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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 13;67(Pt 5):o1107. doi: 10.1107/S1600536811010944

7-Diethyl­amino-2-oxo-2H-chromene-3-carbohydrazide

Li-Jun Zhang a, Bing-Zhu Yin a,*
PMCID: PMC3089128  PMID: 21754425

Abstract

The asymmetric unit of the title compound, C14H17N3O3, contains two independent mol­ecules with different conformations of the ethyl groups. In the crystal, inter­molecular N—H⋯O hydrogen bonds link the mol­ecules into ribbons extending along the a axis.

Related literature

For the bioactivity and chemiluminescence of coumarin derivatives, see: Munasinghe et al. (2007). For a related structure, see: Yu et al. (2009). For details of the synthesis, see: Ma et al. (2010).graphic file with name e-67-o1107-scheme1.jpg

Experimental

Crystal data

  • C14H17N3O3

  • M r = 275.31

  • Triclinic, Inline graphic

  • a = 9.3438 (19) Å

  • b = 12.771 (3) Å

  • c = 12.978 (3) Å

  • α = 95.17 (3)°

  • β = 110.13 (3)°

  • γ = 106.18 (3)°

  • V = 1366.4 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 290 K

  • 0.14 × 0.12 × 0.11 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.987, T max = 0.990

  • 13506 measured reflections

  • 6186 independent reflections

  • 3402 reflections with I > 2σ(I)

  • R int = 0.030

Refinement

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.117

  • S = 1.01

  • 6186 reflections

  • 383 parameters

  • 6 restraints

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

  • Δρmax = 0.18 e Å−3

  • Δρmin = −0.19 e Å−3

Data collection: RAPID-AUTO (Rigaku Corporation, 1998); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC & Rigaku Corporation, 2002); 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: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811010944/cv5061sup1.cif

e-67-o1107-sup1.cif (23.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010944/cv5061Isup2.hkl

e-67-o1107-Isup2.hkl (302.8KB, 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
N2—H2⋯O2 0.86 (3) 2.01 (2) 2.7098 (18) 137 (2)
N5—H5⋯O5 0.87 (3) 2.03 (2) 2.733 (2) 138 (2)
N6—H6B⋯O3 0.86 (3) 2.30 (1) 3.131 (2) 164 (2)
N3—H3A⋯O3i 0.87 (3) 2.20 (1) 3.002 (2) 155 (2)
N3—H3B⋯O6ii 0.87 (3) 2.23 (1) 3.039 (2) 154 (2)

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

Acknowledgments

The authors acknowledge financial support from the National Natural Science Foundation of China (grant No. 21062022) and the Open Project of the State Key Laboratory of Supra­molecular Structure and Materials, Jilin University.

supplementary crystallographic information

Comment

Coumarin derivatives have received considerable attention since their diverse bioactivities and chemiluminescence (Munasinghe et al. 2007). Herein, we report the crystal structure of the title compound, an important organic intermediate and a fluorescent tagging agent for chemosensors.

In the title compound, all bond lengths and angles are normal and comparable to those observed in the related struture (Yu et al., 2009). There are two independent molecules in the asymmetric unit with different conformation of the ethyl groups (Fig. 1). Except for four terminal carbon atoms, the other non-hydrogen atoms are nearly coplanar for two components [mean deviations from the mean planes are 0.065 (1) and 0.07 (1), respectively] and form an angle of 19.39 (4) °. Intermolecuar N—H···O hydrogen bonds (Table 1) link the molecules into ribbons extended along axis a.

Experimental

The title compound was prepared according to the literature (Ma et al., 2010). Single crystals suitable for X-ray diffraction were prepared by slow evaporation a mixture of dichloromethane and petroleum (60–90 °C) at room temperature.

Refinement

C-bound H-atoms were placed in calculated positions with C—H = 0.93, 096 or 0.97 Å and were included in the refinement in the riding model with Uiso(H) = 1.2 or 1.5 Ueq(C). The H of nitrogen atom were located from differecne Fourier Map and refined with N—H bond lengths restrained to 0.87 (3) Å, and with Uiso(H) = 1.5 Ueq(N).

Figures

Fig. 1.

Fig. 1.

Two independent molecules of the title compound, with the atom numbering. Displacement ellipsoids of non-H atoms are drawn at the 30% probalility level.

