0.0056 (5) | 0.0014 (5) | 0.0006 (4) |
C10 | 0.0223 (6) | 0.0363 (9) | 0.0247 (7) | 0.0069 (6) | 0.0028 (6) | 0.0037 (6) |
Br1—C7 | 1.9679 (17) | C6—C6i | 1.459 (3) |
C1—C2 | 1.390 (2) | C7—H7A | 0.99 |
C1—C6 | 1.404 (2) | C7—H7B | 0.99 |
C1—C8 | 1.5226 (19) | C8—C1i | 1.5226 (19) |
C2—C3 | 1.395 (2) | C8—C9i | 1.5426 (19) |
C2—H2 | 0.95 | C8—C9 | 1.5426 (19) |
C3—C4 | 1.403 (2) | C9—C10 | 1.516 (3) |
C3—C7 | 1.492 (2) | C9—H9A | 0.99 |
C4—C5 | 1.388 (2) | C9—H9B | 0.99 |
C4—H4 | 0.95 | C10—H10A | 0.98 |
C5—C6 | 1.400 (2) | C10—H10B | 0.98 |
C5—H5 | 0.95 | C10—H10C | 0.98 |
C2—C1—C6 | 120.28 (13) | C3—C7—H7B | 109.3 |
C2—C1—C8 | 128.63 (13) | Br1—C7—H7B | 109.3 |
C6—C1—C8 | 111.08 (12) | H7A—C7—H7B | 108.0 |
C1—C2—C3 | 119.47 (14) | C1—C8—C1i | 100.90 (16) |
C1—C2—H2 | 120.3 | C1—C8—C9i | 112.46 (8) |
C3—C2—H2 | 120.3 | C1i—C8—C9i | 111.01 (8) |
C2—C3—C4 | 119.92 (14) | C1—C8—C9 | 111.01 (8) |
C2—C3—C7 | 120.41 (15) | C1i—C8—C9 | 112.46 (8) |
C4—C3—C7 | 119.66 (14) | C9i—C8—C9 | 108.88 (17) |
C5—C4—C3 | 121.14 (14) | C10—C9—C8 | 115.02 (14) |
C5—C4—H4 | 119.4 | C10—C9—H9A | 108.5 |
C3—C4—H4 | 119.4 | C8—C9—H9A | 108.5 |
C4—C5—C6 | 118.63 (14) | C10—C9—H9B | 108.5 |
C4—C5—H5 | 120.7 | C8—C9—H9B | 108.5 |
C6—C5—H5 | 120.7 | H9A—C9—H9B | 107.5 |
C5—C6—C1 | 120.55 (14) | C9—C10—H10A | 109.5 |
C5—C6—C6i | 130.98 (9) | C9—C10—H10B | 109.5 |
C1—C6—C6i | 108.47 (8) | H10A—C10—H10B | 109.5 |
C3—C7—Br1 | 111.64 (11) | C9—C10—H10C | 109.5 |
C3—C7—H7A | 109.3 | H10A—C10—H10C | 109.5 |
Br1—C7—H7A | 109.3 | H10B—C10—H10C | 109.5 |
C6—C1—C2—C3 | 0.9 (2) | C8—C1—C6—C6i | −0.10 (19) |
C8—C1—C2—C3 | 179.90 (12) | C2—C3—C7—Br1 | 110.20 (15) |
C1—C2—C3—C4 | −0.6 (2) | C4—C3—C7—Br1 | −71.06 (18) |
C1—C2—C3—C7 | 178.13 (14) | C2—C1—C8—C1i | −179.00 (18) |
C2—C3—C4—C5 | 0.1 (2) | C6—C1—C8—C1i | 0.04 (7) |
C7—C3—C4—C5 | −178.62 (15) | C2—C1—C8—C9i | 62.65 (18) |
C3—C4—C5—C6 | 0.0 (2) | C6—C1—C8—C9i | −118.31 (14) |
C4—C5—C6—C1 | 0.3 (2) | C2—C1—C8—C9 | −59.61 (18) |
C4—C5—C6—C6i | −179.5 (2) | C6—C1—C8—C9 | 119.43 (14) |
C2—C1—C6—C5 | −0.8 (2) | C1—C8—C9—C10 | −58.97 (16) |
C8—C1—C6—C5 | −179.91 (12) | C1i—C8—C9—C10 | 53.24 (17) |
C2—C1—C6—C6i | 179.03 (15) | C9i—C8—C9—C10 | 176.71 (16) |
Symmetry code: (i) −x, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
C4—H4···Br1ii | 0.95 | 2.88 | 3.8058 (16) | 164 |
C7—H7B···Cg1iii | 0.99 | 2.71 | 3.5589 (17) | 144 |
Symmetry codes: (ii) −x+1/2, y+1/2, z; (iii) −x, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C19H20Br2 |
Mr | 408.17 |
Crystal system, space group | Orthorhombic, Pbcn |
Temperature (K) | 100 |
a, b, c (Å) | 10.9244 (2), 8.8066 (2), 17.4316 (4) |
V (Å3) | 1677.04 (6) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 4.83 |
Crystal size (mm) | 0.58 × 0.49 × 0.40 |
Data collection | |
Diffractometer | Bruker SMART APEX II CCD area-detector |
