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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Jan 16;66(Pt 2):o360. doi: 10.1107/S1600536810001005

Dimethyl 5-amino-2,4,6-triiodo­isophthalate

Pei Zou a,*, Shi-Neng Luo a, Min-Hao Xie a, Ya-Ling Liu a, Jun Wu a
PMCID: PMC2979769  PMID: 21579785

Abstract

The title compound, C10H8I3NO4, crystallizes with two mol­ecules in the asymmetric unit. The I atoms and the benzene ring plane in the two mol­ecules are approximately coplanar, the I atoms deviating by −0.1631 (1), 0.0704 (1) and −0.0507 (1) Å from the mean plane of the benzene ring in one mol­ecule and by 0.1500 (1), −0.0034 (1) and −0.1213 (1) Å in the other. The planes of the ester groups are almost orthogonal to those of the benzene rings in both mol­ecules, forming dihedral angles of 83.5 (3), 76.4 (3), 97.3 (1) and 75.7 (1)°. The mean planes of the benzene rings in two mol­ecules are inclined at 69.8 (3)° with respect to each other. In the crystal, inter­molecular I⋯O inter­actions link the mol­ecules into infinite chains. In addition, N—H⋯O and non-classical C—H⋯O hydrogen bonds are observed.

Related literature

For general background to 1,3,5-triiodobenzene derivatives, see: Morin et al. (1987); Singh & Rathore (1980); Stacul et al. (2001); Yu & Watson (1999). For a related structure, see: Beck & Sheldrick (2008).graphic file with name e-66-0o360-scheme1.jpg

Experimental

Crystal data

  • C10H8I3NO4

  • M r = 586.87

  • Triclinic, Inline graphic

  • a = 8.4423 (17) Å

  • b = 10.3545 (19) Å

  • c = 18.365 (3) Å

  • α = 75.158 (5)°

  • β = 80.045 (5)°

  • γ = 89.728 (6)°

  • V = 1527.2 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 6.15 mm−1

  • T = 93 K

  • 0.40 × 0.33 × 0.13 mm

Data collection

  • Rigaku SPIDER diffractometer

  • Absorption correction: empirical (using intensity measurements) (North et al., 1968) T min = 0.193, T max = 0.495

  • 10344 measured reflections

  • 5251 independent reflections

  • 4488 reflections with I > 2σ(I)

  • R int = 0.036

Refinement

  • R[F 2 > 2σ(F 2)] = 0.035

  • wR(F 2) = 0.067

  • S = 0.98

  • 5251 reflections

  • 325 parameters

  • 24 restraints

  • H-atom parameters constrained

  • Δρmax = 1.10 e Å−3

  • Δρmin = −1.19 e Å−3

Data collection: RAPID-AUTO (Rigaku, 2004); cell refinement: RAPID-AUTO; data reduction: RAPID-AUTO; 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: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810001005/pv2251sup1.cif

e-66-0o360-sup1.cif (22.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810001005/pv2251Isup2.hkl

e-66-0o360-Isup2.hkl (257.1KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N1A—H1A⋯I2A 0.88 2.74 3.224 (5) 116
N1A—H1A⋯O4Bi 0.88 2.48 3.036 (7) 122
N1A—H1B⋯I3A 0.88 2.72 3.211 (5) 117
N1B—H1C⋯I2B 0.88 2.73 3.212 (5) 116
N1B—H1D⋯I3B 0.88 2.73 3.222 (5) 116
N1B—H1D⋯O2Aii 0.88 2.43 3.026 (7) 125
C8B—H8E⋯O2Biii 0.98 2.54 3.516 (9) 171
C10A—H10A⋯O2Biv 0.98 2.58 3.499 (9) 155
C10A—H10B⋯O4Av 0.98 2.54 3.519 (9) 173

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic.

Acknowledgments

The authors acknowledge financial support from the Jiangsu Institute of Nuclear Medicine.

supplementary crystallographic information

Comment

The 1,3,5-triiodobenzene core has been the basis of many contrast agents (Yu & Watson, 1999). The title compound is useful as an important intermediate for the preparation of iodinated X-ray contrast agent, such as iotalamic acid, ioxitalamic acid, and ioxilan, which are used clinically all over the world (Morin et al., 1987; Singh et al., 1980; Stacul et al., 2001). In this paper, we present the crystal structure of the title compound.