Crystal data

C14H17N3O3 Z = 4
Mr = 275.31 F(000) = 584
Triclinic, P1 Dx = 1.338 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.3438 (19) Å Cell parameters from 8202 reflections
b = 12.771 (3) Å θ = 3.2–27.5°
c = 12.978 (3) Å µ = 0.10 mm1
α = 95.17 (3)° T = 290 K
β = 110.13 (3)° Block, yellow
γ = 106.18 (3)° 0.14 × 0.12 × 0.11 mm
V = 1366.4 (5) Å3

Data collection

Rigaku R-AXIS RAPID diffractometer 6186 independent reflections
Radiation source: fine-focus sealed tube 3402 reflections with I > 2σ(I)
graphite Rint = 0.030
ω scans θmax = 27.5°, θmin = 3.2°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) h = −12→10
Tmin = 0.987, Tmax = 0.990 k = −16→16
13506 measured reflections l = −16→16

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)] = 0.045 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.117 H atoms treated by a mixture of independent and constrained refinement
S = 1.01 w = 1/[σ2(Fo2) + (0.0543P)2] where P = (Fo2 + 2Fc2)/3
6186 reflections (Δ/σ)max = 0.005
383 parameters Δρmax = 0.18 e Å3
6 restraints Δρmin = −0.19 e Å3