Absorption correction | Multi-scan (SADABS; Bruker, 2005) |
Tmin, Tmax | 0.106, 0.246 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 69232, 5609, 3854 |
Rint | 0.045 |
(sin θ/λ)max (Å−1) | 0.928 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.042, 0.140, 1.06 |
No. of reflections | 5609 |
No. of parameters | 96 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.23, −1.42 |
Computer programs: APEX2 (Bruker, 2005), SAINT (Bruker, 2005), SHELXTL (Sheldrick, 1998) and PLATON (Spek, 2003).
D—H···A | D—H | H···A | D···A | D—H···A |
C4—H4···Br1i | 0.95 | 2.88 | 3.8058 (16) | 164 |
C7—H7B···Cg1ii | 0.99 | 2.71 | 3.5589 (17) | 144 |
Symmetry codes: (i) −x+1/2, y+1/2, z; (ii) −x, −y+1, −z+1. |
Fluorene and its polymeric derivatives have been used as laser-generating (Bazyl, 1986) or photo-active fluorescent materials (Johansson et al., 2001). Homopolymers and copolymers of fluorene derivatives have emerged as the most attractive blue-emitting materials due to their high effiency and excellent thermal stability (Lee & Tsuysui, 2000). Fluorene derivatives can also be used as potential anti-HIV and anticancer drugs (Abdel-Rahman et al., 1994). In view of this wide range of activities associated with fluorene derivatives, the X-ray crystal structure determination of 2,7-bis(bromomethyl)-9,9-diethylfluorene was undertaken.
The asymmetric unit of the title compound contains one half-molecule (Fig.1). The other half is generated by a crystallographic twofold axis of symmetry; this axis passes through the atom C8 and the mid-point of the C6—C6A bond [symmetry code: (A) -x, y, 1/2 - z] and is parallel to the b axis of the unit cell.
The C—C distances in the benzene ring lie in the range 1.388 (2)–1.403 (2) Å. The C6—C6A distance of 1.459 (3) Å is longer than the normal Csp2—Csp2 bond distance, but comparable to that observed in similar structures (McFarlane et al., 2005, 2006; Leclerc et al., 1998; Hu et al., 2005, 2006). The angles subtended at C8 lie in the range 100.9 (2)–112.46 (8)°, deviating significantly from the ideal tetrahedral angle of ca 109.5°.
The three fused rings are essentially coplanar, the dihedral angles formed by the five-membered ring with the two benzene rings being 0.46 (7)°. The non-hydrogen atoms of the two symmetry-related ethyl groups are coplanar, and this plane is perpendicular to the plane of the fused-ring system [dihedral angle 89.8 (1)°].
In the crystal structure the molecules are linked by C4—H4···Br1i [symmetry code: (i) 1/2 - x, 1/2 + y, z] hydrogen bonds into zigzag layers parallel to the ab plane. Such a layer, viewed approximately along the c axis, is shown in Fig.2. The adjacent layers are cross-linked by C—H···π hydrogen bonds (Table 1) involving the C1—C6 benzene ring (centroid Cg1) and Br1···Br1(1 - x, 1 - y, 1 - z) short contacts [3.3774 (3) Å] into a three-dimensional framework (Fig.3).