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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Apr 28;68(Pt 5):o1570–o1571. doi: 10.1107/S1600536812018235

(1S,2E,6R,7aR)-1,6-Dihy­droxy-2-(4-nitro­benzyl­idene)-2,3,5,6,7,7a-hexa­hydro-1H-pyrrolizin-3-one

F L Oliveira a, K R L Freire b, R Aparicio a,*, F Coelho b
PMCID: PMC3344666  PMID: 22590428

Abstract

The crystal structure of the title compound, C14H14N2O5, contains two distinct conformers in the asymmetric unit. The compound has three defined stereocenters, two of them contiguous, and a C=C double bond with an E conformation. The stereocenters exhibit the same chirality in both conformers, with significant differences in the conformation of the five-membered rings of the pyrrolizine unit (both either in a twist or in an envelope form) and in the dihedral angles between the corresponding mean planes and the benzene rings. A prominent feature is a change from almost coplanar rings in one conformer to a new conformation in the second conformer, in which the mean plane of a five-membered ring is almost perpendicular to the benzene ring, with a dihedral angle 87.19 (8)°; the corresponding angle in the first conformer is 14.02 (10)°. In the crystal, molecules are linked by O—H⋯O and C—H⋯O hydrogen bonds. Crystallographic data were essential to confirm the configuration of the double bond, which was unclear from the available two-dimensional NMR data. In addition, reliable Flack and Hooft parameters were obtained, allowing for the correct absolute structure to be determined.

Related literature  

For the preparation of the title compound, see: Freire et al. (2011). For the use of this type of compound as LFA-1 (Lymphocyte Function-Associated Anti­gen-1) inhibitors, see: Baumann (2007). For related structures, see: Oliveira et al. (2012a ,b ).graphic file with name e-68-o1570-scheme1.jpg

Experimental  

Crystal data  

  • C14H14N2O5

  • M r = 290.27

  • Monoclinic, Inline graphic

  • a = 6.8289 (6) Å

  • b = 7.0433 (6) Å

  • c = 26.618 (3) Å

  • β = 92.335 (4)°

  • V = 1279.2 (2) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 0.98 mm−1

  • T = 100 K

  • 0.39 × 0.23 × 0.06 mm

Data collection  

  • Bruker Kappa APEXII DUO diffractometer

  • Absorption correction: numerical (SADABS; Bruker, 2010) T min = 0.844, T max = 1.000

  • 41060 measured reflections

  • 4038 independent reflections

  • 3986 reflections with I > 2σ(I)

  • R int = 0.037

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.025

  • wR(F 2) = 0.067

  • S = 1.01

  • 4038 reflections

  • 383 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.15 e Å−3

  • Δρmin = −0.16 e Å−3

  • Absolute structure: Flack (1983) and Hooft et al. (2008); Hooft parameter = 0.04(4), 1539 Bijvoet pairs

  • Flack parameter: 0.03 (11)

Data collection: APEX2 (Bruker, 2010); cell refinement: SAINT (Bruker, 2010); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812018235/pv2525sup1.cif

e-68-o1570-sup1.cif (36.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812018235/pv2525Isup2.hkl

e-68-o1570-Isup2.hkl (197.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812018235/pv2525Isup3.cml

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
O3—H3⋯O1′i 0.82 1.93 2.7303 (14) 166
O1—H1A⋯O2ii 0.82 1.89 2.6993 (15) 169
O3′—H3′⋯O3iii 0.82 1.95 2.7585 (15) 171
O1′—H1A′⋯O3′iv 0.82 1.93 2.7451 (15) 174
C1′—H1′⋯O2′ii 0.98 2.52 3.3655 (17) 144
C1′—H1′⋯O5′v 0.98 2.55 3.3242 (19) 136
C10—H10⋯O1vi 0.93 2.54 3.126 (2) 121
C12′—H12′⋯O3′vii 0.93 2.57 3.5014 (18) 174
C13—H13⋯O4i 0.93 2.51 3.2644 (19) 138
C13′—H13′⋯O5′i 0.93 2.51 3.1160 (18) 123

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

Acknowledgments

The authors acknowledge the Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP), the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES) and the Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) for financial support. FLO and KRLF were supported by bursaries from CAPES and CNPq, respectively. KRLF is currently a FAPESP post-doctoral fellow. RA and FC are recipients of research grants from CNPq.

supplementary crystallographic information

Comment

The title compound, a new asymmetric benzyl-pyrrolizidinone, has been prepared from a Morita-Baylis-Hillman adduct using a straight forward synthetic sequence developed in our laboratory (Freire et al., 2011). It can be used as a prototype to design new mediators of the activity of LFA-1 (lymphocyte function-associated antigen 1), with potential applications in the treatment of autoimmune diseases and as anti-inflammatory drugs (Baumann, 2007). The title compound has three defined stereocenters, two of them contiguous, and a double bond with E configuration, an information which was not clear from two-dimensional-NOESY NMR studies. A crystal structure determination of the titlte compound has allowed us to establish its correct configuration, which is reported in this article.

