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The title compound, C19H18ClN3O, contains two molecules in the asymmetric unit, each with a Z conformation.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680202353X/dn6049sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680202353X/dn6049Isup2.hkl
Contains datablock I

CCDC reference: 204683

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.046
  • wR factor = 0.114
  • Data-to-parameter ratio = 14.0

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
REFLT_03 From the CIF: _diffrn_reflns_theta_max 26.36 From the CIF: _reflns_number_total 6167 TEST2: Reflns within _diffrn_reflns_theta_max Count of symmetry unique reflns 6803 Completeness (_total/calc) 90.65% Alert C: < 95% complete
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

Toutes les benzodiazépines possèdent à des degrés divers des propriétés pharmacologiques identiques: anxiolytiques, sédatives ou hypnotiques, anticonvulsantes et myorelaxantes (Bailly & de Chouly, 1999). Au cours d'une large étude de dérivés benzodiazépiniques, il a été montré que l'introduction d'un hétérocycle à cinq ou six chaînons sur le cycle diazépinique accroît notablement l'activité biologique de la molécule (Raban et al., 1977; Aiello et al., 1978). Développant nos travaux de recherche concernant la synthèse de nouvelles 1,4-benzodiazépines susceptibles de présenter une activité biologique (Benelbaghdadi et al., 1997, 1998, 2000; Essaber et al., 1998; Baouid et al., 1994, 1996), nous décrivons ici le comportement du Diazépam (ValiumR) (Sternbach et al., 1962) en présence du N,N-diméthyl-formamide diméthyl acétal. Cette réaction (Pinto & Fryer, 1993) conduit à un composé de stéréochimie Z ou E dont la structure n'est pas déterminée. L'analyse des spectres de RMN 1H et 13C confirme la présence d'un seul isomère géométrique, cependant elle ne permet pas de trancher entre les deux structures isomères. L'étude cristallographique par diffraction des rayons X a permis de déterminer la stéréochimie exacte du produit obtenu: la structure cristalline du composé montre qu'il s'agit de l'isomère Z (Fig. 1). Le composé cristallize dans le système triclinique, avec 2 molécules indépendantes dans l'unité asymétrique. Ces deux molécules sont parfaitement identiques, comme le montre le tableau des distances et angles de liaison, Table 1 e t leur conformation est comparable. En effet, dans les deux cas, le bicycle benzodiazépine comporte deux fragments plans: (i) le cycle benzo et les 2 atomes voisins du cycle à sept chaînons: N1C5-C11 pour la première molécule et N31C35-C41 pour la deuxième; (ii) le groupement N1C2N4C5 pour la première et N31/C32/C34/C35 pour la deuxième molécule. Ces deux fragments font un angle dièdre de 40.4 (3) e t 47.4 (3)°, respectivement. pour chaque molécule. L'atome C3 (ou C33) porteur du groupement diméthylaminométhylène est à 0.414 (3) Å du plan N1/C2/N4/C5 [C33 à 0.397 (3) Å de N31/C32/N34/C35]. Quelques interactions intermoléculaires sont à noter: (i) entre l'atome de chlore Cl1 et les atomes H18 [2.755 (2) Å] et H16B [2.854 (2) Å]; (ii) entre l'atome d'oxygène O1 et les atomes H15C [2.537 (3) Å] et H9 [2.598 (3) Å]; (iii) enfin, entre l'atome d'oxygène O2 et l'atome H21 [2.570 (3) Å].

Experimental top

Le monocristal est obtenu par recristallization à températute ambiante dans le mélange dichlorométhane–éthanol (1/1).

