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Journal logoSTRUCTURAL
CHEMISTRY
ISSN: 2053-2296

N-(2-Hydr­­oxy-3-iodo-5-nitro­benzyl­­idene)-3-nitro­aniline: conformational isomers linked into complex sheets by five C—H⋯O hydrogen bonds and a two-centre iodo–nitro inter­action

CROSSMARK_Color_square_no_text.svg

aDepartment of Chemistry, University of Aberdeen, Meston Walk, Old Aberdeen AB24 3UE, Scotland, bInstituto de Química, Departamento de Química Inorgânica, Universidade Federal do Rio de Janeiro, CP 68563, 21945-970 Rio de Janeiro, RJ, Brazil, and cSchool of Chemistry, University of St Andrews, Fife KY16 9ST, Scotland
*Correspondence e-mail: cg@st-andrews.ac.uk

(Received 26 May 2006; accepted 30 May 2006; online 30 June 2006)

The title compound, C13H8IN3O5, crystallizes with Z′ = 2 in the space group P21/n. The two independent mol­ecules, which are both almost planar, are conformational isomers. The mol­ecules are linked into complex sheets by a combination of five independent C—H⋯O hydrogen bonds and an almost linear two-centre iodo–nitro inter­action.

Comment

We have recently reported the supra­molecular structures of imines containing iodo and nitro groups, for example, N-(2-iodo­benzyl­idene)-3-nitro­aniline, 2-IC6H4CH=NC6H4NO2-3′ (Wardell et al., 2002[Wardell, J. L., Wardell, S. M. S. V., Skakle, J. M. S., Low, J. N. & Glidewell, C. (2002). Acta Cryst. C58, o428-o430.]), and the various isomeric N-(nitro­benzyl­idene)iodo­anilines, O2NC6H4CH=NC6H4I (Glidewell et al., 2002[Glidewell, C., Howie, R. A., Low, J. N., Skakle, J. M. S., Wardell, S. M. S. V. & Wardell, J. L. (2002). Acta Cryst. B58, 864-876.]), several of which crystallize in two polymorphic forms (Ferguson et al., 2005[Ferguson, G., Glidewell, C., Low, J. N., Skakle, J. M. S. & Wardell, J. L. (2005). Acta Cryst. C61, o445-o449.]). We have now continued our studies in this area with the title compound, (I)[link], an imine containing an additional nitro group as well as a hard hydrogen-bonding donor group.

Compound (I)[link] crystallizes with Z′ = 2 in the space group P21/n (Fig. 1[link]). In each of the independent mol­ecules there is an intra­molecular O—H⋯N hydrogen bond, forming an S(6) motif (Bernstein et al., 1995[Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555-1573.]), and these inter­actions undoubtedly influence the mol­ecular conformations. Both mol­ecules are nearly planar. The overall conformation in each is defined by five torsion angles (Table 1[link]), and it is striking that in mol­ecule A the two nitro groups are on the same edge of the mol­ecule, whereas in mol­ecule B these substituents are on opposite edges (Fig. 1[link]). The two mol­ecules are thus conformational isomers, and this alone suffices to preclude any possible additional symmetry.

Within the mol­ecules, the bond distances show some inter­esting patterns (Table 1[link]), consequent upon the mutually

[Scheme 1]
para arrangement in the iodinated rings of the electron-donor hydroxyl substituent and the electron-acceptor nitro group; in the non-iodinated rings, there is no possibility of any conjugative inter­actions. Thus, the C—O bonds are significantly shorter than is typical in simple phenols (mean value 1.362 Å; Allen et al., 1987[Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1-19.]). Of the C—N bonds to the nitro groups, the bonds C5A—N5A and C5B—N5B are both somewhat shorter than the mean value for simple aromatic nitro compounds (1.468 Å), whereas the bonds C13A—N13A and C13B—N13B are both considerably longer. The N—O bonds involving atoms N5A and N5B are shorter than those involving atoms N13A and N13B. Finally, there is some evidence of C—C bond fixation within the iodinated rings. These observations, taken together, provide some evidence in favour of polarized form (Ia)[link] (see scheme) as a modest contributor to the overall mol­ecular electronic structure.

Within the selected asymmetric unit, the two mol­ecules are linked by two C—H⋯O hydrogen bonds (Fig. 1[link] and Table 2[link]), and this bimolecular aggregate can be regarded as the basic building block within the supra­molecular structure. Three further C—H⋯O hydrogen bonds and a two-centre iodo–nitro inter­action then link these aggregates into complex sheets, the formation of which can be readily analysed in terms of one-dimensional substructures.

In the principal substructure, atom C14B at (x, y, z) acts as hydrogen-bond donor to atom O14B at (−x, −y, 1 − z), so generating by inversion a centrosymmetric R22(10) motif centred at (0, 0, [{1 \over 2}]). At the same time, atom I3B at (x, y, z) forms a two-centre inter­action with atom O13A at (−x, 1 − y, 1 − z), with dimensions I⋯O = 3.173 (4) Å and C—I⋯O = 175.6 (2)°, so generating by inversion an R44(28) (Starbuck et al., 1999[Starbuck, J., Norman, N. C. & Orpen, A. G. (1999). New J. Chem. 23, 969-972.]) motif centred at (0, [{1 \over 2}],  [{1 \over 2}]). Propagation by inversion of these two inter­actions then generates a chain running parallel to the [010] direction containing R22(10) rings centred at (0, n, [{1 \over 2}]) (n = zero or integer) and R44(28) rings centred at (0, n + [{1 \over 2}], [{1 \over 2}]) (n = zero or integer), together with two types of S(6) ring and an R22(14) ring (Fig. 2[link]).