In the crystal structure of the title compound, an asymmetric unit contains two distinct conformers, molecule 1 (Fig. 1) and molecule 2 (Fig. 2), whose stereocenters exhibit the same chirality. In molecule 1, the five membered rings N1/C3/C2/C1/C7A and N1/C5/C6/C7/C7A of the pyrrolizine moiety exhibit C1- and C7-envelope conformations, respectively, with C1 and C7 atoms displaced from the mean-planes formed by the remaining rings atoms by 0.3194 (14) and 0.592 (2) Å, respectively. The mean planes of these rings have a dihedral angle of 23.47 (10)°, and are almost coplanar to the benzene ring, with which they form dihedral angles of 24.52 (9)° and 14.02 (10)°, respectively. The molecule 2 exhibits the rings N1'/C7A'/C1'/C2'/C3' and N1'/C7A'/C7'/C6'/C5' in a twisted conformation on C7A'-C1' and N1'-C7A', respectively, with a dihedral angle between their mean planes equal to 58.07 (8)°. The dihedral angle between the mean planes of the ring N1'/C7A'/C1'/C2'/C3' and the benzene ring is 34.75 (7)°. The ring N1'/C7A'/C7'/C6'/C5' is almost perpendicular to the latter with a corresponding angle equal to 87.19 (8)°. The atom C1' lies 0.3200 (14) Å out of the plane formed by the rest of the ring atoms (N1'/C7A'/C2'/C3'). The corresponding measurement for the atom C7A' in relation to the mean plane formed by the other atoms in the ring (N1'/C7'/C6'/C5') is 0.4771 (13) Å. In the crystal, the molecules are held together by intermolecular hydrogen bonds (Tab. 1 and Fig. 3).

Experimental

The title compound was prepared by a synthetic sequence recently described in the literature (Freire et al., 2011) and purified by flash silica gel column chromatography (CH2Cl2 : MeOH – solvent gradient: 100:0 to 95:05) to afford 0.07 g (as a white solid) in 83% yield. It was then recrystallized using the liquid-vapor saturation method, dissolved in ethanol and crystallized subject to the vapor pressure of a second less polar liquid (ethyl ether), in a closed camera, providing the slow formation of crystals.

Refinement

The calculated Flack parameter was F = 0.03 (11) (Flack, 1983). Analysis of the absolute structure was also performed using likelihood methods (Hooft et al., 2008) as implemented in PLATON (Spek, 2009). The resulting value for the Hooft parameter was y = 0.04 (4), with a calculated probability for an inverted structure equal to 1x10-109. These results unequivocally indicate that the absolute structure has been correctly assigned. All H atoms were placed in calculated positions with O—H = 0.82 Å and C—H = 0.93, 0.97 and 0.98 Å for aryl, methylene and methyne H-atoms, respectively, and refined in the riding model approximation with Uiso(H) = 1.5 Ueq(O) or 1.2 Ueq(C).

Figures

Fig. 1.

Fig. 1.

A view of molecule 1 with the atom numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are presented as small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

A view of molecule 2 with the atom numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are presented as small spheres of arbitrary radius.

Fig. 3.

Fig. 3.

A view of the hydrogen bonding interactions (dotted lines) in the crystal structure of the title compound. H atoms non-participating in hydrogen-bonding were omitted for clarity.

Crystal data

C14H14N2O5 F(000) = 608
Mr = 290.27 Dx = 1.507 Mg m3
Monoclinic, P21 Cu Kα radiation, λ = 1.54178 Å
a = 6.8289 (6) Å Cell parameters from 4038 reflections
b = 7.0433 (6) Å θ = 1.7–67.8°
c = 26.618 (3) Å µ = 0.98 mm1
β = 92.335 (4)° T = 100 K
V = 1279.2 (2) Å3 Plate, orange
Z = 4 0.39 × 0.23 × 0.06 mm

Data collection

Bruker Kappa APEXII DUO diffractometer 4038 independent reflections
Radiation source: fine-focus sealed tube 3986 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.037
Bruker APEX CCD area–detector scans θmax = 67.8°, θmin = 1.7°
Absorption correction: numerical (SADABS; Bruker, 2010) h = −8→8
Tmin = 0.844, Tmax = 1.000 k = −8→6
41060 measured reflections l = −31→31

Refinement

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)] = 0.025 H-atom parameters constrained
wR(F2) = 0.067 w = 1/[σ2(Fo2) + (0.0419P)2 + 0.3034P] where P = (Fo2 + 2Fc2)/3
S = 1.01 (Δ/σ)max = 0.001
4038 reflections Δρmax = 0.15 e Å3
383 parameters Δρmin = −0.16 e Å3
1 restraint Absolute structure: Flack (1983) and Hooft et al. (2008); Hooft parameter = 0.04(4), 1539 Bijvoet pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.03 (11)

