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Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Volume 68| Part 5| May 2012| Page o1567

4-(2,3-Dimeth­­oxy­phen­yl)-1H-pyrrole-3-carbo­nitrile

aEngineering Research Center of Pesticides of Heilongjiang University, Heilongjiang University, Harbin 150050, People's Republic of China, and bDalian Songliao Chemical Industry Corporation, Dalian 116031, People's Republic of China
*Correspondence e-mail: hgf1000@163.com

(Received 14 April 2012; accepted 24 April 2012; online 28 April 2012)

The asymmetric unit of the title compound, C13H12N2O2, obtained in a search for analogs of the fungicide fludioxonil [systematic name: 4-(2,2-difluoro-1,3-benzodioxol-4-yl)-1H-pyrrole-3-carbonitrile], contains two independent mol­ecules, A and B. The benzene and pyrrole rings are inclined to each other at 38.5 (1) and 29.3 (1)° in mol­ecules A and B, respectively. In the crystal, bifurcated N—H⋯(O,O) hydrogen bonds link A mol­ecules into chains along [001], while B mol­ecules are linked into layers parallel to the bc plane via bifurcated N—H⋯(N,N) hydrogen bonds.

Related literature

For the synthesis of the title compound, see: Pfluger et al. (1989[Pfluger, R. W., Indermulle, J. & Felix, F. (1989). Eur. Patent 0378046A1.]).

[Scheme 1]

Experimental

Crystal data
  • C13H12N2O2

  • Mr = 228.25

  • Monoclinic, P 21 /c

  • a = 17.527 (4) Å

  • b = 9.6576 (19) Å

  • c = 14.237 (3) Å

  • β = 106.92 (3)°

  • V = 2305.5 (8) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 293 K

  • 0.69 × 0.67 × 0.53 mm

Data collection
  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995[Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.]) Tmin = 0.941, Tmax = 0.954

  • 21190 measured reflections

  • 5215 independent reflections

  • 3907 reflections with I > 2σ(I)

  • Rint = 0.042

Refinement
  • R[F2 > 2σ(F2)] = 0.045

  • wR(F2) = 0.129

  • S = 1.07

  • 5215 reflections

  • 320 parameters

  • 2 restraints

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

  • Δρmax = 0.36 e Å−3

  • Δρmin = −0.15 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H11⋯N2i 0.90 (1) 2.38 (2) 3.086 (2) 136 (2)
N1—H11⋯N2ii 0.90 (1) 2.55 (2) 3.250 (2) 136 (2)
N3—H31⋯O4iii 0.89 (1) 2.12 (1) 2.9327 (16) 151 (2)
N3—H31⋯O3iii 0.89 (1) 2.38 (2) 3.0709 (18) 134 (2)
Symmetry codes: (i) [x, -y+{\script{5\over 2}}, z+{\script{1\over 2}}]; (ii) [-x+1, y+{\script{1\over 2}}, -z+{\script{1\over 2}}]; (iii) [x, -y+{\script{1\over 2}}, z+{\script{1\over 2}}].

Data collection: RAPID-AUTO (Rigaku, 1998[Rigaku (1998). RAPID-AUTO. Rigaku Corporation, Tokyo, Japan.]); cell refinement: RAPID-AUTO; data reduction: CrystalClear (Rigaku/MSC, 2002[Rigaku/MSC (2002). CrystalClear. Rigaku/MSC Inc., The Woodlands, Texas, USA.]); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: SHELXL97.

Supporting information


Comment top

The title compound, (I), is the analogue of Fludioxonil, which is kind of fungicide developed and produced by Novartis. Herein, we report the synthesis and crystal structure of (I).

The asymmetric unit of (I) (Fig. 1), obtained in a search for analogs of Fludioxonil, contains two independent molecules, A and B, respectively. The benzene and pyrrole rings are inclined to each other at 38.5 (1)° in molecules A and 29.3 (1)° in molecules B. In the crystal (Fig. 2), intermolecular bifurcated N—H···O hydrogen bonds (Table 1) link molecules A into chains in [001], while molecules B are linked into layers parallel to bc plane via bifurcated N—H···N hydrogen bonds (Table 1).

Related literature top

For the synthesis of the title compound, see: Pfluger et al. (1989).

Experimental top

The title compound was prepared by the reaction of (Z)-2-cyano-3-(2,3-dimethoxyphenyl)acrylamide and 1-(isocyanomethylsulfonyl)-4-methylbenzene under alkaline condition (Pfluger et al., 1989). A colourless block crystal suitable for X-ray diffraction was obtained by the recrystallization of (I) from methanol.