The asymmetric unit of the title compound (Fig. 1) contains two crystallographically independent molecules (A and B) in an asymmetric unit. The three I atoms deviate from the mean-planes of the phenyl rings, respectively, by -0.1631 (1), 0.0704 (1) and -0.0507 (1) Å for molecule A and 0.1500 (1), -0.0034 (1) and -0.1213 (1) Å for molecule B. Bond lengths and angles are comparable to those observed in a related structure (Beck & Sheldrick, 2008). The planes of the ester groups in both molecule are almost orthogonal to the benzene ring, as indicated by the dihedral angles of 83.5 (3)° (C10A/O3A/C9A/O4A; C1A—C6A), 76.4 (3)°(C8A/O1A/C7A/O2A; C1A—C6A), 97.3 (1)° (C10B/O3B/C9B/O4B; C1B—C6B) and 75.7 (1)° (C8B/O1B/C7B/O2B; C1B—C6B). The dihedral angle between the rings (C1A—C6A) and (C1B—C6B) is 69.8 (3)°.

In the crystal structure, intermolecular I···O interactions link the molecules into infinite one-dimensional chains (Fig. 2). In addition, C—H···O hydrogen bonds and N—H···O hydrogen bonds are observed.

Experimental

A mixture of 5-amino-2,4,6-triiodoisophthaloyl dichloride (2.97 g, 5 mmol) and methanol (15 ml) was heated under reflux for four hours to produce dimethyl 5-amino-2,4,6-triiodoisophthalate. It was recrystallized from a methanol solution by slowly evaporating the solvents to obtain crystals suitable for X-ray single-crystal diffraction.

Refinement

All H atoms were initially located from a difference Fourier map and then were regenerated at ideal positions and treated as riding, with N—H = 0.88 Å, C—H = 0.98 Å and Uiso(H) = 1.2Ueq (N), Uiso(H) = 1.5Ueq (C). The final difference map showed electron density in the vicinity of I3B atom and was deemed meaningless.

Figures

Fig. 1.

Fig. 1.

A view of the title compound with the atomic numbering scheme. Displacement ellipsoids were drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Partial view of molecular structure. Molecules are linked into infinite one dimensional chains by I···O interactions (dashed lines).

Crystal data

C10H8I3NO4 Z = 4
Mr = 586.87 F(000) = 1064
Triclinic, P1 Dx = 2.553 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.4423 (17) Å Cell parameters from 4796 reflections
b = 10.3545 (19) Å θ = 3.1–27.5°
c = 18.365 (3) Å µ = 6.15 mm1
α = 75.158 (5)° T = 93 K
β = 80.045 (5)° Chunk, colorless
γ = 89.728 (6)° 0.40 × 0.33 × 0.13 mm
V = 1527.2 (5) Å3

Data collection

Rigaku SPIDER diffractometer 5251 independent reflections
Radiation source: Rotating anode 4488 reflections with I > 2σ(I)
graphite Rint = 0.036
ω scans θmax = 25.0°, θmin = 3.1°
Absorption correction: empirical (using intensity measurements) (North et al., 1968) h = −7→10
Tmin = 0.193, Tmax = 0.495 k = −12→12
10344 measured reflections l = −21→21

Refinement

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)] = 0.035 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.067 H-atom parameters constrained
S = 0.98 w = 1/[σ2(Fo2) + (0.0226P)2] where P = (Fo2 + 2Fc2)/3
5251 reflections (Δ/σ)max = 0.001
325 parameters Δρmax = 1.10 e Å3
24 restraints Δρmin = −1.19 e Å3

