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The molecular components, 2C14H10Br2·C14H10, are arranged in separate stacks in this ordered structure. There is no evidence of π–π intermolecular interaction. Di­phenyl­ethyne lies on a crystallographic inversion centre. The structure can be represented as centrosymmetric trimolecular units, held together by a C—H...ring interaction between a stilbene and each of the phenyl groups of the di­phenyl­ethyne (H...Cgring 2.66 Å; Cgring indicates a ring centroid).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680200942X/cm6007sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680200942X/cm6007Isup2.hkl
Contains datablock I

CCDC reference: 189416

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.006 Å
  • R factor = 0.055
  • wR factor = 0.148
  • Data-to-parameter ratio = 17.9

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
ABSTM_02 Alert C The ratio of expected to reported Tmax/Tmin(RR) is > 1.10 Tmin and Tmax reported: 0.946 0.999 Tmin and Tmax expected: 0.335 0.494 RR = 1.395 Please check that your absorption correction is appropriate. RINTA_01 Alert C The value of Rint is greater than 0.10 Rint given 0.103 PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(21) - C(22) = 1.44 Ang. General Notes
ABSTM_02 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 0.495 Tmax scaled 0.494 Tmin scaled 0.468
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
3 Alert Level C = Please check

Computing details top

Data collection: DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998); cell refinement: DENZO and COLLECT; data reduction: DENZO and COLLECT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 1999).

Cis-1,2-dibromo-1,2-diphenylethene, diphenylethyne (2:1) top
Crystal data top
C14H10Br2·0.5C14H10Dx = 1.646 Mg m3
Mr = 427.15Melting point = 68–71 K
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 14.8445 (5) ÅCell parameters from 13506 reflections
b = 5.7702 (3) Åθ = 1.0–27.1°
c = 20.741 (9) ŵ = 4.70 mm1
β = 104.037 (2)°T = 150 K
V = 1723.5 (8) Å3Block, colourless
Z = 40.30 × 0.20 × 0.15 mm
F(000) = 844
Data collection top
Enraf–Nonius KappaCCD area-detector
diffractometer
3718 independent reflections
Radiation source: Enraf–Nonius FR591 rotating anode2614 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.103
Detector resolution: 9.091 pixels mm-1θmax = 27.1°, θmin = 2.8°
φ and ω scansh = 1918
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
k = 67
Tmin = 0.946, Tmax = 0.999l = 2326
11791 measured reflections
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)] = 0.055Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.148H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0826P)2]
where P = (Fo2 + 2Fc2)/3
3718 reflections(Δ/σ)max = 0.002
208 parametersΔρmax = 0.76 e Å3
0 restraintsΔρmin = 0.95 e Å3
Special details top

Experimental. PLEASE NOTE cell_measurement_ fields are not relevant to area detector data, the entire data set is used to refine the cell, which is indexed from all observed reflections in a 10 degree phi range.

