organic compounds
1-Chloromethyl-4-nitrobenzene
aDepartment of Chemistry, Government College University, Lahore 54000, Pakistan, and bDepartment of Physics, Faculty of Arts and Sciences, Erciyes University, 38039 Kayseri, Turkey
*Correspondence e-mail: akkurt@erciyes.edu.tr
In the title compound, C7H6ClNO2, the nitro group is almost coplanar with the aromatic ring [dihedral angle = 2.9 (2)°], but the Cl atom deviates from the ring plane by 1.129 (1) Å. In the crystal, molecules are linked by weak C—H⋯O interactions to generate chains.
Related literature
For background on the toxicity of nitro-aromatic compounds, see: Moreno et al. (1986). For the synthesis of the title compound, see: Livermore & Sealock (1947). For bond-length data, see: Allen et al. (1987).
Experimental
Crystal data
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Data collection
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Data collection: APEX2 (Bruker, 2007); cell SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999), PARST (Nardelli, 1983) and PLATON (Spek, 2009).
Supporting information
10.1107/S1600536810022191/hb5491sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810022191/hb5491Isup2.hkl
The title p-nitrobenzyl chloride was prepared by adding 5.3 ml of benzyl chloride slowly and with stirring to 27.5 ml of a mixture of equal parts of concentrated nitric and sulfuric acids cooled to 283 K. The temperature rose to 303 K during the 10 min required for the addition. The mixture was stirred for 30 min and then poured into 50 g of crushed ice. The crude material was recrystallized from ethanol. Product obtained was dissolved in ethanol and crystallized by slow evaporation of the solvent to yield colourless needles of (I) in an over-all yield of 46% (Livermore & Sealock, 1947).
H atoms were positioned geometrically (C—H = 0.93 and 0.97 Å) and allowed to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C).
Data collection: APEX2 (Bruker, 2007); cell
SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999), PARST (Nardelli, 1983) and PLATON (Spek, 2009).C7H6ClNO2 | F(000) = 352 |
Mr = 171.58 | Dx = 1.501 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 1957 reflections |
a = 4.7434 (1) Å | θ = 3.3–26.7° |
b = 6.4189 (2) Å | µ = 0.45 mm−1 |
c = 24.9413 (11) Å | T = 296 K |
V = 759.40 (4) Å3 | Needle, colourless |
Z = 4 | 0.35 × 0.11 × 0.10 mm |
Bruker APEXII CCD diffractometer | 1586 reflections with I > 2σ(I) |
Radiation source: sealed tube | Rint = 0.018 |
Graphite monochromator | θmax = 28.3°, θmin = 3.3° |
ϕ and ω scans | h = −5→6 |
4389 measured reflections | k = −8→5 |
1816 independent reflections | l = −33→17 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.041 | H-atom parameters constrained |
wR(F2) = 0.103 | w = 1/[σ2(Fo2) + (0.049P)2 + 0.1709P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max < 0.001 |
1816 reflections | Δρmax = 0.33 e Å−3 |
100 parameters | Δρmin = −0.34 e Å−3 |
0 restraints | Absolute structure: Flack (1983), 662 Freidel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.02 (11) |
C7H6ClNO2 | V = 759.40 (4) Å3 |
Mr = 171.58 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 4.7434 (1) Å | µ = 0.45 mm−1 |
b = 6.4189 (2) Å | T = 296 K |
c = 24.9413 (11) Å | 0.35 × 0.11 × 0.10 mm |
Bruker APEXII CCD diffractometer | 1586 reflections with I > 2σ(I) |
4389 measured reflections | Rint = 0.018 |
1816 independent reflections |
