Literature DB >> 22412645

4,4,5,5-Tetra-methyl-2-[1,3,6,8-tetra-bromo-7-(4,4,5,5-tetra-methyl-1,3,2-dioxaborolan-2-yl)pyren-2-yl]-1,3,2-dioxaborolane.

Ying Chen, Wen-Tao Yu, Zhi-Qiang Liu, Ping Yu.   

Abstract

The complete mol-ecule of the title compound, C(28)H(28)B(2)Br(4)O(4), is generated by the application of a centre of inversion. In the mol-ecule, the BO(2) plane is perpendicular to that through the pyrene ring [dihedral angle = 86.27 (13)°]. In the crystal, mol-ecules stack into columns along the b axis, the closest contact between these being of the type C-Br⋯π.

Entities:  

Year:  2012        PMID: 22412645      PMCID: PMC3297842          DOI: 10.1107/S1600536812006095

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background to the reactions of pyrene, see: Miura & Yamano (1995 ▶). For the structure of the non-brominated derivative, see: Coventry et al. (2005 ▶).

Experimental

Crystal data

C28H28B2Br4O4 M = 769.76 Monoclinic, a = 15.5047 (10) Å b = 7.5136 (5) Å c = 13.9191 (9) Å β = 113.961 (1)° V = 1481.78 (17) Å3 Z = 2 Mo Kα radiation μ = 5.46 mm−1 T = 296 K 0.34 × 0.24 × 0.16 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.258, T max = 0.475 8745 measured reflections 3344 independent reflections 2488 reflections with I > 2σ(I) R int = 0.026

