Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536810024311/fk2020sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536810024311/fk2020Isup2.hkl |
CCDC reference: 786740
Key indicators
- Single-crystal X-ray study
- T = 100 K
- Mean (C-C) = 0.003 Å
- R factor = 0.016
- wR factor = 0.034
- Data-to-parameter ratio = 25.9
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT480_ALERT_4_C Long H...A H-Bond Reported H6A .. BR2 .. 2.96 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H6A .. BR2 .. 2.98 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H5 .. BR1 .. 3.11 Ang. PLAT912_ALERT_4_C Missing # of FCF Reflections Above STh/L= 0.600 35
Alert level G PLAT154_ALERT_1_G The su's on the Cell Angles are Equal (x 10000) 300 Deg.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 1 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 0 ALERT type 3 Indicator that the structure quality may be low 4 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
The title compound was prepared as described by Rivera et al. (2001) by treatment of a solution of 2,3-bis[{[(1,1-dimethylethyl)dimethylsilyl]oxy}methyl]- 6,7-bis[(phenylmethoxy)methyl]-naphthalene in chloroform with gaseous HBr. The compound was obtained as a colourless microcrystalline solid. Yield: 87%. Crystals suitable for X-ray diffraction were grown by slow evaporation of a solution in EtOH/hexane/CH2Cl2. M.p. (decomp.) 230–231° C (lit. 230° C). 1H NMR (CDCl3): δ = 7.83 (s, 4H), 4.84 (s, 8H) p.p.m..
The title compound is poorly soluble (< 1 g/L) in most organic solvents at room temperature, but is much more soluble in aromatic solvents, such as toluene or chlorobenzene, upon reflux.
Hydrogen atoms were included at calculated positions using a riding model with aromatic C—H 0.95, methylene C—H 0.99 Å. The U(H) values were fixed at 1.2 × Ueq(C) of the parent C atom.
Data collection: CrysAlis PRO (Oxford Diffraction, 2009); cell refinement: CrysAlis PRO (Oxford Diffraction, 2009); data reduction: CrysAlis PRO (Oxford Diffraction, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP (Siemens, 1994); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).
C14H12Br4 | Z = 1 |
Mr = 499.88 | F(000) = 236 |
Triclinic, P1 | Dx = 2.254 Mg m−3 |
Hall symbol: -P 1 | Melting point: 503 K |
a = 6.6144 (2) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 7.1770 (2) Å | Cell parameters from 9533 reflections |
c = 8.7761 (3) Å | θ = 2.4–30.7° |
α = 84.744 (3)° | µ = 10.91 mm−1 |
β = 78.251 (3)° | T = 100 K |
γ = 64.555 (3)° | Prism, colourless |
V = 368.32 (2) Å3 | 0.20 × 0.06 × 0.04 mm |
Oxford Diffraction Xcalibur Eos diffractometer | 2122 independent reflections |
Radiation source: Enhance (Mo) X-ray Source | 1716 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.031 |
