organic papers
o1182
Yu, Wang and Miao C19H16F3N3O2S DOI: 10.1107/S1600536802017348 Acta Cryst.(2002). E58, o1182±o1184 Acta Crystallographica Section EStructure Reports
Online
ISSN 1600-5368
1,5-Dimethyl-4-{[(
E
)-3-oxo-3-(2-thienyl)-
1-(trifluoromethyl)-1-propenyl]amino}-2-phenyl-1,2-dihydro-3
H
-pyrazol-3-one
Ming Yu,aJin-Ling Wangb* and Fang-Ming Miaob
aDepartment of Scientific Technology, The
Scientific and Technology University of Tianjin, Tianjin 300222, People's Republic of China, andbCollege of Chemical and Life Science, Tianjin Normal University, Tianjin 300074, People's Republic of China
Correspondence e-mail: wangjinling43@eyou.com
Key indicators Single-crystal X-ray study T= 297 K
Mean(C±C) = 0.005 AÊ Disorder in main residue Rfactor = 0.056 wRfactor = 0.172
Data-to-parameter ratio = 11.3
For details of how these key indicators were automatically derived from the article, see http://journals.iucr.org/e.
#2002 International Union of Crystallography Printed in Great Britain ± all rights reserved
In the title compound, C19H16F3N3O2S, the side-chain
carbonyl group, the adjacent double bond and the amine N atom are essentially coplanar, with the largest deviation from the mean plane being 0.010 (2) AÊ. A strong intramolecular
NÐH O hydrogen bond [N O 2.702 (3) AÊ and NÐH O
139 (3)] is observed, leading to an enamine tautomer in the
solid state.
Comment
Schiff base ligands derived from 4-aminoantipyrine, such as salicylidene-4-aminoantipyrine, 5-chlorosalicylidene-4-amino-antipyrine, 2,4-dihydroxybenzylidene-4-amino5-chlorosalicylidene-4-amino-antipyrine, 1-naphthylidene-4-aminoantipyrine and 2-hydroxy-acetophenonylidene-4-aminoantipyrine, have been reported by McLendon & Martell (1976) and by Radhakrishnan & Joseph (1976). In order to study the coordination properties of Schiff base compounds, we have synthesized some of these compounds, and we report here the structure of the title compound, (I).
A view of the molecule of (I) is shown in Fig. 1. Atoms C6, C7, C8 and O1 of the thenoyltri¯uoroacetone moiety and atom N3 of 4-aminoantipyrine are essentially coplanar, the largest deviation from the mean plane being 0.010 (2) AÊ for atom C6; the dihedral angle between this plane and the thienyl plane is 22.48 (3). The bond lengths within this part of the
molecule [N3ÐC6 = 1.340 (4) AÊ, C6ÐC7 = 1.401 (4) AÊ, C7Ð C8 = 1.396 (4) AÊ and C8ÐO1 = 1.235 (4) AÊ] lie between the classical double- and single-bond lengths. These results clearly indicate that there is electron delocalization over this segment. An intramolecular hydrogen bond is observed (Table 1), which indicates that the molecule exists as the enamine tautomer. This situation is completely different from that of 3- (2,3-dihydro-1,5-dimethyl-3-oxo-2-phenylpyrazol-4-ylimino)-4,4,4-tri¯uoro-1-(2-thienyl)butane-1,2-dione (Wang et al., 2002), but similar to that of pyrazolinehydrazide (Liuet al., 2001). The displacements of atoms C5 and C21 from the
pyrazolinone ring are 0.454 (7) and ÿ0.479 (5) AÊ, respec-tively, showing that the methyl group bonded to N1 and the phenyl group bonded to N2 are on opposite sides of the ring. Intermolecular contact distances of interest are: O2 S1i =
3.040 (4) AÊ, C4ÐH41 O1i = 3.380 (4) AÊ [angle of
135.01 (4) at H41], C4ÐH41 F2i = 2.930 (4) AÊ [angle of
138.96 (4) at H41], C5ÐH53 F2Ai= 3.418 (5) AÊ [angle of
163.71 (5) at H53], C4ÐH42 O1ii= 3.380 (4) AÊ [angle of
135.01 (5) at H42], and C4ÐH43 F2Aiii = 3.366 (5) AÊ
[angle of 116.32 (5)at H43] [symmetry codes: (i) 1ÿx,ÿy,
1ÿz; (ii)ÿ1 +x, y, z; (iii)ÿx,ÿy, 1ÿz].
