organic compounds
2,4-Diiodoaniline
aSchool of Physical and Chemical Sciences, Queensland University of Technology, GPO Box 2434, Brisbane, Qld 4001, Australia
*Correspondence e-mail: g.smith@qut.edu.au
The structure of the title compound, C6H5I2N, shows a weak intermolecular amine–amine N—H⋯N hydrogen-bonding interaction, giving a helical chain which extends along the a axis. An intramolecular N—H⋯I hydrogen bond is also observed.
Related literature
For related structures, see: Garden et al. (2002). For the synthesis, see: Dains et al. (1935); Hodgson & Marsden (1937); O'Neil (2001). For graph-set analysis of hydrogen bonding, see: Etter et al. (1990).
Experimental
Crystal data
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Data collection: CrysAlis CCD (Oxford Diffraction, 2008); cell CrysAlis RED (Oxford Diffraction, 2008); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008) within WinGX (Farrugia, 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008) within WinGX (Farrugia, 1999); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: PLATON.
Supporting information
10.1107/S1600536809030438/is2440sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809030438/is2440Isup2.hkl
The title compound was formed in the attempted synthesis of a proton-transfer salt of 4,5-dichlorophthalic acid with 4-iodoaniline by heating together under reflux for 10 minutes 1 mmol quantities of the two reagents in 50 ml of 50% ethanol-water. After concentration to ca 30 ml, partial room temperature evaporation of the hot-filtered solution gave colourless needle prisms of 2,4-diiodoaniline [m.p. 368–389 K (O'Neil, 2001)] as the major product. This conversion of 4-iodoaniline to 2,4-diiodoaniline in the solid state has been reported previously (Dains et al., 1935).
The hydrogen atoms of the amino group were located in a difference Fourier map and their positional and isotropic displacement parameters were refined freely. Other H-atoms were included in the
in calculated positions [C—H = 0.93 Å) and treated using a riding model approximation, with Uiso(H) = 1.2Ueq(C).Data collection: CrysAlis CCD (Oxford Diffraction, 2008); cell
CrysAlis RED (Oxford Diffraction, 2008); data reduction: CrysAlis RED (Oxford Diffraction, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008) within WinGX (Farrugia, 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008) within WinGX (Farrugia, 1999); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: PLATON (Spek, 2009).C6H5I2N | Dx = 2.806 Mg m−3 |
Mr = 344.91 | Melting point = 368–369 K |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 5620 reflections |
a = 4.3870 (1) Å | θ = 3.0–32.2° |
b = 10.9626 (3) Å | µ = 7.62 mm−1 |
c = 16.9778 (4) Å | T = 200 K |
V = 816.51 (3) Å3 | Needle, colourless |
Z = 4 | 0.30 × 0.18 × 0.18 mm |
F(000) = 616 |
Oxford Diffraction Gemini-S Ultra CCD-detector diffractometer | 1873 independent reflections |
Radiation source: Enhance (Mo) X-ray tube | 1790 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.024 |
ω scans | θmax = 27.5°, θmin = 3.0° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −5→5 |
Tmin = 0.146, Tmax = 0.250 | k = −13→14 |
6739 measured reflections | l = −22→18 |
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)] = 0.018 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.038 | w = 1/[σ2(Fo2) + (0.0207P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.05 | (Δ/σ)max = 0.003 |
1873 reflections | Δρmax = 0.38 e Å−3 |