Special details

Experimental. (See detailed section in the paper)
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
C1 0.21139 (18) 0.57501 (13) 1.19989 (14) 0.0463 (4)
C2 0.13466 (18) 0.48762 (12) 1.24574 (13) 0.0436 (4)
C3 0.13127 (19) 0.50961 (13) 1.35921 (14) 0.0492 (4)
C4 0.06725 (18) 0.38172 (12) 1.18533 (13) 0.0463 (4)
H4 0.0150 0.3265 1.2146 0.056*
C5 0.07300 (18) 0.35191 (12) 1.08046 (13) 0.0443 (4)
C6 0.15295 (17) 0.43610 (12) 1.03866 (13) 0.0426 (4)
C7 0.17389 (18) 0.41745 (13) 0.93993 (14) 0.0494 (4)
H7 0.2289 0.4764 0.9159 0.059*
C8 0.11153 (18) 0.30841 (13) 0.87521 (13) 0.0484 (4)
C9 0.02840 (19) 0.22172 (13) 0.91645 (14) 0.0524 (4)
H9 −0.0144 0.1489 0.8754 0.063*
C10 0.01086 (19) 0.24390 (13) 1.01450 (14) 0.0516 (4)
H10 −0.0443 0.1855 1.0391 0.062*
C11 0.0769 (2) 0.17291 (15) 0.71424 (16) 0.0645 (5)
H11A 0.0960 0.1239 0.7666 0.077*
H11B 0.1411 0.1699 0.6698 0.077*
C12 −0.0988 (2) 0.13259 (17) 0.63824 (16) 0.0768 (6)
H12A −0.1625 0.1375 0.6817 0.115*
H12B −0.1295 0.0565 0.6013 0.115*
H12C −0.1168 0.1780 0.5832 0.115*
C13 0.2090 (2) 0.37670 (15) 0.72996 (15) 0.0640 (5)
H13A 0.1828 0.4430 0.7462 0.077*
H13B 0.1687 0.3532 0.6491 0.077*
C14 0.3890 (2) 0.40375 (17) 0.77862 (19) 0.0777 (6)
H14A 0.4301 0.4333 0.8577 0.116*
H14B 0.4371 0.4580 0.7430 0.116*
H14C 0.4149 0.3373 0.7662 0.116*
C15 0.2466 (2) 0.11381 (14) 1.16812 (14) 0.0526 (4)
C16 0.36577 (19) 0.22392 (14) 1.21170 (14) 0.0506 (4)
C17 0.3901 (2) 0.29587 (15) 1.31736 (15) 0.0556 (4)
C18 0.4607 (2) 0.26342 (14) 1.15444 (14) 0.0544 (4)
H18 0.5359 0.3349 1.1819 0.065*
C19 0.44932 (19) 0.20030 (13) 1.05563 (14) 0.0493 (4)
C20 0.33527 (18) 0.09381 (13) 1.01525 (13) 0.0466 (4)
C21 0.31367 (19) 0.02453 (13) 0.92049 (14) 0.0512 (4)
H21 0.2345 −0.0454 0.8962 0.061*
C22 0.41151 (19) 0.05924 (13) 0.85967 (14) 0.0494 (4)
C23 0.5282 (2) 0.16798 (14) 0.90010 (14) 0.0547 (4)
H23 0.5936 0.1939 0.8614 0.066*
C24 0.5454 (2) 0.23412 (14) 0.99384 (15) 0.0571 (4)
H24 0.6236 0.3045 1.0184 0.069*
C25 0.4975 (2) 0.02687 (16) 0.70252 (16) 0.0687 (5)
H25A 0.5055 −0.0386 0.6639 0.082*
H25B 0.6054 0.0717 0.7547 0.082*
C26 0.4354 (3) 0.09271 (17) 0.61840 (16) 0.0806 (6)
H26A 0.3285 0.0490 0.5663 0.121*
H26B 0.5055 0.1117 0.5786 0.121*
H26C 0.4322 0.1596 0.6563 0.121*
C27 0.2699 (2) −0.11834 (14) 0.72177 (16) 0.0646 (5)
H27A 0.2679 −0.1551 0.7837 0.078*
H27B 0.2989 −0.1627 0.6727 0.078*
C28 0.1023 (2) −0.11651 (16) 0.65768 (16) 0.0717 (5)
H28A 0.0664 −0.0811 0.7077 0.108*
H28B 0.0299 −0.1915 0.6253 0.108*
H28C 0.1040 −0.0758 0.5992 0.108*
N1 0.12851 (17) 0.28688 (11) 0.77682 (12) 0.0596 (4)
N2 0.19388 (19) 0.61432 (12) 1.41508 (12) 0.0581 (4)
H2 0.231 (2) 0.6657 (13) 1.3829 (16) 0.087*
N3 0.1989 (2) 0.64809 (13) 1.52280 (14) 0.0672 (4)
H3B 0.268 (2) 0.6211 (18) 1.5658 (15) 0.101*
H3A 0.1032 (15) 0.6189 (17) 1.5226 (19) 0.101*
N4 0.39535 (17) −0.00890 (12) 0.76634 (12) 0.0579 (4)
N5 0.3063 (2) 0.25209 (14) 1.37695 (14) 0.0663 (4)
H5 0.241 (2) 0.1841 (10) 1.3507 (18) 0.099*
N6 0.3254 (2) 0.30988 (17) 1.48147 (15) 0.0782 (5)
H6B 0.270 (3) 0.3544 (18) 1.470 (2) 0.117*
H6A 0.4263 (14) 0.3504 (18) 1.5136 (19) 0.117*
O1 0.21779 (13) 0.54484 (8) 1.09751 (9) 0.0493 (3)