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
Br10.55860 (4)0.41738 (10)0.08283 (2)0.0458 (2)
Br20.39224 (3)0.74326 (8)0.11248 (2)0.03678 (19)
C10.5219 (3)0.3848 (8)0.1643 (2)0.0270 (9)
C20.4530 (3)0.5159 (8)0.1751 (2)0.0268 (9)
C30.5766 (3)0.2153 (8)0.2110 (2)0.0268 (10)
C40.6070 (3)0.0098 (8)0.1873 (2)0.0293 (10)
H40.59290.01900.14090.038*
C50.6576 (3)0.1518 (8)0.2308 (2)0.0303 (10)
H50.67640.29250.21410.039*
C60.6808 (3)0.1085 (8)0.2987 (2)0.0309 (10)
H60.71640.21790.32860.040*
C70.6518 (3)0.0947 (8)0.3226 (2)0.0296 (10)
H70.66700.12420.36900.038*
C80.6005 (3)0.2562 (7)0.2790 (2)0.0247 (9)
H80.58160.39630.29590.032*
C90.4140 (3)0.5057 (8)0.2344 (2)0.0277 (9)
C100.3636 (3)0.3103 (8)0.2446 (2)0.0307 (10)
H100.35510.18410.21420.040*
C110.3260 (3)0.3032 (9)0.2996 (2)0.0365 (11)
H110.29060.17250.30650.047*
C120.3394 (3)0.4827 (9)0.3440 (2)0.0342 (11)
H120.31490.47400.38220.044*
C130.3885 (3)0.6765 (9)0.3335 (2)0.0323 (10)
H130.39650.80170.36410.042*
C140.4259 (3)0.6900 (8)0.2792 (2)0.0297 (10)
H140.45950.82390.27230.039*
C210.0314 (3)0.4395 (8)0.0025 (2)0.0298 (10)
C220.1070 (3)0.2943 (8)0.0099 (2)0.0272 (9)
C230.1989 (3)0.3597 (9)0.0163 (2)0.0327 (10)
H230.21220.50100.04020.042*
C240.2706 (3)0.2210 (9)0.0078 (3)0.0388 (12)
H240.33320.26750.02530.050*
C250.2511 (4)0.0119 (9)0.0267 (3)0.0402 (12)
H250.30040.08310.03320.052*
C260.1613 (4)0.0558 (8)0.0508 (2)0.0391 (12)
H260.14850.19980.07340.051*
C270.0886 (3)0.0822 (8)0.0430 (2)0.0330 (10)
H270.02630.03300.06010.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0533 (3)0.0566 (4)0.0297 (3)0.0133 (3)0.0145 (2)0.0060 (2)
Br20.0353 (3)0.0369 (3)0.0344 (3)0.0050 (2)0.0013 (2)0.0055 (2)
C10.032 (2)0.026 (3)0.022 (2)0.0041 (19)0.0041 (18)0.0001 (18)
C20.0252 (19)0.024 (2)0.029 (2)0.0000 (18)0.0016 (18)0.0000 (19)
C30.0236 (19)0.028 (3)0.030 (2)0.0003 (18)0.0083 (19)0.0012 (19)
C40.027 (2)0.030 (3)0.033 (2)0.0004 (19)0.0106 (19)0.007 (2)
C50.031 (2)0.023 (2)0.040 (3)0.0023 (19)0.014 (2)0.006 (2)
C60.027 (2)0.026 (3)0.040 (3)0.0009 (18)0.008 (2)0.009 (2)
C70.032 (2)0.028 (3)0.030 (2)0.0015 (19)0.010 (2)0.003 (2)
C80.027 (2)0.023 (2)0.025 (2)0.0010 (17)0.0064 (18)0.0025 (17)
C90.0243 (19)0.030 (3)0.027 (2)0.0029 (19)0.0031 (18)0.0011 (19)
C100.026 (2)0.027 (3)0.036 (3)0.0010 (18)0.002 (2)0.002 (2)
C110.031 (2)0.037 (3)0.041 (3)0.002 (2)0.007 (2)0.006 (2)
C120.030 (2)0.041 (3)0.031 (2)0.008 (2)0.006 (2)0.005 (2)
C130.033 (2)0.034 (3)0.027 (2)0.005 (2)0.002 (2)0.003 (2)
C140.030 (2)0.022 (2)0.035 (2)0.0006 (19)0.003 (2)0.003 (2)
C210.031 (2)0.027 (3)0.029 (2)0.0033 (18)0.003 (2)0.003 (2)
