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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jul 31;64(Pt 8):o1645. doi: 10.1107/S1600536808023611

3′,6′-Bis(ethyl­amino)-2-[(2-hydroxy­ethyl)­amino]-2′,7′-dimethylspiro­[isoindoline-1,9′-xanthen]-3-one

Mao-Zhong Tian a,*, Xiao-Jun Peng b
PMCID: PMC2962210  PMID: 21203332

Abstract

In the title compound, C28H32N4O3, the dihedral angle between the planes of the xanthene ring system and the spiro­lactam ring is 85.99 (3)°. Mol­ecules are linked by inter­molecular O—H⋯O and N—H⋯O hydrogen-bonding inter­actions.

Related literature

For the synthesis and related structures of rhodamine dyes, see: Ko et al. (2006); Wu et al. (2007); Zhang et al. (2008). For related literature on the photophysical properties and applications of rhodamine dyes, see: Lakowicz (2006).graphic file with name e-64-o1645-scheme1.jpg

Experimental

Crystal data

  • C28H32N4O3

  • M r = 472.58

  • Triclinic, Inline graphic

  • a = 9.3195 (18) Å

  • b = 9.4770 (16) Å

  • c = 15.384 (3) Å

  • α = 94.722 (18)°

  • β = 107.592 (13)°

  • γ = 98.924 (13)°

  • V = 1267.4 (4) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 298 (2) K

  • 0.30 × 0.20 × 0.15 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: none

  • 8770 measured reflections

  • 4305 independent reflections

  • 3144 reflections with I > 2σ(I)

  • R int = 0.024

Refinement

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.121

  • S = 1.06

  • 4305 reflections

  • 325 parameters

  • 4 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.34 e Å−3

  • Δρmin = −0.20 e Å−3

Data collection: APEX2 (Bruker 2005); cell refinement: APEX2; data reduction: APEX2; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808023611/zl2122sup1.cif

e-64-o1645-sup1.cif (26KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023611/zl2122Isup2.hkl

e-64-o1645-Isup2.hkl (210.9KB, 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
N3—H3A⋯O3i 0.898 (16) 2.185 (18) 3.044 (2) 160 (2)
O3—H3C⋯O1ii 0.82 1.98 2.770 (2) 162

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

Financial support in part by the Natural Science Foundation of China (20376010 and 20472012) and Shanxi Scholarship Council of China (200310) is gratefully acknowledged.

supplementary crystallographic information

Comment

Among many fluorescent compounds, rhodamine dyes are known to have excellent photophysical properties, (Lakowicz, 2006) and they are one of the most widely used fluorophores for labeling and sensing biomolecules (Ko et al., 2006; Wu et al., 2007). There are a few single-crystal reports about rhodamine derivatives bearing a lactam moiety (Wu et al., 2007; Zhang et al., 2008). Detailed information on their molecular and crystal structures is necessary to understand their photophysical and photochemical properties.

In agreement with other reported models, (Wu et al., 2007) the main skeleton of the title molecule is formed by the xanthene ring and the spirolactam-ring. As shown in Figure 1, the atoms of the xanthene ring and spirolactam-rings are both nearly planar and are almost perpendicular to each other. R.m.s. deviations from planarity are 0.028 (1) Å for the xanthene ring and 0.033 (0) Å for the spirolactam-ring, respectively. The dihedral angle between the planes of the xanthene ring and the spirolactam ring is 85.99 (3)°.

Analysis of the crystal packing of the title molecule (Figure 2), shows that the molecules of the title compound are connected via intermolecular N3—H3A···O3 and O3—H3C···O1 hydrogen bonds (Table 1). The oxygen atom on the spirolactam-ring acts as acceptor for an O—H···O hydrogen bond from a neighboring molecule. The oxygen atom of the hydroxyl group in turn acts as acceptor for a N—H···O hydrogen bond from again another molecule, thus forming a chain with two consecutive hydrogen bonds of the type N—H···O—H···O═C. Via these hydrogen bonds molecules are connected into double stranded chains as shown in Figure 2.