O2 0.27280 (15) 0.67378 (9) 1.24139 (10) 0.0638 (3)
O3 0.07200 (17) 0.43205 (10) 1.39865 (11) 0.0697 (4)
O4 0.23680 (13) 0.05352 (9) 1.07136 (9) 0.0542 (3)
O5 0.15179 (15) 0.06693 (10) 1.20795 (11) 0.0694 (4)
O6 0.48723 (17) 0.39132 (11) 1.34921 (11) 0.0751 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0444 (9) 0.0409 (9) 0.0559 (10) 0.0098 (7) 0.0261 (8) 0.0083 (8)
C2 0.0416 (8) 0.0405 (8) 0.0540 (10) 0.0136 (7) 0.0244 (8) 0.0110 (7)
C3 0.0499 (9) 0.0471 (9) 0.0602 (11) 0.0185 (8) 0.0302 (8) 0.0131 (8)
C4 0.0442 (9) 0.0412 (9) 0.0556 (10) 0.0098 (7) 0.0238 (8) 0.0152 (8)
C5 0.0424 (8) 0.0398 (8) 0.0497 (9) 0.0092 (7) 0.0195 (7) 0.0114 (7)
C6 0.0362 (8) 0.0362 (8) 0.0508 (10) 0.0065 (7) 0.0163 (7) 0.0063 (7)
C7 0.0488 (9) 0.0415 (9) 0.0561 (10) 0.0046 (7) 0.0268 (8) 0.0080 (8)
C8 0.0442 (9) 0.0478 (9) 0.0495 (10) 0.0091 (8) 0.0199 (8) 0.0051 (8)
C9 0.0530 (10) 0.0374 (8) 0.0553 (11) 0.0043 (8) 0.0177 (8) 0.0028 (8)
C10 0.0530 (10) 0.0392 (8) 0.0568 (11) 0.0031 (8) 0.0236 (8) 0.0107 (8)
C11 0.0749 (13) 0.0558 (11) 0.0622 (12) 0.0167 (10) 0.0326 (10) 0.0004 (9)
C12 0.0884 (15) 0.0648 (12) 0.0565 (12) 0.0097 (11) 0.0179 (11) 0.0050 (10)
C13 0.0696 (12) 0.0645 (12) 0.0595 (12) 0.0189 (10) 0.0313 (10) 0.0050 (9)
C14 0.0777 (14) 0.0684 (13) 0.1055 (17) 0.0265 (11) 0.0537 (13) 0.0260 (12)
C15 0.0563 (10) 0.0527 (10) 0.0567 (11) 0.0170 (9) 0.0300 (9) 0.0196 (9)
C16 0.0521 (10) 0.0534 (10) 0.0534 (10) 0.0198 (8) 0.0252 (8) 0.0191 (8)
C17 0.0559 (10) 0.0583 (11) 0.0579 (11) 0.0219 (10) 0.0240 (9) 0.0202 (9)
C18 0.0549 (10) 0.0469 (9) 0.0607 (11) 0.0109 (8) 0.0250 (9) 0.0161 (9)
C19 0.0505 (9) 0.0470 (9) 0.0515 (10) 0.0100 (8) 0.0245 (8) 0.0168 (8)
C20 0.0456 (9) 0.0469 (9) 0.0530 (10) 0.0114 (8) 0.0265 (8) 0.0208 (8)
C21 0.0521 (10) 0.0441 (9) 0.0586 (11) 0.0078 (8) 0.0276 (9) 0.0168 (8)
C22 0.0505 (9) 0.0503 (9) 0.0535 (10) 0.0155 (8) 0.0261 (8) 0.0192 (8)
C23 0.0531 (10) 0.0576 (10) 0.0560 (11) 0.0089 (8) 0.0296 (9) 0.0208 (9)
C24 0.0576 (10) 0.0482 (10) 0.0611 (11) 0.0010 (8) 0.0297 (9) 0.0161 (9)
C25 0.0768 (13) 0.0694 (12) 0.0750 (13) 0.0238 (11) 0.0470 (11) 0.0165 (11)
C26 0.0798 (14) 0.0811 (14) 0.0630 (13) 0.0053 (12) 0.0223 (11) 0.0185 (11)
C27 0.0742 (13) 0.0515 (10) 0.0740 (13) 0.0163 (10) 0.0409 (11) 0.0064 (9)
C28 0.0660 (12) 0.0690 (12) 0.0765 (14) 0.0100 (10) 0.0366 (11) 0.0004 (10)
N1 0.0636 (9) 0.0501 (8) 0.0602 (9) 0.0039 (7) 0.0324 (8) 0.0005 (7)
N2 0.0738 (10) 0.0494 (9) 0.0568 (10) 0.0158 (8) 0.0362 (8) 0.0081 (7)
N3 0.0833 (12) 0.0614 (10) 0.0638 (11) 0.0183 (9) 0.0431 (10) 0.0042 (8)
N4 0.0605 (9) 0.0560 (9) 0.0631 (10) 0.0128 (7) 0.0359 (8) 0.0124 (8)
N5 0.0763 (11) 0.0713 (10) 0.0619 (10) 0.0225 (9) 0.0404 (9) 0.0155 (9)
N6 0.0926 (13) 0.0951 (14) 0.0573 (11) 0.0356 (11) 0.0380 (10) 0.0145 (10)
O1 0.0545 (6) 0.0380 (6) 0.0568 (7) 0.0050 (5) 0.0322 (6) 0.0062 (5)
O2 0.0802 (8) 0.0391 (6) 0.0750 (8) 0.0036 (6) 0.0481 (7) 0.0033 (6)
O3 0.0996 (10) 0.0517 (7) 0.0758 (9) 0.0195 (7) 0.0587 (8) 0.0168 (7)
O4 0.0581 (7) 0.0490 (6) 0.0606 (7) 0.0078 (5) 0.0360 (6) 0.0146 (6)
O5 0.0763 (9) 0.0634 (8) 0.0779 (9) 0.0078 (7) 0.0526 (8) 0.0166 (7)
O6 0.0871 (10) 0.0642 (9) 0.0697 (9) 0.0104 (8) 0.0380 (8) 0.0079 (7)

