supplementary materials


Acta Cryst. (2008). E64, o2300    [ doi:10.1107/S1600536808036076 ]

2-Chloro-4-iodoaniline

Y.-H. Xu, C. Wang and F. Qu

Abstract top

The title dihaloaniline, C6H5ClIN, shows no significant hydrogen bonds nor the commonly observed I...I interactions in the crystal structure, although an amino group and an I atom are available for such contacts. The crystal structure is stabilized by weak interactions involving the amine functionality as donor group and N or halogen atoms as acceptors.

Comment top

Although structurally simple and readily available, few crystal structures of dihaloanilines have been measured. A total of 10 structures were found in the 2007 CSD; the refcodes are CAJWEQ, CAJWEQ01 (Goubitz et al., 2001), DCHLAN, DCHLAN01 (Sakurai et al., 1963), KUMTER (Cox, 2001), WEMDAT, WEMDEX, WEMDIB, WEMDOH, WEMDUN (Dou et al., 1993). 2-Chloro-4-iodoaniline, (I), an aniline with two different halogen substituents, was first synthesized 90 years ago (Dains et al., 1918), yet its crystal structure is reported here for the first time.

The asymmetric unit contains one molecule (Fig. 1). The N atom is not coplanar with the aromatic ring; H atoms of the amino group are also out of the halogenated benzene ring, but in the opposite direction to that of the N atom. So, the C(Ar)NH2 group has a pyramidal shape. This is similar to the structure of aniline at 252 K (Fukuyo et al., 1982), 2-iodoaniline at 100 K (Parkin et al., 2005) and 4-iodoaniline at 203 K (Dey et al., 2003).

Despite the presence of amino, chloro and iodo groups, no classic interactions associated with them, such as hydrogen bonds, Cl···Cl, or I···I contacts were observed in the crystal structure of (I). Instead, weak interactions such as N—H···N, N—H···I, and N—H···Cl are found to provide stability to the crystal (Fig. 2).

Related literature top

The title compound was first synthesized 90 years ago (Dains et al., 1918). For structures of halogenated anilines, see: Cox (2001); Dey et al. (2003); Dou et al. (1993); Fukuyo et al. (1982); Goubitz et al. (2001); Parkin et al. (2005); Sakurai et al. (1963).

Experimental top

The compound was purchased from TCI America Laboratory Chemicals as colorless block crystals suitable for single-crystal X-ray diffraction measurement.

Refinement top

H atoms were found in a difference map and those on the aromatic ring subsequently placed in idealized positions with C—H distances of 0.95 Å and isotropic displacement parameters equal to 1.2Ueq of the carrier C atom. Amine H atoms H1N and H2N were refined freely but were restrained to converge to the same N—H bond lengths, with a standard deviation of 0.02 Å. Isotropic displacement parameters for H1N and H2N were computed as 1.5Ueq(N1)

