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The title compound, C8H6Cl3NO, also known as N-(2,4,5-tri­chloro­phenyl)­acet­amide, is an organic non-linear optical material. It crystallizes in the monoclinic system, in the non-centrosymmetric space group Pn.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802013417/ob6158sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802013417/ob6158Isup2.hkl
Contains datablock I

CCDC reference: 193785

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.023
  • wR factor = 0.062
  • Data-to-parameter ratio = 16.4

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry

General Notes

REFLT_03 From the CIF: _diffrn_reflns_theta_max 28.03 From the CIF: _reflns_number_total 1956 Count of symmetry unique reflns 1139 Completeness (_total/calc) 171.73% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 817 Fraction of Friedel pairs measured 0.717 Are heavy atom types Z>Si present yes Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and CAMERON (Watkin et al., 1996); software used to prepare material for publication: PLATON (Spek, 1990).

N-[2,4,5-trichlorophenyl]acetamide top
Crystal data top
C8H6Cl3NOF(000) = 240
Mr = 238.49Dx = 1.691 Mg m3
Monoclinic, PnMelting point: 464 K
Hall symbol: P -2yacMo Kα radiation, λ = 0.71073 Å
a = 3.9015 (8) ÅCell parameters from 825 reflections
b = 12.658 (3) Åθ = 3.9–27.7°
c = 9.6687 (19) ŵ = 0.93 mm1
β = 101.186 (5)°T = 293 K
V = 468.42 (17) Å3Needle, colourles
Z = 20.56 × 0.28 × 0.27 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1956 independent reflections
Radiation source: fine-focus sealed tube1903 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.014
φ and ω scansθmax = 28.0°, θmin = 1.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 55
Tmin = 0.624, Tmax = 0.787k = 1616
3931 measured reflectionsl = 1211
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.023H-atom parameters constrained
wR(F2) = 0.062 w = 1/[σ2(Fo2) + (0.0438P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
1956 reflectionsΔρmax = 0.18 e Å3
119 parametersΔρmin = 0.20 e Å3
0 restraintsAbsolute structure: (Flack, 1983), 817 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.04 (4)
Special details top

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All e.s.d.'s are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

