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The title compound, C9H9Cl3, is being used as a platform for new tripodal receptors. Two mol­ecules make up the asymmetric unit; weak intermolecular hydrogen bonding is observed between methyl­ene H atoms and the chlorine of an adjacent mol­ecule. There are also C-H...[pi] interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100003875/qb0195sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100003875/qb0195Isup2.hkl
Contains datablock I

CCDC reference: 144722

Comment top

Two molecules make up the asymmetric unit of the title compound, (I). Weak intermolecular hydrogen bonding is observed (full details in Table 1) between a methylene H atom H18B and chlorine Cl4 of an adjacent molecule. There are also C—H···πi interactions with H···ring-centroid separations of 3.07–3.31 Å (Table 1).

Experimental top

The title compound was prepared following literature methods (Cochrane et al., 1968) and was recrystallized from toluene.

Computing details top

Data collection: CAD-4-PC (Nonius, 1993); cell refinement: CAD-4-PC (Nonius, 1993); data reduction: XCAD4 (Harms, 1995); program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Siemens, 1994); software used to prepare material for publication: SHELXTL (Siemens, 1994).

(I) top
Crystal data top
C9H9Cl3Z = 4
Mr = 223.51F(000) = 456
Triclinic, P1Dx = 1.474 Mg m3
a = 8.7124 (12) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.0659 (5) ÅCell parameters from 25 reflections
c = 12.7901 (15) Åθ = 10.4–14.9°
α = 87.537 (8)°µ = 0.85 mm1
β = 86.992 (10)°T = 163 K
γ = 87.873 (8)°Fragment, colourless
V = 1007.3 (2) Å30.30 × 0.30 × 0.25 mm
Data collection top
Nonius CAD-4
diffractometer
3047 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.025
Graphite monochromatorθmax = 26.0°, θmin = 2.2°
ωθ scansh = 910
Absorption correction: ψ scan
Siemens, 1994
k = 1111
Tmin = 0.722, Tmax = 0.809l = 1515
6800 measured reflections3 standard reflections every 120 min
3943 independent reflections intensity decay: 1%
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)] = 0.032Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.088H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0424P)2 + 0.2112P]
where P = (Fo2 + 2Fc2)/3
3943 reflections(Δ/σ)max = 0.001
217 parametersΔρmax = 0.31 e Å3
0 restraintsΔρmin = 0.34 e Å3
Crystal data top
C9H9Cl3γ = 87.873 (8)°
Mr = 223.51V = 1007.3 (2) Å3
Triclinic, P1Z = 4
a = 8.7124 (12) ÅMo Kα radiation
b = 9.0659 (5) ŵ = 0.85 mm1
c = 12.7901 (15) ÅT = 163 K
α = 87.537 (8)°0.30 × 0.30 × 0.25 mm
β = 86.992 (10)°
Data collection top
Nonius CAD-4
diffractometer
3047 reflections with I > 2σ(I)
Absorption correction: ψ scan
Siemens, 1994
Rint = 0.025
Tmin = 0.722, Tmax = 0.8093 standard reflections every 120 min
6800 measured reflections intensity decay: 1%
3943 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0320 restraints
wR(F2) = 0.088H-atom parameters constrained
S = 1.04Δρmax = 0.31 e Å3
3943 reflectionsΔρmin = 0.34 e Å3
217 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 on F2 for ALL reflections except for 0 with very negative F2 or flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating R_factor_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*/UeqOcc. (<1)