Computing details top

Data collection: KappaCCD Reference Manual (Nonius, 1998); data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. Dessin ORTEPIII (Burnett & Johnson, 1996) de la molécule. Les ellipsoides de vibration des atomes ont une probabilité de 50%..
(I) top
Crystal data top
C19H18ClN3OZ = 4
Mr = 339.81F(000) = 712
Triclinic, P1Dx = 1.357 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.2793 (2) ÅCell parameters from 22942 reflections
b = 9.4256 (2) Åθ = 1–26.4°
c = 20.6390 (8) ŵ = 0.24 mm1
α = 84.713 (1)°T = 293 K
β = 80.583 (1)°Plate, red
γ = 69.210 (1)°0.4 × 0.3 × 0.1 mm
V = 1663.73 (8) Å3
Data collection top
Nonius KappaCCD
diffractometer
5488 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.033
Graphite monochromatorθmax = 26.4°, θmin = 2.4°
ϕ scansh = 011
22942 measured reflectionsk = 910
6167 independent reflectionsl = 2425
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.046Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.114H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0441P)2 + 0.9016P]
where P = (Fo2 + 2Fc2)/3
6155 reflections(Δ/σ)max = 0.001
439 parametersΔρmax = 0.40 e Å3
0 restraintsΔρmin = 0.49 e Å3
Crystal data top
C19H18ClN3Oγ = 69.210 (1)°
Mr = 339.81V = 1663.73 (8) Å3
Triclinic, P1Z = 4
a = 9.2793 (2) ÅMo Kα radiation
b = 9.4256 (2) ŵ = 0.24 mm1
c = 20.6390 (8) ÅT = 293 K
α = 84.713 (1)°0.4 × 0.3 × 0.1 mm
β = 80.583 (1)°
Data collection top
Nonius KappaCCD
diffractometer
5488 reflections with I > 2σ(I)
22942 measured reflectionsRint = 0.033
6167 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0460 restraints
wR(F2) = 0.114H-atom parameters constrained
S = 1.05Δρmax = 0.40 e Å3
6155 reflectionsΔρmin = 0.49 e Å3
439 parameters
Special details top