Experimental

Sodium borohydride (15.2 mg, 0.4 mmol) was slowly added to a solution of 3',6'-bis(ethylamino)-2',7'-dimethyl-2-(2-oxoethylideneamino)spiro [isoindoline-1,9'-xanthen]-3-one (132 mg, 0.3 mmol) in ethanol (20 ml). The reaction mixture was stirred for 2 h at room temperature and the solvent was totally removed under reduced pressure. The crude product was dissolved in CH2Cl2 (20 ml) and 3 ml of an aqueous solution of K2CO3 was added. The organic layer was separated and dried over MgSO4. After filtration, the solvent was removed under reduced pressure. The residue was placed on a silica gel column (200–300 mesh). The column was eluted with a mixture (2:1, v/v) of petroleum ether /ethyl acetate, to give 131.5 mg of the title compound (93%). Crystals were grown by dissolving the compound in CH2Cl2 and slowly diffusing n-hexane into the solution.

Refinement

Geometrically constrained hydrogen atoms were placed in calculated positions and refined using the riding model (C—H = 0.93-0.96 Å, and O—H = 0.82 Å), with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C, O). All amine hydrogen atoms were located in difference density Fourier maps, were introduced with a distance restraint (N—H = 0.89 (2) Å) and refined freely. The isotropic displacement parameter was set to Uiso(H) = 1.2Ueq(N).

Figures

Fig. 1.

Fig. 1.

The structure of the title compound, showing the atom-numbering scheme and displacement ellipsoids at the 30% probability level. H atoms are represented as small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

The molecular packing of the title compound showing the double stranded hydrogen bond connected chains. Dashed lines indicate hydrogen bonds.

Crystal data

C28H32N4O3 Z = 2
Mr = 472.58 F000 = 504
Triclinic, P1 Dx = 1.238 Mg m3
Hall symbol: -P 1 Mo Kα radiation λ = 0.71073 Å
a = 9.3195 (18) Å Cell parameters from 2583 reflections
b = 9.4770 (16) Å θ = 2.3–26.8º
c = 15.384 (3) Å µ = 0.08 mm1
α = 94.722 (18)º T = 298 (2) K
β = 107.592 (13)º Block, colourless
γ = 98.924 (13)º 0.30 × 0.20 × 0.15 mm
V = 1267.4 (4) Å3

Data collection

Bruker APEXII CCD area-detector diffractometer 3144 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.024
Monochromator: graphite θmax = 25.0º
T = 298(2) K θmin = 2.2º
φ and ω scans h = −11→11
Absorption correction: none k = −11→11
8770 measured reflections l = −18→18
4305 independent reflections

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)] = 0.045 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.121   w = 1/[σ2(Fo2) + (0.068P)2 + 0.1313P] where P = (Fo2 + 2Fc2)/3
S = 1.07 (Δ/σ)max < 0.001
4305 reflections Δρmax = 0.34 e Å3
325 parameters Δρmin = −0.19 e Å3
4 restraints Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.028 (8)