CG10.77090.91480.99310.000*0.00
CG20.40170.64870.41300.000*0.00
Cl10.70846 (6)1.22898 (6)1.19291 (5)0.04240 (15)
Cl20.76314 (8)0.96538 (7)0.68983 (5)0.05327 (18)
Cl30.99777 (7)0.60395 (7)1.14646 (5)0.05110 (18)
C10.6838 (2)1.0217 (2)1.04751 (16)0.0300 (4)
C20.7504 (2)1.0557 (2)0.94906 (16)0.0307 (4)
H20.73701.15260.91890.037*
C30.8365 (2)0.9498 (2)0.89384 (16)0.0287 (4)
C40.8578 (2)0.8088 (2)0.93919 (16)0.0284 (4)
H40.91790.73640.90230.034*
C50.7921 (2)0.7730 (2)1.03801 (16)0.0285 (4)
C60.7045 (2)0.8797 (2)1.09119 (16)0.0307 (4)
H60.65800.85541.15830.037*
C70.5904 (2)1.1365 (3)1.10597 (19)0.0413 (6)
H7A0.50481.08921.14710.050*
H7B0.54571.20981.05550.050*
C80.9036 (3)0.9864 (3)0.78633 (18)0.0405 (5)
H8A0.99430.92030.77120.049*
H8B0.93801.08950.78270.049*
C90.8161 (2)0.6214 (2)1.08663 (19)0.0381 (5)
H9A0.81250.54731.03220.046*
H9B0.73240.60161.14020.046*
Cl40.78510 (8)0.85386 (8)0.37208 (5)0.05551 (19)
Cl50.06273 (6)0.64646 (6)0.62442 (4)0.03996 (15)
Cl60.40637 (6)0.52473 (6)0.12134 (4)0.03606 (14)
C110.5510 (2)0.6791 (2)0.43654 (15)0.0273 (4)
C120.4263 (2)0.7430 (2)0.49244 (15)0.0294 (4)
H120.44340.80750.54690.035*
C130.2770 (2)0.7131 (2)0.46929 (15)0.0276 (4)
C140.2535 (2)0.6201 (2)0.38843 (16)0.0281 (4)
H140.15150.60200.37070.034*
C150.3768 (2)0.5532 (2)0.33302 (15)0.0259 (4)
C160.5258 (2)0.5834 (2)0.35807 (15)0.0267 (4)
H160.61100.53790.32100.032*
C170.7125 (2)0.7122 (2)0.46102 (17)0.0347 (5)
H17A0.77890.62160.45510.042*
H17B0.71410.74480.53380.042*
C180.1429 (3)0.7802 (2)0.53021 (19)0.0381 (5)
H18A0.06330.81530.48170.046*
H18B0.17650.86630.56710.046*
C190.3500 (2)0.4480 (2)0.24951 (16)0.0308 (4)
H19A0.23970.42500.25170.037*
H19B0.40970.35470.26300.037*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0360 (3)0.0463 (3)0.0466 (3)0.0067 (2)0.0108 (2)0.0194 (3)
Cl20.0716 (4)0.0566 (4)0.0310 (3)0.0024 (3)0.0043 (3)0.0066 (3)
Cl30.0445 (3)0.0404 (3)0.0701 (4)0.0031 (2)0.0273 (3)0.0045 (3)
C10.0199 (9)0.0382 (11)0.0328 (11)0.0010 (8)0.0039 (8)0.0104 (9)
C20.0257 (10)0.0291 (10)0.0374 (11)0.0008 (8)0.0031 (9)0.0000 (9)
C30.0231 (10)0.0349 (11)0.0280 (10)0.0046 (8)0.0007 (8)0.0006 (8)
C40.0206 (9)0.0307 (10)0.0341 (11)0.0005 (8)0.0005 (8)0.0062 (8)
C50.0213 (9)0.0324 (10)0.0322 (11)0.0031 (8)0.0059 (8)0.0019 (8)
C60.0209 (10)0.0475 (12)0.0239 (10)0.0037 (9)0.0015 (8)0.0026 (9)
C70.0257 (11)0.0541 (14)0.0459 (14)0.0055 (10)0.0059 (10)0.0225 (11)
C80.0390 (12)0.0450 (13)0.0363 (12)0.0047 (10)0.0081 (10)0.0024 (10)
C90.0282 (11)0.0393 (12)0.0467 (13)0.0053 (9)0.0074 (10)0.0098 (10)
Cl40.0556 (4)0.0688 (4)0.0441 (3)0.0393 (3)0.0075 (3)0.0128 (3)
Cl50.0300 (3)0.0498 (3)0.0399 (3)0.0083 (2)0.0105 (2)0.0096 (2)
Cl60.0323 (3)0.0493 (3)0.0265 (3)0.0026 (2)0.0009 (2)0.0015 (2)
C110.0235 (10)0.0327 (10)0.0251 (10)0.0049 (8)0.0016 (8)0.0077 (8)
C120.0338 (11)0.0287 (10)0.0257 (10)0.0041 (8)0.0010 (8)0.0008 (8)
C130.0250 (10)0.0269 (10)0.0301 (11)0.0010 (8)0.0034 (8)0.0034 (8)
C140.0211 (9)0.0323 (10)0.0306 (11)0.0037 (8)0.0006 (8)0.0032 (8)
C150.0255 (10)0.0278 (10)0.0239 (10)0.0034 (8)0.0009 (8)0.0039 (8)
C160.0222 (9)0.0314 (10)0.0255 (10)0.0009 (8)0.0040 (8)0.0045 (8)