Special details

Experimental. [α]D20 + 28° (c 2, MeOH); IR (Film, νmax): 3308, 2974, 2924, 2864, 1699, 1671, 1644, 1596, 1523, 1513, 1435, 1381, 1346, 1314, 1264, 1244, 1220, 1202, 1133, 1104, 1075, 1055 cm-1; 1H NMR (400 MHz, CD3OD) δ 1.49 (ddd, J = 13.2, 8.3, 5.1 Hz, 1H, H-7 A); 2.49 (ddd, J = 13.3, 7.4, 6.2 Hz, 1H, H-7B); 3.38 (dd, J = 12.4, 5.8 Hz, 1H, H-5 A); 3.68 (dd, J = 12.4, 3.0 Hz, 1H, H-5B); 3.80 (td, J = 8.1, 2.4 Hz, 1H, H-7 C); 4.56 (qd, J = 5.8, 3.3 Hz 1H, H-6); 5.01 (t, J = 2.4 Hz, 1H, H-1); 7.45 (d, J = 2.3 Hz, 1H, H-4); 8.01 (d, J = 8.8 Hz, 2H, Ar); 8.26 (d, J = 8.9 Hz, 2H, Ar); 13C NMR (62.5 MHz, CD3CN) 39.2; 53.3; 68.4; 71.5; 72.5; 124.3; 132.4; 133.2; 140.5; 141.8; 148.6; 170.9; HRMS (ESI-TOF) m/z Calc. for C14H15N2O5 [M + H]+: 291.0981. Found 291.0989.
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
O4 0.39324 (16) 0.4194 (2) 1.13861 (4) 0.0321 (3)
O3 1.01737 (15) 0.58119 (18) 0.71964 (4) 0.0225 (2)
H3 1.1038 0.5564 0.7002 0.034*
O5 0.64579 (19) 0.4992 (2) 1.18584 (4) 0.0403 (3)
O2 1.35576 (15) 0.51910 (18) 0.90371 (4) 0.0242 (3)
O1 0.69151 (14) 0.31660 (18) 0.90951 (4) 0.0229 (2)
H1A 0.5821 0.3645 0.9071 0.034*
O4' −0.02923 (16) 0.27989 (18) 0.37824 (4) 0.0276 (3)
O3' 0.64995 (14) −0.31144 (17) 0.68320 (4) 0.0213 (2)
H3' 0.7590 −0.3523 0.6914 0.032*
O5' −0.20844 (14) 0.44237 (19) 0.42810 (4) 0.0253 (2)
O2' 0.89538 (14) 0.19376 (18) 0.63315 (4) 0.0246 (2)
O1' 0.32974 (14) 0.45702 (17) 0.66785 (4) 0.0208 (2)
H1A' 0.4302 0.5197 0.6722 0.031*
N1 1.11842 (16) 0.4299 (2) 0.84513 (4) 0.0190 (3)
N2' −0.05497 (17) 0.3612 (2) 0.41818 (5) 0.0200 (3)
C8' 0.3952 (2) 0.3245 (2) 0.53145 (5) 0.0186 (3)
N1' 0.67054 (17) 0.15506 (19) 0.69496 (5) 0.0182 (3)
N2 0.5662 (2) 0.4640 (2) 1.14448 (5) 0.0268 (3)
C11 0.6877 (2) 0.4734 (2) 1.10041 (6) 0.0230 (3)
C10 0.6000 (2) 0.5089 (3) 1.05377 (6) 0.0243 (3)
H10 0.4657 0.5303 1.0504 0.029*
C9 0.7149 (2) 0.5122 (3) 1.01205 (6) 0.0231 (3)
H9 0.6577 0.5391 0.9805 0.028*
C8 0.9165 (2) 0.4754 (2) 1.01693 (5) 0.0204 (3)
C4 1.0493 (2) 0.4734 (2) 0.97498 (5) 0.0203 (3)
H4 1.1813 0.4820 0.9848 0.024*
C2 1.0161 (2) 0.4615 (2) 0.92537 (5) 0.0182 (3)
C1 0.83077 (19) 0.4455 (2) 0.89178 (5) 0.0181 (3)
H1 0.7706 0.5712 0.8877 0.022*
C7A 0.9103 (2) 0.3801 (2) 0.84114 (5) 0.0184 (3)
H7C 0.8963 0.2421 0.8379 0.022*