C220.036 (2)0.024 (2)0.023 (2)0.0034 (19)0.0087 (19)0.0035 (18)
C230.037 (2)0.027 (3)0.033 (2)0.000 (2)0.007 (2)0.000 (2)
C240.031 (2)0.044 (3)0.041 (3)0.006 (2)0.008 (2)0.010 (2)
C250.050 (3)0.037 (3)0.039 (3)0.019 (2)0.020 (2)0.012 (2)
C260.062 (3)0.023 (3)0.035 (3)0.007 (2)0.017 (3)0.001 (2)
C270.042 (2)0.028 (3)0.030 (2)0.007 (2)0.011 (2)0.002 (2)
Geometric parameters (Å, º) top
Br1—C11.907 (4)C11—C121.368 (7)
Br2—C21.912 (4)C11—H110.9500
C1—C21.334 (6)C12—C131.381 (7)
C1—C31.474 (6)C12—H120.9500
C2—C91.481 (6)C13—C141.371 (6)
C3—C81.388 (6)C13—H130.9500
C3—C41.400 (6)C14—H140.9500
C4—C51.384 (7)C21—C21i1.188 (9)
C4—H40.9500C21—C221.439 (6)
C5—C61.390 (7)C22—C231.393 (6)
C5—H50.9500C22—C271.397 (6)
C6—C71.381 (7)C23—C241.377 (7)
C6—H60.9500C23—H230.9500
C7—C81.390 (6)C24—C251.396 (7)
C7—H70.9500C24—H240.9500
C8—H80.9500C25—C261.362 (8)
C9—C141.396 (6)C25—H250.9500
C9—C101.398 (6)C26—C271.382 (7)
C10—C111.387 (7)C26—H260.9500
C10—H100.9500C27—H270.9500
C2—C1—C3126.1 (4)C12—C11—H11119.7
C2—C1—Br1119.2 (3)C10—C11—H11119.7
C3—C1—Br1114.7 (3)C11—C12—C13120.2 (4)
C1—C2—C9125.9 (4)C11—C12—H12119.9
C1—C2—Br2122.0 (3)C13—C12—H12119.9
C9—C2—Br2112.1 (3)C14—C13—C12120.6 (5)
C8—C3—C4118.4 (4)C14—C13—H13119.7
C8—C3—C1121.3 (4)C12—C13—H13119.7
C4—C3—C1120.3 (4)C13—C14—C9119.5 (4)
C5—C4—C3120.8 (4)C13—C14—H14120.2
C5—C4—H4119.6C9—C14—H14120.2
C3—C4—H4119.6C21i—C21—C22178.8 (6)
C4—C5—C6120.1 (4)C23—C22—C27119.0 (4)
C4—C5—H5120.0C23—C22—C21121.1 (4)
C6—C5—H5120.0C27—C22—C21119.9 (4)
C7—C6—C5119.6 (4)C24—C23—C22120.5 (5)
C7—C6—H6120.2C24—C23—H23119.8
C5—C6—H6120.2C22—C23—H23119.8
C6—C7—C8120.4 (4)C23—C24—C25119.8 (5)
C6—C7—H7119.8C23—C24—H24120.1
C8—C7—H7119.8C25—C24—H24120.1
C3—C8—C7120.7 (4)C26—C25—C24120.0 (4)
C3—C8—H8119.6C26—C25—H25120.0
C7—C8—H8119.6C24—C25—H25120.0
C14—C9—C10119.9 (4)C25—C26—C27120.9 (5)
C14—C9—C2120.8 (4)C25—C26—H26119.5
C10—C9—C2119.3 (4)C27—C26—H26119.5
C11—C10—C9119.0 (4)C26—C27—C22119.8 (5)
C11—C10—H10120.5C26—C27—H27120.1
C9—C10—H10120.5C22—C27—H27120.1
C12—C11—C10120.6 (5)
C4—C3—C1—C2144.5 (5)C10—C9—C2—Br2111.1 (4)
C3—C1—C2—C94.2 (7)C14—C9—C2—C1112.5 (5)
C1—C2—C9—C1068.6 (6)Br1—C1—C2—Br22.0 (5)
C4—C3—C1—Br137.2 (5)
Symmetry code: (i) x, y+1, z.
Torsion Angles (°) in cis-stilbenes. top
CompoundC4-C3-C1-C2C14-C9-C2-C1C3-C1-C2-C9
1,2-dibromo_(obs)144.5 (4)112.9 (5)-4.4 (7)
1,2-dibromo_(calc)1201140.2
1,2-dichloro_(obs)133.7111.3-8.7
1,2-dichloro_(calc)1221150.3
4-ClPh-1,2-dichloro_(obs)129.3128.07.1
4-ClPh-1,2-dichloro_(calc)1181150.1
cis-stilbene_(calc)1211170.1
 

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