Refinement top

H atoms bound to C atoms were placed in calculated positions and treated as riding on their parent atoms, with C—H = 0.93 - 0.96 Å and with Uiso(H) = 1.2 - 1.5 Ueq(C). N-bound H atoms were located in a difference Fourier map and were isotropically refined with restraint O—N = 0.90 (1) Å.

Computing details top

Data collection: RAPID-AUTO (Rigaku, 1998); cell refinement: RAPID-AUTO (Rigaku, 1998); data reduction: CrystalClear (Rigaku/MSC, 2002); 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: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Two independent molecules in the asymmetric unit of (I) showing the atomic numbering and 50% probability displacement ellipsoids.
[Figure 2] Fig. 2. A portion of the crystal packing showing hydrogen bonds as dashed lines. H atoms omitted for clarity.
4-(2,3-Dimethoxyphenyl)-1H-pyrrole-3-carbonitrile top
Crystal data top
C13H12N2O2F(000) = 960
Mr = 228.25Dx = 1.315 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 16853 reflections
a = 17.527 (4) Åθ = 3.0–27.5°
b = 9.6576 (19) ŵ = 0.09 mm1
c = 14.237 (3) ÅT = 293 K
β = 106.92 (3)°Block, yellow
V = 2305.5 (8) Å30.69 × 0.67 × 0.53 mm
Z = 8
Data collection top
Rigaku R-AXIS RAPID
diffractometer
5215 independent reflections
Radiation source: fine-focus sealed tube3907 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.042
ω scanθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
h = 2222
Tmin = 0.941, Tmax = 0.954k = 1212
21190 measured reflectionsl = 1718
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.129 w = 1/[σ2(Fo2) + (0.0652P)2 + 0.2588P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
5215 reflectionsΔρmax = 0.36 e Å3
320 parametersΔρmin = 0.15 e Å3
2 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0100 (14)
Crystal data top
C13H12N2O2V = 2305.5 (8) Å3
Mr = 228.25Z = 8
Monoclinic, P21/cMo Kα radiation
a = 17.527 (4) ŵ = 0.09 mm1
b = 9.6576 (19) ÅT = 293 K
c = 14.237 (3) Å0.69 × 0.67 × 0.53 mm
β = 106.92 (3)°
Data collection top
Rigaku R-AXIS RAPID
diffractometer
5215 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
3907 reflections with I > 2σ(I)
Tmin = 0.941, Tmax = 0.954Rint = 0.042
21190 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0452 restraints
wR(F2) = 0.129H atoms treated by a mixture of independent and constrained refinement
S = 1.07Δρmax = 0.36 e Å3
5215 reflectionsΔρmin = 0.15 e Å3
320 parameters
Special details top