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2σ(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
O2 0.69421 (15) 0.29618 (12) 0.25724 (9) 0.0457 (3)
C16 0.8939 (2) 0.3280 (2) 0.19461 (12) 0.0433 (5)
H16A 0.8966 0.2307 0.1971 0.052*
C14 0.5894 (2) 0.35022 (18) 0.29116 (11) 0.0364 (4)
C10 0.4573 (2) 0.52933 (18) 0.32506 (12) 0.0393 (4)
H10A 0.4422 0.6240 0.3249 0.047*
C9 0.5676 (2) 0.49027 (17) 0.28839 (11) 0.0346 (4)
C20 0.7802 (2) 0.53260 (18) 0.22210 (11) 0.0353 (4)
N1 0.73649 (16) 0.72826 (14) 0.32209 (9) 0.0371 (4)
C8 0.66223 (19) 0.59937 (17) 0.25166 (11) 0.0342 (4)
C15 0.7889 (2) 0.38924 (18) 0.22530 (11) 0.0374 (4)
C13 0.5043 (2) 0.25175 (19) 0.32712 (13) 0.0441 (5)
H13A 0.5219 0.1578 0.3280 0.053*
C17 0.9953 (2) 0.4115 (2) 0.16000 (12) 0.0443 (5)
C19 0.8840 (2) 0.6140 (2) 0.18778 (12) 0.0425 (4)
H19A 0.8801 0.7111 0.1853 0.051*
C11 0.3697 (2) 0.43659 (19) 0.36141 (12) 0.0410 (4)
O1 0.72540 (17) 0.96667 (13) 0.35009 (10) 0.0621 (4)
N4 1.0976 (2) 0.3528 (2) 0.12588 (12) 0.0589 (5)
H4A 1.175 (2) 0.413 (2) 0.1209 (16) 0.071*
C7 0.56703 (19) 0.67124 (18) 0.17571 (11) 0.0354 (4)
C12 0.3930 (2) 0.29227 (19) 0.36189 (12) 0.0431 (5)
C18 0.9910 (2) 0.5596 (2) 0.15757 (12) 0.0449 (5)
N2 0.82046 (17) 0.70879 (16) 0.41102 (10) 0.0422 (4)
H2A 0.787 (2) 0.7625 (19) 0.4486 (12) 0.051*
C2 0.5870 (2) 0.81693 (19) 0.20269 (12) 0.0414 (4)
N3 0.3075 (2) 0.19768 (18) 0.39963 (14) 0.0619 (5)
H3A 0.216 (2) 0.216 (2) 0.3996 (16) 0.074*
C21 0.2564 (3) 0.4877 (2) 0.40272 (15) 0.0576 (5)
H21A 0.2557 0.5875 0.3962 0.086*
H21B 0.2854 0.4766 0.4668 0.086*
H21C 0.1559 0.4317 0.3714 0.086*
C1 0.6898 (2) 0.85141 (18) 0.29889 (13) 0.0422 (4)
C6 0.4744 (2) 0.6098 (2) 0.08895 (12) 0.0443 (5)
H6A 0.4597 0.5111 0.0707 0.053*
C26 1.1000 (3) 0.6534 (2) 0.12199 (15) 0.0609 (6)
H26A 1.0818 0.7503 0.1259 0.091*
H26B 1.0843 0.6173 0.0590 0.091*
H26C 1.2035 0.6524 0.1584 0.091*
C5 0.4036 (2) 0.6986 (3) 0.02931 (13) 0.0561 (6)
H5A 0.3403 0.6588 −0.0297 0.067*
C4 0.4252 (3) 0.8445 (3) 0.05583 (15) 0.0609 (6)
H4B 0.3777 0.9021 0.0142 0.073*
C3 0.5162 (3) 0.9066 (2) 0.14321 (15) 0.0565 (6)
H3B 0.5299 1.0050 0.1617 0.068*
C22 0.3242 (3) 0.0484 (2) 0.40404 (18) 0.0770 (7)
H22A 0.2842 0.0130 0.4511 0.092*
H22B 0.4325 0.0445 0.4227 0.092*
C25 1.2242 (4) 0.1710 (4) 0.0779 (2) 0.1053 (11)
H25A 1.2292 0.0705 0.0766 0.158*
H25B 1.3230 0.2277 0.1123 0.158*
H25C 1.1947 0.1941 0.0161 0.158*
C24 1.1072 (3) 0.2038 (3) 0.12294 (18) 0.0750 (7)
H24A 1.0077 0.1456 0.0886 0.090*
H24B 1.1361 0.1791 0.1850 0.090*
C23 0.2464 (4) −0.0473 (3) 0.3172 (2) 0.1070 (11)
H23A 0.2638 −0.1433 0.3251 0.160*
H23B 0.2859 −0.0138 0.2703 0.160*
H23C 0.1383 −0.0475 0.2995 0.160*
C28 1.0649 (2) 0.7337 (2) 0.52897 (13) 0.0526 (5)
H28A 1.0422 0.6325 0.5356 0.063*
H28B 1.1749 0.7618 0.5430 0.063*