C170.0285 (11)0.0425 (12)0.0332 (11)0.0098 (9)0.0033 (9)0.0049 (9)
C180.0326 (11)0.0372 (12)0.0432 (13)0.0008 (9)0.0095 (10)0.0021 (10)
C190.0275 (10)0.0356 (11)0.0290 (10)0.0048 (8)0.0024 (8)0.0002 (9)
Geometric parameters (Å, º) top
Cl1—C71.806 (2)Cl4—C171.790 (2)
Cl2—C81.803 (2)Cl5—C181.805 (2)
Cl3—C91.793 (2)Cl6—C191.804 (2)
C1—C21.386 (3)C11—C161.386 (3)
C1—C61.390 (3)C11—C121.391 (3)
C1—C71.498 (3)C11—C171.501 (3)
C2—C31.390 (3)C12—C131.388 (3)
C2—H20.9500C12—H120.9500
C3—C41.391 (3)C13—C141.390 (3)
C3—C81.494 (3)C13—C181.495 (3)
C4—C51.391 (3)C14—C151.391 (3)
C4—H40.9500C14—H140.9500
C5—C61.389 (3)C15—C161.393 (3)
C5—C91.496 (3)C15—C191.495 (3)
C6—H60.9500C16—H160.9500
C7—H7A0.9900C17—H17A0.9900
C7—H7B0.9900C17—H17B0.9900
C8—H8A0.9900C18—H18A0.9900
C8—H8B0.9900C18—H18B0.9900
C9—H9A0.9900C19—H19A0.9900
C9—H9B0.9900C19—H19B0.9900
C2—C1—C6119.20 (19)C16—C11—C12119.67 (18)
C2—C1—C7120.3 (2)C16—C11—C17119.75 (18)
C6—C1—C7120.5 (2)C12—C11—C17120.58 (19)
C1—C2—C3120.84 (19)C13—C12—C11120.52 (18)
C1—C2—H2119.6C13—C12—H12119.7
C3—C2—H2119.6C11—C12—H12119.7
C2—C3—C4119.28 (19)C12—C13—C14119.18 (18)
C2—C3—C8120.34 (19)C12—C13—C18120.53 (19)
C4—C3—C8120.37 (19)C14—C13—C18120.29 (18)
C5—C4—C3120.59 (19)C13—C14—C15121.05 (18)
C5—C4—H4119.7C13—C14—H14119.5
C3—C4—H4119.7C15—C14—H14119.5
C6—C5—C4119.22 (19)C14—C15—C16118.92 (18)
C6—C5—C9120.4 (2)C14—C15—C19120.58 (18)
C4—C5—C9120.36 (19)C16—C15—C19120.49 (18)
C5—C6—C1120.86 (19)C11—C16—C15120.62 (18)
C5—C6—H6119.6C11—C16—H16119.7
C1—C6—H6119.6C15—C16—H16119.7
C1—C7—Cl1110.59 (14)C11—C17—Cl4110.06 (14)
C1—C7—H7A109.5C11—C17—H17A109.6
Cl1—C7—H7A109.5Cl4—C17—H17A109.6
C1—C7—H7B109.5C11—C17—H17B109.6
Cl1—C7—H7B109.5Cl4—C17—H17B109.6
H7A—C7—H7B108.1H17A—C17—H17B108.2
C3—C8—Cl2110.50 (15)C13—C18—Cl5110.43 (15)
C3—C8—H8A109.5C13—C18—H18A109.6
Cl2—C8—H8A109.5Cl5—C18—H18A109.6
C3—C8—H8B109.5C13—C18—H18B109.6
Cl2—C8—H8B109.5Cl5—C18—H18B109.6
H8A—C8—H8B108.1H18A—C18—H18B108.1
C5—C9—Cl3110.81 (14)C15—C19—Cl6111.25 (14)
C5—C9—H9A109.5C15—C19—H19A109.4
Cl3—C9—H9A109.5Cl6—C19—H19A109.4
C5—C9—H9B109.5C15—C19—H19B109.4
Cl3—C9—H9B109.5Cl6—C19—H19B109.4
H9A—C9—H9B108.1H19A—C19—H19B108.0
C6—C1—C2—C30.2 (3)C16—C11—C12—C130.9 (3)
C7—C1—C2—C3179.63 (18)C17—C11—C12—C13179.60 (17)
C1—C2—C3—C41.1 (3)C11—C12—C13—C140.9 (3)
C1—C2—C3—C8178.05 (19)C11—C12—C13—C18179.25 (18)
C2—C3—C4—C50.9 (3)C12—C13—C14—C152.2 (3)
C8—C3—C4—C5178.20 (18)C18—C13—C14—C15178.05 (18)
C3—C4—C5—C60.0 (3)C13—C14—C15—C161.5 (3)
C3—C4—C5—C9179.68 (18)C13—C14—C15—C19177.16 (18)
C4—C5—C6—C10.9 (3)C12—C11—C16—C151.5 (3)
C9—C5—C6—C1178.81 (18)C17—C11—C16—C15178.96 (17)
C2—C1—C6—C50.8 (3)C14—C15—C16—C110.3 (3)
C7—C1—C6—C5179.36 (18)C19—C15—C16—C11179.01 (17)
C2—C1—C7—Cl193.8 (2)C16—C11—C17—Cl483.0 (2)
C6—C1—C7—Cl186.3 (2)C12—C11—C17—Cl497.5 (2)
C2—C3—C8—Cl283.9 (2)C12—C13—C18—Cl5102.3 (2)
C4—C3—C8—Cl295.2 (2)C14—C13—C18—Cl577.9 (2)
C6—C5—C9—Cl398.0 (2)C14—C15—C19—Cl6111.33 (18)
C4—C5—C9—Cl381.8 (2)C16—C15—C19—Cl670.0 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C18—H18B···Cl4i0.992.723.682 (2)163
C7—H7A···CG1ii0.993.073.509 (2)108
C7—H7B···CG1ii0.993.123.509 (2)105
C17—H17A···CG2iii0.993.313.729 (2)107
Symmetry codes: (i) x+1, y+2, z+1; (ii) x+1, y+2, z+2; (iii) x+1, y+1, z+1.