90 parameters | Δρmin = −0.47 e Å−3 |
0 restraints | Absolute structure: Flack (1983), 737 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: −0.03 (4) |
C6H5I2N | V = 816.51 (3) Å3 |
Mr = 344.91 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 4.3870 (1) Å | µ = 7.62 mm−1 |
b = 10.9626 (3) Å | T = 200 K |
c = 16.9778 (4) Å | 0.30 × 0.18 × 0.18 mm |
Oxford Diffraction Gemini-S Ultra CCD-detector diffractometer | 1873 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1790 reflections with I > 2σ(I) |
Tmin = 0.146, Tmax = 0.250 | Rint = 0.024 |
6739 measured reflections |
R[F2 > 2σ(F2)] = 0.018 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.038 | Δρmax = 0.38 e Å−3 |
S = 1.05 | Δρmin = −0.47 e Å−3 |
1873 reflections | Absolute structure: Flack (1983), 737 Friedel pairs |
90 parameters | Absolute structure parameter: −0.03 (4) |
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 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. |
x | y | z | Uiso*/Ueq | ||
I2 | 0.57888 (5) | 0.42657 (2) | 1.08868 (1) | 0.0293 (1) | |
I4 | 0.48489 (5) | 0.28546 (2) | 0.75021 (1) | 0.0330 (1) | |
N1 | 0.1721 (9) | 0.6552 (3) | 1.0212 (2) | 0.0291 (11) | |
C1 | 0.2299 (7) | 0.5690 (3) | 0.9630 (2) | 0.0218 (9) | |
C2 | 0.4096 (8) | 0.4658 (3) | 0.97570 (19) | 0.0221 (9) | |
C3 | 0.4807 (8) | 0.3859 (3) | 0.9156 (2) | 0.0247 (9) | |
C4 | 0.3689 (8) | 0.4074 (3) | 0.8407 (2) | 0.0235 (10) | |
C5 | 0.1876 (8) | 0.5075 (3) | 0.8256 (2) | 0.0260 (11) | |
C6 | 0.1216 (9) | 0.5877 (3) | 0.8865 (2) | 0.0278 (11) | |
H3 | 0.60280 | 0.31820 | 0.92530 | 0.0300* | |
H5 | 0.11070 | 0.52100 | 0.77530 | 0.0310* | |
H6 | 0.00190 | 0.65580 | 0.87610 | 0.0330* | |
H11 | 0.190 (8) | 0.626 (3) | 1.062 (2) | 0.038 (9)* | |
H12 | 0.043 (8) | 0.704 (4) | 1.010 (2) | 0.040 (9)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
I2 | 0.0335 (1) | 0.0341 (1) | 0.0202 (1) | 0.0009 (1) | −0.0038 (1) | 0.0021 (1) |
I4 | 0.0383 (1) | 0.0389 (1) | 0.0219 (1) | 0.0022 (1) | 0.0017 (1) | −0.0069 (1) |
N1 | 0.037 (2) | 0.0222 (16) | 0.028 (2) | 0.0055 (15) | −0.0021 (16) | 0.0013 (15) |
C1 | 0.0214 (15) | 0.0191 (16) | 0.0248 (18) | −0.0039 (15) | 0.0014 (14) | 0.0021 (14) |
C2 | 0.0251 (16) | 0.0226 (16) | 0.0186 (17) | −0.0034 (15) | −0.0009 (14) | 0.0032 (11) |
C3 | 0.0289 (18) | 0.0218 (14) | 0.0234 (17) | −0.0007 (11) | −0.0010 (16) | 0.0015 (12) |
C4 | 0.0252 (17) | 0.0226 (18) | 0.0228 (18) | −0.0031 (13) | 0.0028 (14) | −0.0029 (13) |
C5 | 0.027 (2) | 0.0313 (19) | 0.0197 (19) | −0.0028 (14) | −0.0018 (15) | 0.0044 (14) |
C6 | 0.0323 (19) | 0.0236 (18) | 0.0276 (19) | 0.0028 (15) | 0.0007 (15) | 0.0051 (13) |
I2—C2 | 2.101 (3) | C2—C3 | 1.381 (5) |
I4—C4 | 2.099 (3) | C3—C4 | 1.383 (5) |
N1—C1 | 1.391 (5) | C4—C5 | 1.379 (5) |
N1—H12 | 0.80 (4) | C5—C6 | 1.388 (5) |
N1—H11 | 0.77 (3) | C3—H3 | 0.9300 |
C1—C6 | 1.398 (5) | C5—H5 | 0.9300 |
C1—C2 | 1.396 (5) | C6—H6 | 0.9300 |
H11—N1—H12 | 124 (4) | I4—C4—C3 | 118.6 (2) |
C1—N1—H11 | 110 (3) | C3—C4—C5 | 120.7 (3) |
C1—N1—H12 | 114 (3) | C4—C5—C6 | 119.1 (3) |
N1—C1—C6 | 119.9 (3) | C1—C6—C5 | 121.9 (3) |
N1—C1—C2 | 123.0 (3) | C2—C3—H3 | 120.00 |
C2—C1—C6 | 117.0 (3) | C4—C3—H3 | 120.00 |
I2—C2—C1 | 120.4 (2) | C4—C5—H5 | 120.00 |
I2—C2—C3 | 117.7 (2) | C6—C5—H5 | 121.00 |
C1—C2—C3 | 121.9 (3) | C1—C6—H6 | 119.00 |
C2—C3—C4 | 119.4 (3) | C5—C6—H6 | 119.00 |
I4—C4—C5 | 120.7 (2) | ||
N1—C1—C2—I2 | 5.0 (5) | C1—C2—C3—C4 | −0.7 (5) |
N1—C1—C2—C3 | −175.5 (3) | C2—C3—C4—I4 | 179.3 (3) |