Refinement

R[F 2 > 2σ(F 2)] = 0.035 wR(F 2) = 0.109 S = 1.01 3344 reflections 176 parameters H-atom parameters constrained Δρmax = 0.60 e Å−3 Δρmin = −0.67 e Å−3 Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: OLEX-2 (Dolomanov et al., 2009 ▶) and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812006095/tk5049sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812006095/tk5049Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536812006095/tk5049Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C28H28B2Br4O4F(000) = 756
Mr = 769.76Dx = 1.725 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3344 reflections
a = 15.5047 (10) Åθ = 2.9–27.4°
b = 7.5136 (5) ŵ = 5.46 mm1
c = 13.9191 (9) ÅT = 296 K
β = 113.961 (1)°Pod, colourless
V = 1481.78 (17) Å30.34 × 0.24 × 0.16 mm
Z = 2
Bruker APEXII CCD diffractometer3344 independent reflections
Radiation source: fine-focus sealed tube2488 reflections with i > 2σ(I)
Graphite monochromatorRint = 0.026
φ and ω scansθmax = 27.5°, θmin = 2.9°
Absorption correction: multi-scan (SADABS; Bruker, 2009)h = −20→18
Tmin = 0.258, Tmax = 0.475k = −9→9
8745 measured reflectionsl = −9→18
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.035Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.109H-atom parameters constrained
S = 1.01w = 1/[σ2(Fo2) + (0.0653P)2 + 0.4343P] where P = (Fo2 + 2Fc2)/3
3344 reflections(Δ/σ)max = 0.007
176 parametersΔρmax = 0.60 e Å3
0 restraintsΔρmin = −0.67 e Å3
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.
xyzUiso*/Ueq
Br10.77662 (3)0.70726 (6)0.97202 (4)0.07199 (18)
Br20.58141 (3)0.07842 (5)0.79828 (3)0.06680 (17)
O10.73711 (17)0.4128 (3)0.75325 (18)0.0521 (6)
O20.81831 (17)0.2540 (4)0.89972 (18)0.0603 (7)
C10.8075 (4)0.3192 (8)0.6352 (3)0.0949 (17)
H1A0.76190.22480.61140.142*
H1B0.86520.28120.63160.142*
H1C0.78350.42180.59140.142*
C20.8258 (2)0.3653 (5)0.7461 (3)0.0537 (9)
C30.6666 (2)0.4017 (4)0.8923 (2)0.0380 (6)
C40.5917 (2)0.2876 (4)0.8788 (2)0.0395 (7)
C50.5247 (2)0.3199 (4)0.9201 (2)0.0377 (6)
C60.4480 (2)0.2033 (4)0.9060 (3)0.0503 (8)
H60.44170.09850.86810.060*
C70.3844 (2)0.2413 (5)0.9460 (3)0.0522 (9)
H70.33480.16280.93450.063*
C80.6087 (2)0.6003 (4)0.9941 (2)0.0404 (7)
C90.6728 (2)0.5543 (4)0.9499 (3)0.0424 (7)
C100.8662 (3)0.2212 (5)0.8302 (3)0.0588 (10)
C110.8343 (5)0.0358 (6)0.7828 (6)0.119 (2)
H11A0.8451−0.04860.83820.178*
H11B0.86970.00150.74290.178*
H11C0.76830.03870.73750.178*
C120.8844 (4)0.5382 (7)0.7748 (5)0.0971 (17)
H12A0.84600.63590.73640.146*
H12B0.93780.52610.75710.146*
H12C0.90590.56000.84890.146*
C130.9711 (3)0.2251 (10)0.8940 (4)0.113 (2)
H13A0.98820.33480.93250.169*
H13B1.00320.21600.84790.169*
H13C0.98890.12690.94230.169*
C140.53370 (18)0.4799 (4)0.9788 (2)0.0340 (6)
B10.7425 (2)0.3542 (5)0.8473 (3)0.0397 (7)
U11U22U33U12U13U23
Br10.0592 (3)0.0748 (3)0.1085 (4)−0.02956 (19)0.0614 (3)−0.0371 (2)
Br20.0623 (3)0.0677 (3)0.0883 (3)−0.01639 (18)0.0490 (2)−0.0388 (2)
O10.0482 (13)0.0696 (15)0.0472 (13)0.0173 (11)0.0281 (11)0.0108 (11)
O20.0525 (14)0.0954 (19)0.0458 (13)0.0283 (13)0.0331 (12)0.0213 (13)