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) top
xyzUiso*/Ueq
Cl10.41321 (7)0.09461 (7)0.19881 (3)0.05967 (17)
Cl21.10756 (9)0.60058 (7)0.14629 (3)0.0598 (2)
O11.02787 (17)0.28705 (18)0.02985 (8)0.0587 (4)
O20.6718 (2)0.7854 (2)0.49955 (8)0.0601 (5)
N10.93016 (17)0.13511 (18)0.09963 (7)0.0378 (3)
N40.68355 (16)0.42737 (17)0.14433 (6)0.0327 (3)
N140.61201 (19)0.63359 (19)0.02564 (8)0.0424 (4)
N310.70066 (19)0.8538 (2)0.39146 (8)0.0359 (4)
N340.9873 (2)0.89007 (19)0.41573 (8)0.0336 (4)
N441.1243 (2)0.6768 (2)0.52536 (8)0.0441 (5)
C20.9157 (2)0.2734 (2)0.06716 (8)0.0376 (4)
C30.7674 (2)0.4009 (2)0.08065 (8)0.0329 (4)
C50.65232 (18)0.32414 (19)0.18348 (8)0.0297 (3)
C60.5537 (2)0.1124 (2)0.18589 (8)0.0341 (4)
H60.46550.16890.21590.041*
C70.5617 (2)0.0251 (2)0.16571 (9)0.0388 (4)
C80.6853 (2)0.1081 (2)0.12173 (9)0.0436 (4)
H80.68830.20360.10770.052*
C90.8031 (2)0.0513 (2)0.09902 (9)0.0419 (4)
H90.88960.10630.06790.050*
C100.8003 (2)0.0863 (2)0.11976 (8)0.0327 (4)
C110.67269 (19)0.17139 (19)0.16335 (7)0.0301 (3)
C121.0843 (2)0.0173 (2)0.08998 (10)0.0505 (5)
H12A1.16200.06000.09410.061*
H12B1.10330.02230.04700.061*
H12C1.08890.06320.12250.061*
C130.7389 (2)0.5109 (2)0.03122 (8)0.0350 (4)
H130.82740.49140.00250.042*
C150.6097 (3)0.7347 (3)0.03222 (12)0.0659 (7)
H15A0.57010.83810.01890.079*
H15B0.54410.72070.06060.079*
H15C0.71350.71210.05520.079*
C160.4619 (2)0.6554 (3)0.06473 (10)0.0526 (5)
H16A0.38480.67260.03620.063*
H16B0.43410.74160.09160.063*
H16C0.46710.56650.09230.063*
C170.57242 (19)0.3695 (2)0.25112 (8)0.0311 (3)
C180.4728 (2)0.5172 (2)0.26245 (9)0.0431 (4)
H180.45730.59180.22690.052*
C190.3948 (3)0.5591 (3)0.32470 (10)0.0521 (5)
H190.32560.66150.33200.062*
C200.4155 (2)0.4536 (3)0.37682 (9)0.0500 (5)
H200.36040.48290.41980.060*
C210.5159 (2)0.3071 (3)0.36663 (9)0.0434 (5)
H210.53180.23380.40270.052*
C220.5941 (2)0.2645 (2)0.30426 (8)0.0358 (4)
H220.66390.16200.29800.043*
C320.7588 (2)0.8058 (2)0.45090 (9)0.0377 (5)
C330.9209 (2)0.7920 (2)0.45328 (9)0.0342 (4)
C350.9852 (2)0.9168 (2)0.35370 (9)0.0299 (4)
C361.0286 (2)0.7684 (2)0.25409 (9)0.0332 (4)
H361.12300.78930.23970.040*
C370.9867 (3)0.6780 (2)0.21759 (9)0.0381 (5)
C380.8512 (3)0.6458 (2)0.23640 (10)0.0407 (5)
H380.82380.58330.20990.049*
C390.7576 (2)0.7053 (2)0.29368 (10)0.0377 (5)
H390.66260.68510.30750.045*
C400.7984 (2)0.7950 (2)0.33227 (9)0.0298 (4)
C410.9339 (2)0.8295 (2)0.31202 (8)0.0285 (4)
C420.5330 (3)0.8898 (3)0.39358 (12)0.0514 (6)
H42A0.47780.95880.42800.062*
H42B0.50240.93590.35220.062*
H42C0.50900.79820.40190.062*
C430.9873 (3)0.7035 (2)0.50488 (9)0.0386 (5)
H430.91580.65720.52800.046*
C451.1660 (3)0.5755 (3)0.58224 (12)0.0571 (6)