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
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)

x y z Uiso*/Ueq
I1A 0.38817 (5) 0.22093 (4) 0.17667 (3) 0.01707 (12)
I2A −0.17168 (6) 0.58657 (5) 0.16991 (3) 0.02695 (14)
I3A −0.09149 (5) 0.19121 (4) 0.46691 (2) 0.01540 (11)
I1B 0.64018 (5) 0.26656 (5) 0.82446 (3) 0.02072 (12)
I2B 0.38563 (5) 0.31590 (4) 0.53036 (2) 0.01505 (11)
I3B 0.08377 (6) −0.09395 (5) 0.82042 (3) 0.02305 (13)
O1A 0.3577 (5) 0.1765 (4) 0.3694 (2) 0.0153 (11)
O2A 0.1825 (5) 0.0114 (4) 0.3694 (3) 0.0165 (11)
O3A 0.2236 (5) 0.5535 (4) 0.0837 (3) 0.0192 (11)
O4A 0.1008 (5) 0.3729 (4) 0.0665 (3) 0.0168 (11)
O1B 0.2646 (5) 0.1247 (4) 0.9244 (2) 0.0158 (11)
O2B 0.3971 (5) −0.0629 (4) 0.9177 (2) 0.0168 (11)
O3B 0.7581 (5) 0.3230 (4) 0.6314 (3) 0.0155 (11)
O4B 0.5834 (5) 0.4882 (4) 0.6325 (3) 0.0155 (11)
N1A −0.2391 (6) 0.4225 (5) 0.3477 (3) 0.0200 (14)
H1A −0.2936 0.4861 0.3225 0.024*
H1B −0.2724 0.3864 0.3968 0.024*
N1B 0.1464 (6) 0.0829 (5) 0.6453 (3) 0.0198 (14)
H1C 0.1508 0.1200 0.5961 0.024*
H1D 0.0726 0.0197 0.6698 0.024*
C1A 0.1312 (7) 0.2407 (6) 0.3123 (4) 0.0084 (14)
C2A 0.1852 (8) 0.2955 (6) 0.2348 (4) 0.0126 (15)
C3A 0.0967 (8) 0.3922 (6) 0.1933 (4) 0.0130 (15)
C4A −0.0451 (8) 0.4349 (6) 0.2320 (4) 0.0134 (15)
C5A −0.1032 (8) 0.3800 (6) 0.3106 (4) 0.0140 (15)
C6A −0.0100 (7) 0.2800 (6) 0.3494 (4) 0.0097 (14)
C7A 0.2236 (8) 0.1295 (7) 0.3534 (4) 0.0150 (15)
C8A 0.4678 (8) 0.0755 (7) 0.3980 (4) 0.0258 (19)
H8A 0.5618 0.1190 0.4079 0.039*
H8B 0.5026 0.0254 0.3599 0.039*
H8C 0.4132 0.0141 0.4457 0.039*
C9A 0.1392 (8) 0.4374 (6) 0.1075 (4) 0.0138 (15)
C10A 0.2670 (9) 0.6031 (7) 0.0006 (4) 0.0276 (19)
H10A 0.3284 0.6885 −0.0122 0.041*
H10B 0.1689 0.6162 −0.0218 0.041*
H10C 0.3327 0.5380 −0.0200 0.041*
C1B 0.3607 (8) 0.1014 (6) 0.8020 (4) 0.0139 (15)
C2B 0.4819 (7) 0.1978 (6) 0.7639 (4) 0.0129 (15)
C3B 0.4876 (8) 0.2602 (6) 0.6861 (4) 0.0140 (15)
C4B 0.3739 (7) 0.2233 (6) 0.6478 (4) 0.0128 (15)
C5B 0.2547 (8) 0.1237 (6) 0.6838 (4) 0.0160 (16)
C6B 0.2527 (7) 0.0631 (6) 0.7624 (4) 0.0138 (15)
C7B 0.3465 (7) 0.0435 (6) 0.8873 (4) 0.0124 (15)
C8B 0.2448 (9) 0.0829 (7) 1.0074 (4) 0.0273 (19)
H8D 0.1836 0.1490 1.0292 0.041*
H8E 0.3509 0.0758 1.0226 0.041*
H8F 0.1867 −0.0042 1.0264 0.041*
C9B 0.6117 (8) 0.3721 (6) 0.6468 (4) 0.0133 (15)
C10B 0.8891 (8) 0.4222 (7) 0.6051 (4) 0.0260 (18)
H10D 0.9907 0.3782 0.5952 0.039*
H10E 0.8941 0.4700 0.6444 0.039*
H10F 0.8715 0.4859 0.5578 0.039*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