Two further C—H⋯O hydrogen bonds link the [010] chains into sheets. The type A mol­ecules (Fig. 1[link]) at (x, y, z) and (−x, −y, 1 − z) form part of the chain along (0, y, [{1 \over 2}]) (Fig. 2[link]). The C14A atoms at (x, y, z) and (−x, −y, 1 − z), act as hydrogen-bond donors to, respectively, atoms O51A at ([{3\over 2}] − x, [{1\over 2}] + y, [{1\over 2}] − z) and (−[{3\over 2}] + x, −[{1\over 2}] − y, [{1\over 2}] + z), which themselves lie in the [010] chains along ([{3 \over 2}], y, 0) and ([-{3 \over 2}], y, 1), respectively. Hence, the propagation of this hydrogen bond by the 21 screw axes along [3(2m + 1)/4, y, (1 − 2m)/4] (m = zero or integer) links the [010] chains into a (103) sheet. The formation of this sheet is reinforced by the final C—H⋯O hydrogen bond, in which atom C16A at (x, y, z) acts as hydrogen-bond donor to atom O13B at ([{3\over 2}] + x, [{1\over 2}] − y, −[{1\over 2}] + z), so forming a C22(18)­C22(18)[R22(14)] chain of rings running parallel to the [30[\overline{1}]] direction and generated by the n-glide plane at y = [{1 \over 4}] (Fig. 3[link]).

There are no direction-specific inter­actions between adjacent sheets. In particular, C—H⋯π(arene) hydrogen bonds and aromatic ππ stacking inter­actions are absent from the structure of (I)[link].

[Figure 1]
Figure 1
The two independent mol­ecules of compound (I)[link], showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radii. The intra­molecular O—H⋯N hydrogen bonds and the two C—H⋯O hydrogen bonds within the selected asymmetric unit are indicated by dashed lines.
[Figure 2]
Figure 2
A stereoview of part of the crystal structure of compound (I)[link], showing the formation of a chain along [010] built from hydrogen bonds and iodo–nitro inter­actions, and containing five different rings. For the sake of clarity, H atoms not involved in the motifs shown have been omitted.
[Figure 3]
Figure 3
A stereoview of part of the crystal structure of compound (I)[link], showing the formation of a hydrogen-bonded chain of rings along [30[\overline{1}]]. For the sake of clarity, H atoms not involved in the motifs shown have been omitted.

Experimental

A solution of 3-nitro­aniline (1.38 g, 10 mmol) and 2-hydr­oxy-3-iodo-5-nitro­benzaldehyde (0.55 g, 10 mmol) (Garden et al., 2004[Garden, S. J., da Cunha, F. R., Glidewell, C., Low, J. N., Skakle, J. M. S. & Wardell, J. L. (2004). Acta Cryst. C60, o12-o14.]) in methanol (30 ml) was heated under reflux for 45 min. The mixture was then cooled and the solvent was removed under reduced pressure. Crystallization from ethanol of the resulting solid product gave crystals of (I)[link] suitable for single-crystal X-ray diffraction.

Crystal data
  • C13H8IN3O5

  • Mr = 413.12

  • Monoclinic, P 21 /n

  • a = 9.2957 (4) Å

  • b = 27.5905 (13) Å

  • c = 11.0084 (5) Å

  • β = 93.830 (2)°

  • V = 2817.1 (2) Å3

  • Z = 8

  • Dx = 1.948 Mg m−3

  • Mo Kα radiation

  • μ = 2.30 mm−1

  • T = 291 (2) K

  • Plate, colourless

  • 0.30 × 0.22 × 0.05 mm

Data collection
  • Bruker SMART 1000 CCD area-detector diffractometer

  • φ and ω scans

  • Absorption correction: multi-scan (SADABS; Bruker, 2000[Bruker (2000). SADABS (Version 2.03) and SAINT (Version 6.02a). Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.545, Tmax = 0.893

  • 29048 measured reflections

  • 10158 independent reflections

  • 4201 reflections with I > 2σ(I)

  • Rint = 0.068

  • θmax = 32.5°

Refinement
  • Refinement on F2

  • R[F2 > 2σ(F2)] = 0.050

  • wR(F2) = 0.093

  • S = 0.87

  • 10158 reflections

  • 399 parameters

  • H-atom parameters constrained

  • w = 1/[σ2(Fo2) + (0.0298P)2] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max = 0.001

  • Δρmax = 0.72 e Å−3

  • Δρmin = −0.51 e Å−3

Table 1
Selected geometric parameters (Å, °)

C1A—C2A 1.411 (5)
C2A—C3A 1.406 (5)
C3A—C4A 1.377 (5)
C4A—C5A 1.387 (5)
C5A—C6A 1.380 (5)
C6A—C1A 1.394 (5)
C2A—O2A 1.327 (4)
C5A—N5A 1.457 (5)
N5A—O51A 1.217 (4)
N5A—O52A 1.229 (4)
C13A—N13A 1.484 (5)
N13A—O13A 1.198 (5)
N13A—O14A 1.207 (4)
C1B—C2B 1.419 (5)
C2B—C3B 1.414 (5)
C3B—C4B 1.368 (5)
C4B—C5B 1.388 (5)
C5B—C6B 1.359 (5)
C6B—C1B 1.388 (5)
C2B—O2B 1.311 (4)
C5B—N5B 1.463 (5)
N5B—O51B 1.204 (4)
N5B—O52B 1.232 (4)
C13B—N13B 1.475 (5)
N13B—O13B 1.215 (5)
N13B—O14B 1.208 (4)
C12A—C13A—N13A—O13A −7.1 (7)
C1A—C7A—N1A—C11A −177.1 (4)
N1A—C7A—C1A—C2A 0.4 (7)
C7A—N1A—C11A—C12A −0.1 (7)
C4A—C5A—N5A—O51A 8.2 (6)
C12B—C13B—N13B—O13B 5.5 (7)
C1B—C7B—N1B—C11B −179.4 (4)
N1B—C7B—C1B—C2B 1.1 (6)
C7B—N1B—C11B—C12B 176.9 (4)
C4B—C5B—N5B—O51B 1.2 (7)