C27 0.9862 (2) 0.7548 (2) 0.43216 (13) 0.0529 (5)
H27A 1.0096 0.8557 0.4249 0.063*
H27B 1.0219 0.6986 0.3901 0.063*
O3 1.01619 (16) 0.81677 (16) 0.59124 (9) 0.0627 (4)
H3C 1.0814 0.8896 0.6149 0.094*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O2 0.0503 (8) 0.0360 (7) 0.0620 (8) 0.0138 (6) 0.0308 (7) 0.0100 (6)
C16 0.0461 (11) 0.0459 (10) 0.0416 (10) 0.0196 (9) 0.0147 (9) 0.0048 (8)
C14 0.0355 (10) 0.0375 (9) 0.0364 (9) 0.0076 (8) 0.0123 (8) 0.0030 (7)
C10 0.0409 (11) 0.0355 (9) 0.0440 (10) 0.0087 (8) 0.0167 (9) 0.0051 (8)
C9 0.0357 (10) 0.0342 (9) 0.0333 (9) 0.0050 (7) 0.0111 (8) 0.0036 (7)
C20 0.0347 (10) 0.0390 (9) 0.0325 (9) 0.0078 (8) 0.0112 (8) 0.0025 (7)
N1 0.0386 (9) 0.0354 (8) 0.0364 (8) 0.0039 (6) 0.0131 (7) 0.0015 (6)
C8 0.0358 (10) 0.0333 (9) 0.0336 (9) 0.0051 (7) 0.0130 (8) 0.0004 (7)
C15 0.0368 (10) 0.0412 (10) 0.0336 (9) 0.0080 (8) 0.0103 (8) 0.0037 (7)
C13 0.0489 (12) 0.0335 (9) 0.0525 (11) 0.0073 (8) 0.0196 (9) 0.0089 (8)
C17 0.0381 (11) 0.0623 (12) 0.0342 (10) 0.0176 (9) 0.0109 (8) 0.0021 (8)
C19 0.0421 (11) 0.0439 (10) 0.0447 (10) 0.0081 (8) 0.0184 (9) 0.0069 (8)
C11 0.0392 (11) 0.0430 (10) 0.0431 (10) 0.0052 (8) 0.0183 (9) 0.0043 (8)
O1 0.0694 (10) 0.0368 (7) 0.0717 (10) 0.0053 (7) 0.0168 (8) −0.0085 (7)
N4 0.0516 (12) 0.0751 (13) 0.0613 (11) 0.0260 (10) 0.0282 (9) 0.0067 (9)
C7 0.0344 (10) 0.0409 (9) 0.0361 (9) 0.0091 (7) 0.0170 (8) 0.0082 (7)
C12 0.0442 (11) 0.0432 (10) 0.0431 (10) 0.0024 (8) 0.0181 (9) 0.0078 (8)
C18 0.0409 (11) 0.0559 (11) 0.0405 (10) 0.0086 (9) 0.0177 (9) 0.0042 (8)
N2 0.0365 (9) 0.0524 (9) 0.0341 (8) 0.0025 (7) 0.0100 (7) 0.0016 (7)
C2 0.0420 (11) 0.0412 (10) 0.0465 (11) 0.0110 (8) 0.0193 (9) 0.0103 (8)
N3 0.0665 (13) 0.0475 (10) 0.0872 (13) 0.0061 (9) 0.0472 (11) 0.0188 (9)
C21 0.0587 (14) 0.0569 (12) 0.0715 (14) 0.0131 (10) 0.0391 (12) 0.0143 (10)
C1 0.0452 (11) 0.0318 (9) 0.0529 (11) 0.0036 (8) 0.0229 (9) 0.0030 (8)
C6 0.0424 (11) 0.0547 (11) 0.0391 (10) 0.0133 (9) 0.0165 (9) 0.0034 (8)
C26 0.0521 (13) 0.0742 (14) 0.0654 (14) 0.0082 (11) 0.0337 (11) 0.0098 (11)
C5 0.0484 (13) 0.0871 (16) 0.0380 (11) 0.0237 (11) 0.0157 (9) 0.0102 (10)
C4 0.0665 (15) 0.0788 (16) 0.0540 (13) 0.0355 (12) 0.0269 (12) 0.0315 (11)
C3 0.0665 (14) 0.0491 (11) 0.0667 (14) 0.0234 (10) 0.0304 (12) 0.0209 (10)
C22 0.092 (2) 0.0648 (15) 0.0916 (19) 0.0074 (13) 0.0534 (16) 0.0264 (13)
C25 0.099 (2) 0.125 (2) 0.117 (2) 0.064 (2) 0.0545 (19) −0.0001 (19)
C24 0.0710 (17) 0.0829 (17) 0.0834 (17) 0.0393 (14) 0.0322 (14) 0.0044 (13)
C23 0.139 (3) 0.0716 (18) 0.117 (3) −0.0130 (18) 0.070 (2) 0.0006 (17)
C28 0.0421 (12) 0.0554 (12) 0.0539 (12) 0.0079 (9) 0.0088 (10) −0.0005 (9)
C27 0.0392 (12) 0.0676 (13) 0.0495 (12) 0.0039 (10) 0.0148 (9) 0.0041 (9)
O3 0.0519 (9) 0.0710 (9) 0.0563 (9) −0.0028 (7) 0.0162 (7) −0.0104 (7)

