Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Sep 26;68(Pt 10):o3009. doi: 10.1107/S1600536812039712

N,N′-Dibenzyl-N′′-(2-chloro-2,2-difluoro­acet­yl)phospho­ric triamide

Mehrdad Pourayoubi a,*, Mojtaba Keikha a, Jerry P Jasinski b, Amanda C Keeley b
PMCID: PMC3470367  PMID: 23125780

Abstract

In the title mol­ecule, C16H17ClF2N3O2P, the N—H unit of the C(=O)NHP(=O) fragment adopts a syn orientation with respect to the P=O group. The two F atoms and the Cl atom of the ClF2C group are disordered over two sets of sites with refined occupancies of 0.605 (6) and 0.395 (6). In the crystal, mol­ecules are linked via N—H⋯O=C hydrogen bonds the and the (N—H⋯)(N—H⋯)O=P group into chains along [010].

Related literature  

For related structures with a P(=O)[NHC(=O)CClF2] fragment, and for reference values of P=O, C=O and P—N bond lengths and P—N—C bond angles, see: Pourayoubi et al. (2011); Raissi Shabari et al. (2011); Pourayoubi & Saneei (2011). For the double hydrogen-bond acceptor capability of the phosphoryl O atom in phospho­ramidates, see: Pourayoubi et al. (2012). For the synthesis of the starting material, CClF2C(=O)NHP(=O)Cl2, see: Iriarte et al. (2008).graphic file with name e-68-o3009-scheme1.jpg

Experimental  

Crystal data  

  • C16H17ClF2N3O2P

  • M r = 387.75

  • Monoclinic, Inline graphic

  • a = 12.9734 (5) Å

  • b = 4.9900 (2) Å

  • c = 13.7750 (4) Å

  • β = 96.482 (3)°

  • V = 886.06 (6) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.34 mm−1

  • T = 173 K

  • 0.35 × 0.22 × 0.12 mm

Data collection  

  • Oxford Xcalibur (Eos, Gemini) diffractometer

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2010) T min = 0.890, T max = 0.960

  • 9633 measured reflections

  • 5460 independent reflections

  • 4909 reflections with I > 2σ(I)

  • R int = 0.025

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.051

  • wR(F 2) = 0.122

  • S = 1.09

  • 5460 reflections

  • 263 parameters

  • 18 restraints

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

  • Δρmax = 0.55 e Å−3

  • Δρmin = −0.71 e Å−3

  • Absolute structure: Flack (1983), with 2216 Friedel pairs

  • Flack parameter: 0.06 (11)

Data collection: CrysAlis PRO (Oxford Diffraction, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis RED (Oxford Diffraction, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL and enCIFer (Allen et al., 2004).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812039712/lh5506sup1.cif

e-68-o3009-sup1.cif (27.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812039712/lh5506Isup2.hkl

e-68-o3009-Isup2.hkl (267.3KB, 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
N1—H1N⋯O1i 0.88 (2) 2.30 (3) 3.092 (3) 151 (3)
N2—H2N⋯O1i 0.86 (2) 2.05 (2) 2.867 (3) 158 (3)
N3—H3N⋯O2ii 0.86 (2) 2.01 (2) 2.854 (3) 166 (3)

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

Acknowledgments

MP thanks Ferdowsi University of Mashhad for a Research University Grant (No. 15144/2). JPJ acknowledges the NSF-MRI program (grant No. CHE1039027) for funds to purchase the X-ray diffractometer.

supplementary crystallographic information

Comment

In the previous studies, the structures of some compounds with a P(O)[NHC(O)CClF2] fragment have been investigated; for example, [4-CH3-C6H4NH]2P(O)[NHC(O)CClF2] (Pourayoubi, Tarahhomi et al., 2011), [(C6H5CH2)(CH3)N]2P(O)[NHC(O)CClF2] (Raissi Shabari et al., 2011) and [(CH3)2CHNH]2P(O)[NHC(O)CClF2] (Pourayoubi & Saneei, 2011). Here, the structure determination of the title compound (Fig. 1) is reported.