Detector resolution: 16.1419 pixels mm-1 | θmax = 30.0°, θmin = 2.4° |
ω–scan | h = −9→9 |
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | k = −10→10 |
Tmin = 0.356, Tmax = 1.000 | l = −11→12 |
17701 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)] = 0.016 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.034 | H-atom parameters constrained |
S = 0.92 | w = 1/[σ2(Fo2) + (0.0181P)2] where P = (Fo2 + 2Fc2)/3 |
2122 reflections | (Δ/σ)max = 0.001 |
82 parameters | Δρmax = 0.50 e Å−3 |
0 restraints | Δρmin = −0.49 e Å−3 |
C14H12Br4 | γ = 64.555 (3)° |
Mr = 499.88 | V = 368.32 (2) Å3 |
Triclinic, P1 | Z = 1 |
a = 6.6144 (2) Å | Mo Kα radiation |
b = 7.1770 (2) Å | µ = 10.91 mm−1 |
c = 8.7761 (3) Å | T = 100 K |
α = 84.744 (3)° | 0.20 × 0.06 × 0.04 mm |
β = 78.251 (3)° |
Oxford Diffraction Xcalibur Eos diffractometer | 2122 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | 1716 reflections with I > 2σ(I) |
Tmin = 0.356, Tmax = 1.000 | Rint = 0.031 |
17701 measured reflections |
R[F2 > 2σ(F2)] = 0.016 | 0 restraints |
wR(F2) = 0.034 | H-atom parameters constrained |
S = 0.92 | Δρmax = 0.50 e Å−3 |
2122 reflections | Δρmin = −0.49 e Å−3 |
82 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 | 0.64988 (3) | −0.00387 (3) | 0.24985 (2) | 0.01628 (5) | |
Br2 | 0.23208 (3) | 0.72525 (3) | 0.44061 (2) | 0.01672 (5) | |
C1 | −0.0170 (3) | 0.4100 (3) | 0.02483 (19) | 0.0108 (3) | |
C2 | 0.0922 (3) | 0.2877 (3) | 0.14549 (19) | 0.0122 (3) | |
H2 | 0.0699 | 0.1672 | 0.1791 | 0.015* | |
C3 | 0.2297 (3) | 0.3393 (3) | 0.21518 (19) | 0.0111 (3) | |
C4 | 0.2621 (3) | 0.5223 (3) | 0.16547 (19) | 0.0110 (3) | |
C5 | 0.1575 (3) | 0.6419 (3) | 0.04994 (19) | 0.0112 (3) | |
H5 | 0.1791 | 0.7633 | 0.0185 | 0.013* | |
C6 | 0.3431 (3) | 0.2029 (3) | 0.34014 (19) | 0.0136 (3) | |
H6A | 0.2495 | 0.1316 | 0.3945 | 0.016* | |
H6B | 0.3563 | 0.2876 | 0.4173 | 0.016* | |
C7 | 0.4062 (3) | 0.5854 (3) | 0.24055 (18) | 0.0135 (3) | |
H7A | 0.4559 | 0.6799 | 0.1704 | 0.016* | |
H7B | 0.5437 | 0.4620 | 0.2592 | 0.016* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.01360 (10) | 0.01494 (10) | 0.01724 (10) | −0.00349 (8) | −0.00312 (7) | 0.00232 (7) |
Br2 | 0.01615 (10) | 0.01865 (11) | 0.01468 (9) | −0.00544 (8) | −0.00321 (7) | −0.00581 (7) |
C1 | 0.0099 (8) | 0.0112 (9) | 0.0093 (8) | −0.0031 (7) | 0.0001 (6) | −0.0012 (6) |
C2 | 0.0130 (8) | 0.0120 (9) | 0.0105 (8) | −0.0053 (7) | 0.0000 (7) | −0.0003 (6) |
C3 | 0.0085 (8) | 0.0127 (9) | 0.0087 (8) | −0.0016 (7) | −0.0006 (6) | −0.0008 (6) |
C4 | 0.0092 (8) | 0.0139 (9) | 0.0097 (8) | −0.0050 (7) | 0.0011 (6) | −0.0040 (6) |
C5 | 0.0111 (8) | 0.0104 (8) | 0.0120 (8) | −0.0055 (7) | 0.0012 (6) | −0.0020 (6) |