I1A 0.0142 (3) 0.0210 (3) 0.0134 (3) 0.00420 (19) 0.00138 (19) −0.0023 (2)
I2A 0.0343 (3) 0.0252 (3) 0.0207 (3) 0.0188 (2) −0.0082 (2) −0.0030 (2)
I3A 0.0146 (3) 0.0179 (2) 0.0123 (2) 0.00037 (18) 0.00006 (19) −0.00286 (19)
I1B 0.0208 (3) 0.0254 (3) 0.0153 (3) −0.0088 (2) −0.0064 (2) −0.0017 (2)
I2B 0.0154 (3) 0.0171 (2) 0.0116 (2) −0.00127 (18) −0.00228 (19) −0.00199 (19)
I3B 0.0247 (3) 0.0223 (3) 0.0187 (3) −0.0151 (2) 0.0029 (2) −0.0032 (2)
O1A 0.010 (3) 0.019 (3) 0.018 (3) 0.006 (2) −0.009 (2) −0.004 (2)
O2A 0.013 (3) 0.013 (3) 0.023 (3) 0.001 (2) −0.005 (2) −0.002 (2)
O3A 0.023 (3) 0.019 (3) 0.013 (3) −0.006 (2) −0.001 (2) 0.000 (2)
O4A 0.022 (3) 0.014 (2) 0.018 (3) −0.002 (2) −0.008 (2) −0.005 (2)
O1B 0.016 (3) 0.020 (3) 0.012 (3) 0.008 (2) 0.000 (2) −0.006 (2)
O2B 0.023 (3) 0.010 (3) 0.013 (3) 0.002 (2) −0.002 (2) 0.005 (2)
O3B 0.011 (3) 0.017 (3) 0.019 (3) −0.0020 (19) 0.004 (2) −0.008 (2)
O4B 0.015 (3) 0.011 (3) 0.019 (3) 0.0012 (19) −0.003 (2) 0.000 (2)
N1A 0.021 (4) 0.022 (3) 0.014 (3) 0.015 (3) −0.003 (3) 0.000 (3)
N1B 0.020 (3) 0.024 (3) 0.015 (3) −0.012 (3) −0.003 (3) −0.004 (3)
C1A 0.005 (3) 0.010 (3) 0.011 (4) 0.000 (3) 0.001 (3) −0.003 (3)
C2A 0.016 (4) 0.010 (3) 0.014 (4) 0.001 (3) −0.006 (3) −0.005 (3)
C3A 0.013 (4) 0.007 (3) 0.020 (4) 0.001 (3) −0.005 (3) −0.006 (3)
C4A 0.013 (3) 0.011 (2) 0.016 (3) 0.004 (2) −0.005 (2) −0.003 (2)
C5A 0.017 (4) 0.013 (4) 0.013 (4) 0.003 (3) −0.001 (3) −0.006 (3)
C6A 0.011 (2) 0.007 (2) 0.009 (2) −0.002 (2) 0.000 (2) −0.001 (2)
C7A 0.014 (4) 0.018 (4) 0.012 (4) 0.002 (3) 0.003 (3) −0.005 (3)
C8A 0.022 (5) 0.022 (4) 0.038 (5) 0.009 (3) −0.017 (4) −0.009 (4)
C9A 0.010 (3) 0.012 (2) 0.017 (3) 0.005 (2) −0.002 (2) 0.000 (2)
C10A 0.030 (3) 0.028 (3) 0.022 (3) −0.007 (2) −0.005 (2) −0.003 (2)
C1B 0.015 (4) 0.008 (3) 0.013 (4) 0.001 (3) 0.003 (3) 0.005 (3)
C2B 0.010 (4) 0.016 (4) 0.017 (4) 0.001 (3) −0.004 (3) −0.009 (3)
C3B 0.013 (4) 0.012 (4) 0.012 (4) 0.000 (3) 0.003 (3) 0.003 (3)
C4B 0.013 (4) 0.010 (3) 0.014 (4) −0.001 (3) 0.000 (3) −0.003 (3)
C5B 0.011 (4) 0.015 (4) 0.025 (4) 0.004 (3) −0.012 (3) −0.007 (3)
C6B 0.010 (4) 0.007 (3) 0.023 (4) 0.000 (3) 0.001 (3) −0.004 (3)
C7B 0.011 (4) 0.016 (4) 0.009 (4) −0.004 (3) 0.005 (3) −0.004 (3)
C8B 0.033 (5) 0.038 (5) 0.012 (4) 0.016 (4) −0.001 (3) −0.011 (4)
C9B 0.016 (4) 0.015 (4) 0.008 (4) −0.007 (3) −0.001 (3) −0.002 (3)
C10B 0.008 (4) 0.031 (5) 0.040 (5) −0.002 (3) −0.001 (3) −0.014 (4)