Atoms F1, F2 and Cl1 were refined as disordered over two sets of sites with occupancies of 0.605 (6) and 0.395 (6). The N—H unit of the C(O)NHP(O) fragment adopts a syn orientation with respect to the phosphoryl group. The P atom is bonded in a distorted tetrahedral environment as has been noted for other phosphoric triamides. The P═O, C═O and P—N bond lengths and P—N—C bond angles are within the expected values (Pourayoubi, Tarahhomi et al., 2011; Raissi Shabari et al., 2011; Pourayoubi & Saneei, 2011).

In the crystal, the O atom of P═O group acts as a double-hydrogen bond acceptor (Pourayoubi et al., 2012) and molecules are linked by N—H···O═C hydrogen bonds and (N—H···)2O═P group, into a linear arrangement along the b axis (Fig. 2).

Experimental

ClF2CC(O)NHP(O)Cl2 was prepared according to the literature method reported by Iriarte et al. (2008).

To a solution of ClF2CC(O)NHP(O)Cl2 (0.473 g, 1.92 mmol) in dry chloroform (25 ml), a solution of benzylamine (0.823 g, 7.68 mmol) in the same solvent (5 ml) was added at 273 K. After 6 h stirring, the solvent was removed and the product was washed with distilled water and recrystallized from CH3CN at room temperature.

Refinement

H atoms H1N, H2N and H3N were located in a difference Fourier map and were refined with Uiso(H) = 1.2Ueq(N), giving N—H distances of 0.88 (2) or 0.86 (2) Å. The other H atoms were placed in calculated positions with 0.95 Å for CH, 0.99 Å for CH2 and with Uiso(H) = 1.2Ueq(C). F atoms F1 and F2 and chlorine Cl1 are disordered over two sets of sites with occupancies of 0.605 (6) and 0.395 (6).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound. Displacement ellipsoids are given at the 30% probability level and H atoms are drawn as small spheres of arbitrary radii. The atoms of the minor component of disorder are labeled with suffix 'A'.

Fig. 2.

Fig. 2.

Crystal packing of title compound viewed approximately along the a axis. The N—H···O hydrogen bonds are shown by dashed lines. H atoms not involved in hydrogen bonding have been removed for clarity.

Crystal data

C16H17ClF2N3O2P F(000) = 400
Mr = 387.75 Dx = 1.453 Mg m3
Monoclinic, P21 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2yb Cell parameters from 3176 reflections
a = 12.9734 (5) Å θ = 3.3–32.2°
b = 4.9900 (2) Å µ = 0.34 mm1
c = 13.7750 (4) Å T = 173 K
β = 96.482 (3)° Block, colourless
V = 886.06 (6) Å3 0.35 × 0.22 × 0.12 mm
Z = 2

Data collection

Oxford Xcalibur (Eos, Gemini) diffractometer 5460 independent reflections
Radiation source: Enhance (Mo) X-ray Source 4909 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.025
Detector resolution: 16.1500 pixels mm-1 θmax = 32.2°, θmin = 3.3°
ω scans h = −18→19
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2010) k = −7→6
Tmin = 0.890, Tmax = 0.960 l = −9→20
9633 measured 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)] = 0.051 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.122 w = 1/[σ2(Fo2) + (0.048P)2 + 0.3968P] where P = (Fo2 + 2Fc2)/3
S = 1.09 (Δ/σ)max = 0.001
5460 reflections Δρmax = 0.55 e Å3
263 parameters Δρmin = −0.71 e Å3
18 restraints Absolute structure: Flack (1983), with 2216 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.06 (11)