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
Cl10.39502 (10)0.23324 (3)0.52793 (4)0.0478 (1)
Cl20.29487 (14)0.52921 (3)0.91216 (6)0.0567 (2)
Cl30.08347 (11)0.35322 (4)1.11287 (5)0.0523 (1)
O10.4013 (5)0.00582 (11)0.93830 (15)0.0634 (5)
N10.1720 (4)0.08189 (10)0.72976 (14)0.0377 (4)
C10.2040 (4)0.18756 (11)0.77550 (16)0.0337 (4)
C20.3008 (4)0.26574 (12)0.69005 (17)0.0355 (5)
C30.3274 (4)0.37098 (13)0.73118 (18)0.0386 (4)
C40.2604 (4)0.39830 (12)0.86157 (18)0.0375 (5)
C50.1658 (4)0.32125 (13)0.94911 (17)0.0367 (4)
C60.1335 (4)0.21694 (13)0.90534 (18)0.0367 (4)
C70.2734 (5)0.00256 (13)0.81432 (18)0.0386 (4)
C80.2160 (7)0.10773 (14)0.7419 (2)0.0533 (6)
H10.082620.070040.642650.0452*
H30.389490.422320.671760.0463*
H60.063750.166080.963580.0440*
H8A0.347870.160860.800130.0799*
H8B0.291240.104330.653190.0799*
H8C0.027900.125290.726060.0799*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0664 (3)0.0492 (2)0.0301 (2)0.0091 (2)0.0148 (2)0.0044 (2)
Cl20.0854 (3)0.0338 (2)0.0503 (3)0.0029 (2)0.0121 (2)0.0071 (2)
Cl30.0778 (3)0.0469 (2)0.0354 (2)0.0066 (2)0.0191 (2)0.0052 (2)
O10.1068 (12)0.0406 (6)0.0321 (7)0.0117 (7)0.0132 (7)0.0005 (5)
N10.0541 (7)0.0315 (6)0.0245 (7)0.0007 (5)0.0005 (5)0.0001 (5)
C10.0399 (7)0.0319 (7)0.0268 (7)0.0012 (5)0.0001 (6)0.0024 (5)
C20.0409 (8)0.0388 (8)0.0256 (8)0.0019 (5)0.0033 (6)0.0001 (6)
C30.0464 (8)0.0358 (7)0.0320 (8)0.0048 (6)0.0039 (6)0.0038 (6)
C40.0434 (8)0.0310 (7)0.0357 (9)0.0013 (5)0.0020 (6)0.0033 (5)
C50.0441 (8)0.0369 (7)0.0282 (8)0.0053 (6)0.0048 (6)0.0020 (6)
C60.0447 (8)0.0355 (7)0.0296 (8)0.0018 (6)0.0068 (6)0.0035 (6)
C70.0498 (8)0.0344 (7)0.0295 (8)0.0018 (6)0.0026 (6)0.0029 (6)
C80.0847 (13)0.0340 (8)0.0372 (10)0.0040 (8)0.0020 (9)0.0009 (6)
Geometric parameters (Å, º) top
Cl1—C21.7277 (17)C3—C41.380 (2)
Cl2—C41.7256 (16)C4—C51.387 (2)
Cl3—C51.7237 (17)C5—C61.385 (2)
O1—C71.210 (2)C7—C81.501 (2)
N1—C11.4067 (19)C3—H30.93
N1—C71.357 (2)C6—H60.93
N1—H10.86C8—H8A0.96
C1—C61.387 (2)C8—H8B0.96
C1—C21.388 (2)C8—H8C0.96
C2—C31.388 (2)
Cl1···N12.9823 (16)C2···Cl1vi3.6008 (19)
Cl1···C1i3.6186 (18)C2···C1i3.599 (2)
Cl1···C2i3.6008 (19)C2···C6i3.556 (2)
Cl1···Cl2ii3.6614 (10)C3···C5i3.586 (2)
Cl1···C8iii3.617 (2)C3···Cl2ix3.597 (2)
Cl2···C3iv3.597 (2)C5···Cl3i3.6455 (19)
Cl2···Cl3ii3.6222 (11)C5···C3vi3.586 (2)
Cl2···Cl33.1670 (10)C6···O12.865 (2)
Cl2···Cl1v3.6614 (10)C6···C2vi3.556 (2)
Cl3···C5vi3.6455 (19)C8···O1vii3.223 (3)
Cl3···Cl2v3.6222 (11)C8···Cl1x3.617 (2)
Cl3···Cl23.1670 (10)C7···H62.7868
Cl1···H12.7400C8···H8Ci2.9917
Cl1···H8Avii2.9023H1···Cl12.7400
Cl2···H3iv3.1304H1···H8B2.3478
Cl3···H3v3.0227H1···O1vii2.1872
O1···C62.865 (2)H3···Cl2ix3.1304
O1···N1viii3.022 (2)H3···Cl3ii3.0227
O1···C8viii3.223 (3)H6···O12.4564
O1···H62.4564H6···C72.7868
O1···H1viii2.1872H6···H8Bx2.4204
O1···H8Bviii2.6381H8A···Cl1viii2.9023
N1···Cl12.9823 (16)H8B···H12.3478
N1···O1vii3.022 (2)H8B···O1vii2.6381
C1···Cl1vi3.6186 (18)H8B···H6iii2.4204
C1···C2vi3.599 (2)H8C···C8vi2.9917
C1—N1—C7124.18 (14)Cl3—C5—C6118.84 (13)
C7—N1—H1117.91C1—C6—C5120.66 (15)
C1—N1—H1117.91N1—C7—C8114.71 (15)
N1—C1—C6121.22 (14)O1—C7—N1122.92 (16)
N1—C1—C2120.58 (14)O1—C7—C8122.37 (16)
C2—C1—C6118.18 (14)C2—C3—H3120.49
C1—C2—C3121.84 (15)C4—C3—H3120.48
Cl1—C2—C3118.11 (12)C1—C6—H6119.67
Cl1—C2—C1120.05 (12)C5—C6—H6119.66
C2—C3—C4119.02 (15)C7—C8—H8A109.47
C3—C4—C5120.07 (15)C7—C8—H8B109.47
Cl2—C4—C3118.77 (12)C7—C8—H8C109.47
Cl2—C4—C5121.16 (13)H8A—C8—H8B109.48
C4—C5—C6120.20 (15)H8A—C8—H8C109.46
Cl3—C5—C4120.95 (13)H8B—C8—H8C109.47
C7—N1—C1—C2140.98 (18)C1—C2—C3—C40.9 (2)
C7—N1—C1—C640.3 (3)Cl1—C2—C3—C4178.65 (12)
C1—N1—C7—O10.2 (3)C2—C3—C4—Cl2179.86 (12)
C1—N1—C7—C8179.58 (18)C2—C3—C4—C50.4 (2)
C2—C1—C6—C51.2 (2)Cl2—C4—C5—C6178.82 (13)
N1—C1—C2—Cl11.8 (2)Cl2—C4—C5—Cl30.7 (2)
C6—C1—C2—C30.1 (2)C3—C4—C5—C60.9 (2)
N1—C1—C2—C3178.64 (15)C3—C4—C5—Cl3179.59 (13)
C6—C1—C2—Cl1179.46 (12)C4—C5—C6—C11.7 (2)
N1—C1—C6—C5179.96 (15)Cl3—C5—C6—C1178.73 (13)
Symmetry codes: (i) x+1, y, z; (ii) x+1/2, y+1, z1/2; (iii) x+1/2, y, z1/2; (iv) x+1/2, y+1, z+1/2; (v) x1/2, y+1, z+1/2; (vi) x1, y, z; (vii) x1/2, y, z1/2; (viii) x+1/2, y, z+1/2; (ix) x1/2, y+1, z1/2; (x) x1/2, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1vii0.862.193.022 (2)164
C6—H6···O10.932.462.865 (2)107
Symmetry code: (vii) x1/2, y, z1/2.
 

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