Geometric parameters (Å, °)

I1A—C2A 2.110 (6) C1A—C7A 1.502 (8)
I2A—C4A 2.096 (6) C2A—C3A 1.394 (8)
I3A—C6A 2.110 (6) C3A—C4A 1.412 (9)
I1B—C2B 2.111 (6) C3A—C9A 1.504 (9)
I2B—C4B 2.109 (6) C4A—C5A 1.410 (9)
I3B—C6B 2.103 (6) C5A—C6A 1.416 (8)
O1A—C7A 1.341 (7) C8A—H8A 0.9800
O1A—C8A 1.453 (7) C8A—H8B 0.9800
O2A—C7A 1.220 (7) C8A—H8C 0.9800
O3A—C9A 1.333 (7) C10A—H10A 0.9800
O3A—C10A 1.461 (8) C10A—H10B 0.9800
O4A—C9A 1.209 (7) C10A—H10C 0.9800
O1B—C7B 1.332 (7) C1B—C6B 1.377 (9)
O1B—C8B 1.455 (7) C1B—C2B 1.392 (8)
O2B—C7B 1.213 (7) C1B—C7B 1.511 (9)
O3B—C9B 1.346 (7) C2B—C3B 1.402 (9)
O3B—C10B 1.444 (7) C3B—C4B 1.392 (8)
O4B—C9B 1.195 (7) C3B—C9B 1.510 (8)
N1A—C5A 1.360 (8) C4B—C5B 1.395 (9)
N1A—H1A 0.8800 C5B—C6B 1.417 (9)
N1A—H1B 0.8800 C8B—H8D 0.9800
N1B—C5B 1.377 (8) C8B—H8E 0.9800
N1B—H1C 0.8800 C8B—H8F 0.9800
N1B—H1D 0.8800 C10B—H10D 0.9800
C1A—C2A 1.384 (8) C10B—H10E 0.9800
C1A—C6A 1.381 (8) C10B—H10F 0.9800
C7A—O1A—C8A 115.3 (5) O3A—C10A—H10B 109.5
C9A—O3A—C10A 114.4 (5) H10A—C10A—H10B 109.5
C7B—O1B—C8B 115.8 (5) O3A—C10A—H10C 109.5
C9B—O3B—C10B 114.8 (5) H10A—C10A—H10C 109.5
C5A—N1A—H1A 120.0 H10B—C10A—H10C 109.5
C5A—N1A—H1B 120.0 C6B—C1B—C2B 120.1 (6)
H1A—N1A—H1B 120.0 C6B—C1B—C7B 120.9 (6)
C5B—N1B—H1C 120.0 C2B—C1B—C7B 119.0 (6)
C5B—N1B—H1D 120.0 C3B—C2B—C1B 119.3 (6)
H1C—N1B—H1D 120.0 C3B—C2B—I1B 119.5 (5)
C2A—C1A—C6A 121.1 (6) C1B—C2B—I1B 120.8 (5)
C2A—C1A—C7A 118.0 (5) C2B—C3B—C4B 119.6 (6)
C6A—C1A—C7A 120.8 (6) C2B—C3B—C9B 119.0 (6)
C1A—C2A—C3A 119.8 (6) C4B—C3B—C9B 121.3 (6)
C1A—C2A—I1A 120.6 (4) C3B—C4B—C5B 122.3 (6)
C3A—C2A—I1A 119.3 (5) C3B—C4B—I2B 119.3 (5)
C2A—C3A—C4A 118.9 (6) C5B—C4B—I2B 118.4 (5)
C2A—C3A—C9A 120.5 (6) N1B—C5B—C4B 122.4 (6)
C4A—C3A—C9A 120.2 (5) N1B—C5B—C6B 121.1 (6)
C3A—C4A—C5A 122.3 (5) C4B—C5B—C6B 116.5 (6)
C3A—C4A—I2A 118.5 (5) C1B—C6B—C5B 122.1 (6)
C5A—C4A—I2A 119.2 (5) C1B—C6B—I3B 118.6 (5)
N1A—C5A—C4A 122.0 (6) C5B—C6B—I3B 119.2 (5)