Table 2
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O2A—H2A⋯N1A 0.82 1.85 2.580 (4) 148
O2B—H2B⋯N1B 0.82 1.81 2.549 (4) 149
C7A—H7A⋯O52B 0.93 2.37 3.263 (5) 160
C7B—H7B⋯O52A 0.93 2.36 3.254 (5) 162
C14A—H14A⋯O51Ai 0.93 2.53 3.372 (6) 151
C14B—H14B⋯O14Bii 0.93 2.51 3.279 (6) 141
C16A—H16A⋯O13Biii 0.93 2.47 3.377 (5) 166
Symmetry codes: (i) [-x+{\script{3\over 2}}, y+{\script{1\over 2}}, -z+{\script{1\over 2}}]; (ii) -x, -y, -z+1; (iii) [x+{\script{3\over 2}}], [-y+{\script{1\over 2}}], [z-{\script{1\over 2}}].

The space group P21/n was uniquely assigned from the systematic absences. All H atoms were located in difference maps and then treated as riding atoms, with C—H = 0.93 Å, O—H = 0.82 Å and Uiso(H) = 1.2Ueq(C) or 1.5Ueq(O).

Data collection: SMART (Bruker, 1998[Bruker (1998). SMART. Version 5.0. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2000[Bruker (2000). SADABS (Version 2.03) and SAINT (Version 6.02a). Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997[Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997[Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.]); molecular graphics: PLATON (Spek, 2003[Spek, A. L. (2003). J. Appl. Cryst. 36, 7-13.]); software used to prepare material for publication: SHELXL97 and PRPKAPPA (Ferguson, 1999[Ferguson, G. (1999). PRPKAPPA. University of Guelph, Canada.]).

Supporting information


Comment top

We have recently reported the supramolecular structures of imines containing iodo and nitro groups, for example N-(2-iodobenzylidene)-3-nitroaniline, 2-IC6H4CH NC6H4NO2-3' (Wardell et al., 2002), and the various isomeric N-(nitrobenzylidene)iodoanilines, O2NC6H4CHNC6H4I (Glidewell et al., 2002), several of which crystallize in two polymorphic forms (Ferguson et al., 2005). We have now continued our studies in this area with the title compound, (I), an imine containing an additional nitro group as well as a hard hydrogen-bonding donor group.

Compound (I) crystallizes with Z' = 2 in space group P21/n (Fig. 1). In each of the independent molecules there is an intramolecular O—H···N hydrogen bond, forming an S(6) motif (Bernstein et al., 1995), and these interactions undoubtedly influence the molecular conformations. Both molecules are nearly planar. The overall conformation in each is defined by five torsion angles (Table 1), and it is striking that in molecule A (Fig. 1) the two nitro groups are on the same edge of the molecule, whereas in molecule B these substituents are on opposite edges. The two molecules are thus conformational isomers, and this alone suffices to preclude any possible additional symmetry.

Within the molecules, the bond distances show some interesting patterns (Table 1), consequent upon the mutually para arrangement in the iodinated rings of the electron-donor hydroxyl substituent and the electron-acceptor nitro group; in the non-iodinated rings, there is no possibility of any conjugative interactions. Thus, the C—O bonds are significantly shorter than is typical in simple phenols (mean value 1.362 Å; Allen et al., 1987). Of the C—N bonds to the nitro groups, the bonds C5A—N5A and C5B—N5B are both somewhat shorter than the mean value for simple aromatic nitro compounds (1.468 Å), whereas the bonds C13A—N13A and C13B—N13B are both considerably longer. The N—O bonds involving atoms N5A and N5B are consistently shorter than those involving atoms N13A and N13B. Finally, there is some evidence of C—C bond fixation within the iodinated rings. These observations, taken together, provide some evidence in favour of the polarized form, (Ia), as a modest contributor to the overall molecular electronic structure.

Within the selected asymmetric unit, the two molecules are linked by two C—H···O hydrogen bonds (Fig. 1, Table 2), and this bimolecular aggregate can be regarded as the basic building block within the supramolecular structure. Three further C—H···O hydrogen bonds and a two-centre iodo···nitro interaction then link these aggregates into complex sheets, the formation of which can be readily analysed in terms of one-dimensional sub-structures.

In the principal sub-structure, atom C14B at (x, y, z) acts as hydrogen-bond donor to atom O14B at (−x, −y, 1 − z), so generating by inversion a centrosymmetric R22(10) motif centred at (0, 0, 1/2). At the same time, atom I3B at (x, y, z) forms a two-centre interaction with atom O13A at (−x, 1 − y, 1 − z), with dimensions I···Oi = 3.173 (4) Å and C—I···Oi = 175.6 (2)° [symmetry code: (i) −x, 1 − y, 1 − z], so generating by inversion an R44(28) (Starbuck et al., 1999) motif centred at (0, 1/2, 1/2). Propagation by inversion of these two interactions then generates a chain running parallel to the [010] direction containing R22(10) rings centred at (0, n, 1/2) (n = zero or integer) and R44(28) rings centred at (0, n + 1/2, 1/2) (n = zero or integer), together with two types of S(6) ring and an R22(14) ring (Fig. 2).