Geometric parameters (Å, °)

O2—C15 1.375 (2) C2—C1 1.477 (3)
O2—C14 1.381 (2) N3—C22 1.452 (3)
C16—C15 1.388 (2) N3—H3A 0.898 (16)
C16—C17 1.394 (3) C21—H21A 0.9600
C16—H16A 0.9300 C21—H21B 0.9600
C14—C9 1.376 (2) C21—H21C 0.9600
C14—C13 1.388 (3) C6—C5 1.385 (3)
C10—C11 1.373 (3) C6—H6A 0.9300
C10—C9 1.395 (2) C26—H26A 0.9600
C10—H10A 0.9300 C26—H26B 0.9600
C9—C8 1.510 (2) C26—H26C 0.9600
C20—C15 1.378 (2) C5—C4 1.375 (3)
C20—C19 1.397 (2) C5—H5A 0.9300
C20—C8 1.512 (2) C4—C3 1.378 (3)
N1—C1 1.346 (2) C4—H4B 0.9300
N1—N2 1.399 (2) C3—H3B 0.9300
N1—C8 1.487 (2) C22—C23 1.464 (4)
C8—C7 1.519 (2) C22—H22A 0.9700
C13—C12 1.391 (3) C22—H22B 0.9700
C13—H13A 0.9300 C25—C24 1.514 (3)
C17—N4 1.383 (2) C25—H25A 0.9600
C17—C18 1.413 (3) C25—H25B 0.9600
C19—C18 1.370 (2) C25—H25C 0.9600
C19—H19A 0.9300 C24—H24A 0.9700
C11—C12 1.418 (2) C24—H24B 0.9700
C11—C21 1.506 (2) C23—H23A 0.9600
O1—C1 1.229 (2) C23—H23B 0.9600
N4—C24 1.426 (3) C23—H23C 0.9600
N4—H4A 0.872 (16) C28—O3 1.412 (2)
C7—C6 1.373 (2) C28—C27 1.493 (3)
C7—C2 1.376 (2) C28—H28A 0.9700
C12—N3 1.386 (2) C28—H28B 0.9700
C18—C26 1.502 (3) C27—H27A 0.9700
N2—C27 1.465 (2) C27—H27B 0.9700
N2—H2A 0.892 (14) O3—H3C 0.8200
C2—C3 1.390 (3)
C15—O2—C14 118.45 (13) H21A—C21—H21B 109.5
C15—C16—C17 120.39 (17) C11—C21—H21C 109.5
C15—C16—H16A 119.8 H21A—C21—H21C 109.5
C17—C16—H16A 119.8 H21B—C21—H21C 109.5
C9—C14—O2 123.10 (16) O1—C1—N1 125.40 (18)
C9—C14—C13 121.84 (16) O1—C1—C2 128.51 (17)
O2—C14—C13 115.05 (15) N1—C1—C2 106.06 (14)
C11—C10—C9 124.05 (16) C7—C6—C5 118.23 (18)
C11—C10—H10A 118.0 C7—C6—H6A 120.9
C9—C10—H10A 118.0 C5—C6—H6A 120.9
C14—C9—C10 116.65 (16) C18—C26—H26A 109.5
C14—C9—C8 122.29 (15) C18—C26—H26B 109.5
C10—C9—C8 121.01 (14) H26A—C26—H26B 109.5
C15—C20—C19 116.72 (16) C18—C26—H26C 109.5
C15—C20—C8 122.27 (16) H26A—C26—H26C 109.5
C19—C20—C8 120.99 (15) H26B—C26—H26C 109.5
C1—N1—N2 124.66 (14) C4—C5—C6 121.15 (19)
C1—N1—C8 114.93 (14) C4—C5—H5A 119.4
N2—N1—C8 118.93 (13) C6—C5—H5A 119.4
N1—C8—C9 110.24 (13) C5—C4—C3 120.93 (19)
N1—C8—C20 111.05 (13) C5—C4—H4B 119.5
C9—C8—C20 110.54 (13) C3—C4—H4B 119.5
N1—C8—C7 99.20 (12) C4—C3—C2 117.61 (19)
C9—C8—C7 113.69 (14) C4—C3—H3B 121.2
C20—C8—C7 111.64 (13) C2—C3—H3B 121.2
O2—C15—C20 123.17 (15) N3—C22—C23 114.1 (2)
O2—C15—C16 115.15 (15) N3—C22—H22A 108.7
C20—C15—C16 121.68 (17) C23—C22—H22A 108.7