N1A—C5A—C6A 121.8 (6) O2B—C7B—O1B 124.9 (6)
C4A—C5A—C6A 116.2 (6) O2B—C7B—C1B 125.3 (6)
C1A—C6A—C5A 121.6 (6) O1B—C7B—C1B 109.7 (5)
C1A—C6A—I3A 120.1 (4) O1B—C8B—H8D 109.5
C5A—C6A—I3A 118.3 (4) O1B—C8B—H8E 109.5
O2A—C7A—O1A 124.4 (6) H8D—C8B—H8E 109.5
O2A—C7A—C1A 124.1 (6) O1B—C8B—H8F 109.5
O1A—C7A—C1A 111.4 (5) H8D—C8B—H8F 109.5
O1A—C8A—H8A 109.5 H8E—C8B—H8F 109.5
O1A—C8A—H8B 109.5 O4B—C9B—O3B 125.0 (6)
H8A—C8A—H8B 109.5 O4B—C9B—C3B 124.3 (6)
O1A—C8A—H8C 109.5 O3B—C9B—C3B 110.7 (5)
H8A—C8A—H8C 109.5 O3B—C10B—H10D 109.5
H8B—C8A—H8C 109.5 O3B—C10B—H10E 109.5
O4A—C9A—O3A 125.5 (6) H10D—C10B—H10E 109.5
O4A—C9A—C3A 122.5 (6) O3B—C10B—H10F 109.5
O3A—C9A—C3A 112.0 (6) H10D—C10B—H10F 109.5
O3A—C10A—H10A 109.5 H10E—C10B—H10F 109.5
C6A—C1A—C2A—C3A 0.2 (9) C6B—C1B—C2B—C3B 3.2 (10)
C7A—C1A—C2A—C3A 175.5 (6) C7B—C1B—C2B—C3B −174.7 (6)
C6A—C1A—C2A—I1A −173.9 (5) C6B—C1B—C2B—I1B 176.3 (5)
C7A—C1A—C2A—I1A 1.4 (8) C7B—C1B—C2B—I1B −1.6 (8)
C1A—C2A—C3A—C4A 1.6 (9) C1B—C2B—C3B—C4B −1.0 (10)
I1A—C2A—C3A—C4A 175.7 (5) I1B—C2B—C3B—C4B −174.2 (5)
C1A—C2A—C3A—C9A −170.6 (6) C1B—C2B—C3B—C9B 175.4 (6)
I1A—C2A—C3A—C9A 3.6 (8) I1B—C2B—C3B—C9B 2.3 (8)
C2A—C3A—C4A—C5A −2.0 (10) C2B—C3B—C4B—C5B −1.2 (10)
C9A—C3A—C4A—C5A 170.1 (6) C9B—C3B—C4B—C5B −177.6 (6)
C2A—C3A—C4A—I2A 177.3 (4) C2B—C3B—C4B—I2B −179.2 (5)
C9A—C3A—C4A—I2A −10.5 (8) C9B—C3B—C4B—I2B 4.5 (9)
C3A—C4A—C5A—N1A 179.3 (6) C3B—C4B—C5B—N1B −177.1 (6)
I2A—C4A—C5A—N1A 0.0 (9) I2B—C4B—C5B—N1B 0.8 (9)
C3A—C4A—C5A—C6A 0.7 (9) C3B—C4B—C5B—C6B 1.3 (10)
I2A—C4A—C5A—C6A −178.7 (4) I2B—C4B—C5B—C6B 179.2 (4)
C2A—C1A—C6A—C5A −1.6 (10) C2B—C1B—C6B—C5B −3.3 (10)
C7A—C1A—C6A—C5A −176.7 (6) C7B—C1B—C6B—C5B 174.6 (6)
C2A—C1A—C6A—I3A 178.6 (5) C2B—C1B—C6B—I3B 175.1 (5)
C7A—C1A—C6A—I3A 3.5 (8) C7B—C1B—C6B—I3B −7.1 (8)
N1A—C5A—C6A—C1A −177.5 (6) N1B—C5B—C6B—C1B 179.4 (6)
C4A—C5A—C6A—C1A 1.1 (9) C4B—C5B—C6B—C1B 1.0 (10)
N1A—C5A—C6A—I3A 2.3 (8) N1B—C5B—C6B—I3B 1.1 (9)