Two further C—H···O hydrogen bonds link the [010] chains into sheets. The type A molecules (Fig. 1) at (x, y, z) and (−x, −y, 1 − z) form part of the chain along (0, y, 1/2) (Fig. 2). The atoms C14A at (x, y, z) and (−x, −y, 1 − z), act as hydrogen-bond donors to, respectively, atoms O51A at (3/2 − x, 1/2 + y, 1/2 − z) and (−3/2 + x, −1/2 − y, 1/2 + z), which themselves lie in the [010] chains along (3/2, y, 0) and (−3/2, y, 1), respectively. Hence, the propagation of this hydrogen bond by the 21screw axes along [3(2m + 1)/4, y, (1 − 2m)/4] (m = zero or integer) links the [010] chains into a (103) sheet. The formation of this sheet is reinforced by the final C—H···O hydrogen bond, in which atom C16A at (x, y, z) acts as hydrogen-bond donor to atom O13B at (3/2 + x, 1/2 − y, −1/2 + z), so forming a C22(18) C22(18)[R22(14)] chain of rings running parallel to the [301] direction and generated by the n-glide plane at y = 1/4 (Fig. 3).

There are no direction-specific interactions between adjacent sheets. In particular, C—H···π(arene) hydrogen bonds and aromatic ππ stacking interactions are absent from the structure of (I).

Experimental top

A solution of 3-nitroaniline (1.38 g, 10 mmol) and 2-hydroxy-3-iodo-5-nitrobenzaldehyde (0.55 g, 10 mmol) (Garden et al., 2004) in methanol (30 ml) was heated under reflux for 45 min. The mixture was then cooled and the solvent was removed under reduced pressure. Crystallization from ethanol of the resulting solid product gave crystals of (I) suitable for single-crystal X-ray diffraction.

Refinement top

The space group P21/n was uniquely assigned from the systematic absences. All H atoms were located in difference maps and then treated as riding atoms, with C—H = 0.93 Å and O—H = 0.82 Å, and with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(O).

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97 and PRPKAPPA (Ferguson, 1999).

