1,4-Bis(chloro­meth­yl)naphthalene

Tariq, M.I.; Tahir, M.N.; Hussain, I.; Roohi, A.

doi:10.1107/S1600536808022757

organic compounds

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ISSN: 2056-9890

Volume 64| Part 8| August 2008| Page o1596

doi:10.1107/S1600536808022757

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1,4-Bis(chloromethyl)naphthalene

Muhammad Ilyas Tariq,^a M. Nawaz Tahir,^b ^* Ishtiaq Hussain ^a and Ayesha Roohi ^c

^aDepartment of Chemistry, University of Sargodha, Sargodha, Pakistan, ^bDepartment of Physics, University of Sargodha, Sargodha, Pakistan, and ^cInstitute of Chemistry, University of the Punjab, Lahore 54590, Pakistan
^*Correspondence e-mail: dmntahir_uos@yahoo.com

(Received 16 July 2008; accepted 19 July 2008; online 26 July 2008)

In the title molecule, C₁₂H₁₀Cl₂, the torsion angles C_r—C_r—C_m—Cl around the C_m—C_r bonds have values of −104.1 (4) and −101.9 (4)°, where C_m is a methylene and C_r is a ring C atom. The molecules related by translation along the b axis are arranged into stacks by π–π interactions between unsubstituted and substituted aromatic rings of the naphthalene ring system (centroid–centroid distance = 3.940 Å).

Related literature

For related literature, see: Basaran et al. (1992 ); Gabe & Glusker (1971 ); Garriz et al. (2004 ); Ikeda et al. (1987 ); Kazakov (2003 ); Li et al. (2004 ); Mitchell & Iyer (1989 ); Tariq et al. (2008 ); Zhang et al. (1989 , 2007 ).

Experimental

Crystal data

C₁₂H₁₀Cl₂
M_r = 225.10
Monoclinic, P 2₁ /c
a = 13.6887 (11) Å
b = 4.5835 (3) Å
c = 17.8278 (13) Å
β = 109.666 (4)°
V = 1053.31 (13) Å³
Z = 4
Mo Kα radiation
μ = 0.57 mm⁻¹
T = 296 (2) K
0.25 × 0.08 × 0.04 mm

Data collection

Bruker Kappa APEX2 diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2005 ) T_min = 0.943, T_max = 0.974
10310 measured reflections
2073 independent reflections
1220 reflections with I > 2σ(I)
R_int = 0.049

Refinement

R[F² > 2σ(F²)] = 0.053
wR(F²) = 0.167
S = 1.05
2073 reflections
127 parameters
H-atom parameters constrained
Δρ_max = 0.79 e Å⁻³
Δρ_min = −0.28 e Å⁻³

Data collection: APEX2 (Bruker, 2007 ); cell refinement: APEX2; 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 for Windows (Farrugia, 1997 ) and PLATON (Spek, 2003 ); software used to prepare material for publication: WinGX (Farrugia, 1999 ) and PLATON.

Supporting information

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808022757/gk2159sup1.cif

Structure factors: contains datablock I. DOI: 10.1107/S1600536808022757/gk2159Isup2.hkl

checkCIF report

Comment top

Naphthalene acetic acid (NAA) is well known growth regulator/stimulator for different varieties of fruits and vegetables (Garriz et al., 2004; Li et al., 2004). Its synthesis has developed a great interest among the chemists and several methods have been reported. One of them is chloromethylation of naphthalene using methylene chloride in the presence of catalysts (Kazakov, 2003; Mitchell & Iyer, 1989; Zhang et al., 1989). During the synthesis of NAA, using formaline and a mixture of acids as a source of insertion of methylene group (Ikeda et al., 1987; Tariq et al., 2008), the title compound has been isolated.

The crystal structures of 1,4-bis(bromomethyl)benzene (Zhang et al., 2007), 1,4-bis(chloromethyl)benzene (Basaran et al., 1992) and 9,10-bis(chloromethyl)anthracene (Gabe & Glusker, 1971) were published but no analogous derivatives of naphthalene have been reported.