C7 0.84455 (19) 0.4745 (3) 0.79203 (5) 0.0200 (3)
H7A 0.8157 0.6079 0.7970 0.024*
H7B 0.7298 0.4122 0.7770 0.024*
C6 1.0236 (2) 0.4485 (3) 0.75953 (5) 0.0197 (3)
H6 1.0251 0.3191 0.7460 0.024*
C12 0.8871 (2) 0.4445 (3) 1.10728 (6) 0.0242 (3)
H12 0.9440 0.4252 1.1392 0.029*
C13 0.9999 (2) 0.4452 (3) 1.06502 (6) 0.0224 (3)
H13 1.1343 0.4251 1.0689 0.027*
C5 1.2005 (2) 0.4771 (3) 0.79686 (5) 0.0219 (3)
H5A 1.3075 0.3927 0.7893 0.026*
H5B 1.2468 0.6073 0.7964 0.026*
C3 1.1863 (2) 0.4727 (2) 0.89175 (5) 0.0187 (3)
C11' 0.1040 (2) 0.3571 (2) 0.45687 (6) 0.0184 (3)
C10' 0.0645 (2) 0.4121 (2) 0.50562 (5) 0.0185 (3)
H10' −0.0580 0.4598 0.5130 0.022*
C9' 0.2104 (2) 0.3945 (2) 0.54290 (6) 0.0193 (3)
H9' 0.1857 0.4294 0.5757 0.023*
C4' 0.5558 (2) 0.2916 (2) 0.56866 (5) 0.0193 (3)
H4' 0.6804 0.2868 0.5558 0.023*
C2' 0.5490 (2) 0.2677 (2) 0.61826 (5) 0.0179 (3)
C3' 0.7287 (2) 0.2047 (2) 0.64785 (5) 0.0186 (3)
C5' 0.7559 (2) −0.0070 (2) 0.72222 (6) 0.0220 (3)
H5A' 0.7835 0.0247 0.7573 0.026*
H5B' 0.8765 −0.0475 0.7074 0.026*
C6' 0.5976 (2) −0.1640 (2) 0.71715 (5) 0.0190 (3)
H6' 0.5717 −0.2175 0.7502 0.023*
C7' 0.4137 (2) −0.0660 (3) 0.69485 (5) 0.0200 (3)
H7A' 0.3879 −0.1059 0.6603 0.024*
H7B' 0.3006 −0.0968 0.7142 0.024*
C7A' 0.4561 (2) 0.1466 (2) 0.69725 (5) 0.0176 (3)
H7C' 0.4138 0.1998 0.7291 0.021*
C1' 0.3793 (2) 0.2681 (2) 0.65274 (5) 0.0169 (3)
H1' 0.2651 0.2069 0.6362 0.020*
C13' 0.4305 (2) 0.2780 (2) 0.48130 (6) 0.0199 (3)
H13' 0.5548 0.2371 0.4732 0.024*
C12' 0.2860 (2) 0.2915 (2) 0.44377 (5) 0.0198 (3)
H12' 0.3100 0.2577 0.4108 0.024*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O4 0.0276 (6) 0.0393 (8) 0.0296 (6) 0.0024 (6) 0.0041 (4) 0.0055 (6)
O3 0.0216 (5) 0.0263 (6) 0.0200 (5) 0.0046 (5) 0.0061 (4) 0.0038 (5)
O5 0.0488 (7) 0.0514 (9) 0.0208 (6) −0.0125 (7) 0.0030 (5) −0.0045 (6)
O2 0.0145 (5) 0.0288 (7) 0.0290 (6) 0.0000 (5) −0.0015 (4) −0.0011 (5)
O1 0.0162 (5) 0.0249 (6) 0.0280 (5) −0.0014 (5) 0.0051 (4) 0.0020 (5)
O4' 0.0290 (6) 0.0305 (7) 0.0233 (5) −0.0010 (5) 0.0004 (4) −0.0059 (5)
O3' 0.0184 (5) 0.0207 (6) 0.0247 (5) 0.0009 (5) −0.0004 (4) −0.0056 (5)
O5' 0.0194 (5) 0.0293 (7) 0.0272 (5) 0.0044 (5) 0.0025 (4) 0.0036 (5)
O2' 0.0146 (5) 0.0271 (6) 0.0322 (5) 0.0012 (5) 0.0031 (4) 0.0004 (5)
O1' 0.0176 (5) 0.0155 (6) 0.0296 (5) 0.0005 (4) 0.0043 (4) −0.0030 (5)