C6 | 0.0111 (8) | 0.0156 (9) | 0.0115 (8) | −0.0033 (7) | −0.0017 (7) | 0.0003 (7) |
C7 | 0.0128 (8) | 0.0177 (9) | 0.0101 (8) | −0.0064 (7) | −0.0017 (7) | −0.0023 (7) |
Br1—C6 | 1.9801 (16) | C4—C7 | 1.493 (2) |
Br2—C7 | 1.9806 (16) | C5—C1i | 1.422 (2) |
C1—C2 | 1.418 (2) | C2—H2 | 0.9500 |
C1—C1i | 1.420 (3) | C5—H5 | 0.9500 |
C1—C5i | 1.422 (2) | C6—H6A | 0.9900 |
C2—C3 | 1.377 (2) | C6—H6B | 0.9900 |
C3—C4 | 1.436 (2) | C7—H7A | 0.9900 |
C3—C6 | 1.494 (2) | C7—H7B | 0.9900 |
C4—C5 | 1.363 (2) | ||
C2—C1—C1i | 118.85 (18) | C1—C2—H2 | 119.2 |
C2—C1—C5i | 122.57 (15) | C4—C5—H5 | 119.0 |
C1i—C1—C5i | 118.58 (19) | C1i—C5—H5 | 119.0 |
C3—C2—C1 | 121.68 (15) | C3—C6—H6A | 109.6 |
C2—C3—C4 | 119.29 (15) | Br1—C6—H6A | 109.6 |
C2—C3—C6 | 119.30 (15) | C3—C6—H6B | 109.6 |
C4—C3—C6 | 121.41 (15) | Br1—C6—H6B | 109.6 |
C5—C4—C3 | 119.70 (15) | H6A—C6—H6B | 108.1 |
C5—C4—C7 | 119.52 (15) | C4—C7—H7A | 109.6 |
C3—C4—C7 | 120.77 (15) | Br2—C7—H7A | 109.6 |
C4—C5—C1i | 121.90 (15) | C4—C7—H7B | 109.6 |
C3—C6—Br1 | 110.35 (11) | Br2—C7—H7B | 109.6 |
C4—C7—Br2 | 110.18 (11) | H7A—C7—H7B | 108.1 |
C3—C2—H2 | 119.2 | ||
C1i—C1—C2—C3 | 0.0 (3) | C6—C3—C4—C7 | −1.7 (2) |
C5i—C1—C2—C3 | 179.24 (16) | C3—C4—C5—C1i | −0.5 (2) |
C1—C2—C3—C4 | 0.5 (2) | C7—C4—C5—C1i | −179.53 (15) |
C1—C2—C3—C6 | −179.09 (15) | C2—C3—C6—Br1 | 92.22 (16) |
C2—C3—C4—C5 | −0.2 (2) | C4—C3—C6—Br1 | −87.36 (16) |
C6—C3—C4—C5 | 179.34 (15) | C5—C4—C7—Br2 | 99.15 (16) |
C2—C3—C4—C7 | 178.76 (15) | C3—C4—C7—Br2 | −79.86 (17) |
Symmetry code: (i) −x, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C6—H6A···Br2ii | 0.99 | 2.96 | 3.7967 (17) | 143 |
C6—H6A···Br2iii | 0.99 | 2.98 | 3.7359 (16) | 134 |
C5—H5···Br1iv | 0.95 | 3.11 | 3.9399 (16) | 147 |
Symmetry codes: (ii) x, y−1, z; (iii) −x, −y+1, −z+1; (iv) −x+1, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | C14H12Br4 |
Mr | 499.88 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 100 |
a, b, c (Å) | 6.6144 (2), 7.1770 (2), 8.7761 (3) |
α, β, γ (°) | 84.744 (3), 78.251 (3), 64.555 (3) |
V (Å3) | 368.32 (2) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 10.91 |
Crystal size (mm) | 0.20 × 0.06 × 0.04 |
Data collection | |
Diffractometer | Oxford Diffraction Xcalibur Eos diffractometer |
Absorption correction | Multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) |
Tmin, Tmax | 0.356, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 17701, 2122, 1716 |
Rint | 0.031 |
(sin θ/λ)max (Å−1) | 0.704 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.016, 0.034, 0.92 |
No. of reflections | 2122 |
No. of parameters | 82 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.50, −0.49 |
Computer programs: CrysAlis PRO (Oxford Diffraction, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), XP (Siemens, 1994).