The bond lengths in the naphthalene system are in the range of 1.344 (6)–1.425 (5) Å. The Cl atoms deviate in opposite directions from the plane of the naphthalene ring by 1.660 (6) Å and 1.559 (6) Å. The closest contacts of Cl atoms with neighbouring molecules are: 3.491 (5) Å for Cl1···C9ⁱ and 3.5581 (16) Å for Cl2···Cl2ⁱⁱ [symmetry codes: (i) -x, 1 - y, -z; (ii) 1 - x, 1 - y, 1 - z].

Related literature top

For related literature, see: Basaran et al. (1992); Gabe & Glusker (1971); Garriz et al. (2004); Ikeda et al. (1987); Kazakov (2003); Li et al. (2004); Mitchell & Iyer (1989); Tariq et al. (2008); Zhang et al. (1989, 2007).

Experimental top

A mixture of naphthalene (40.0 g), paraformaldehyde (35.0 g), glacial acetic acid (82.0 ml), H₃PO₄ (52.0 ml) and concentrated HCl (114.0 ml) was heated in a water bath at 358 K with vigorous stirring for 2 h. Thereafter, the mixture was cooled to room temperature. A solid product was obtained and isolated. It was thoroughly washed with water, ether and n-hexane, respectively in order to remove unreacted material. The product was further purified in hot methanol. Needle-shaped colorless crystals (m.p. 394-396 K) were obtained by recrystallization from ethyl acetate.

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: APEX2 (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 for Windows (Farrugia, 1997) and PLATON (Spek, 2003); software used to prepare material for publication: WinGX (Farrugia, 1999) and PLATON (Spek, 2003).

Figures top

	Fig. 1. The ORTEP diagram of the title compound with displacement ellipsoids at the 50% probability level. H-atoms are shown by small circles of arbitrary radii.
	Fig. 2. The crystal packing diagram.

1,4-Bis(chloromethyl)naphthalene top

Crystal data top

C₁₂H₁₀Cl₂	F(000) = 464
M_r = 225.10	D_x = 1.419 Mg m⁻³
Monoclinic, P2₁/c	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc	Cell parameters from 2073 reflections
a = 13.6887 (11) Å	θ = 1.6–26.0°
b = 4.5835 (3) Å	µ = 0.57 mm⁻¹
c = 17.8278 (13) Å	T = 296 K
β = 109.666 (4)°	Needle, colourless
V = 1053.31 (13) Å³	0.25 × 0.08 × 0.04 mm
Z = 4

Data collection top

Bruker Kappa APEX2 diffractometer	2073 independent reflections
Radiation source: fine-focus sealed tube	1220 reflections with I > 2σ(I)
Graphite monochromator	R_int = 0.049
Detector resolution: 7.40 pixels mm^-1	θ_max = 26.0°, θ_min = 1.6°
ω scans	h = −16→16
Absorption correction: multi-scan (SADABS; Bruker, 2005)	k = −5→5
T_min = 0.943, T_max = 0.974	l = −21→21
10310 measured reflections

Refinement top

Refinement on F²	Primary atom site location: structure-invariant direct methods
Least-squares matrix: full	Secondary atom site location: difference Fourier map
R[F² > 2σ(F²)] = 0.053	Hydrogen site location: inferred from neighbouring sites
wR(F²) = 0.167	H-atom parameters constrained
S = 1.05	w = 1/[σ²(F_o²) + (0.0763P)² + 0.5487P] where P = (F_o² + 2F_c²)/3
2073 reflections	(Δ/σ)_max < 0.001
127 parameters	Δρ_max = 0.79 e Å⁻³
0 restraints	Δρ_min = −0.28 e Å⁻³

Crystal data top

C₁₂H₁₀Cl₂	V = 1053.31 (13) Å³
M_r = 225.10	Z = 4
Monoclinic, P2₁/c	Mo Kα radiation
a = 13.6887 (11) Å	µ = 0.57 mm⁻¹
b = 4.5835 (3) Å	T = 296 K
c = 17.8278 (13) Å	0.25 × 0.08 × 0.04 mm
β = 109.666 (4)°