Figures top
[Figure 1] Fig. 1. The two independent molecules of compound (I), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radii. The intramolecular O—H···N hydrogen bonds and the two C—H.·O hydrogen bonds within the selected asymmetric unit are indicated by dashed lines.
[Figure 2] Fig. 2. A stereoview of part of the crystal structure of compound (I), showing the formation of a chain along [010] built from hydrogen bonds and iodo···nitro interactions, and containing five different rings. For the sake of clarity, H atoms not involved in the motifs shown have been omitted.
[Figure 3] Fig. 3. A stereoview of part of the crystal structure of compound (I), showing the formation of a hydrogen-bonded chain of rings along [301]. For the sake of clarity, H atoms not involved in the motifs shown have been omitted.
N-(2-Hydroxy-3-iodo-5-nitrobenzylidene)-3-nitroaniline top
Crystal data top
C13H8IN3O5F(000) = 1600
Mr = 413.12Dx = 1.948 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 10158 reflections
a = 9.2957 (4) Åθ = 2.0–32.5°
b = 27.5905 (13) ŵ = 2.30 mm1
c = 11.0084 (5) ÅT = 291 K
β = 93.830 (2)°Plate, colourless
V = 2817.1 (2) Å30.30 × 0.22 × 0.05 mm
Z = 8
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
10158 independent reflections
Radiation source: Bruker-Nonius FR591 rotating anode4201 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.068
ϕ/ω scansθmax = 32.5°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 1214
Tmin = 0.545, Tmax = 0.893k = 4140
29048 measured reflectionsl = 1416
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.050Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.093H-atom parameters constrained
S = 0.87 w = 1/[σ2(Fo2) + (0.0298P)2]
where P = (Fo2 + 2Fc2)/3
10158 reflections(Δ/σ)max = 0.001
399 parametersΔρmax = 0.72 e Å3
0 restraintsΔρmin = 0.51 e Å3
Crystal data top
C13H8IN3O5V = 2817.1 (2) Å3
Mr = 413.12Z = 8
Monoclinic, P21/nMo Kα radiation
a = 9.2957 (4) ŵ = 2.30 mm1
b = 27.5905 (13) ÅT = 291 K
c = 11.0084 (5) Å0.30 × 0.22 × 0.05 mm
β = 93.830 (2)°
Data collection top
Bruker SMART 1000 CCD area-detector
diffractometer
10158 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
4201 reflections with I > 2σ(I)
Tmin = 0.545, Tmax = 0.893Rint = 0.068
29048 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0500 restraints
wR(F2) = 0.093H-atom parameters constrained
S = 0.87Δρmax = 0.72 e Å3
10158 reflectionsΔρmin = 0.51 e Å3
399 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C1A0.7396 (4)0.32517 (14)0.2209 (4)0.0415 (10)
C2A0.8625 (4)0.30384 (15)0.1745 (4)0.0421 (10)
C3A0.8740 (4)0.25305 (14)0.1702 (4)0.0409 (10)
C4A0.7664 (4)0.22415 (14)0.2109 (4)0.0437 (10)
C5A0.6448 (4)0.24585 (14)0.2533 (4)0.0417 (10)
C6A0.6301 (4)0.29554 (15)0.2596 (4)0.0424 (10)
O2A0.9685 (3)0.33075 (10)0.1356 (3)0.0554 (8)
I3A1.06008 (3)0.222130 (10)0.10789 (3)0.05289 (10)
N5A0.5291 (4)0.21515 (14)0.2923 (3)0.0538 (10)
O51A0.5482 (3)0.17160 (12)0.2999 (4)0.0795 (11)
O52A0.4151 (3)0.23460 (11)0.3152 (3)0.0687 (10)
C7A0.7259 (4)0.37732 (14)0.2311 (4)0.0473 (11)
N1A0.8246 (3)0.40571 (12)0.1978 (3)0.0481 (9)
C11A0.8200 (4)0.45685 (14)0.2106 (4)0.0451 (10)
C12A0.7079 (4)0.48208 (14)0.2607 (4)0.0495 (11)
C13A0.7214 (4)0.53096 (14)0.2715 (4)0.0514 (11)
C14A0.8390 (5)0.55672 (16)0.2374 (5)0.0655 (14)
C15A0.9482 (5)0.53111 (17)0.1880 (5)0.0767 (16)
C16A0.9380 (5)0.48180 (17)0.1743 (5)0.0642 (14)
N13A0.6041 (4)0.55855 (14)0.3252 (4)0.0645 (11)
O13A0.4970 (4)0.53663 (12)0.3453 (4)0.1098 (16)
O14A0.6206 (4)0.60154 (12)0.3412 (4)0.0835 (12)
C1B0.0925 (4)0.30637 (14)0.4377 (4)0.0389 (9)
C2B0.0316 (4)0.32694 (15)0.4857 (4)0.0430 (10)
C3B0.0414 (4)0.37800 (15)0.4930 (4)0.0446 (10)
C4B0.0665 (4)0.40661 (15)0.4539 (4)0.0495 (11)
C5B0.1856 (4)0.38511 (15)0.4065 (4)0.0471 (11)
C6B0.2002 (4)0.33623 (15)0.3984 (4)0.0480 (11)
O2B0.1357 (3)0.29980 (10)0.5232 (3)0.0551 (8)
I3B0.22515 (3)0.408833 (11)0.56081 (3)0.06011 (11)
N5B0.3001 (4)0.41635 (15)0.3659 (4)0.0703 (12)
O51B0.2877 (4)0.45952 (13)0.3771 (5)0.128 (2)
O52B0.4033 (3)0.39706 (12)0.3204 (4)0.0836 (12)
C7B0.1070 (4)0.25474 (15)0.4298 (4)0.0446 (10)
N1B0.0085 (3)0.22593 (12)0.4636 (3)0.0430 (8)
C11B0.0187 (4)0.17463 (14)0.4586 (4)0.0440 (10)
C12B0.0938 (4)0.14925 (15)0.5043 (4)0.0475 (11)
C13B0.0864 (4)0.09943 (15)0.5059 (4)0.0507 (11)
C14B0.0262 (5)0.07417 (16)0.4619 (4)0.0574 (12)
C15B0.1353 (5)0.10006 (16)0.4145 (4)0.0585 (13)