H45A1.26860.50250.57170.068*
H45B1.16420.63370.61840.068*
H45C1.09260.52370.59420.068*
C461.2269 (3)0.7605 (3)0.50123 (12)0.0504 (6)
H46A1.33170.69900.50710.060*
H46B1.22180.78640.45540.060*
H46C1.19560.85160.52520.060*
C471.0485 (2)1.0366 (2)0.32333 (9)0.0309 (4)
C481.1417 (2)1.0834 (2)0.35716 (10)0.0382 (5)
H481.17101.03340.39810.046*
C491.1931 (3)1.2007 (3)0.33217 (12)0.0469 (5)
H491.25801.23030.35590.056*
C501.1519 (3)1.2755 (3)0.27389 (12)0.0466 (5)
H501.18661.35800.25700.056*
C511.0595 (3)1.2311 (3)0.23951 (11)0.0445 (5)
H511.03041.28310.19880.053*
C521.0089 (2)1.1123 (2)0.26384 (10)0.0350 (4)
H520.94591.08190.23930.042*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0604 (3)0.0478 (4)0.0814 (4)0.0323 (3)0.0050 (3)0.0087 (3)
Cl20.0833 (4)0.0523 (4)0.0364 (3)0.0160 (3)0.0099 (2)0.0142 (2)
O10.0441 (8)0.0563 (10)0.0585 (9)0.0096 (7)0.0158 (7)0.0108 (7)
O20.0543 (9)0.0878 (12)0.0365 (7)0.0308 (8)0.0106 (6)0.0060 (7)
N10.0336 (7)0.0373 (9)0.0332 (7)0.0045 (6)0.0006 (6)0.0038 (6)
N40.0376 (7)0.0326 (8)0.0270 (7)0.0128 (6)0.0002 (6)0.0019 (5)
N140.0456 (9)0.0388 (10)0.0415 (8)0.0134 (7)0.0091 (7)0.0052 (6)
N310.0291 (7)0.0462 (10)0.0323 (7)0.0133 (6)0.0004 (6)0.0007 (6)
N340.0396 (8)0.0387 (9)0.0265 (7)0.0168 (6)0.0051 (6)0.0005 (5)
N440.0554 (10)0.0461 (10)0.0346 (8)0.0180 (8)0.0148 (7)0.0063 (7)
C20.0383 (9)0.0408 (11)0.0298 (8)0.0120 (7)0.0007 (7)0.0013 (7)
C30.0372 (9)0.0342 (10)0.0267 (8)0.0132 (7)0.0008 (6)0.0011 (6)
C50.0314 (8)0.0300 (9)0.0278 (8)0.0108 (6)0.0027 (6)0.0027 (6)
C60.0380 (9)0.0312 (10)0.0335 (8)0.0120 (7)0.0054 (7)0.0033 (6)
C70.0443 (10)0.0344 (11)0.0413 (10)0.0157 (8)0.0124 (8)0.0002 (7)
C80.0574 (12)0.0307 (11)0.0439 (10)0.0125 (8)0.0132 (9)0.0068 (7)
C90.0505 (11)0.0335 (11)0.0327 (9)0.0032 (8)0.0039 (8)0.0065 (7)
C100.0373 (9)0.0311 (10)0.0249 (7)0.0063 (7)0.0048 (6)0.0009 (6)
C110.0364 (8)0.0289 (9)0.0241 (7)0.0099 (7)0.0048 (6)0.0009 (6)
C120.0367 (10)0.0503 (13)0.0470 (11)0.0010 (8)0.0012 (8)0.0073 (9)
C130.0406 (9)0.0352 (10)0.0296 (8)0.0151 (7)0.0020 (7)0.0009 (6)
C150.0699 (15)0.0586 (16)0.0650 (15)0.0186 (12)0.0228 (12)0.0274 (12)
C160.0427 (11)0.0603 (14)0.0487 (11)0.0082 (9)0.0086 (9)0.0076 (9)
C170.0344 (8)0.0352 (10)0.0268 (8)0.0165 (7)0.0003 (6)0.0057 (6)
C180.0533 (11)0.0360 (11)0.0375 (9)0.0137 (8)0.0001 (8)0.0068 (7)
C190.0555 (12)0.0484 (13)0.0465 (11)0.0124 (9)0.0061 (9)0.0199 (9)
C200.0540 (12)0.0697 (15)0.0320 (9)0.0307 (11)0.0082 (8)0.0183 (9)
C210.0506 (11)0.0617 (14)0.0272 (8)0.0322 (10)0.0028 (7)0.0012 (8)
C220.0390 (9)0.0405 (11)0.0310 (8)0.0180 (8)0.0033 (7)0.0021 (7)
C320.0429 (10)0.0420 (11)0.0286 (8)0.0173 (8)0.0029 (7)0.0012 (7)
C330.0431 (9)0.0391 (10)0.0248 (8)0.0187 (7)0.0023 (7)0.0010 (6)