Computing details top

Data collection: COLLECT (Nonius, 2002); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and local procedures.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), with displacement ellipsoids drawn at the 50% probability level (arbitrary spheres for the H atoms).
[Figure 2] Fig. 2. A packing diagram of (I) down the a axis.
2-Chloro-4-iodoaniline top
Crystal data top
C6H5ClINF(000) = 472
Mr = 253.46Dx = 2.282 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 1019 reflections
a = 5.6277 (2) Åθ = 1.0–27.5°
b = 8.7859 (3) ŵ = 4.61 mm1
c = 14.9217 (5) ÅT = 90 K
V = 737.79 (4) Å3Rounded block, colourless
Z = 40.22 × 0.15 × 0.10 mm
Data collection top
Nonius KappaCCD
diffractometer
1696 independent reflections
Radiation source: fine-focus sealed tube1587 reflections with I > 2σ(I)
graphiteRint = 0.033
Detector resolution: 18 pixels mm-1θmax = 27.5°, θmin = 2.7°
ω scans at fixed χ = 55°h = 77
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
k = 1111
Tmin = 0.424, Tmax = 0.630l = 1919
5635 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.024 w = 1/[σ2(Fo2) + (0.P)2 + 0.4678P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.046(Δ/σ)max = 0.001
S = 1.14Δρmax = 1.18 e Å3
1696 reflectionsΔρmin = 0.76 e Å3
89 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
1 restraintExtinction coefficient: 0.0021 (3)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), 681 Friedel pairs
Secondary atom site location: difference Fourier mapFlack parameter: 0.03 (3)
Crystal data top
C6H5ClINV = 737.79 (4) Å3
Mr = 253.46Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 5.6277 (2) ŵ = 4.61 mm1
b = 8.7859 (3) ÅT = 90 K
c = 14.9217 (5) Å0.22 × 0.15 × 0.10 mm
Data collection top
Nonius KappaCCD
diffractometer
1696 independent reflections
Absorption correction: multi-scan
(SCALEPACK; Otwinowski & Minor, 1997)
1587 reflections with I > 2σ(I)
Tmin = 0.424, Tmax = 0.630Rint = 0.033
5635 measured reflectionsθmax = 27.5°
Refinement top
R[F2 > 2σ(F2)] = 0.024H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.046Δρmax = 1.18 e Å3
S = 1.14Δρmin = 0.76 e Å3
1696 reflectionsAbsolute structure: Flack (1983), 681 Friedel pairs
89 parametersFlack parameter: 0.03 (3)
1 restraint
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.48590 (4)0.17882 (2)0.730162 (15)0.01928 (9)
Cl10.46148 (17)0.51349 (10)0.40305 (6)0.0194 (2)
N10.9067 (6)0.6647 (5)0.4646 (2)0.0188 (8)
H1N1.048 (5)0.679 (5)0.474 (3)0.028*
H2N0.882 (7)0.656 (5)0.411 (2)0.028*
C10.6370 (6)0.3328 (4)0.6386 (2)0.0133 (7)
C20.5194 (7)0.3639 (3)0.5594 (2)0.0138 (7)
H20.37640.31210.54480.017*
C30.6128 (6)0.4711 (4)0.5018 (2)0.0145 (8)
C40.8253 (6)0.5480 (4)0.5199 (3)0.0152 (8)
C50.9422 (6)0.5117 (4)0.5999 (2)0.0166 (8)
H51.08750.56110.61420.020*
C60.8494 (7)0.4049 (4)0.6588 (3)0.0163 (8)
H60.93120.38120.71270.020*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.02354 (13)0.01764 (13)0.01666 (14)0.00271 (12)0.00379 (13)0.00106 (9)
Cl10.0189 (5)0.0231 (4)0.0163 (4)0.0003 (4)0.0036 (4)0.0007 (3)
N10.0163 (16)0.0192 (18)0.0208 (18)0.0046 (15)0.0035 (15)0.0025 (15)
C10.0136 (16)0.0101 (17)0.0161 (19)0.0001 (15)0.0027 (15)0.0029 (16)
C20.0142 (18)0.0107 (15)0.0165 (17)0.0005 (16)0.003 (2)0.0046 (13)
C30.0134 (18)0.0133 (17)0.0169 (19)0.0020 (16)0.0006 (16)0.0017 (16)
C40.0121 (18)0.0129 (18)0.020 (2)0.0043 (15)0.0034 (16)0.0031 (17)
C50.0096 (18)0.0154 (17)0.025 (2)0.0007 (14)0.0002 (16)0.0053 (15)
C60.0172 (19)0.0182 (19)0.0133 (18)0.0019 (16)0.0003 (16)0.0034 (16)
Geometric parameters (Å, °) top
I1—C12.103 (4)C2—C31.379 (5)
Cl1—C31.742 (4)C2—H20.9500
N1—C41.394 (5)C3—C41.400 (5)
N1—H1N0.82 (3)C4—C51.400 (5)
N1—H2N0.81 (3)C5—C61.387 (5)
C1—C21.382 (5)C5—H50.9500
C1—C61.386 (5)C6—H60.9500
C4—N1—H1N110 (3)C4—C3—Cl1118.6 (3)
C4—N1—H2N117 (3)N1—C4—C5121.2 (3)
H1N—N1—H2N110 (5)N1—C4—C3121.4 (3)
C2—C1—C6120.6 (3)C5—C4—C3117.2 (3)
C2—C1—I1119.3 (3)C6—C5—C4121.1 (3)
C6—C1—I1120.1 (3)C6—C5—H5119.4
C3—C2—C1119.0 (3)C4—C5—H5119.4
C3—C2—H2120.5C1—C6—C5119.7 (3)
C1—C2—H2120.5C1—C6—H6120.1
C2—C3—C4122.3 (3)C5—C6—H6120.1
C2—C3—Cl1119.1 (3)
C6—C1—C2—C31.9 (5)Cl1—C3—C4—C5179.8 (3)
I1—C1—C2—C3176.5 (2)N1—C4—C5—C6174.2 (3)
C1—C2—C3—C41.2 (5)C3—C4—C5—C60.5 (5)
C1—C2—C3—Cl1178.6 (3)C2—C1—C6—C51.5 (5)
C2—C3—C4—N1174.7 (3)I1—C1—C6—C5176.9 (2)
Cl1—C3—C4—N15.1 (5)C4—C5—C6—C10.3 (5)
C2—C3—C4—C50.0 (5)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1N···N1i0.82 (3)2.61 (3)3.359 (4)153 (4)
N1—H1N···Cl1ii0.82 (3)2.94 (4)3.515 (4)129 (4)
N1—H2N···I1iii0.81 (3)3.16 (3)3.807 (4)139 (4)
Symmetry codes: (i) x+1/2, −y+3/2, −z+1; (ii) x+1, y, z; (iii) −x+3/2, −y+1, z−1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1N···N1i0.82 (3)2.61 (3)3.359 (4)153 (4)
N1—H1N···Cl1ii0.82 (3)2.94 (4)3.515 (4)129 (4)
N1—H2N···I1iii0.81 (3)3.16 (3)3.807 (4)139 (4)
Symmetry codes: (i) x+1/2, −y+3/2, −z+1; (ii) x+1, y, z; (iii) −x+3/2, −y+1, z−1/2.
Acknowledgements top

Y-HX thanks Dr Sihui Long for helpful discussions and invaluable suggestions.

references
References top

Cox, P. J. (2001). Acta Cryst. E57, o1203–o1205.

Dains, F. B., Vaughan, T. H. & Janney, W. M. (1918). J. Am. Chem. Soc. 40, 930–936.

Dey, A., Jetti, R. K. R., Boese, R. & Desiraju, G. R. (2003). CrystEngComm, 5, 248–252.

Dou, S. Q., Weiden, N. & Weiss, A. (1993). Acta Chim. Hung. 130, 497–522.

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

Fukuyo, M., Hirotsu, K. & Higuchi, T. (1982). Acta Cryst. B38, 640–643.

Goubitz, K., Sonneveld, E. J. & Schenk, H. (2001). Z. Kristallogr. 216, 176–181.

Nonius (2002). COLLECT. Nonius BV, Delft, The Netherlands.

Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.

Parkin, A., Spanswick, C. K., Pulham, C. R. & Wilson, C. C. (2005). Acta Cryst. E61, o1087–o1089.

Sakurai, T., Sundaralingam, M. & Jeffrey, G. A. (1963). Acta Cryst. 16, 354–363.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.