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 > 2sigma(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) top
xyzUiso*/Ueq
C10.39205 (11)1.20321 (18)0.36418 (13)0.0544 (4)
H10.36811.18730.41350.065*
C20.38722 (9)1.11726 (16)0.28632 (11)0.0448 (3)
C30.43351 (10)1.18515 (16)0.23130 (12)0.0477 (4)
C40.46329 (11)1.30598 (18)0.27889 (13)0.0568 (4)
H40.49561.36950.25940.068*
C50.45012 (12)1.13911 (17)0.14436 (13)0.0554 (4)
C60.34673 (9)0.98238 (16)0.26304 (11)0.0454 (3)
C70.31916 (11)0.9373 (2)0.16570 (12)0.0570 (4)
H70.32350.99550.11550.068*
C80.28560 (12)0.8080 (2)0.14306 (13)0.0660 (5)
H80.26850.77920.07790.079*
C90.27712 (11)0.72099 (19)0.21594 (13)0.0604 (5)
H90.25450.63380.19990.072*
C100.30215 (10)0.76306 (17)0.31290 (12)0.0506 (4)
C110.33585 (9)0.89520 (17)0.33612 (11)0.0460 (4)
C120.41738 (13)0.8724 (2)0.50009 (15)0.0778 (6)
H12A0.40050.78070.51080.117*
H12B0.43190.92240.56100.117*
H12C0.46260.86690.47500.117*
C130.26965 (15)0.54613 (19)0.37083 (17)0.0765 (6)
H13A0.21680.54410.32590.115*
H13B0.26960.50150.43100.115*
H13C0.30560.49850.34240.115*
C140.14006 (10)0.23868 (16)0.28910 (11)0.0449 (3)
H140.14420.30420.33820.054*
C150.12366 (8)0.26671 (14)0.19105 (10)0.0367 (3)
C160.12262 (9)0.13441 (14)0.14436 (11)0.0401 (3)
C170.13847 (10)0.03501 (16)0.21709 (12)0.0495 (4)
H170.14110.06000.20780.059*
C180.10455 (10)0.10123 (13)0.04287 (12)0.0463 (4)
C190.10576 (8)0.40571 (13)0.14708 (9)0.0342 (3)
C200.06180 (9)0.49956 (15)0.18607 (10)0.0412 (3)
H200.04520.47410.24000.049*
C210.04304 (9)0.62910 (15)0.14515 (11)0.0444 (3)
H210.01390.68970.17200.053*
C220.06663 (9)0.67063 (14)0.06522 (11)0.0410 (3)
H220.05300.75790.03790.049*
C230.11099 (8)0.58046 (13)0.02615 (9)0.0338 (3)
C240.13089 (8)0.44940 (12)0.06761 (9)0.0321 (3)
C250.25651 (11)0.3560 (2)0.07426 (16)0.0661 (5)
H25A0.28040.44470.07130.099*
H25B0.28120.28770.04360.099*
H25C0.26400.33100.14160.099*
C260.11184 (11)0.73558 (14)0.10410 (12)0.0512 (4)
H26A0.05460.73550.12740.077*
H26B0.13310.74240.15890.077*
H26C0.12960.81320.06110.077*
N10.43741 (10)1.31580 (15)0.35841 (11)0.0587 (4)
H110.4537 (12)1.3808 (17)0.4048 (12)0.076 (6)*
N20.46384 (13)1.10171 (18)0.07500 (13)0.0791 (5)
N30.14938 (9)0.09944 (14)0.30346 (10)0.0520 (3)
H310.1571 (12)0.0577 (18)0.3613 (9)0.067 (6)*
N40.08913 (12)0.06891 (14)0.03785 (11)0.0673 (5)
O10.35427 (8)0.94207 (13)0.43141 (8)0.0585 (3)
O20.29473 (8)0.68584 (13)0.39028 (9)0.0643 (3)
O30.17371 (6)0.36250 (9)0.02440 (7)0.0399 (2)
O40.13875 (7)0.61031 (9)0.05192 (7)0.0430 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0560 (10)0.0636 (10)0.0478 (9)0.0014 (7)0.0218 (8)0.0090 (7)
C20.0403 (8)0.0564 (9)0.0368 (8)0.0044 (6)0.0099 (6)0.0027 (6)
C30.0506 (9)0.0526 (8)0.0402 (8)0.0041 (7)0.0139 (7)0.0015 (6)
C40.0611 (11)0.0568 (9)0.0547 (10)0.0027 (7)0.0202 (8)0.0005 (8)
C50.0730 (12)0.0506 (9)0.0484 (10)0.0023 (7)0.0267 (9)0.0056 (7)
C60.0373 (8)0.0590 (9)0.0381 (8)0.0022 (6)0.0078 (6)0.0060 (7)
C70.0553 (10)0.0752 (11)0.0369 (9)0.0056 (8)0.0080 (7)0.0048 (8)
C80.0687 (12)0.0823 (13)0.0395 (9)0.0126 (9)0.0041 (8)0.0158 (9)
C90.0592 (11)0.0633 (10)0.0512 (10)0.0085 (8)0.0043 (8)0.0137 (8)
C100.0459 (9)0.0583 (9)0.0445 (9)0.0010 (7)0.0082 (7)0.0042 (7)
C110.0393 (8)0.0597 (9)0.0364 (8)0.0012 (6)0.0070 (6)0.0083 (7)
C120.0730 (14)0.0918 (15)0.0520 (12)0.0152 (11)0.0078 (10)0.0013 (10)
C130.0929 (16)0.0524 (10)0.0781 (14)0.0012 (10)0.0154 (12)0.0024 (9)
C140.0548 (9)0.0509 (8)0.0335 (8)0.0055 (6)0.0198 (7)0.0001 (6)
C150.0418 (7)0.0404 (7)0.0316 (7)0.0012 (5)0.0163 (6)0.0001 (5)
C160.0520 (9)0.0369 (7)0.0359 (7)0.0040 (6)0.0201 (6)0.0031 (5)
C170.0647 (10)0.0432 (8)0.0461 (9)0.0056 (7)0.0251 (8)0.0094 (6)
C180.0721 (11)0.0280 (6)0.0448 (9)0.0042 (6)0.0263 (8)0.0019 (6)
C190.0388 (7)0.0358 (6)0.0278 (6)0.0021 (5)0.0095 (5)0.0047 (5)
C200.0435 (8)0.0484 (8)0.0353 (7)0.0013 (6)0.0169 (6)0.0097 (6)
C210.0433 (8)0.0454 (8)0.0457 (8)0.0069 (6)0.0147 (7)0.0145 (6)
C220.0461 (8)0.0329 (6)0.0411 (8)0.0054 (5)0.0082 (6)0.0064 (6)
C230.0404 (7)0.0315 (6)0.0278 (6)0.0012 (5)0.0070 (5)0.0049 (5)
C240.0377 (7)0.0306 (6)0.0284 (6)0.0005 (5)0.0105 (5)0.0067 (5)
C250.0521 (11)0.0758 (12)0.0785 (14)0.0151 (8)0.0316 (10)0.0034 (10)
C260.0683 (11)0.0337 (7)0.0520 (9)0.0018 (6)0.0180 (8)0.0101 (6)