Special details

Experimental. IR (KBr, ν, cm-1): 3253, 1718, 1457, 1419, 1282, 1215, 1139, 1073, 977, 873, 735 and 688.
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 Occ. (<1)
P1 0.51645 (5) 0.70594 (13) 0.19236 (4) 0.01939 (13)
Cl1 0.2161 (2) 0.5360 (8) 0.3959 (2) 0.0795 (10) 0.605 (6)
F1 0.3784 (5) 0.5030 (15) 0.4995 (4) 0.086 (2) 0.605 (6)
F2 0.3555 (5) 0.8763 (7) 0.4479 (3) 0.073 (2) 0.605 (6)
Cl1A 0.3973 (4) 0.6102 (13) 0.5203 (3) 0.0829 (18) 0.395 (6)
F1A 0.2518 (6) 0.4471 (17) 0.4089 (7) 0.066 (3) 0.395 (6)
F2A 0.2775 (5) 0.8461 (12) 0.3861 (5) 0.058 (2) 0.395 (6)
O1 0.54403 (15) 0.9827 (4) 0.16821 (14) 0.0261 (4)
O2 0.4173 (2) 0.3092 (5) 0.3189 (2) 0.0528 (8)
N1 0.45241 (18) 0.5364 (5) 0.10546 (18) 0.0266 (5)
H1N 0.460 (3) 0.362 (5) 0.106 (3) 0.032*
N2 0.61194 (18) 0.5089 (5) 0.22963 (16) 0.0241 (4)
H2N 0.601 (3) 0.340 (5) 0.226 (2) 0.029*
N3 0.4401 (2) 0.7487 (5) 0.28612 (18) 0.0288 (5)
H3N 0.428 (3) 0.909 (5) 0.305 (2) 0.035*
C1 0.3635 (2) 0.6492 (6) 0.0436 (2) 0.0294 (6)
H1B 0.3792 0.6516 −0.0251 0.035*
H1A 0.3527 0.8367 0.0637 0.035*
C2 0.2652 (2) 0.4925 (6) 0.04980 (19) 0.0270 (5)
C3 0.2351 (2) 0.2941 (6) −0.0179 (2) 0.0309 (6)
H3A 0.2759 0.2598 −0.0696 0.037*
C4 0.1463 (3) 0.1456 (7) −0.0111 (3) 0.0391 (7)
H4A 0.1267 0.0093 −0.0577 0.047*
C5 0.0860 (2) 0.1951 (9) 0.0635 (2) 0.0432 (7)
H5A 0.0247 0.0937 0.0679 0.052*
C6 0.1150 (3) 0.3920 (9) 0.1315 (3) 0.0457 (9)
H6A 0.0742 0.4238 0.1835 0.055*
C7 0.2035 (2) 0.5440 (8) 0.1241 (2) 0.0364 (7)
H7A 0.2219 0.6832 0.1698 0.044*
C8 0.6884 (2) 0.5876 (6) 0.3112 (2) 0.0286 (6)
H8A 0.6577 0.5637 0.3733 0.034*
H8B 0.7050 0.7800 0.3048 0.034*
C9 0.7871 (2) 0.4274 (6) 0.31541 (19) 0.0263 (5)
C10 0.8070 (2) 0.2410 (7) 0.2450 (2) 0.0303 (6)
H10A 0.7574 0.2120 0.1899 0.036*
C11 0.8993 (3) 0.0966 (8) 0.2550 (3) 0.0401 (7)
H11A 0.9121 −0.0311 0.2067 0.048*
C12 0.9720 (3) 0.1367 (8) 0.3341 (3) 0.0453 (9)
H12A 1.0345 0.0358 0.3409 0.054*
C13 0.9537 (3) 0.3244 (9) 0.4035 (3) 0.0505 (10)
H13A 1.0045 0.3561 0.4575 0.061*
C14 0.8624 (3) 0.4658 (8) 0.3949 (2) 0.0403 (7)
H14A 0.8502 0.5920 0.4439 0.048*
C15 0.4032 (3) 0.5428 (6) 0.3344 (3) 0.0405 (8)