C350.0281 (8)0.0335 (10)0.0282 (8)0.0110 (6)0.0026 (6)0.0005 (6)
C360.0343 (9)0.0365 (10)0.0277 (8)0.0110 (7)0.0010 (6)0.0013 (6)
C370.0501 (10)0.0332 (10)0.0268 (8)0.0091 (8)0.0033 (7)0.0013 (6)
C380.0562 (11)0.0366 (11)0.0374 (9)0.0187 (8)0.0142 (8)0.0012 (7)
C390.0404 (9)0.0417 (11)0.0382 (9)0.0200 (8)0.0118 (7)0.0044 (7)
C400.0304 (8)0.0328 (10)0.0278 (8)0.0106 (6)0.0049 (6)0.0029 (6)
C410.0310 (8)0.0299 (9)0.0257 (7)0.0106 (6)0.0054 (6)0.0020 (6)
C420.0304 (10)0.0629 (15)0.0581 (12)0.0144 (9)0.0017 (8)0.0033 (10)
C430.0505 (11)0.0404 (11)0.0281 (8)0.0186 (8)0.0030 (7)0.0011 (7)
C450.0712 (15)0.0549 (14)0.0442 (11)0.0166 (11)0.0205 (10)0.0112 (9)
C460.0541 (12)0.0562 (14)0.0487 (11)0.0231 (10)0.0166 (9)0.0029 (9)
C470.0279 (8)0.0325 (10)0.0321 (8)0.0108 (6)0.0019 (6)0.0008 (6)
C480.0375 (9)0.0417 (11)0.0420 (10)0.0174 (8)0.0098 (7)0.0009 (7)
C490.0392 (10)0.0473 (13)0.0617 (12)0.0214 (9)0.0092 (9)0.0040 (9)
C500.0435 (10)0.0376 (12)0.0617 (12)0.0196 (8)0.0013 (9)0.0035 (9)
C510.0461 (11)0.0409 (12)0.0445 (10)0.0143 (8)0.0052 (8)0.0094 (8)
C520.0336 (9)0.0389 (11)0.0348 (9)0.0134 (7)0.0062 (7)0.0030 (7)
Geometric parameters (Å, º) top
Cl1—C71.7446 (19)C17—C221.398 (2)
Cl2—C371.7403 (18)C18—C191.385 (3)
O1—C21.228 (2)C18—H180.9601
O2—C321.225 (2)C19—C201.385 (3)
N1—C21.382 (2)C19—H190.9599
N1—C101.425 (2)C20—C211.377 (3)
N1—C121.463 (2)C20—H200.9601
N4—C51.289 (2)C21—C221.388 (2)
N4—C31.408 (2)C21—H210.9599
N14—C131.338 (2)C22—H220.9598
N14—C161.447 (3)C32—C331.471 (3)
N14—C151.456 (3)C33—C431.376 (2)
N31—C321.393 (2)C35—C411.479 (2)
N31—C401.425 (2)C35—C471.491 (2)
N31—C421.463 (2)C36—C371.377 (3)
N34—C351.285 (2)C36—C411.400 (2)
N34—C331.399 (2)C36—H360.9600
N44—C431.336 (2)C37—C381.381 (3)
N44—C461.446 (3)C38—C391.383 (3)
N44—C451.456 (2)C38—H380.9600
C2—C31.476 (2)C39—C401.391 (2)
C3—C131.373 (2)C39—H390.9601
C5—C111.474 (2)C40—C411.399 (2)
C5—C171.493 (2)C42—H42A0.9600
C6—C71.372 (3)C42—H42B0.9600
C6—C111.401 (2)C42—H42C0.9600
C6—H60.9601C43—H430.9600
C7—C81.380 (3)C45—H45A0.9600
C8—C91.379 (3)C45—H45B0.9600
C8—H80.9601C45—H45C0.9600
C9—C101.393 (3)C46—H46A0.9600
C9—H90.9600C46—H46B0.9600
C10—C111.402 (2)C46—H46C0.9600
C12—H12A0.9600C47—C521.395 (2)
C12—H12B0.9600C47—C481.398 (2)
C12—H12C0.9600C48—C491.378 (3)
C13—H130.9601C48—H480.9604
C15—H15A0.9600C49—C501.380 (3)
C15—H15B0.9600C49—H490.9599
C15—H15C0.9600C50—C511.382 (3)
C16—H16A0.9600C50—H500.9599
C16—H16B0.9600C51—C521.387 (3)
C16—H16C0.9600C51—H510.9601
C17—C181.386 (3)C52—H520.9601
C2—N1—C10122.23 (14)C19—C20—H20120.0
C2—N1—C12116.42 (15)C20—C21—C22120.27 (18)
C10—N1—C12117.16 (16)C20—C21—H21120.0
C5—N4—C3124.29 (15)C22—C21—H21119.7