N10.0666 (10)0.0571 (8)0.0538 (9)0.0045 (7)0.0197 (7)0.0142 (7)
N20.1202 (16)0.0723 (10)0.0624 (11)0.0016 (10)0.0540 (11)0.0017 (8)
N30.0651 (9)0.0563 (8)0.0386 (7)0.0013 (6)0.0215 (6)0.0155 (6)
N40.1232 (15)0.0392 (7)0.0459 (9)0.0045 (8)0.0349 (9)0.0068 (6)
O10.0641 (8)0.0702 (7)0.0402 (6)0.0024 (6)0.0139 (5)0.0099 (5)
O20.0721 (9)0.0633 (7)0.0540 (7)0.0162 (6)0.0129 (6)0.0030 (6)
O30.0560 (6)0.0333 (5)0.0364 (5)0.0080 (4)0.0229 (5)0.0015 (4)
O40.0650 (7)0.0311 (5)0.0372 (5)0.0047 (4)0.0214 (5)0.0041 (4)
Geometric parameters (Å, º) top
C1—N11.363 (2)C14—C151.368 (2)
C1—C21.368 (2)C14—H140.9300
C1—H10.9300C15—C161.4379 (19)
C2—C31.439 (2)C15—C191.4758 (19)
C2—C61.474 (2)C16—C171.380 (2)
C3—C41.374 (2)C16—C181.423 (2)
C3—C51.423 (2)C17—N31.341 (2)
C4—N11.340 (2)C17—H170.9300
C4—H40.9300C18—N41.145 (2)
C5—N21.141 (2)C19—C241.3937 (18)
C6—C111.394 (2)C19—C201.4044 (18)
C6—C71.398 (2)C20—C211.379 (2)
C7—C81.378 (3)C20—H200.9300
C7—H70.9300C21—C221.379 (2)
C8—C91.376 (3)C21—H210.9300
C8—H80.9300C22—C231.3871 (18)
C9—C101.382 (2)C22—H220.9300
C9—H90.9300C23—O41.3674 (16)
C10—O21.368 (2)C23—C241.3972 (18)
C10—C111.405 (2)C24—O31.3837 (15)
C11—O11.3765 (18)C25—O31.419 (2)
C12—O11.415 (2)C25—H25A0.9600
C12—H12A0.9600C25—H25B0.9600
C12—H12B0.9600C25—H25C0.9600
C12—H12C0.9600C26—O41.4261 (17)
C13—O21.421 (2)C26—H26A0.9600
C13—H13A0.9600C26—H26B0.9600
C13—H13B0.9600C26—H26C0.9600
C13—H13C0.9600N1—H110.896 (9)
C14—N31.363 (2)N3—H310.891 (9)
N1—C1—C2109.57 (15)C16—C15—C19129.77 (12)
N1—C1—H1125.2C17—C16—C18122.83 (13)
C2—C1—H1125.2C17—C16—C15107.38 (13)
C1—C2—C3104.65 (14)C18—C16—C15129.69 (12)
C1—C2—C6129.11 (15)N3—C17—C16108.00 (14)
C3—C2—C6126.21 (14)N3—C17—H17126.0
C4—C3—C5123.36 (16)C16—C17—H17126.0
C4—C3—C2108.18 (14)N4—C18—C16177.05 (16)
C5—C3—C2128.43 (15)C24—C19—C20117.71 (12)
N1—C4—C3107.66 (15)C24—C19—C15122.78 (11)
N1—C4—H4126.2C20—C19—C15119.52 (12)
C3—C4—H4126.2C21—C20—C19120.62 (13)
N2—C5—C3179.6 (2)C21—C20—H20119.7
C11—C6—C7117.97 (15)C19—C20—H20119.7
C11—C6—C2121.82 (13)C22—C21—C20121.39 (12)
C7—C6—C2120.20 (15)C22—C21—H21119.3
C8—C7—C6121.00 (17)C20—C21—H21119.3
C8—C7—H7119.5C21—C22—C23119.08 (13)
C6—C7—H7119.5C21—C22—H22120.5
C9—C8—C7120.61 (16)C23—C22—H22120.5
C9—C8—H8119.7O4—C23—C22124.55 (12)
C7—C8—H8119.7O4—C23—C24115.48 (11)
C8—C9—C10120.06 (17)C22—C23—C24119.97 (13)
C8—C9—H9120.0O3—C24—C19121.18 (11)
C10—C9—H9120.0O3—C24—C23117.56 (11)
O2—C10—C9124.55 (16)C19—C24—C23121.21 (11)
O2—C10—C11115.97 (14)O3—C25—H25A109.5
C9—C10—C11119.45 (16)O3—C25—H25B109.5
O1—C11—C6119.56 (14)H25A—C25—H25B109.5
O1—C11—C10119.51 (14)O3—C25—H25C109.5
C6—C11—C10120.84 (14)H25A—C25—H25C109.5
O1—C12—H12A109.5H25B—C25—H25C109.5
O1—C12—H12B109.5O4—C26—H26A109.5
H12A—C12—H12B109.5O4—C26—H26B109.5
O1—C12—H12C109.5H26A—C26—H26B109.5
H12A—C12—H12C109.5O4—C26—H26C109.5
H12B—C12—H12C109.5H26A—C26—H26C109.5
O2—C13—H13A109.5H26B—C26—H26C109.5
O2—C13—H13B109.5C4—N1—C1109.95 (14)
H13A—C13—H13B109.5C4—N1—H11124.0 (14)
O2—C13—H13C109.5C1—N1—H11125.5 (14)
H13A—C13—H13C109.5C17—N3—C14109.96 (12)
H13B—C13—H13C109.5C17—N3—H31125.4 (12)
N3—C14—C15109.19 (13)C14—N3—H31124.4 (12)
N3—C14—H14125.4C11—O1—C12115.88 (14)
C15—C14—H14125.4C10—O2—C13117.22 (14)
C14—C15—C16105.46 (12)C24—O3—C25114.36 (12)
C14—C15—C19124.65 (13)C23—O4—C26117.41 (11)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H11···N2i0.90 (1)2.38 (2)3.086 (2)136 (2)
N1—H11···N2ii0.90 (1)2.55 (2)3.250 (2)136 (2)
N3—H31···O4iii0.89 (1)2.12 (1)2.9327 (16)151 (2)
N3—H31···O3iii0.89 (1)2.38 (2)3.0709 (18)134 (2)
Symmetry codes: (i) x, y+5/2, z+1/2; (ii) x+1, y+1/2, z+1/2; (iii) x, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC13H12N2O2
Mr228.25
Crystal system, space groupMonoclinic, P21/c
Temperature (K)293
a, b, c (Å)17.527 (4), 9.6576 (19), 14.237 (3)
β (°) 106.92 (3)
V3)2305.5 (8)
Z8
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.69 × 0.67 × 0.53
Data collection
DiffractometerRigaku R-AXIS RAPID
diffractometer
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.941, 0.954
No. of measured, independent and
observed [I > 2σ(I)] reflections
21190, 5215, 3907
Rint0.042
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.045, 0.129, 1.07
No. of reflections5215
No. of parameters320
No. of restraints2
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.36, 0.15