C14—C13—C12 120.58 (16) N3—C22—H22B 108.7
C14—C13—H13A 119.7 C23—C22—H22B 108.7
C12—C13—H13A 119.7 H22A—C22—H22B 107.6
N4—C17—C16 121.86 (18) C24—C25—H25A 109.5
N4—C17—C18 118.95 (18) C24—C25—H25B 109.5
C16—C17—C18 119.18 (16) H25A—C25—H25B 109.5
C18—C19—C20 124.05 (17) C24—C25—H25C 109.5
C18—C19—H19A 118.0 H25A—C25—H25C 109.5
C20—C19—H19A 118.0 H25B—C25—H25C 109.5
C10—C11—C12 117.97 (16) N4—C24—C25 110.7 (2)
C10—C11—C21 121.09 (16) N4—C24—H24A 109.5
C12—C11—C21 120.90 (16) C25—C24—H24A 109.5
C17—N4—C24 123.02 (19) N4—C24—H24B 109.5
C17—N4—H4A 116.6 (15) C25—C24—H24B 109.5
C24—N4—H4A 118.1 (15) H24A—C24—H24B 108.1
C6—C7—C2 120.62 (16) C22—C23—H23A 109.5
C6—C7—C8 128.39 (15) C22—C23—H23B 109.5
C2—C7—C8 110.96 (15) H23A—C23—H23B 109.5
N3—C12—C13 122.25 (17) C22—C23—H23C 109.5
N3—C12—C11 118.83 (17) H23A—C23—H23C 109.5
C13—C12—C11 118.89 (16) H23B—C23—H23C 109.5
C19—C18—C17 117.97 (17) O3—C28—C27 110.65 (16)
C19—C18—C26 121.36 (18) O3—C28—H28A 109.5
C17—C18—C26 120.67 (17) C27—C28—H28A 109.5
N1—N2—C27 113.12 (14) O3—C28—H28B 109.5
N1—N2—H2A 105.2 (12) C27—C28—H28B 109.5
C27—N2—H2A 109.7 (13) H28A—C28—H28B 108.1
C7—C2—C3 121.43 (18) N2—C27—C28 109.01 (16)
C7—C2—C1 108.54 (15) N2—C27—H27A 109.9
C3—C2—C1 130.03 (17) C28—C27—H27A 109.9
C12—N3—C22 122.85 (18) N2—C27—H27B 109.9
C12—N3—H3A 117.2 (16) C28—C27—H27B 109.9
C22—N3—H3A 115.2 (16) H27A—C27—H27B 108.3
C11—C21—H21A 109.5 C28—O3—H3C 109.5
C11—C21—H21B 109.5
C15—O2—C14—C9 4.9 (2) C9—C8—C7—C6 −65.7 (2)
C15—O2—C14—C13 −176.33 (15) C20—C8—C7—C6 60.2 (2)
O2—C14—C9—C10 179.82 (15) N1—C8—C7—C2 −0.61 (17)
C13—C14—C9—C10 1.1 (3) C9—C8—C7—C2 116.38 (16)
O2—C14—C9—C8 −2.9 (3) C20—C8—C7—C2 −117.72 (16)
C13—C14—C9—C8 178.39 (15) C14—C13—C12—N3 −178.99 (18)
C11—C10—C9—C14 −1.2 (3) C14—C13—C12—C11 −1.1 (3)
C11—C10—C9—C8 −178.52 (16) C10—C11—C12—N3 178.97 (18)
C1—N1—C8—C9 −115.45 (16) C21—C11—C12—N3 1.2 (3)
N2—N1—C8—C9 51.36 (19) C10—C11—C12—C13 1.0 (3)
C1—N1—C8—C20 121.68 (16) C21—C11—C12—C13 −176.80 (17)
N2—N1—C8—C20 −71.50 (18) C20—C19—C18—C17 1.0 (3)
C1—N1—C8—C7 4.12 (17) C20—C19—C18—C26 −179.60 (17)
N2—N1—C8—C7 170.93 (14) N4—C17—C18—C19 177.03 (17)
C14—C9—C8—N1 −124.27 (17) C16—C17—C18—C19 −1.4 (3)
C10—C9—C8—N1 52.9 (2) N4—C17—C18—C26 −2.4 (3)
C14—C9—C8—C20 −1.1 (2) C16—C17—C18—C26 179.15 (17)
C10—C9—C8—C20 176.09 (14) C1—N1—N2—C27 −86.1 (2)