C4A—C5A—C6A—I3A −179.1 (5) C4B—C5B—C6B—I3B −177.3 (5)
C8A—O1A—C7A—O2A 8.7 (9) C8B—O1B—C7B—O2B 3.7 (9)
C8A—O1A—C7A—C1A −170.6 (5) C8B—O1B—C7B—C1B −178.6 (5)
C2A—C1A—C7A—O2A −100.9 (8) C6B—C1B—C7B—O2B 82.7 (9)
C6A—C1A—C7A—O2A 74.4 (9) C2B—C1B—C7B—O2B −99.4 (8)
C2A—C1A—C7A—O1A 78.4 (7) C6B—C1B—C7B—O1B −95.0 (7)
C6A—C1A—C7A—O1A −106.3 (7) C2B—C1B—C7B—O1B 82.9 (7)
C10A—O3A—C9A—O4A 1.3 (9) C10B—O3B—C9B—O4B 8.4 (9)
C10A—O3A—C9A—C3A −179.4 (5) C10B—O3B—C9B—C3B −170.5 (5)
C2A—C3A—C9A—O4A 79.0 (8) C2B—C3B—C9B—O4B −102.1 (8)
C4A—C3A—C9A—O4A −93.0 (8) C4B—C3B—C9B—O4B 74.3 (9)
C2A—C3A—C9A—O3A −100.4 (7) C2B—C3B—C9B—O3B 76.8 (8)
C4A—C3A—C9A—O3A 87.6 (7) C4B—C3B—C9B—O3B −106.8 (7)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1A—H1A···I2A 0.88 2.74 3.224 (5) 116
N1A—H1A···O4Bi 0.88 2.48 3.036 (7) 122
N1A—H1B···I3A 0.88 2.72 3.211 (5) 117
N1B—H1C···I2B 0.88 2.73 3.212 (5) 116
N1B—H1D···I3B 0.88 2.73 3.222 (5) 116
N1B—H1D···O2Aii 0.88 2.43 3.026 (7) 125
C8B—H8E···O2Biii 0.98 2.54 3.516 (9) 171
C10A—H10A···O2Biv 0.98 2.58 3.499 (9) 155
C10A—H10B···O4Av 0.98 2.54 3.519 (9) 173

Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x, −y, −z+1; (iii) −x+1, −y, −z+2; (iv) x, y+1, z−1; (v) −x, −y+1, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2251).

References

  1. Beck, T. & Sheldrick, G. M. (2008). Acta Cryst. E64, o1286. [DOI] [PMC free article] [PubMed]
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  3. North, A. C. T., Phillips, D. C. & Mathews, F. S. (1968). Acta Cryst. A24, 351–359.
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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810001005/pv2251sup1.cif

e-66-0o360-sup1.cif (22.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810001005/pv2251Isup2.hkl

e-66-0o360-Isup2.hkl (257.1KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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