N1 0.0135 (5) 0.0232 (7) 0.0204 (6) 0.0020 (6) 0.0018 (4) −0.0001 (6)
N2' 0.0218 (6) 0.0180 (7) 0.0205 (6) −0.0023 (6) 0.0027 (5) 0.0034 (5)
C8' 0.0214 (7) 0.0141 (8) 0.0205 (7) −0.0017 (6) 0.0036 (6) 0.0026 (6)
N1' 0.0153 (6) 0.0176 (7) 0.0215 (6) 0.0003 (5) −0.0026 (5) −0.0014 (5)
N2 0.0366 (7) 0.0233 (8) 0.0206 (6) 0.0000 (7) 0.0035 (5) 0.0014 (6)
C11 0.0309 (8) 0.0168 (9) 0.0216 (7) −0.0010 (7) 0.0046 (6) −0.0016 (7)
C10 0.0246 (7) 0.0254 (9) 0.0229 (7) 0.0033 (7) 0.0010 (6) −0.0015 (7)
C9 0.0272 (8) 0.0226 (9) 0.0192 (7) 0.0040 (7) −0.0011 (6) −0.0010 (7)
C8 0.0243 (7) 0.0162 (8) 0.0206 (7) −0.0016 (7) 0.0000 (5) −0.0024 (6)
C4 0.0184 (7) 0.0185 (9) 0.0238 (7) 0.0003 (6) −0.0015 (5) 0.0004 (7)
C2 0.0170 (7) 0.0159 (8) 0.0217 (7) 0.0015 (6) 0.0007 (5) 0.0016 (6)
C1 0.0160 (6) 0.0182 (8) 0.0201 (7) 0.0005 (6) 0.0013 (5) 0.0007 (7)
C7A 0.0146 (6) 0.0179 (8) 0.0228 (7) −0.0010 (6) 0.0003 (5) 0.0001 (6)
C7 0.0146 (6) 0.0249 (9) 0.0204 (7) 0.0008 (6) 0.0005 (5) 0.0005 (7)
C6 0.0190 (7) 0.0207 (8) 0.0194 (7) 0.0010 (7) 0.0018 (5) −0.0003 (7)
C12 0.0326 (8) 0.0200 (9) 0.0195 (7) −0.0045 (7) −0.0043 (6) 0.0007 (7)
C13 0.0231 (7) 0.0187 (8) 0.0251 (7) −0.0019 (7) −0.0023 (6) −0.0003 (7)
C5 0.0169 (7) 0.0283 (9) 0.0210 (7) 0.0003 (7) 0.0047 (5) −0.0013 (7)
C3 0.0187 (7) 0.0145 (8) 0.0228 (7) 0.0034 (6) −0.0004 (5) 0.0008 (6)
C11' 0.0200 (7) 0.0140 (8) 0.0214 (7) −0.0016 (6) 0.0014 (5) 0.0032 (6)
C10' 0.0181 (6) 0.0151 (8) 0.0226 (7) 0.0013 (6) 0.0057 (5) 0.0012 (6)
C9' 0.0226 (7) 0.0166 (8) 0.0192 (7) −0.0001 (6) 0.0048 (6) 0.0009 (6)
C4' 0.0176 (6) 0.0158 (8) 0.0248 (7) −0.0009 (6) 0.0056 (6) −0.0001 (6)
C2' 0.0164 (7) 0.0134 (8) 0.0239 (7) 0.0001 (6) 0.0012 (5) −0.0005 (6)
C3' 0.0173 (7) 0.0147 (8) 0.0238 (7) −0.0008 (6) 0.0002 (5) −0.0035 (7)
C5' 0.0217 (7) 0.0198 (9) 0.0240 (7) 0.0001 (7) −0.0054 (5) −0.0009 (7)
C6' 0.0202 (7) 0.0197 (9) 0.0172 (6) 0.0013 (7) 0.0014 (5) 0.0003 (6)
C7' 0.0181 (6) 0.0197 (8) 0.0222 (7) −0.0012 (7) −0.0014 (5) 0.0009 (7)
C7A' 0.0150 (6) 0.0200 (9) 0.0179 (7) 0.0002 (6) 0.0008 (5) −0.0025 (6)
C1' 0.0169 (7) 0.0149 (8) 0.0190 (6) 0.0007 (6) 0.0006 (5) −0.0032 (6)
C13' 0.0191 (7) 0.0171 (8) 0.0240 (7) 0.0018 (6) 0.0080 (6) 0.0031 (7)
C12' 0.0233 (7) 0.0181 (8) 0.0182 (6) −0.0003 (7) 0.0052 (6) 0.0004 (6)