C16B0.1336 (4)0.14985 (16)0.4124 (4)0.0514 (11)
N13B0.2059 (4)0.07247 (15)0.5560 (4)0.0675 (12)
O13B0.3092 (4)0.09588 (12)0.5844 (4)0.0943 (13)
O14B0.1970 (4)0.02889 (12)0.5645 (4)0.0867 (12)
H4A0.77510.19060.20990.052*
H6A0.54790.30910.28930.051*
H2A0.94680.35950.13960.083*
H7A0.64390.39040.26250.057*
H12A0.62700.46600.28580.059*
H14A0.84450.59020.24730.079*
H15A1.02920.54730.16390.092*
H16A1.01190.46500.13990.077*
H4B0.06010.44020.45900.059*
H6B0.28170.32290.36690.058*
H2B0.11740.27120.51110.083*
H7B0.18970.24180.39950.054*
H12B0.17250.16540.53330.057*
H14B0.02850.04050.46410.069*
H15B0.21190.08360.38330.070*
H16B0.20860.16690.38030.062*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1A0.031 (2)0.045 (2)0.049 (3)0.0070 (18)0.0061 (19)0.003 (2)
C2A0.031 (2)0.050 (3)0.046 (3)0.0040 (19)0.0074 (19)0.002 (2)
C3A0.027 (2)0.046 (2)0.050 (3)0.0050 (18)0.0087 (19)0.000 (2)
C4A0.041 (2)0.046 (2)0.045 (3)0.008 (2)0.0071 (19)0.002 (2)
C5A0.032 (2)0.047 (2)0.047 (3)0.0023 (18)0.0067 (19)0.001 (2)
C6A0.029 (2)0.055 (3)0.044 (3)0.0048 (18)0.0054 (19)0.007 (2)
O2A0.0409 (16)0.0458 (16)0.082 (2)0.0023 (14)0.0223 (16)0.0047 (18)
I3A0.04261 (16)0.05769 (18)0.0606 (2)0.01476 (14)0.02029 (14)0.00158 (16)
N5A0.041 (2)0.063 (3)0.059 (2)0.0084 (19)0.0167 (18)0.012 (2)
O51A0.071 (2)0.047 (2)0.125 (3)0.0056 (17)0.042 (2)0.004 (2)
O52A0.0349 (16)0.074 (2)0.100 (3)0.0055 (15)0.0251 (17)0.0183 (19)
C7A0.040 (2)0.050 (3)0.052 (3)0.008 (2)0.007 (2)0.004 (2)
N1A0.038 (2)0.045 (2)0.062 (2)0.0051 (16)0.0080 (17)0.0005 (19)
C11A0.036 (2)0.042 (2)0.058 (3)0.0056 (19)0.009 (2)0.002 (2)
C12A0.038 (2)0.041 (2)0.071 (3)0.0013 (19)0.015 (2)0.005 (2)
C13A0.044 (3)0.042 (3)0.069 (3)0.005 (2)0.009 (2)0.005 (2)
C14A0.060 (3)0.044 (3)0.094 (4)0.006 (2)0.017 (3)0.008 (3)
C15A0.051 (3)0.060 (3)0.123 (5)0.015 (2)0.029 (3)0.008 (3)
C16A0.043 (3)0.062 (3)0.090 (4)0.002 (2)0.023 (3)0.001 (3)
N13A0.060 (3)0.045 (2)0.091 (3)0.009 (2)0.020 (2)0.005 (2)
O13A0.082 (3)0.055 (2)0.202 (5)0.0031 (19)0.083 (3)0.012 (3)
O14A0.084 (3)0.047 (2)0.120 (3)0.0045 (18)0.019 (2)0.025 (2)
C1B0.028 (2)0.047 (2)0.042 (3)0.0005 (18)0.0054 (18)0.000 (2)
C2B0.035 (2)0.049 (2)0.047 (3)0.0011 (19)0.0110 (19)0.001 (2)
C3B0.029 (2)0.058 (3)0.048 (3)0.0003 (19)0.0100 (19)0.002 (2)
C4B0.044 (2)0.046 (2)0.060 (3)0.001 (2)0.015 (2)0.004 (2)
C5B0.031 (2)0.051 (3)0.061 (3)0.0104 (19)0.018 (2)0.002 (2)
C6B0.033 (2)0.058 (3)0.055 (3)0.0046 (19)0.014 (2)0.005 (2)
O2B0.0374 (16)0.0538 (17)0.077 (2)0.0032 (14)0.0260 (15)0.0060 (18)
I3B0.04633 (17)0.0628 (2)0.0742 (2)0.00891 (14)0.02602 (16)0.00050 (17)
N5B0.046 (2)0.060 (3)0.107 (4)0.013 (2)0.027 (2)0.001 (3)
O51B0.101 (3)0.049 (2)0.246 (6)0.021 (2)0.097 (4)0.010 (3)
O52B0.0451 (19)0.081 (2)0.130 (3)0.0077 (17)0.045 (2)0.005 (2)
C7B0.036 (2)0.058 (3)0.041 (3)0.002 (2)0.0105 (19)0.004 (2)
N1B0.0344 (18)0.050 (2)0.046 (2)0.0031 (16)0.0094 (16)0.0010 (18)
C11B0.043 (2)0.045 (2)0.044 (3)0.0024 (19)0.008 (2)0.001 (2)
C12B0.037 (2)0.049 (3)0.058 (3)0.003 (2)0.011 (2)0.004 (2)
C13B0.044 (2)0.052 (3)0.057 (3)0.004 (2)0.014 (2)0.002 (2)
C14B0.055 (3)0.050 (3)0.070 (3)0.004 (2)0.017 (3)0.001 (2)
C15B0.051 (3)0.058 (3)0.068 (3)0.008 (2)0.016 (2)0.003 (3)
C16B0.040 (2)0.057 (3)0.059 (3)0.002 (2)0.019 (2)0.002 (2)
N13B0.059 (3)0.056 (3)0.091 (3)0.013 (2)0.027 (2)0.004 (2)
O13B0.058 (2)0.064 (2)0.167 (4)0.0051 (18)0.055 (2)0.003 (2)
O14B0.088 (3)0.045 (2)0.132 (3)0.0091 (18)0.046 (2)0.004 (2)
Geometric parameters (Å, º) top
C1A—C2A1.411 (5)C1B—C2B1.419 (5)
C2A—C3A1.406 (5)C2B—C3B1.414 (5)
C3A—C4A1.377 (5)C3B—C4B1.368 (5)
C4A—C5A1.387 (5)C4B—C5B1.388 (5)
C5A—C6A1.380 (5)C5B—C6B1.359 (5)
C6A—C1A1.394 (5)C6B—C1B1.388 (5)
C2A—O2A1.327 (4)C2B—O2B1.311 (4)
C5A—N5A1.457 (5)C5B—N5B1.463 (5)
N5A—O51A1.217 (4)N5B—O51B1.204 (4)
N5A—O52A1.229 (4)N5B—O52B1.232 (4)
C13A—N13A1.484 (5)C13B—N13B1.475 (5)
N13A—O13A1.198 (5)N13B—O13B1.215 (5)
N13A—O14A1.207 (4)N13B—O14B1.208 (4)
C1A—C7A1.450 (5)C1B—C7B1.434 (5)
C3A—I3A2.086 (3)C3B—I3B2.090 (4)
C4A—H4A0.93C4B—H4B0.93
C6A—H6A0.93C6B—H6B0.93
O2A—H2A0.82O2B—H2B0.82
C7A—N1A1.279 (5)C7B—N1B1.286 (5)
C7A—H7A0.93C7B—H7B0.93
N1A—C11A1.419 (5)N1B—C11B1.420 (5)
C11A—C16A1.377 (6)C11B—C12B1.381 (5)
C11A—C12A1.398 (5)C11B—C16B1.393 (5)
C12A—C13A1.359 (5)C12B—C13B1.376 (5)
C12A—H12A0.93C12B—H12B0.93
C13A—C14A1.377 (6)C13B—C14B1.372 (5)
C14A—C15A1.378 (6)C14B—C15B1.372 (6)
C14A—H14A0.93C14B—H14B0.93