Data collection top

Bruker Kappa APEX2 diffractometer	2073 independent reflections
Absorption correction: multi-scan (SADABS; Bruker, 2005)	1220 reflections with I > 2σ(I)
T_min = 0.943, T_max = 0.974	R_int = 0.049
10310 measured reflections

Refinement top

R[F² > 2σ(F²)] = 0.053	0 restraints
wR(F²) = 0.167	H-atom parameters constrained
S = 1.05	Δρ_max = 0.79 e Å⁻³
2073 reflections	Δρ_min = −0.28 e Å⁻³
127 parameters

Special details top

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 esds 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

	x	y	z	U_iso*/U_eq
Cl1	0.15383 (10)	0.5096 (3)	−0.06255 (6)	0.0825 (5)
Cl2	0.41801 (9)	0.6216 (3)	0.40488 (6)	0.0694 (4)
C1	0.2211 (3)	0.3836 (7)	0.1364 (2)	0.0438 (11)
C2	0.2846 (3)	0.4596 (8)	0.0908 (2)	0.0479 (12)
C3	0.3638 (3)	0.6492 (9)	0.1214 (2)	0.0566 (14)
C4	0.3843 (3)	0.7720 (8)	0.1975 (3)	0.0572 (14)
C5	0.3249 (3)	0.7058 (7)	0.2432 (2)	0.0472 (11)
C6	0.2416 (3)	0.5067 (7)	0.2133 (2)	0.0428 (11)
C7	0.1764 (3)	0.4271 (8)	0.2572 (2)	0.0537 (12)
C8	0.0976 (3)	0.2349 (10)	0.2267 (3)	0.0635 (16)
C9	0.0776 (3)	0.1120 (9)	0.1520 (3)	0.0642 (16)
C10	0.1366 (3)	0.1849 (8)	0.1080 (2)	0.0546 (12)
C11	0.2650 (3)	0.3370 (10)	0.0095 (2)	0.0681 (17)
C12	0.3470 (3)	0.8534 (9)	0.3220 (2)	0.0631 (16)
H3	0.40549	0.69924	0.09161	0.0680*
H4	0.43949	0.90101	0.21711	0.0681*
H7	0.18769	0.50745	0.30737	0.0642*
H8	0.05609	0.18432	0.25656	0.0759*
H9	0.02356	−0.02056	0.13242	0.0771*
H10	0.12179	0.10348	0.05762	0.0655*
H11A	0.25290	0.12868	0.01017	0.0818*
H11B	0.32575	0.36693	−0.00605	0.0818*
H12A	0.28193	0.91087	0.32822	0.0755*
H12B	0.38692	1.02904	0.32298	0.0755*

Atomic displacement parameters (Å²) top

	U¹¹	U²²	U³³	U¹²	U¹³	U²³
Cl1	0.0917 (9)	0.0956 (9)	0.0466 (7)	0.0066 (7)	0.0055 (6)	0.0041 (6)
Cl2	0.0783 (8)	0.0692 (7)	0.0492 (6)	0.0150 (5)	0.0065 (5)	0.0007 (5)
C1	0.043 (2)	0.0421 (18)	0.042 (2)	0.0109 (16)	0.0085 (16)	0.0062 (16)
C2	0.050 (2)	0.050 (2)	0.043 (2)	0.0115 (18)	0.0149 (17)	0.0073 (17)
C3	0.053 (2)	0.064 (2)	0.055 (3)	0.005 (2)	0.021 (2)	0.015 (2)
C4	0.048 (2)	0.049 (2)	0.064 (3)	−0.0019 (18)	0.005 (2)	0.010 (2)
C5	0.053 (2)	0.0411 (19)	0.041 (2)	0.0119 (17)	0.0071 (18)	0.0081 (16)
C6	0.041 (2)	0.0400 (18)	0.044 (2)	0.0095 (16)	0.0097 (16)	0.0065 (16)
C7	0.052 (2)	0.058 (2)	0.051 (2)	0.0138 (19)	0.0173 (19)	0.0106 (18)
C8	0.051 (2)	0.069 (3)	0.075 (3)	0.009 (2)	0.027 (2)	0.020 (2)
C9	0.054 (3)	0.061 (2)	0.070 (3)	−0.005 (2)	0.011 (2)	0.011 (2)
C10	0.056 (2)	0.051 (2)	0.049 (2)	0.0012 (18)	0.0074 (19)	0.0033 (18)
C11	0.079 (3)	0.072 (3)	0.055 (3)	0.014 (2)	0.025 (2)	0.004 (2)
C12	0.072 (3)	0.049 (2)	0.057 (3)	0.010 (2)	0.007 (2)	−0.0009 (19)