R[F2 > 2σ(F2)] = 0.041 | H-atom parameters constrained |
wR(F2) = 0.103 | Δρmax = 0.33 e Å−3 |
S = 1.04 | Δρmin = −0.34 e Å−3 |
1816 reflections | Absolute structure: Flack (1983), 662 Freidel pairs |
100 parameters | Absolute structure parameter: 0.02 (11) |
0 restraints |
Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su'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 on F2 for ALL reflections except those 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-obs 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 | ||
Cl1 | 0.75015 (18) | 0.45250 (12) | 0.22343 (3) | 0.0812 (3) | |
O1 | 1.4188 (4) | −0.3381 (3) | 0.07002 (7) | 0.0621 (6) | |
O2 | 1.4761 (4) | −0.0854 (3) | 0.01453 (7) | 0.0601 (6) | |
N1 | 1.3647 (3) | −0.1634 (3) | 0.05351 (7) | 0.0434 (5) | |
C1 | 1.1532 (4) | −0.0398 (3) | 0.08269 (7) | 0.0364 (5) | |
C2 | 1.0829 (4) | 0.1540 (3) | 0.06377 (7) | 0.0421 (6) | |
C3 | 0.8901 (4) | 0.2704 (3) | 0.09215 (8) | 0.0437 (6) | |
C4 | 0.7690 (4) | 0.1928 (3) | 0.13883 (7) | 0.0393 (5) | |
C5 | 0.8402 (5) | −0.0046 (3) | 0.15629 (8) | 0.0472 (6) | |
C6 | 1.0341 (5) | −0.1235 (3) | 0.12836 (8) | 0.0459 (6) | |
C7 | 0.5663 (5) | 0.3213 (4) | 0.17034 (8) | 0.0533 (7) | |
H2 | 1.16370 | 0.20560 | 0.03250 | 0.0510* | |
H3 | 0.84040 | 0.40230 | 0.08000 | 0.0520* | |
H5 | 0.75690 | −0.05800 | 0.18710 | 0.0570* | |
H6 | 1.08280 | −0.25630 | 0.14000 | 0.0550* | |
H7A | 0.42040 | 0.23280 | 0.18530 | 0.0640* | |
H7B | 0.47710 | 0.42290 | 0.14710 | 0.0640* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0957 (5) | 0.0831 (5) | 0.0647 (4) | 0.0041 (4) | 0.0047 (4) | −0.0299 (3) |
O1 | 0.0677 (11) | 0.0514 (9) | 0.0671 (10) | 0.0222 (8) | −0.0024 (8) | 0.0041 (8) |
O2 | 0.0584 (10) | 0.0629 (11) | 0.0591 (9) | 0.0072 (8) | 0.0175 (8) | 0.0010 (8) |
N1 | 0.0412 (8) | 0.0450 (9) | 0.0440 (8) | 0.0046 (8) | −0.0047 (7) | −0.0051 (7) |
C1 | 0.0336 (8) | 0.0382 (9) | 0.0374 (8) | 0.0008 (7) | −0.0048 (7) | −0.0001 (7) |
C2 | 0.0446 (10) | 0.0451 (11) | 0.0366 (9) | 0.0024 (9) | 0.0012 (7) | 0.0076 (8) |
C3 | 0.0496 (11) | 0.0409 (10) | 0.0406 (9) | 0.0079 (9) | −0.0016 (8) | 0.0079 (8) |
C4 | 0.0362 (9) | 0.0460 (10) | 0.0357 (8) | 0.0024 (9) | −0.0033 (7) | −0.0008 (7) |
C5 | 0.0526 (11) | 0.0495 (12) | 0.0394 (9) | −0.0012 (9) | 0.0046 (8) | 0.0080 (8) |
C6 | 0.0500 (11) | 0.0405 (10) | 0.0471 (10) | 0.0015 (9) | 0.0001 (9) | 0.0084 (8) |
C7 | 0.0510 (12) | 0.0613 (13) | 0.0475 (11) | 0.0111 (12) | 0.0033 (9) | −0.0004 (10) |
Cl1—C7 | 1.795 (2) | C4—C7 | 1.491 (3) |
O1—N1 | 1.222 (3) | C5—C6 | 1.383 (3) |
O2—N1 | 1.215 (2) | C2—H2 | 0.9300 |
N1—C1 | 1.472 (3) | C3—H3 | 0.9300 |
C1—C2 | 1.372 (3) | C5—H5 | 0.9300 |
C1—C6 | 1.380 (3) | C6—H6 | 0.9300 |
C2—C3 | 1.377 (3) | C7—H7A | 0.9700 |
C3—C4 | 1.391 (3) | C7—H7B | 0.9700 |
C4—C5 | 1.382 (3) | ||
O1—N1—O2 | 123.83 (19) | C1—C2—H2 | 121.00 |
O1—N1—C1 | 118.12 (17) | C3—C2—H2 | 121.00 |
O2—N1—C1 | 118.05 (18) | C2—C3—H3 | 120.00 |
N1—C1—C2 | 118.98 (16) | C4—C3—H3 | 120.00 |
N1—C1—C6 | 118.51 (17) | C4—C5—H5 | 120.00 |
C2—C1—C6 | 122.51 (18) | C6—C5—H5 | 120.00 |
C1—C2—C3 | 118.48 (17) | C1—C6—H6 | 121.00 |
C2—C3—C4 | 120.69 (18) | C5—C6—H6 | 121.00 |
C3—C4—C5 | 119.43 (18) | Cl1—C7—H7A | 110.00 |
C3—C4—C7 | 120.64 (18) | Cl1—C7—H7B | 110.00 |
C5—C4—C7 | 119.93 (18) | C4—C7—H7A | 110.00 |
C4—C5—C6 | 120.65 (18) | C4—C7—H7B | 110.00 |
C1—C6—C5 | 118.22 (18) | H7A—C7—H7B | 108.00 |
Cl1—C7—C4 | 109.58 (16) | ||