D—H···A | D—H | H···A | D···A | D—H···A |
C6—H6A···Br2i | 0.99 | 2.96 | 3.7967 (17) | 143.4 |
C6—H6A···Br2ii | 0.99 | 2.98 | 3.7359 (16) | 134.0 |
C5—H5···Br1iii | 0.95 | 3.11 | 3.9399 (16) | 147.2 |
Symmetry codes: (i) x, y−1, z; (ii) −x, −y+1, −z+1; (iii) −x+1, −y+1, −z. |
Cg is the centroid of the C1–C5,C1(-x, 1-y, -z) ring. |
System C—Br···Br—C or C—Br···Cg | Br···Br or Br···Cg | C—Br···Br (or C—Br···Cg), Br···Br—C | Operator |
C6—Br1···Br2—C7 | 3.8972 (3) | 76.45 (5), 134.79 (5) | 1-x, 1-y, 1-z |
C7—Br2···Br2—C7 | 3.8873 (4) | 134.93 (5) × 2 | -x, 2-y, 1-z |
C7—Br2···Br2—C7 | 3.8913 (4) | 76.72 (5) × 2 | 1-x, 1-y, 1-z |
C6—Br1···Cg | 3.89 | 158 | 1+x, -1+y, z |
The title compound is a symmetric rigid molecule with four bromomethyl groups. The bromine atoms can be easily substituted by other nucleophiles, which offers the opportunity of employing the compound as a building block for construction of various functional architectures. The title compound was prepared to serve as a spacer between two tetrathiafulvalene (TTF) groups in TTF-containing molecular tweezers (Skibiński et al., 2009). It was first employed as an intermediate in the preparation of triple-layered [2.2]naphthalenophane (Otsubo et al., 1983), and several other triple-layered cyclophanes (Otsubo et al., 1983; Yano et al., 1999). It was also used as an intermediate in the synthesis of H-bonded molecular capsules (Valdes et al., 1995; Rivera et al., 2001).
The molecule of the title compound is shown in Fig. 1. It displays crystallographic inversion symmetry (operator #1 - x, 1 - y, 1 - z); for this reason, the crystallographic numbering does not correspond to the IUPAC numbering scheme. Bond lengths and angles may be considered normal; the bromine atoms are directed to opposite sides of the ring system, with C(2)—C(3)—C(6)—Br(1) 92.22 (16), C(3)—C(4)—C(7)—Br2 - 79.86 (17)°, which leads to a +/-/-/+ pattern of Br atoms about the ring plane for the IUPAC-numbered C2,3,6,7; this contrasts with the -/-/+/+ pattern in 1,2,4,5-tetrakis(bromomethyl)benzene (Jones & Kuś, 2007), which is also inversion-symmetric.
Details of the packing interactions are given in the Tables. The molecules pack in layers parallel to (101). Within the layers, the contacts Br1···Br2, the longer Br2···Br2 and the shorter H6A···Br2 are observed. These combine to form columns of interactions parallel to the b axis; chains of molecules parallel to [101] (horizontal in Fig. 2) are also formed. The contacts Br2···Br2 (the shorter), H6A···Br2 (the longer) and Br1···Cg (Cg = centre of gravity of the ring C1–5 and C1#1) link the layers (Fig. 3). H5···Br1 3.11 Å between the layers is a borderline interaction. The Br···Cg interaction could alternatively be interpreted as Br···C5, which at 3.450 (2) Å is by far the shortest of the six Br···C contacts; it is often unclear which is the better interpretation in such systems (Jones & Kuś, 2010). Despite the presence of the naphthalene ring systems, there are no significant Cg···Cg interactions. The shortest H···Cg contact is H7A···Cg (1 - x,1 - y,-z) 3.10 Å between layers, but this is both long and has a narrow angle (124°). We can conclude that the crystal packing of the title compound is dominated by the contacts involving bromomethylene groups.