Geometric parameters (Å, º)

O4—N2 1.2262 (18) C1—C7A 1.5439 (19)
O3—C6 1.414 (2) C1—H1 0.9800
O3—H3 0.8200 C7A—C7 1.518 (2)
O5—N2 1.2328 (18) C7A—H7C 0.9800
O2—C3 1.2321 (19) C7—C6 1.5374 (18)
O1—C1 1.4100 (19) C7—H7A 0.9700
O1—H1A 0.8200 C7—H7B 0.9700
O4'—N2' 1.2266 (18) C6—C5 1.5455 (19)
O3'—C6' 1.4316 (19) C6—H6 0.9800
O3'—H3' 0.8200 C12—C13 1.389 (2)
O5'—N2' 1.2319 (17) C12—H12 0.9300
O2'—C3' 1.2209 (18) C13—H13 0.9300
O1'—C1' 1.434 (2) C5—H5A 0.9700
O1'—H1A' 0.8200 C5—H5B 0.9700
N1—C3 1.3409 (19) C11'—C12' 1.384 (2)
N1—C5 1.4608 (18) C11'—C10' 1.391 (2)
N1—C7A 1.4637 (17) C10'—C9' 1.383 (2)
N2'—C11' 1.4657 (19) C10'—H10' 0.9300
C8'—C9' 1.400 (2) C9'—H9' 0.9300
C8'—C13' 1.405 (2) C4'—C2' 1.334 (2)
C8'—C4' 1.466 (2) C4'—H4' 0.9300
N1'—C3' 1.3760 (19) C2'—C3' 1.498 (2)
N1'—C5' 1.461 (2) C2'—C1' 1.5073 (19)
N1'—C7A' 1.4696 (17) C5'—C6' 1.549 (2)
N2—C11 1.4655 (19) C5'—H5A' 0.9700
C11—C10 1.379 (2) C5'—H5B' 0.9700
C11—C12 1.381 (2) C6'—C7' 1.531 (2)
C10—C9 1.386 (2) C6'—H6' 0.9800
C10—H10 0.9300 C7'—C7A' 1.526 (2)
C9—C8 1.402 (2) C7'—H7A' 0.9700
C9—H9 0.9300 C7'—H7B' 0.9700
C8—C13 1.396 (2) C7A'—C1' 1.537 (2)
C8—C4 1.467 (2) C7A'—H7C' 0.9800
C4—C2 1.333 (2) C1'—H1' 0.9800
C4—H4 0.9300 C13'—C12' 1.379 (2)
C2—C3 1.497 (2) C13'—H13' 0.9300
C2—C1 1.5236 (19) C12'—H12' 0.9300
C6—O3—H3 109.5 C12—C13—H13 119.2
C1—O1—H1A 109.5 C8—C13—H13 119.2
C6'—O3'—H3' 109.5 N1—C5—C6 102.60 (11)
C1'—O1'—H1A' 109.5 N1—C5—H5A 111.2
C3—N1—C5 129.22 (13) C6—C5—H5A 111.2
C3—N1—C7A 114.76 (11) N1—C5—H5B 111.2
C5—N1—C7A 113.38 (11) C6—C5—H5B 111.2
O4'—N2'—O5' 123.76 (13) H5A—C5—H5B 109.2
O4'—N2'—C11' 118.14 (12) O2—C3—N1 125.74 (13)
O5'—N2'—C11' 118.08 (12) O2—C3—C2 127.10 (13)
C9'—C8'—C13' 118.70 (13) N1—C3—C2 107.10 (12)
C9'—C8'—C4' 124.39 (13) C12'—C11'—C10' 122.56 (14)
C13'—C8'—C4' 116.89 (13) C12'—C11'—N2' 118.47 (13)
C3'—N1'—C5' 121.79 (13) C10'—C11'—N2' 118.92 (13)
C3'—N1'—C7A' 111.93 (11) C9'—C10'—C11' 118.88 (13)
C5'—N1'—C7A' 109.02 (12) C9'—C10'—H10' 120.6
O4—N2—O5 123.54 (13) C11'—C10'—H10' 120.6
O4—N2—C11 118.90 (12) C10'—C9'—C8' 120.32 (14)
O5—N2—C11 117.55 (13) C10'—C9'—H9' 119.8
C10—C11—C12 122.37 (14) C8'—C9'—H9' 119.8
C10—C11—N2 119.32 (14) C2'—C4'—C8' 129.29 (14)
C12—C11—N2 118.31 (13) C2'—C4'—H4' 115.4
C11—C10—C9 119.04 (15) C8'—C4'—H4' 115.4
C11—C10—H10 120.5 C4'—C2'—C3' 119.78 (13)
C9—C10—H10 120.5 C4'—C2'—C1' 131.40 (13)
C10—C9—C8 120.56 (14) C3'—C2'—C1' 108.31 (12)
C10—C9—H9 119.7 O2'—C3'—N1' 125.71 (13)
C8—C9—H9 119.7 O2'—C3'—C2' 127.20 (13)
C13—C8—C9 118.40 (14) N1'—C3'—C2' 107.07 (12)
C13—C8—C4 117.06 (13) N1'—C5'—C6' 104.55 (11)
C9—C8—C4 124.50 (13) N1'—C5'—H5A' 110.8
C2—C4—C8 131.99 (14) C6'—C5'—H5A' 110.8
C2—C4—H4 114.0 N1'—C5'—H5B' 110.8
C8—C4—H4 114.0 C6'—C5'—H5B' 110.8