Geometric parameters (Å, °)

C1—O2 1.2131 (19) C16—C17 1.489 (2)
C1—O1 1.3757 (18) C17—O6 1.231 (2)
C1—C2 1.443 (2) C17—N5 1.332 (2)
C2—C4 1.354 (2) C18—C19 1.406 (2)
C2—C3 1.487 (2) C18—H18 0.9300
C3—O3 1.2372 (19) C19—C20 1.393 (2)
C3—N2 1.324 (2) C19—C24 1.406 (2)
C4—C5 1.403 (2) C20—C21 1.367 (2)
C4—H4 0.9300 C20—O4 1.3808 (17)
C5—C6 1.395 (2) C21—C22 1.410 (2)
C5—C10 1.404 (2) C21—H21 0.9300
C6—C7 1.371 (2) C22—N4 1.363 (2)
C6—O1 1.3785 (18) C22—C23 1.422 (2)
C7—C8 1.409 (2) C23—C24 1.350 (2)
C7—H7 0.9300 C23—H23 0.9300
C8—N1 1.3534 (19) C24—H24 0.9300
C8—C9 1.425 (2) C25—N4 1.475 (2)
C9—C10 1.353 (2) C25—C26 1.496 (3)
C9—H9 0.9300 C25—H25A 0.9700
C10—H10 0.9300 C25—H25B 0.9700
C11—N1 1.462 (2) C26—H26A 0.9600
C11—C12 1.502 (3) C26—H26B 0.9600
C11—H11A 0.9700 C26—H26C 0.9600
C11—H11B 0.9700 C27—N4 1.462 (2)
C12—H12A 0.9600 C27—C28 1.507 (3)
C12—H12B 0.9600 C27—H27A 0.9700
C12—H12C 0.9600 C27—H27B 0.9700
C13—N1 1.487 (2) C28—H28A 0.9600
C13—C14 1.501 (3) C28—H28B 0.9600
C13—H13A 0.9700 C28—H28C 0.9600
C13—H13B 0.9700 N2—N3 1.406 (2)
C14—H14A 0.9600 N2—H2 0.86 (3)
C14—H14B 0.9600 N3—H3B 0.87 (3)
C14—H14C 0.9600 N3—H3A 0.87 (3)
C15—O5 1.2187 (18) N5—N6 1.413 (2)
C15—O4 1.3732 (19) N5—H5 0.87 (3)
C15—C16 1.445 (3) N6—H6B 0.86 (3)
C16—C18 1.366 (2) N6—H6A 0.87 (3)
O2—C1—O1 115.01 (14) C16—C18—H18 118.7
O2—C1—C2 127.53 (15) C19—C18—H18 118.7
O1—C1—C2 117.45 (14) C20—C19—C18 117.92 (15)
C4—C2—C1 119.34 (14) C20—C19—C24 116.24 (16)
C4—C2—C3 118.69 (14) C18—C19—C24 125.83 (16)
C1—C2—C3 121.94 (14) C21—C20—O4 116.70 (14)
O3—C3—N2 122.13 (15) C21—C20—C19 123.23 (14)
O3—C3—C2 120.46 (15) O4—C20—C19 120.07 (14)
N2—C3—C2 117.41 (14) C20—C21—C22 119.95 (16)
C2—C4—C5 122.75 (14) C20—C21—H21 120.0
C2—C4—H4 118.6 C22—C21—H21 120.0
C5—C4—H4 118.6 N4—C22—C21 121.31 (16)
C6—C5—C4 117.57 (14) N4—C22—C23 121.43 (15)
C6—C5—C10 116.19 (14) C21—C22—C23 117.25 (16)
C4—C5—C10 126.19 (14) C24—C23—C22 121.02 (15)
C7—C6—O1 116.17 (13) C24—C23—H23 119.5
C7—C6—C5 123.47 (14) C22—C23—H23 119.5
O1—C6—C5 120.35 (13) C23—C24—C19 122.30 (16)
C6—C7—C8 119.52 (15) C23—C24—H24 118.9
C6—C7—H7 120.2 C19—C24—H24 118.9
C8—C7—H7 120.2 N4—C25—C26 113.65 (15)
N1—C8—C7 121.23 (15) N4—C25—H25A 108.8
N1—C8—C9 121.16 (15) C26—C25—H25A 108.8
C7—C8—C9 117.60 (14) N4—C25—H25B 108.8
C10—C9—C8 120.88 (15) C26—C25—H25B 108.8
C10—C9—H9 119.6 H25A—C25—H25B 107.7
C8—C9—H9 119.6 C25—C26—H26A 109.5