C13—N14—C16124.00 (16)C21—C22—C17120.57 (18)
C13—N14—C15119.21 (17)C21—C22—H22119.3
C16—N14—C15115.09 (17)C17—C22—H22120.1
C32—N31—C40118.68 (14)O2—C32—N31119.42 (17)
C32—N31—C42116.05 (15)O2—C32—C33122.71 (17)
C40—N31—C42117.33 (15)N31—C32—C33117.73 (14)
C35—N34—C33124.31 (15)C43—C33—N34121.96 (16)
C43—N44—C46123.93 (16)C43—C33—C32115.31 (16)
C43—N44—C45119.75 (17)N34—C33—C32120.97 (15)
C46—N44—C45115.34 (17)N34—C35—C41123.41 (15)
O1—C2—N1118.98 (17)N34—C35—C47116.45 (15)
O1—C2—C3122.44 (17)C41—C35—C47120.21 (13)
N1—C2—C3118.55 (15)C37—C36—C41120.18 (16)
C13—C3—N4121.51 (16)C37—C36—H36119.8
C13—C3—C2114.42 (15)C41—C36—H36120.1
N4—C3—C2122.08 (15)C36—C37—C38121.55 (16)
N4—C5—C11124.19 (14)C36—C37—Cl2119.39 (14)
N4—C5—C17117.25 (15)C38—C37—Cl2119.06 (15)
C11—C5—C17118.11 (14)C37—C38—C39118.53 (17)
C7—C6—C11120.85 (16)C37—C38—H38120.1
C7—C6—H6119.5C39—C38—H38121.3
C11—C6—H6119.6C38—C39—C40121.19 (17)
C6—C7—C8121.10 (18)C38—C39—H39119.9
C6—C7—Cl1118.06 (14)C40—C39—H39118.9
C8—C7—Cl1120.82 (15)C39—C40—C41119.86 (15)
C7—C8—C9118.67 (18)C39—C40—N31120.11 (15)
C7—C8—H8120.0C41—C40—N31120.03 (15)
C9—C8—H8121.4C40—C41—C36118.66 (16)
C8—C9—C10121.62 (17)C40—C41—C35121.20 (14)
C8—C9—H9120.2C36—C41—C35119.92 (15)
C10—C9—H9118.1N31—C42—H42A109.5
C9—C10—C11119.32 (17)N31—C42—H42B109.5
C9—C10—N1120.01 (16)H42A—C42—H42B109.5
C11—C10—N1120.57 (16)N31—C42—H42C109.5
C10—C11—C6118.41 (16)H42A—C42—H42C109.5
C10—C11—C5123.34 (15)H42B—C42—H42C109.5
C6—C11—C5118.14 (15)N44—C43—C33131.39 (18)
N1—C12—H12A109.5N44—C43—H43120.2
N1—C12—H12B109.5C33—C43—H43108.4
H12A—C12—H12B109.5N44—C45—H45A109.5
N1—C12—H12C109.5N44—C45—H45B109.5
H12A—C12—H12C109.5H45A—C45—H45B109.5
H12B—C12—H12C109.5N44—C45—H45C109.5
N14—C13—C3129.46 (16)H45A—C45—H45C109.5
N14—C13—H13119.9H45B—C45—H45C109.5
C3—C13—H13110.7N44—C46—H46A109.5
N14—C15—H15A109.5N44—C46—H46B109.5
N14—C15—H15B109.5H46A—C46—H46B109.5
H15A—C15—H15B109.5N44—C46—H46C109.5
N14—C15—H15C109.5H46A—C46—H46C109.5
H15A—C15—H15C109.5H46B—C46—H46C109.5
H15B—C15—H15C109.5C52—C47—C48118.10 (16)
N14—C16—H16A109.5C52—C47—C35122.09 (15)
N14—C16—H16B109.5C48—C47—C35119.65 (15)
H16A—C16—H16B109.5C49—C48—C47120.76 (17)
N14—C16—H16C109.5C49—C48—H48119.3
H16A—C16—H16C109.5C47—C48—H48119.9
H16B—C16—H16C109.5C48—C49—C50120.61 (18)
C18—C17—C22118.41 (16)C48—C49—H49119.5
C18—C17—C5120.47 (15)C50—C49—H49119.9
C22—C17—C5121.12 (16)C49—C50—C51119.56 (18)
C19—C18—C17120.82 (19)C49—C50—H50120.4
C19—C18—H18119.2C51—C50—H50120.0
C17—C18—H18120.0C50—C51—C52120.21 (18)
C20—C19—C18120.3 (2)C50—C51—H51119.7
C20—C19—H19119.5C52—C51—H51120.0
C18—C19—H19120.2C51—C52—C47120.75 (17)
C21—C20—C19119.62 (17)C51—C52—H52119.3
C21—C20—H20120.3C47—C52—H52120.0