C16 0.3359 (2) 0.6241 (6) 0.4143 (2) 0.0490 (8)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
P1 0.0211 (3) 0.0136 (2) 0.0242 (3) −0.0009 (3) 0.00582 (19) −0.0014 (2)
Cl1 0.0438 (12) 0.139 (3) 0.0597 (12) 0.0070 (14) 0.0255 (10) −0.0081 (14)
F1 0.076 (4) 0.169 (7) 0.0121 (19) −0.017 (4) 0.0062 (19) −0.016 (3)
F2 0.139 (5) 0.036 (2) 0.056 (3) −0.013 (3) 0.066 (3) −0.0126 (18)
Cl1A 0.076 (3) 0.148 (5) 0.0257 (15) 0.005 (3) 0.0091 (13) −0.0213 (17)
F1A 0.028 (3) 0.079 (6) 0.098 (6) −0.017 (4) 0.036 (4) 0.007 (5)
F2A 0.081 (5) 0.043 (3) 0.060 (4) 0.032 (3) 0.047 (4) 0.012 (3)
O1 0.0319 (10) 0.0160 (9) 0.0322 (9) −0.0018 (7) 0.0107 (7) 0.0004 (7)
O2 0.0767 (19) 0.0144 (10) 0.0769 (18) 0.0017 (12) 0.0504 (16) 0.0025 (11)
N1 0.0229 (10) 0.0199 (11) 0.0361 (11) 0.0025 (9) −0.0006 (8) −0.0079 (9)
N2 0.0240 (10) 0.0158 (10) 0.0316 (11) −0.0011 (8) −0.0008 (8) −0.0015 (9)
N3 0.0405 (13) 0.0129 (12) 0.0366 (11) 0.0009 (9) 0.0198 (10) −0.0012 (8)
C1 0.0263 (12) 0.0335 (18) 0.0281 (12) −0.0024 (10) 0.0009 (9) 0.0050 (10)
C2 0.0218 (12) 0.0308 (14) 0.0281 (12) 0.0024 (10) 0.0014 (9) 0.0067 (10)
C3 0.0275 (13) 0.0332 (16) 0.0321 (13) 0.0026 (11) 0.0033 (11) 0.0008 (11)
C4 0.0366 (16) 0.0320 (19) 0.0477 (17) −0.0011 (12) 0.0000 (13) −0.0013 (12)
C5 0.0271 (13) 0.0458 (19) 0.0568 (18) −0.0050 (17) 0.0047 (12) 0.008 (2)
C6 0.0327 (17) 0.064 (3) 0.0427 (17) −0.0004 (17) 0.0129 (13) 0.0049 (17)
C7 0.0287 (14) 0.049 (2) 0.0314 (13) −0.0020 (14) 0.0042 (11) −0.0040 (13)
C8 0.0296 (13) 0.0269 (14) 0.0284 (12) 0.0019 (11) −0.0006 (10) −0.0036 (10)
C9 0.0252 (12) 0.0265 (13) 0.0270 (12) −0.0032 (10) 0.0025 (9) 0.0035 (10)
C10 0.0260 (12) 0.0340 (17) 0.0309 (12) −0.0004 (12) 0.0030 (9) −0.0017 (11)
C11 0.0298 (15) 0.0427 (19) 0.0494 (18) 0.0062 (14) 0.0113 (13) −0.0021 (15)
C12 0.0297 (15) 0.052 (2) 0.0533 (19) 0.0088 (14) 0.0011 (13) 0.0121 (16)
C13 0.0378 (19) 0.062 (3) 0.0474 (19) 0.0040 (17) −0.0156 (15) 0.0013 (18)
C14 0.0393 (17) 0.0429 (19) 0.0356 (15) 0.0020 (15) −0.0096 (12) −0.0027 (14)
C15 0.060 (2) 0.0165 (13) 0.0516 (18) 0.0013 (13) 0.0366 (16) 0.0015 (12)
C16 0.0641 (16) 0.0245 (15) 0.066 (2) −0.0012 (15) 0.0394 (15) 0.0048 (15)