C4—C2—C3 118.93 (13) H5A'—C5'—H5B' 108.9
C4—C2—C1 133.59 (13) O3'—C6'—C7' 107.72 (12)
C3—C2—C1 107.43 (11) O3'—C6'—C5' 112.42 (12)
O1—C1—C2 114.00 (12) C7'—C6'—C5' 105.71 (13)
O1—C1—C7A 111.46 (13) O3'—C6'—H6' 110.3
C2—C1—C7A 102.77 (11) C7'—C6'—H6' 110.3
O1—C1—H1 109.5 C5'—C6'—H6' 110.3
C2—C1—H1 109.5 C7A'—C7'—C6' 105.95 (12)
C7A—C1—H1 109.5 C7A'—C7'—H7A' 110.5
N1—C7A—C7 102.11 (11) C6'—C7'—H7A' 110.5
N1—C7A—C1 103.90 (11) C7A'—C7'—H7B' 110.5
C7—C7A—C1 121.27 (13) C6'—C7'—H7B' 110.5
N1—C7A—H7C 109.6 H7A'—C7'—H7B' 108.7
C7—C7A—H7C 109.6 N1'—C7A'—C7' 103.06 (12)
C1—C7A—H7C 109.6 N1'—C7A'—C1' 104.75 (11)
C7A—C7—C6 102.61 (11) C7'—C7A'—C1' 117.14 (12)
C7A—C7—H7A 111.2 N1'—C7A'—H7C' 110.5
C6—C7—H7A 111.2 C7'—C7A'—H7C' 110.5
C7A—C7—H7B 111.2 C1'—C7A'—H7C' 110.5
C6—C7—H7B 111.2 O1'—C1'—C2' 111.62 (12)
H7A—C7—H7B 109.2 O1'—C1'—C7A' 112.18 (11)
O3—C6—C5 113.29 (13) C2'—C1'—C7A' 102.81 (11)
O3—C6—C7 110.09 (12) O1'—C1'—H1' 110.0
C5—C6—C7 103.96 (11) C2'—C1'—H1' 110.0
O3—C6—H6 109.8 C7A'—C1'—H1' 110.0
C5—C6—H6 109.8 C12'—C13'—C8' 121.81 (13)
C7—C6—H6 109.8 C12'—C13'—H13' 119.1
C11—C12—C13 117.93 (14) C8'—C13'—H13' 119.1
C11—C12—H12 121.0 C13'—C12'—C11' 117.65 (13)
C13—C12—H12 121.0 C13'—C12'—H12' 121.2
C12—C13—C8 121.61 (14) C11'—C12'—H12' 121.2
O4—N2—C11—C10 26.1 (2) O4'—N2'—C11'—C12' 11.0 (2)
O5—N2—C11—C10 −154.96 (17) O5'—N2'—C11'—C12' −170.61 (15)
O4—N2—C11—C12 −153.41 (17) O4'—N2'—C11'—C10' −166.52 (15)
O5—N2—C11—C12 25.5 (2) O5'—N2'—C11'—C10' 11.9 (2)
C12—C11—C10—C9 1.3 (3) C12'—C11'—C10'—C9' −2.3 (2)
N2—C11—C10—C9 −178.18 (16) N2'—C11'—C10'—C9' 175.13 (14)
C11—C10—C9—C8 1.6 (3) C11'—C10'—C9'—C8' 0.7 (2)
C10—C9—C8—C13 −3.3 (3) C13'—C8'—C9'—C10' 1.8 (2)
C10—C9—C8—C4 179.20 (16) C4'—C8'—C9'—C10' −176.78 (15)
C13—C8—C4—C2 165.53 (19) C9'—C8'—C4'—C2' 20.8 (3)
C9—C8—C4—C2 −16.9 (3) C13'—C8'—C4'—C2' −157.82 (17)
C8—C4—C2—C3 177.05 (17) C8'—C4'—C2'—C3' 170.07 (16)
C8—C4—C2—C1 0.0 (3) C8'—C4'—C2'—C1' −0.8 (3)
C4—C2—C1—O1 −43.3 (3) C5'—N1'—C3'—O2' −36.3 (2)
C3—C2—C1—O1 139.45 (13) C7A'—N1'—C3'—O2' −167.84 (16)
C4—C2—C1—C7A −164.06 (19) C5'—N1'—C3'—C2' 141.93 (13)
C3—C2—C1—C7A 18.68 (16) C7A'—N1'—C3'—C2' 10.41 (17)
C3—N1—C7A—C7 140.96 (14) C4'—C2'—C3'—O2' 10.2 (3)
C5—N1—C7A—C7 −22.39 (18) C1'—C2'—C3'—O2' −177.00 (16)
C3—N1—C7A—C1 14.10 (18) C4'—C2'—C3'—N1' −168.00 (15)
C5—N1—C7A—C1 −149.25 (14) C1'—C2'—C3'—N1' 4.77 (17)
O1—C1—C7A—N1 −141.64 (12) C3'—N1'—C5'—C6' −103.79 (15)
C2—C1—C7A—N1 −19.14 (16) C7A'—N1'—C5'—C6' 28.93 (15)
O1—C1—C7A—C7 104.60 (16) N1'—C5'—C6'—O3' 107.05 (14)
C2—C1—C7A—C7 −132.91 (14) N1'—C5'—C6'—C7' −10.21 (15)
N1—C7A—C7—C6 36.32 (15) O3'—C6'—C7'—C7A' −131.16 (13)
C1—C7A—C7—C6 151.00 (14) C5'—C6'—C7'—C7A' −10.78 (15)
C7A—C7—C6—O3 −159.78 (13) C3'—N1'—C7A'—C7' 102.01 (14)