Geometric parameters (Å, º) top

Cl1—C11	1.810 (4)	C8—C9	1.386 (7)
Cl2—C12	1.814 (4)	C9—C10	1.344 (6)
C1—C2	1.419 (6)	C3—H3	0.9300
C1—C6	1.421 (5)	C4—H4	0.9300
C1—C10	1.425 (5)	C7—H7	0.9300
C2—C3	1.353 (6)	C8—H8	0.9300
C2—C11	1.492 (5)	C9—H9	0.9300
C3—C4	1.407 (6)	C10—H10	0.9300
C4—C5	1.365 (6)	C11—H11A	0.9700
C5—C6	1.417 (5)	C11—H11B	0.9700
C5—C12	1.496 (5)	C12—H12A	0.9700
C6—C7	1.419 (6)	C12—H12B	0.9700
C7—C8	1.357 (6)

Cl1···C10	3.464 (4)	C10···H11A	2.7400
Cl1···C9ⁱ	3.491 (5)	C11···H10	2.6200
Cl2···Cl2ⁱⁱ	3.5581 (16)	C12···H7	2.6400
Cl2···C7	3.578 (4)	H3···H11B	2.2900
Cl1···H12Aⁱⁱⁱ	3.0500	H3···Cl2^viii	3.0800
Cl1···H10	2.9800	H4···H12B	2.3100
Cl2···H12B^iv	3.0400	H4···C4^viii	2.9200
Cl2···H3^v	3.0800	H7···Cl2	3.0900
Cl2···H7	3.0900	H7···C12	2.6400
C1···C4^iv	3.521 (5)	H7···H12A	2.2100
C4···C1^vi	3.521 (5)	H8···C8^ix	3.0300
C6···C9^vi	3.504 (6)	H10···Cl1	2.9800
C6···C12^iv	3.595 (5)	H10···C11	2.6200
C7···Cl2	3.578 (4)	H10···H11A	2.2300
C7···C12^iv	3.448 (6)	H11A···C3^iv	3.0100
C9···C6^iv	3.504 (6)	H11A···C10	2.7400
C9···Cl1ⁱ	3.491 (5)	H11A···H10	2.2300
C10···Cl1	3.464 (4)	H11B···H3	2.2900
C12···C7^vi	3.448 (6)	H12A···C7	2.7200
C12···C6^vi	3.595 (5)	H12A···C7^vi	2.8400
C3···H11A^vi	3.0100	H12A···C8^vi	2.9600
C4···H4^v	2.9200	H12A···H7	2.2100
C7···H12A	2.7200	H12A···Cl1^x	3.0500
C7···H12A^iv	2.8400	H12B···Cl2^vi	3.0400
C8···H8^vii	3.0300	H12B···H4	2.3100
C8···H12A^iv	2.9600