Geometric parameters (Å, º)

P1—O1 1.474 (2) C3—H3A 0.9500
P1—N1 1.617 (2) C4—C5 1.382 (5)
P1—N2 1.619 (2) C4—H4A 0.9500
P1—N3 1.728 (2) C5—C6 1.381 (6)
Cl1—C16 1.607 (3) C5—H5A 0.9500
F1—C16 1.379 (5) C6—C7 1.390 (5)
F2—C16 1.355 (4) C6—H6A 0.9500
Cl1A—C16 1.585 (4) C7—H7A 0.9500
F1A—C16 1.399 (5) C8—C9 1.505 (4)
F2A—C16 1.373 (4) C8—H8A 0.9900
O2—C15 1.203 (4) C8—H8B 0.9900
N1—C1 1.467 (4) C9—C10 1.388 (4)
N1—H1N 0.88 (2) C9—C14 1.396 (4)
N2—C8 1.466 (3) C10—C11 1.391 (4)
N2—H2N 0.86 (2) C10—H10A 0.9500
N3—C15 1.341 (4) C11—C12 1.373 (5)
N3—H3N 0.86 (2) C11—H11A 0.9500
C1—C2 1.507 (4) C12—C13 1.378 (6)
C1—H1B 0.9900 C12—H12A 0.9500
C1—H1A 0.9900 C13—C14 1.373 (5)
C2—C3 1.386 (4) C13—H13A 0.9500
C2—C7 1.393 (4) C14—H14A 0.9500
C3—C4 1.382 (4) C15—C16 1.534 (4)
O1—P1—N1 116.13 (13) C9—C8—H8B 109.0
O1—P1—N2 116.36 (12) H8A—C8—H8B 107.8
N1—P1—N2 103.17 (12) C10—C9—C14 118.1 (3)
O1—P1—N3 103.15 (11) C10—C9—C8 123.6 (2)
N1—P1—N3 109.14 (13) C14—C9—C8 118.3 (3)
N2—P1—N3 108.72 (12) C9—C10—C11 120.2 (3)
C1—N1—P1 122.3 (2) C9—C10—H10A 119.9
C1—N1—H1N 118 (2) C11—C10—H10A 119.9
P1—N1—H1N 117 (2) C12—C11—C10 120.7 (3)
C8—N2—P1 120.50 (19) C12—C11—H11A 119.7
C8—N2—H2N 114 (2) C10—C11—H11A 119.7
P1—N2—H2N 118 (2) C11—C12—C13 119.5 (3)
C15—N3—P1 122.91 (19) C11—C12—H12A 120.2
C15—N3—H3N 119 (2) C13—C12—H12A 120.2
P1—N3—H3N 118 (2) C14—C13—C12 120.3 (3)
N1—C1—C2 112.5 (2) C14—C13—H13A 119.9
N1—C1—H1B 109.1 C12—C13—H13A 119.9
C2—C1—H1B 109.1 C13—C14—C9 121.2 (3)
N1—C1—H1A 109.1 C13—C14—H14A 119.4
C2—C1—H1A 109.1 C9—C14—H14A 119.4
H1B—C1—H1A 107.8 O2—C15—N3 125.7 (3)
C3—C2—C7 118.9 (3) O2—C15—C16 119.6 (3)
C3—C2—C1 120.6 (2) N3—C15—C16 114.6 (2)
C7—C2—C1 120.5 (3) F2—C16—F2A 54.8 (4)
C4—C3—C2 120.8 (3) F2—C16—F1 94.3 (4)
C4—C3—H3A 119.6 F2A—C16—F1 138.5 (4)
C2—C3—H3A 119.6 F2—C16—F1A 136.0 (5)
C5—C4—C3 120.1 (3) F2A—C16—F1A 95.3 (5)
C5—C4—H4A 120.0 F1—C16—F1A 90.2 (5)
C3—C4—H4A 120.0 F2—C16—C15 113.0 (3)
C6—C5—C4 119.9 (3) F2A—C16—C15 110.6 (3)
C6—C5—H5A 120.1 F1—C16—C15 106.8 (4)
C4—C5—H5A 120.1 F1A—C16—C15 107.3 (5)
C5—C6—C7 120.2 (3) F2—C16—Cl1A 70.7 (4)
C5—C6—H6A 119.9 F2A—C16—Cl1A 120.0 (4)
C7—C6—H6A 119.9 F1A—C16—Cl1A 109.2 (5)
C6—C7—C2 120.1 (3) C15—C16—Cl1A 112.5 (3)
C6—C7—H7A 119.9 F2—C16—Cl1 116.7 (4)
C2—C7—H7A 119.9 F2A—C16—Cl1 71.6 (4)
N2—C8—C9 112.7 (2) F1—C16—Cl1 107.5 (4)
N2—C8—H8A 109.0 C15—C16—Cl1 115.7 (3)
C9—C8—H8A 109.0 Cl1A—C16—Cl1 120.6 (3)
N2—C8—H8B 109.0
O1—P1—N1—C1 −45.6 (3) C14—C9—C10—C11 0.6 (5)
N2—P1—N1—C1 −174.1 (2) C8—C9—C10—C11 −178.7 (3)
N3—P1—N1—C1 70.4 (2) C9—C10—C11—C12 −0.3 (5)
O1—P1—N2—C8 53.1 (2) C10—C11—C12—C13 −0.8 (6)
N1—P1—N2—C8 −178.5 (2) C11—C12—C13—C14 1.5 (6)
N3—P1—N2—C8 −62.8 (2) C12—C13—C14—C9 −1.2 (6)
O1—P1—N3—C15 −175.7 (3) C10—C9—C14—C13 0.2 (5)
N1—P1—N3—C15 60.2 (3) C8—C9—C14—C13 179.5 (3)
N2—P1—N3—C15 −51.6 (3) P1—N3—C15—O2 −0.6 (6)
P1—N1—C1—C2 −120.2 (2) P1—N3—C15—C16 −179.3 (2)
N1—C1—C2—C3 −94.8 (3) O2—C15—C16—F2 157.9 (5)
N1—C1—C2—C7 84.9 (3) N3—C15—C16—F2 −23.3 (5)
C7—C2—C3—C4 −1.2 (4) O2—C15—C16—F2A −142.8 (5)
C1—C2—C3—C4 178.4 (3) N3—C15—C16—F2A 36.0 (6)
C2—C3—C4—C5 0.4 (5) O2—C15—C16—F1 55.6 (6)
C3—C4—C5—C6 −0.4 (5) N3—C15—C16—F1 −125.6 (4)
C4—C5—C6—C7 1.2 (6) O2—C15—C16—F1A −40.0 (6)
C5—C6—C7—C2 −2.0 (6) N3—C15—C16—F1A 138.8 (5)
C3—C2—C7—C6 2.0 (5) O2—C15—C16—Cl1A 80.1 (5)
C1—C2—C7—C6 −177.6 (3) N3—C15—C16—Cl1A −101.1 (4)
P1—N2—C8—C9 −162.00 (19) O2—C15—C16—Cl1 −64.0 (5)
N2—C8—C9—C10 5.0 (4) N3—C15—C16—Cl1 114.8 (4)
N2—C8—C9—C14 −174.2 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O1i 0.88 (2) 2.30 (3) 3.092 (3) 151 (3)
N2—H2N···O1i 0.86 (2) 2.05 (2) 2.867 (3) 158 (3)
N3—H3N···O2ii 0.86 (2) 2.01 (2) 2.854 (3) 166 (3)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5506).