C14—C9—C8—C7 125.37 (17) C8—N1—N2—C27 108.48 (17)
C10—C9—C8—C7 −57.4 (2) C6—C7—C2—C3 −0.8 (3)
C15—C20—C8—N1 125.88 (17) C8—C7—C2—C3 177.32 (17)
C19—C20—C8—N1 −55.7 (2) C6—C7—C2—C1 179.23 (16)
C15—C20—C8—C9 3.2 (2) C8—C7—C2—C1 −2.6 (2)
C19—C20—C8—C9 −178.44 (15) C13—C12—N3—C22 −1.5 (3)
C15—C20—C8—C7 −124.42 (17) C11—C12—N3—C22 −179.4 (2)
C19—C20—C8—C7 54.0 (2) N2—N1—C1—O1 6.8 (3)
C14—O2—C15—C20 −2.7 (2) C8—N1—C1—O1 172.78 (17)
C14—O2—C15—C16 178.35 (14) N2—N1—C1—C2 −171.77 (15)
C19—C20—C15—O2 −179.92 (15) C8—N1—C1—C2 −5.82 (19)
C8—C20—C15—O2 −1.5 (3) C7—C2—C1—O1 −173.45 (19)
C19—C20—C15—C16 −1.0 (2) C3—C2—C1—O1 6.6 (3)
C8—C20—C15—C16 177.45 (15) C7—C2—C1—N1 5.1 (2)
C17—C16—C15—O2 179.53 (15) C3—C2—C1—N1 −174.85 (19)
C17—C16—C15—C20 0.5 (3) C2—C7—C6—C5 0.8 (3)
C9—C14—C13—C12 0.0 (3) C8—C7—C6—C5 −177.00 (17)
O2—C14—C13—C12 −178.83 (15) C7—C6—C5—C4 0.1 (3)
C15—C16—C17—N4 −177.69 (16) C6—C5—C4—C3 −1.0 (3)
C15—C16—C17—C18 0.7 (3) C5—C4—C3—C2 1.0 (3)
C15—C20—C19—C18 0.2 (3) C7—C2—C3—C4 −0.1 (3)
C8—C20—C19—C18 −178.24 (16) C1—C2—C3—C4 179.86 (19)
C9—C10—C11—C12 0.2 (3) C12—N3—C22—C23 −79.0 (3)
C9—C10—C11—C21 177.93 (17) C17—N4—C24—C25 177.3 (2)
C16—C17—N4—C24 0.3 (3) N1—N2—C27—C28 178.42 (14)
C18—C17—N4—C24 −178.14 (19) O3—C28—C27—N2 −60.6 (2)
N1—C8—C7—C6 177.36 (17)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N3—H3A···O3i 0.898 (16) 2.185 (18) 3.044 (2) 160 (2)
O3—H3C···O1ii 0.82 1.98 2.770 (2) 162

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZL2122).

References

  1. Bruker (2005). APEX2 Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Ko, S.-K., Yang, Y.-K., Tae, J. & Shin, I. (2006). J. Am. Chem. Soc.128, 14150–14155. [DOI] [PubMed]
  3. Lakowicz, J. R. (2006). TITLE? 3rd ed., p. 67. New York:Springer.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Wu, D., Huang, W., Duan, C.-Y., Lin, Z.-H. & Meng, Q.-J. (2007). Inorg. Chem.46, 1538–1540. [DOI] [PubMed]
  6. Zhang, L.-Z., Peng, X.-J., Gao, S. & Fan, J.-L. (2008). Acta Cryst. E64, o403. [DOI] [PMC free article] [PubMed]

Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808023611/zl2122sup1.cif

e-64-o1645-sup1.cif (26KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808023611/zl2122Isup2.hkl

e-64-o1645-Isup2.hkl (210.9KB, 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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