C15A—C16A1.372 (6)C15B—C16B1.374 (6)
C15A—H15A0.93C15B—H15B0.93
C16A—H16A0.93C16B—H16B0.93
C6A—C1A—C2A119.4 (4)C6B—C1B—C2B120.0 (4)
C6A—C1A—C7A119.2 (3)C6B—C1B—C7B119.9 (3)
C2A—C1A—C7A121.3 (4)C2B—C1B—C7B120.1 (3)
O2A—C2A—C3A119.2 (3)O2B—C2B—C3B120.0 (3)
O2A—C2A—C1A121.3 (4)O2B—C2B—C1B121.6 (4)
C3A—C2A—C1A119.5 (4)C3B—C2B—C1B118.4 (3)
C4A—C3A—C2A120.5 (3)C4B—C3B—C2B120.4 (4)
C4A—C3A—I3A120.4 (3)C4B—C3B—I3B120.8 (3)
C2A—C3A—I3A119.0 (3)C2B—C3B—I3B118.9 (3)
C3A—C4A—C5A119.0 (4)C3B—C4B—C5B119.4 (4)
C3A—C4A—H4A120.5C3B—C4B—H4B120.3
C5A—C4A—H4A120.5C5B—C4B—H4B120.3
C6A—C5A—C4A122.1 (4)C6B—C5B—C4B122.3 (4)
C6A—C5A—N5A119.0 (3)C6B—C5B—N5B119.1 (4)
C4A—C5A—N5A118.9 (4)C4B—C5B—N5B118.6 (4)
C5A—C6A—C1A119.3 (3)C5B—C6B—C1B119.4 (4)
C5A—C6A—H6A120.3C5B—C6B—H6B120.3
C1A—C6A—H6A120.3C1B—C6B—H6B120.3
C2A—O2A—H2A109.5C2B—O2B—H2B109.5
O51A—N5A—O52A122.8 (4)O51B—N5B—O52B123.5 (4)
O51A—N5A—C5A119.2 (3)O51B—N5B—C5B118.3 (4)
O52A—N5A—C5A118.1 (4)O52B—N5B—C5B118.2 (4)
N1A—C7A—C1A121.1 (4)N1B—C7B—C1B121.7 (4)
N1A—C7A—H7A119.4N1B—C7B—H7B119.2
C1A—C7A—H7A119.4C1B—C7B—H7B119.2
C7A—N1A—C11A123.6 (3)C7B—N1B—C11B123.6 (3)
C16A—C11A—C12A119.7 (4)C12B—C11B—C16B120.1 (4)
C16A—C11A—N1A116.0 (4)C12B—C11B—N1B115.9 (3)
C12A—C11A—N1A124.2 (4)C16B—C11B—N1B124.0 (4)
C13A—C12A—C11A117.5 (4)C13B—C12B—C11B118.2 (4)
C13A—C12A—H12A121.2C13B—C12B—H12B120.9
C11A—C12A—H12A121.2C11B—C12B—H12B120.9
C12A—C13A—C14A124.0 (4)C14B—C13B—C12B122.8 (4)
C12A—C13A—N13A118.5 (4)C14B—C13B—N13B119.2 (4)
C14A—C13A—N13A117.5 (4)C12B—C13B—N13B118.0 (4)
C13A—C14A—C15A117.5 (4)C15B—C14B—C13B118.1 (4)
C13A—C14A—H14A121.2C15B—C14B—H14B121.0
C15A—C14A—H14A121.2C13B—C14B—H14B121.0
C16A—C15A—C14A120.3 (4)C14B—C15B—C16B121.3 (4)
C16A—C15A—H15A119.8C14B—C15B—H15B119.4
C14A—C15A—H15A119.8C16B—C15B—H15B119.4
C15A—C16A—C11A121.0 (4)C15B—C16B—C11B119.5 (4)
C15A—C16A—H16A119.5C15B—C16B—H16B120.2
C11A—C16A—H16A119.5C11B—C16B—H16B120.2
O13A—N13A—O14A124.6 (4)O14B—N13B—O13B124.1 (4)
O13A—N13A—C13A117.1 (4)O14B—N13B—C13B118.7 (4)
O14A—N13A—C13A118.2 (4)O13B—N13B—C13B117.1 (4)
C1A—C7A—N1A—C11A177.1 (4)C1B—C7B—N1B—C11B179.4 (4)
N1A—C7A—C1A—C2A0.4 (7)N1B—C7B—C1B—C2B1.1 (6)
C7A—N1A—C11A—C12A0.1 (7)C7B—N1B—C11B—C12B176.9 (4)
C4A—C5A—N5A—O51A8.2 (6)C4B—C5B—N5B—O51B1.2 (7)
C12A—C13A—N13A—O13A7.1 (7)C12B—C13B—N13B—O13B5.5 (7)
C6A—C1A—C2A—O2A179.3 (4)C6B—C1B—C2B—O2B179.7 (4)
C7A—C1A—C2A—O2A1.8 (7)C7B—C1B—C2B—O2B0.3 (6)
C6A—C1A—C2A—C3A1.2 (6)C6B—C1B—C2B—C3B0.5 (6)
C7A—C1A—C2A—C3A177.7 (4)C7B—C1B—C2B—C3B179.4 (4)
O2A—C2A—C3A—C4A179.4 (4)O2B—C2B—C3B—C4B179.9 (4)
C1A—C2A—C3A—C4A0.0 (6)C1B—C2B—C3B—C4B0.4 (7)
O2A—C2A—C3A—I3A1.9 (6)O2B—C2B—C3B—I3B1.2 (6)
C1A—C2A—C3A—I3A177.6 (3)C1B—C2B—C3B—I3B179.0 (3)
C2A—C3A—C4A—C5A1.6 (6)C2B—C3B—C4B—C5B0.2 (7)
I3A—C3A—C4A—C5A179.1 (3)I3B—C3B—C4B—C5B178.4 (3)
C3A—C4A—C5A—C6A2.0 (6)C3B—C4B—C5B—C6B0.7 (7)
C3A—C4A—C5A—N5A177.9 (4)C3B—C4B—C5B—N5B179.6 (4)
C4A—C5A—C6A—C1A0.8 (6)C4B—C5B—C6B—C1B0.6 (7)
N5A—C5A—C6A—C1A179.2 (4)N5B—C5B—C6B—C1B179.5 (4)
C2A—C1A—C6A—C5A0.9 (6)C2B—C1B—C6B—C5B0.1 (7)
C7A—C1A—C6A—C5A178.1 (4)C7B—C1B—C6B—C5B179.9 (4)
C6A—C5A—N5A—O51A171.8 (4)C6B—C5B—N5B—O51B177.7 (5)
C6A—C5A—N5A—O52A8.9 (6)C6B—C5B—N5B—O52B3.2 (7)
C4A—C5A—N5A—O52A171.1 (4)C4B—C5B—N5B—O52B177.8 (4)
C6A—C1A—C7A—N1A179.3 (4)C6B—C1B—C7B—N1B179.0 (4)
C7A—N1A—C11A—C16A177.5 (4)C7B—N1B—C11B—C16B2.5 (7)
C16A—C11A—C12A—C13A0.1 (7)C16B—C11B—C12B—C13B1.8 (7)
N1A—C11A—C12A—C13A177.4 (4)N1B—C11B—C12B—C13B177.5 (4)
C11A—C12A—C13A—C14A0.7 (7)C11B—C12B—C13B—C14B1.3 (7)
C11A—C12A—C13A—N13A179.6 (4)C11B—C12B—C13B—N13B179.3 (4)
C12A—C13A—C14A—C15A0.8 (8)C12B—C13B—C14B—C15B0.1 (7)
N13A—C13A—C14A—C15A179.7 (5)N13B—C13B—C14B—C15B179.3 (4)
C13A—C14A—C15A—C16A0.0 (8)C13B—C14B—C15B—C16B0.9 (7)
C14A—C15A—C16A—C11A0.8 (9)C14B—C15B—C16B—C11B0.3 (7)
C12A—C11A—C16A—C15A0.9 (8)C12B—C11B—C16B—C15B1.1 (7)
N1A—C11A—C16A—C15A176.9 (5)N1B—C11B—C16B—C15B178.2 (4)
C14A—C13A—N13A—O13A173.9 (5)C14B—C13B—N13B—O14B4.8 (7)
C12A—C13A—N13A—O14A175.7 (5)C12B—C13B—N13B—O14B175.8 (5)
C14A—C13A—N13A—O14A3.3 (7)C14B—C13B—N13B—O13B173.9 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2A—H2A···N1A0.821.852.580 (4)148
O2B—H2B···N1B0.821.812.549 (4)149
C7A—H7A···O52B0.932.373.263 (5)160
C7B—H7B···O52A0.932.363.254 (5)162
C14A—H14A···O51Ai0.932.533.372 (6)151
C14B—H14B···O14Bii0.932.513.279 (6)141
C16A—H16A···O13Biii0.932.473.377 (5)166
Symmetry codes: (i) x+3/2, y+1/2, z+1/2; (ii) x, y, z+1; (iii) x+3/2, y+1/2, z1/2.