References

  1. Allen, F. H., Johnson, O., Shields, G. P., Smith, B. R. & Towler, M. (2004). J. Appl. Cryst. 37, 335–338.
  2. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  3. Iriarte, A. G., Erben, M. F., Gholivand, K., Jios, J. L., Ulic, S. E. & Védova, C. O. D. (2008). J. Mol. Struct. 886, 66–71.
  4. Oxford Diffraction (2010). CrysAlis PRO and CrysAlis RED Oxford Diffraction Ltd, Yarnton, Oxfordshire, England.
  5. Pourayoubi, M., Nečas, M. & Negari, M. (2012). Acta Cryst. C68, o51–o56. [DOI] [PubMed]
  6. Pourayoubi, M. & Saneei, A. (2011). Acta Cryst. E67, o665. [DOI] [PMC free article] [PubMed]
  7. Pourayoubi, M., Tarahhomi, A., Saneei, A., Rheingold, A. L. & Golen, J. A. (2011). Acta Cryst. C67, o265–o272. [DOI] [PubMed]
  8. Raissi Shabari, A., Pourayoubi, M. & Saneei, A. (2011). Acta Cryst. E67, o663–o664. [DOI] [PMC free article] [PubMed]
  9. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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/S1600536812039712/lh5506sup1.cif

e-68-o3009-sup1.cif (27.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812039712/lh5506Isup2.hkl

e-68-o3009-Isup2.hkl (267.3KB, 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

RESOURCES