C6—C1—C2—I2 | −178.9 (2) | C2—C3—C4—C5 | 0.0 (5) |
C6—C1—C2—C3 | 0.6 (5) | I4—C4—C5—C6 | −178.5 (3) |
N1—C1—C6—C5 | 176.5 (3) | C3—C4—C5—C6 | 0.9 (5) |
C2—C1—C6—C5 | 0.3 (5) | C4—C5—C6—C1 | −1.0 (5) |
I2—C2—C3—C4 | 178.8 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H11···I2 | 0.77 (3) | 2.81 (3) | 3.283 (4) | 122 (3) |
N1—H12···N1i | 0.80 (4) | 2.30 (4) | 3.106 (5) | 180 (5) |
Symmetry code: (i) x−1/2, −y+3/2, −z+2. |
Experimental details
Crystal data | |
Chemical formula | C6H5I2N |
Mr | 344.91 |
Crystal system, space group | Orthorhombic, P212121 |
Temperature (K) | 200 |
a, b, c (Å) | 4.3870 (1), 10.9626 (3), 16.9778 (4) |
V (Å3) | 816.51 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 7.62 |
Crystal size (mm) | 0.30 × 0.18 × 0.18 |
Data collection | |
Diffractometer | Oxford Diffraction Gemini-S Ultra CCD-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.146, 0.250 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6739, 1873, 1790 |
Rint | 0.024 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.018, 0.038, 1.05 |
No. of reflections | 1873 |
No. of parameters | 90 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.38, −0.47 |
Absolute structure | Flack (1983), 737 Friedel pairs |
Absolute structure parameter | −0.03 (4) |
Computer programs: CrysAlis CCD (Oxford Diffraction, 2008), CrysAlis RED (Oxford Diffraction, 2008), SHELXS97 (Sheldrick, 2008) within WinGX (Farrugia, 1999), SHELXL97 (Sheldrick, 2008) within WinGX (Farrugia, 1999), PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H11···I2 | 0.77 (3) | 2.81 (3) | 3.283 (4) | 122 (3) |
N1—H12···N1i | 0.80 (4) | 2.30 (4) | 3.106 (5) | 180 (5) |
Symmetry code: (i) x−1/2, −y+3/2, −z+2. |
Acknowledgements
The authors acknowledge financial support from the Australian Research Council and the School of Physical and Chemical Sciences, Queensland University of Technology.
References
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Although the crystal structures of a number of nitro-substituted iodoanilines including 3-nitro-2,4-diodoaniline have been reported (Garden et al., 2002), that of the title compound 2,4-diiodoaniline C6H6I2N (I) has not been determined and the structure is reported here. The compound was isolated as the major crystalline product in the attempted synthesis of an adduct of 4,5-dichlorophthalic acid with 4-iodoaniline in aqueous ethanol. This conversion of 4-iodoaniline to 2,4-diiodoaniline has been reported previously (Dains et al., 1935), where solid 4-iodoaniline was observed to undergo a ca 25% conversion to the diiodo analogue in a sealed container over a period of three years. Hodgson & Marsden (1937) also reported the ready formation of the diiodo derivative along with 4-iodoaniline from the reaction of aniline with iodine.
In the structure of (I) (Fig. 1), single weak intermolecular hydrogen bonds are found [N1—H1···N1i, 3.106 (5) Å; symmetry code: (i) x - 1/2, -y + 3/2, -z + 2] [graph set S(4) (Etter et al., 1990)], linking the amine groups of 21 screw-related molecules. These form one-dimensional chains which extend down the a cell direction in the unit cell (Fig. 2).
In this structure there are, not unexpectedly, short intramoleculer N—H···I interactions [N1···I2, 3.283 (4) Å], which are also present in the structure of 2,4-diiodo-3-nitroaniline [3.254 (7) Å (Garden et al., 2002)]. However, unlike the nitro-derivative, no π–π stacking interactions are present in the structure of (I).