Experimental details

Crystal data
Chemical formulaC13H8IN3O5
Mr413.12
Crystal system, space groupMonoclinic, P21/n
Temperature (K)291
a, b, c (Å)9.2957 (4), 27.5905 (13), 11.0084 (5)
β (°) 93.830 (2)
V3)2817.1 (2)
Z8
Radiation typeMo Kα
µ (mm1)2.30
Crystal size (mm)0.30 × 0.22 × 0.05
Data collection
DiffractometerBruker SMART 1000 CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2000)
Tmin, Tmax0.545, 0.893
No. of measured, independent and
observed [I > 2σ(I)] reflections
29048, 10158, 4201
Rint0.068
(sin θ/λ)max1)0.757
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.050, 0.093, 0.87
No. of reflections10158
No. of parameters399
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.72, 0.51

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 2000), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), SHELXL97 and PRPKAPPA (Ferguson, 1999).

Selected geometric parameters (Å, º) top
C1A—C2A1.411 (5)C1B—C2B1.419 (5)
C2A—C3A1.406 (5)C2B—C3B1.414 (5)
C3A—C4A1.377 (5)C3B—C4B1.368 (5)
C4A—C5A1.387 (5)C4B—C5B1.388 (5)
C5A—C6A1.380 (5)C5B—C6B1.359 (5)
C6A—C1A1.394 (5)C6B—C1B1.388 (5)
C2A—O2A1.327 (4)C2B—O2B1.311 (4)
C5A—N5A1.457 (5)C5B—N5B1.463 (5)
N5A—O51A1.217 (4)N5B—O51B1.204 (4)
N5A—O52A1.229 (4)N5B—O52B1.232 (4)
C13A—N13A1.484 (5)C13B—N13B1.475 (5)
N13A—O13A1.198 (5)N13B—O13B1.215 (5)
N13A—O14A1.207 (4)N13B—O14B1.208 (4)
C1A—C7A—N1A—C11A177.1 (4)C1B—C7B—N1B—C11B179.4 (4)
N1A—C7A—C1A—C2A0.4 (7)N1B—C7B—C1B—C2B1.1 (6)
C7A—N1A—C11A—C12A0.1 (7)C7B—N1B—C11B—C12B176.9 (4)
C4A—C5A—N5A—O51A8.2 (6)C4B—C5B—N5B—O51B1.2 (7)
C12A—C13A—N13A—O13A7.1 (7)C12B—C13B—N13B—O13B5.5 (7)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2A—H2A···N1A0.821.852.580 (4)148
O2B—H2B···N1B0.821.812.549 (4)149
C7A—H7A···O52B0.932.373.263 (5)160
C7B—H7B···O52A0.932.363.254 (5)162
C14A—H14A···O51Ai0.932.533.372 (6)151
C14B—H14B···O14Bii0.932.513.279 (6)141
C16A—H16A···O13Biii0.932.473.377 (5)166
Symmetry codes: (i) x+3/2, y+1/2, z+1/2; (ii) x, y, z+1; (iii) x+3/2, y+1/2, z1/2.
 

Acknowledgements

The authors thank the University of Aberdeen for funding the purchase of the diffractometer. JLW thanks CNPq and FAPERJ for financial support.

References

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