C10.124 (4)0.122 (4)0.058 (3)0.044 (4)0.056 (3)0.016 (3)
C20.053 (2)0.070 (2)0.0533 (19)0.0117 (17)0.0365 (17)0.0064 (17)
C30.0304 (14)0.0502 (17)0.0361 (15)0.0019 (12)0.0164 (12)−0.0025 (13)
C40.0353 (15)0.0459 (16)0.0396 (15)0.0015 (12)0.0175 (13)−0.0087 (13)
C50.0303 (14)0.0468 (16)0.0389 (15)−0.0028 (12)0.0171 (13)−0.0058 (13)
C60.0470 (18)0.0480 (19)0.066 (2)−0.0136 (14)0.0337 (17)−0.0207 (16)
C70.0449 (18)0.0520 (19)0.072 (2)−0.0169 (15)0.0358 (18)−0.0202 (17)
C80.0342 (15)0.0481 (17)0.0442 (16)−0.0061 (13)0.0213 (13)−0.0086 (13)
C90.0312 (15)0.0519 (18)0.0493 (18)−0.0071 (13)0.0218 (14)−0.0045 (14)
C100.054 (2)0.073 (2)0.070 (2)0.0207 (18)0.0466 (19)0.0189 (19)
C110.192 (7)0.055 (3)0.183 (6)0.007 (3)0.153 (6)0.004 (3)
C120.103 (4)0.078 (3)0.144 (5)−0.016 (3)0.086 (4)−0.003 (3)
C130.057 (3)0.197 (7)0.090 (4)0.045 (4)0.035 (3)0.029 (4)
C140.0288 (13)0.0408 (15)0.0354 (15)−0.0024 (11)0.0162 (12)−0.0050 (12)
B10.0338 (17)0.0473 (19)0.0427 (19)0.0011 (14)0.0204 (15)−0.0029 (15)
Br1—C91.899 (3)C6—H60.9300
Br2—C41.899 (3)C7—C8i1.432 (4)
O1—B11.351 (4)C7—H70.9300
O1—C21.463 (4)C8—C91.408 (4)
O2—B11.336 (4)C8—C141.419 (4)
O2—C101.460 (4)C8—C7i1.432 (4)
C1—C21.492 (5)C10—C131.504 (6)
C1—H1A0.9600C10—C111.535 (7)
C1—H1B0.9600C11—H11A0.9600
C1—H1C0.9600C11—H11B0.9600
C2—C101.530 (5)C11—H11C0.9600
C2—C121.542 (6)C12—H12A0.9600
C3—C91.380 (4)C12—H12B0.9600
C3—C41.394 (4)C12—H12C0.9600
C3—B11.583 (4)C13—H13A0.9600
C4—C51.397 (4)C13—H13B0.9600
C5—C61.425 (4)C13—H13C0.9600
C5—C141.428 (4)C14—C14i1.426 (5)
C6—C71.345 (4)
B1—O1—C2107.2 (3)C3—C9—Br1116.9 (2)
B1—O2—C10107.7 (2)C8—C9—Br1118.9 (2)
C2—C1—H1A109.5O2—C10—C13109.0 (3)
C2—C1—H1B109.5O2—C10—C2103.1 (2)
H1A—C1—H1B109.5C13—C10—C2116.5 (4)
C2—C1—H1C109.5O2—C10—C11106.1 (3)
H1A—C1—H1C109.5C13—C10—C11110.7 (5)
H1B—C1—H1C109.5C2—C10—C11110.7 (4)
O1—C2—C1109.7 (3)C10—C11—H11A109.5
O1—C2—C10103.0 (2)C10—C11—H11B109.5
C1—C2—C10118.3 (4)H11A—C11—H11B109.5
O1—C2—C12104.4 (3)C10—C11—H11C109.5
C1—C2—C12108.0 (4)H11A—C11—H11C109.5
C10—C2—C12112.5 (4)H11B—C11—H11C109.5
C9—C3—C4116.6 (3)C2—C12—H12A109.5
C9—C3—B1122.0 (3)C2—C12—H12B109.5
C4—C3—B1121.4 (3)H12A—C12—H12B109.5
C3—C4—C5123.7 (3)C2—C12—H12C109.5
C3—C4—Br2117.0 (2)H12A—C12—H12C109.5
C5—C4—Br2119.2 (2)H12B—C12—H12C109.5
C4—C5—C6123.7 (3)C10—C13—H13A109.5
C4—C5—C14117.7 (2)C10—C13—H13B109.5
C6—C5—C14118.6 (2)H13A—C13—H13B109.5
C7—C6—C5121.6 (3)C10—C13—H13C109.5
C7—C6—H6119.2H13A—C13—H13C109.5
C5—C6—H6119.2H13B—C13—H13C109.5
C6—C7—C8i121.6 (3)C8—C14—C14i119.8 (3)
C6—C7—H7119.2C8—C14—C5120.4 (2)
C8i—C7—H7119.2C14i—C14—C5119.8 (3)
C9—C8—C14117.3 (3)O2—B1—O1114.1 (3)
C9—C8—C7i124.0 (3)O2—B1—C3122.8 (3)
C14—C8—C7i118.6 (3)O1—B1—C3123.1 (3)
C3—C9—C8124.2 (3)
D—H···AD—HH···AD···AD—H···A
C4—Br2···Cg1ii1.90 (1)3.48 (1)4.921 (3)130 (1)
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the C3–C5/C8/C9/C14 benzene ring.

D—H⋯AD—HH⋯ADAD—H⋯A
C4—Br2⋯Cg1i1.90 (1)3.48 (1)4.921 (3)130 (1)

Symmetry code: (i) .

  2 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

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