C7A—C7—C6—C5 −38.13 (16) C5'—N1'—C7A'—C7' −35.68 (14)
C10—C11—C12—C13 −2.3 (3) C3'—N1'—C7A'—C1' −21.04 (17)
N2—C11—C12—C13 177.18 (16) C5'—N1'—C7A'—C1' −158.73 (12)
C11—C12—C13—C8 0.5 (3) C6'—C7'—C7A'—N1' 27.53 (14)
C9—C8—C13—C12 2.2 (3) C6'—C7'—C7A'—C1' 141.91 (12)
C4—C8—C13—C12 179.95 (16) C4'—C2'—C1'—O1' −84.7 (2)
C3—N1—C5—C6 −161.69 (16) C3'—C2'—C1'—O1' 103.71 (14)
C7A—N1—C5—C6 −1.32 (18) C4'—C2'—C1'—C7A' 154.90 (17)
O3—C6—C5—N1 143.86 (13) C3'—C2'—C1'—C7A' −16.73 (15)
C7—C6—C5—N1 24.36 (16) N1'—C7A'—C1'—O1' −97.99 (13)
C5—N1—C3—O2 −19.5 (3) C7'—C7A'—C1'—O1' 148.58 (12)
C7A—N1—C3—O2 −179.69 (15) N1'—C7A'—C1'—C2' 22.06 (15)
C5—N1—C3—C2 157.98 (16) C7'—C7A'—C1'—C2' −91.37 (14)
C7A—N1—C3—C2 −2.17 (18) C9'—C8'—C13'—C12' −3.0 (2)
C4—C2—C3—O2 −11.3 (3) C4'—C8'—C13'—C12' 175.74 (15)
C1—C2—C3—O2 166.43 (16) C8'—C13'—C12'—C11' 1.5 (2)
C4—C2—C3—N1 171.22 (16) C10'—C11'—C12'—C13' 1.2 (2)
C1—C2—C3—N1 −11.05 (17) N2'—C11'—C12'—C13' −176.23 (14)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O3—H3···O1′i 0.82 1.93 2.7303 (14) 166
O1—H1A···O2ii 0.82 1.89 2.6993 (15) 169
O3′—H3′···O3iii 0.82 1.95 2.7585 (15) 171
O1′—H1A′···O3′iv 0.82 1.93 2.7451 (15) 174
C1′—H1′···O2′ii 0.98 2.52 3.3655 (17) 144
C1′—H1′···O5′v 0.98 2.55 3.3242 (19) 136
C10—H10···O1vi 0.93 2.54 3.126 (2) 121
C12′—H12′···O3′vii 0.93 2.57 3.5014 (18) 174
C13—H13···O4i 0.93 2.51 3.2644 (19) 138
C13′—H13′···O5′i 0.93 2.51 3.1160 (18) 123

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2525).

References

  1. Baumann, K. O. (2007). WO Patent 2007039286; Chem. Abstr. 146, 421836.
  2. Bruker (2010). APEX2, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  4. Freire, K. R. L., Tormena, C. F. & Coelho, F. (2011). Synlett, 14, 2059–2063.
  5. Hooft, R. W. W., Straver, L. H. & Spek, A. L. (2008). J. Appl. Cryst. 41, 96–103. [DOI] [PMC free article] [PubMed]
  6. Oliveira, F. L., Freire, K. R. L., Aparicio, R. & Coelho, F. (2012a). Acta Cryst. E68, o586. [DOI] [PMC free article] [PubMed]
  7. Oliveira, F. L., Freire, K. R. L., Aparicio, R. & Coelho, F. (2012b). Acta Cryst. E68, o587. [DOI] [PMC free article] [PubMed]
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  10. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

Associated Data

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

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812018235/pv2525sup1.cif

e-68-o1570-sup1.cif (36.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812018235/pv2525Isup2.hkl

e-68-o1570-Isup2.hkl (197.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812018235/pv2525Isup3.cml

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


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