Experimental details

Crystal data
Chemical formulaC9H9Cl3
Mr223.51
Crystal system, space groupTriclinic, P1
Temperature (K)163
a, b, c (Å)8.7124 (12), 9.0659 (5), 12.7901 (15)
α, β, γ (°)87.537 (8), 86.992 (10), 87.873 (8)
V3)1007.3 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.85
Crystal size (mm)0.30 × 0.30 × 0.25
Data collection
DiffractometerNonius CAD-4
diffractometer
Absorption correctionψ scan
Siemens, 1994
Tmin, Tmax0.722, 0.809
No. of measured, independent and
observed [I > 2σ(I)] reflections
6800, 3943, 3047
Rint0.025
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.032, 0.088, 1.04
No. of reflections3943
No. of parameters217
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.31, 0.34

Computer programs: CAD-4-PC (Nonius, 1993), XCAD4 (Harms, 1995), SHELXS86 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), SHELXTL (Siemens, 1994).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C18—H18B···Cl4i0.992.723.682 (2)163
C7—H7A···CG1ii0.993.073.509 (2)108
C7—H7B···CG1ii0.993.123.509 (2)105
C17—H17A···CG2iii0.993.313.729 (2)107
Symmetry codes: (i) x+1, y+2, z+1; (ii) x+1, y+2, z+2; (iii) x+1, y+1, z+1.
 

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