C9—C10—C5 122.33 (15) C25—C26—H26B 109.5
C9—C10—H10 118.8 H26A—C26—H26B 109.5
C5—C10—H10 118.8 C25—C26—H26C 109.5
N1—C11—C12 111.83 (15) H26A—C26—H26C 109.5
N1—C11—H11A 109.3 H26B—C26—H26C 109.5
C12—C11—H11A 109.3 N4—C27—C28 114.99 (15)
N1—C11—H11B 109.3 N4—C27—H27A 108.5
C12—C11—H11B 109.3 C28—C27—H27A 108.5
H11A—C11—H11B 107.9 N4—C27—H27B 108.5
C11—C12—H12A 109.5 C28—C27—H27B 108.5
C11—C12—H12B 109.5 H27A—C27—H27B 107.5
H12A—C12—H12B 109.5 C27—C28—H28A 109.5
C11—C12—H12C 109.5 C27—C28—H28B 109.5
H12A—C12—H12C 109.5 H28A—C28—H28B 109.5
H12B—C12—H12C 109.5 C27—C28—H28C 109.5
N1—C13—C14 111.26 (15) H28A—C28—H28C 109.5
N1—C13—H13A 109.4 H28B—C28—H28C 109.5
C14—C13—H13A 109.4 C8—N1—C11 121.48 (14)
N1—C13—H13B 109.4 C8—N1—C13 122.05 (14)
C14—C13—H13B 109.4 C11—N1—C13 116.37 (13)
H13A—C13—H13B 108.0 C3—N2—N3 123.96 (15)
C13—C14—H14A 109.5 C3—N2—H2 118.5 (14)
C13—C14—H14B 109.5 N3—N2—H2 117.5 (14)
H14A—C14—H14B 109.5 N2—N3—H3B 103.8 (14)
C13—C14—H14C 109.5 N2—N3—H3A 108.3 (16)
H14A—C14—H14C 109.5 H3B—N3—H3A 112 (2)
H14B—C14—H14C 109.5 C22—N4—C27 121.26 (14)
O5—C15—O4 115.15 (15) C22—N4—C25 121.55 (15)
O5—C15—C16 127.16 (16) C27—N4—C25 117.10 (15)
O4—C15—C16 117.69 (14) C17—N5—N6 122.83 (18)
C18—C16—C15 118.90 (16) C17—N5—H5 117.4 (15)
C18—C16—C17 118.62 (16) N6—N5—H5 119.7 (15)
C15—C16—C17 122.48 (15) N5—N6—H6B 108.7 (17)
O6—C17—N5 121.62 (18) N5—N6—H6A 106.1 (17)
O6—C17—C16 120.77 (16) H6B—N6—H6A 107 (2)
N5—C17—C16 117.59 (17) C1—O1—C6 122.45 (12)
C16—C18—C19 122.60 (17) C15—O4—C20 122.81 (13)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N2—H2···O2 0.86 (3) 2.01 (2) 2.7098 (18) 137.(2)
N5—H5···O5 0.87 (3) 2.03 (2) 2.733 (2) 138 (2)
N6—H6B···O3 0.86 (3) 2.30 (1) 3.131 (2) 164 (2)
N3—H3A···O3i 0.87 (3) 2.20 (1) 3.002 (2) 155 (2)
N3—H3B···O6ii 0.87 (3) 2.23 (1) 3.039 (2) 154 (2)

Symmetry codes: (i) −x, −y+1, −z+3; (ii) −x+1, −y+1, −z+3.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV5061).

References

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  4. Rigaku Corporation (1998). 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 global, I. DOI: 10.1107/S1600536811010944/cv5061sup1.cif

e-67-o1107-sup1.cif (23.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010944/cv5061Isup2.hkl

e-67-o1107-Isup2.hkl (302.8KB, hkl)

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


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