Experimental details

Crystal data
Chemical formulaC19H18ClN3O
Mr339.81
Crystal system, space groupTriclinic, P1
Temperature (K)293
a, b, c (Å)9.2793 (2), 9.4256 (2), 20.6390 (8)
α, β, γ (°)84.713 (1), 80.583 (1), 69.210 (1)
V3)1663.73 (8)
Z4
Radiation typeMo Kα
µ (mm1)0.24
Crystal size (mm)0.4 × 0.3 × 0.1
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
22942, 6167, 5488
Rint0.033
(sin θ/λ)max1)0.625
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.046, 0.114, 1.05
No. of reflections6155
No. of parameters439
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.40, 0.49

Computer programs: KappaCCD Reference Manual (Nonius, 1998), DENZO and SCALEPACK (Otwinowski & Minor, 1997), SIR92 (Altomare et al., 1994), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), SHELXL97.

Selected geometric parameters (Å, º) top
Cl1—C71.7446 (19)N31—C421.463 (2)
Cl2—C371.7403 (18)N34—C351.285 (2)
O1—C21.228 (2)N34—C331.399 (2)
O2—C321.225 (2)N44—C431.336 (2)
N1—C21.382 (2)N44—C461.446 (3)
N1—C101.425 (2)N44—C451.456 (2)
N1—C121.463 (2)C2—C31.476 (2)
N4—C51.289 (2)C3—C131.373 (2)
N4—C31.408 (2)C5—C111.474 (2)
N14—C131.338 (2)C10—C111.402 (2)
N14—C161.447 (3)C32—C331.471 (3)
N14—C151.456 (3)C33—C431.376 (2)
N31—C321.393 (2)C35—C411.479 (2)
N31—C401.425 (2)C40—C411.399 (2)
C2—N1—C10122.23 (14)N4—C5—C11124.19 (14)
C5—N4—C3124.29 (15)C9—C10—N1120.01 (16)
C16—N14—C15115.09 (17)C10—C11—C6118.41 (16)
C32—N31—C40118.68 (14)N31—C32—C33117.73 (14)
C35—N34—C33124.31 (15)N34—C33—C32120.97 (15)
C46—N44—C45115.34 (17)N34—C35—C41123.41 (15)
N1—C2—C3118.55 (15)C41—C40—N31120.03 (15)
N4—C3—C2122.08 (15)C40—C41—C35121.20 (14)
 

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