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 ▶).
Experimental
Crystal data
C10H8I3NO4
M r = 586.87
Triclinic,
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
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810001005/pv2251Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. 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)
; (ii)
; (iii)
; (iv)
; (v)
.
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.
A view of the title compound with the atomic numbering scheme. Displacement ellipsoids were drawn at the 50% probability level.
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 m−3 |
| 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 mm−1 |
| 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 Å−3 |
| 24 restraints | Δρmin = −1.19 e Å−3 |
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
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- Rigaku (2004). RAPID-AUTO Rigaku Corporation, Tokyo, Japan.
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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
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810001005/pv2251Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