C2—C1—C6	119.7 (3)	C4—C3—H3	119.00
C2—C1—C10	122.3 (3)	C3—C4—H4	119.00
C6—C1—C10	118.0 (3)	C5—C4—H4	119.00
C1—C2—C3	119.3 (3)	C6—C7—H7	120.00
C1—C2—C11	121.3 (3)	C8—C7—H7	120.00
C3—C2—C11	119.4 (4)	C7—C8—H8	119.00
C2—C3—C4	121.2 (4)	C9—C8—H8	119.00
C3—C4—C5	121.4 (4)	C8—C9—H9	120.00
C4—C5—C6	119.0 (3)	C10—C9—H9	120.00
C4—C5—C12	119.2 (4)	C1—C10—H10	119.00
C6—C5—C12	121.8 (4)	C9—C10—H10	119.00
C1—C6—C5	119.4 (4)	Cl1—C11—H11A	109.00
C1—C6—C7	118.3 (3)	Cl1—C11—H11B	109.00
C5—C6—C7	122.3 (3)	C2—C11—H11A	110.00
C6—C7—C8	120.6 (3)	C2—C11—H11B	109.00
C7—C8—C9	121.5 (4)	H11A—C11—H11B	108.00
C8—C9—C10	119.8 (4)	Cl2—C12—H12A	109.00
C1—C10—C9	121.8 (3)	Cl2—C12—H12B	109.00
Cl1—C11—C2	111.0 (3)	C5—C12—H12A	109.00
Cl2—C12—C5	112.6 (3)	C5—C12—H12B	109.00
C2—C3—H3	119.00	H12A—C12—H12B	108.00

C6—C1—C2—C3	−0.1 (5)	C2—C3—C4—C5	−0.3 (6)
C6—C1—C2—C11	−179.5 (3)	C3—C4—C5—C6	0.7 (6)
C10—C1—C2—C3	−179.8 (4)	C3—C4—C5—C12	−177.1 (4)
C10—C1—C2—C11	0.8 (6)	C4—C5—C6—C1	−0.7 (5)
C2—C1—C6—C5	0.5 (5)	C4—C5—C6—C7	−180.0 (4)
C2—C1—C6—C7	179.8 (3)	C12—C5—C6—C1	177.0 (3)
C10—C1—C6—C5	−179.8 (3)	C12—C5—C6—C7	−2.3 (5)
C10—C1—C6—C7	−0.5 (5)	C4—C5—C12—Cl2	−101.9 (4)
C2—C1—C10—C9	179.3 (4)	C6—C5—C12—Cl2	80.4 (4)
C6—C1—C10—C9	−0.4 (6)	C1—C6—C7—C8	1.0 (6)
C1—C2—C3—C4	0.0 (6)	C5—C6—C7—C8	−179.8 (4)
C11—C2—C3—C4	179.4 (4)	C6—C7—C8—C9	−0.5 (6)
C1—C2—C11—Cl1	75.3 (4)	C7—C8—C9—C10	−0.5 (7)
C3—C2—C11—Cl1	−104.1 (4)	C8—C9—C10—C1	1.0 (6)

Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y+1, −z+1; (iii) x, −y+3/2, z−1/2; (iv) x, y−1, z; (v) −x+1, y−1/2, −z+1/2; (vi) x, y+1, z; (vii) −x, y+1/2, −z+1/2; (viii) −x+1, y+1/2, −z+1/2; (ix) −x, y−1/2, −z+1/2; (x) x, −y+3/2, z+1/2.

Experimental details

Crystal data
Chemical formula	C₁₂H₁₀Cl₂
M_r	225.10
Crystal system, space group	Monoclinic, P2₁/c
Temperature (K)	296
a, b, c (Å)	13.6887 (11), 4.5835 (3), 17.8278 (13)
β (°)	109.666 (4)
V (Å³)	1053.31 (13)
Z	4
Radiation type	Mo Kα
µ (mm⁻¹)	0.57
Crystal size (mm)	0.25 × 0.08 × 0.04

Data collection
Diffractometer	Bruker Kappa APEX2 diffractometer
Absorption correction	Multi-scan (SADABS; Bruker, 2005)
T_min, T_max	0.943, 0.974
No. of measured, independent and observed [I > 2σ(I)] reflections	10310, 2073, 1220
R_int	0.049
(sin θ/λ)_max (Å⁻¹)	0.617

Refinement
R[F² > 2σ(F²)], wR(F²), S	0.053, 0.167, 1.05
No. of reflections	2073
No. of parameters	127
H-atom treatment	H-atom parameters constrained
Δρ_max, Δρ_min (e Å⁻³)	0.79, −0.28

Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2003), WinGX (Farrugia, 1999) and PLATON (Spek, 2003).

Acknowledgements

The authors acknowledge the Higher Education Commission, Islamabad, Pakistan, for funding the purchase of the diffractometer at GCU, Lahore.

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