Computer programs: RAPID-AUTO (Rigaku, 1998), CrystalClear (Rigaku/MSC, 2002), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H11···N2i0.896 (9)2.383 (16)3.086 (2)135.5 (17)
N1—H11···N2ii0.896 (9)2.546 (16)3.250 (2)135.9 (17)
N3—H31···O4iii0.891 (9)2.120 (12)2.9327 (16)151.3 (17)
N3—H31···O3iii0.891 (9)2.383 (15)3.0709 (18)134.2 (15)
Symmetry codes: (i) x, y+5/2, z+1/2; (ii) x+1, y+1/2, z+1/2; (iii) x, y+1/2, z+1/2.
 

Acknowledgements

The authors thank the Project of Innovation Service Platform of Heilongjiang Province (PG09J001) and Heilongjiang University for supporting this work.

References

First citationHigashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.  Google Scholar
First citationPfluger, R. W., Indermulle, J. & Felix, F. (1989). Eur. Patent 0378046A1.  Google Scholar
First citationRigaku (1998). RAPID-AUTO. Rigaku Corporation, Tokyo, Japan.  Google Scholar
First citationRigaku/MSC (2002). CrystalClear. Rigaku/MSC Inc., The Woodlands, Texas, USA.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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Volume 68| Part 5| May 2012| Page o1567
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