O1—N1—C1—C2 | −177.90 (18) | C1—C2—C3—C4 | −0.2 (3) |
O1—N1—C1—C6 | 2.4 (3) | C2—C3—C4—C5 | −1.0 (3) |
O2—N1—C1—C2 | 2.4 (3) | C2—C3—C4—C7 | 178.30 (19) |
O2—N1—C1—C6 | −177.28 (19) | C3—C4—C5—C6 | 1.2 (3) |
N1—C1—C2—C3 | −178.37 (17) | C7—C4—C5—C6 | −178.1 (2) |
C6—C1—C2—C3 | 1.3 (3) | C3—C4—C7—Cl1 | −95.5 (2) |
N1—C1—C6—C5 | 178.55 (18) | C5—C4—C7—Cl1 | 83.8 (2) |
C2—C1—C6—C5 | −1.1 (3) | C4—C5—C6—C1 | −0.2 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7B···O1i | 0.97 | 2.48 | 3.396 (3) | 158 |
Symmetry code: (i) x−1, y+1, z. |
Experimental details
Crystal data | |
Chemical formula | C7H6ClNO2 |
Mr | 171.58 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 296 |
a, b, c (Å) | 4.7434 (1), 6.4189 (2), 24.9413 (11) |
V (Å3) | 759.40 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.45 |
Crystal size (mm) | 0.35 × 0.11 × 0.10 |
Data collection | |
Diffractometer | Bruker APEXII CCD diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4389, 1816, 1586 |
Rint | 0.018 |
(sin θ/λ)max (Å−1) | 0.667 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.041, 0.103, 1.04 |
No. of reflections | 1816 |
No. of parameters | 100 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.33, −0.34 |
Absolute structure | Flack (1983), 662 Freidel pairs |
Absolute structure parameter | 0.02 (11) |
Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997), WinGX (Farrugia, 1999), PARST (Nardelli, 1983) and PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7B···O1i | 0.97 | 2.48 | 3.396 (3) | 158 |
Symmetry code: (i) x−1, y+1, z. |
Footnotes
‡Additional corresponding author, e-mail: azizhej@hotmail.com.
Acknowledgements
The authors are grateful to the Higher Education Commission for providing financial support. Professor Islam Ullah Khan is also gratefully acknowledged for providing single-crystal X-ray diffraction facilities at the Materials Chemistry Laboratory, GC University Lahore.
References
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Bruker (2007). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
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The irreversible binding of the reductive intermediates of nitroaromatic compounds to protein and DNA is thought to be responsible for the carcinogenicity and mutagenicity of this class of compounds. Several studies revealed that some nitro radical metabolites with special features are expected to decompose to form neutral carbon-centered free radicals with not net reduction of the nitro group occurring. The radicals anions of p-and o-nitrobenzyl chloride are known to expel chloride to form the corresponding carbon-centered nitrobenzyl radicals with rate constants of 1 × 104 and 4 × 103 s-1. Such species are highly reactive and could account for the unusual cytotoxicity of these nitrocompounds (Moreno et al., 1986). This structural report on 1-(chloromethyl)-4-nitrobenzene (p-nitrobenzyl chloride) might be helpful to carry out such studies on these nitroaromatic compounds in future.
The title molecule (I), (Fig. 1), is non-planar and the dihedral angle between the plane of the NO2 group and benzene (C1–C6) ring is 2.9 (2)°, while the C5—C4—C7—Cl1 torsion angle is 83.8 (2)°. In (I), the bond lengths (Allen et al., 1987) and angles have values within the normal ranges.
In the crystal structure, there is no classic hydrogen bonds. A weak intermolecular C—H···O interaction contrubutes to the stability of the structure (Table 1, Fig. 2).