The torsion angle C21ÐN2ÐN1ÐC5 is 51.2 (4), close to
the values of 55.6 (3) and 55.7 (3) for the compounds
4-(salicylideneamino)-2-3-dimethyl-1-phenyl-3-pyrazolin-5-one
(Chumakov et al., 2000) and 4-{[(1E)-(2-hydroxyphenyl)
methylidene]amino}-1,5-dimethyl-2-phenyl-2,3-dihydro-1H -pyrazol-3-one (HoÈkeleket al., 2001). By contrast, conjugation leads to a small torsion angle of 7.75 in
4-(antipyrin-4-yl-iminomethyl)benzoic acid (Zhanget al., 2002).
The mean plane through the side-chain carbonyl group, the adjacent double bond and the amino N atom is nearly perpendicular to the pyrazolinone ring, with a dihedral angle of 84.10 (6), close to the value of 82.43 (8)reported by Wang et al. (2002). However, the dihedral angle between the pyrazolinone ring and the phenyl ring is 115.26 (5), quite
different from the value of 41.7 (5)in
4-(salicylideneamino)-2,3-dimethyl-1-phenyl-3-pyrazolin-5-one (Chumakov et al., 2000). These results indicate that the compounds may have quite different coordination properties as ligands to metal ions.
Experimental
Ethanol solutions of 0.1 mol of 4-aminoantipyrine and 0.1 mol of thenoyltri¯uoroacetone were re¯uxed together for 4 h over a steam bath. The excess solvent was removed by evaporation and the concentrated solution was cooled in an ice bath, with stirring. The title compound separated out as a cream-colored powder, which was collected and dried in air (m.p. 434 K). It was recrystallized from
ethanol and dried in a vacuum over CaCl2. The product is stable in
air, and soluble in acetone and ethanol. Elemental analysis for C19H16F3N3O2S, calculated: C 56.01, H 10.31, N 3.96%; found: C
55.87, H 10.16, N 3.94%. Bright-yellow single crystals suitable for X-ray analysis were obtained by slow cooling of a warmed solution in dimethyl sulfoxide.
Crystal data
C19H16F3N3O2S Mr= 407.42
Triclinic,P1
a= 5.8063 (10) AÊ
b= 10.9254 (17) AÊ
c= 15.288 (2) AÊ = 74.790 (3)
= 97.463 (3)
= 94.731 (4) V= 926.7 (2) AÊ3
Z= 2
Dx= 1.460 Mg mÿ3
MoKradiation Cell parameters from 3101
re¯ections = 1.5±25.1
= 0.22 mmÿ1 T= 297 (2) K Prism, yellow 0.350.300.25 mm
Data collection
Bruker SMART 1000 CCD diffractometer
!scans
Absorption correction: multi-scan (SADABS; Bruker, 1999)
Tmin= 0.926,Tmax= 0.946 3860 measured re¯ections
3245 independent re¯ections 2229 re¯ections withI> 2(I)
Rint= 0.018 max= 25.0 h=ÿ5!6
k=ÿ12!8
l=ÿ18!17
Re®nement
Re®nement onF2 R[F2> 2(F2)] = 0.057 wR(F2) = 0.173 S= 1.04 3245 re¯ections 286 parameters
H-atom parameters constrained
w= 1/[2(F
o2) + (0.0983P)2
+ 0.1991P]
whereP= (Fo2+ 2Fc2)/3
(/)max= 0.002 max= 0.33 e AÊÿ3 min=ÿ0.45 e AÊÿ3
Extinction correction:SHELXL97 Extinction coef®cient: 0.011 (4)
Table 1
Hydrogen-bonding geometry (AÊ,).
DÐH A DÐH H A D A DÐH A
N3ÐH3 O1 0.81 (4) 2.04 (4) 2.702 (3) 139 (3)
Some rather high residual electron densities close to the CF3group
and staggered with respect to the F atoms appeared in a difference Fourier map. A disordered distribution of the F atoms was re®ned with geometrical restraints; this led to much lower residual electron density and to lowerRandwR2 values.
Data collection:SMART(Bruker, 1999); cell re®nement:SAINT
(Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to re®ne structure: SHELXL97 (Sheldrick, 1997); molecular graphics:
ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication:WinGX(Farrugia, 1999).
This work was supported by the Foundation of Tianjin Scienti®c Committee (003601711).
References
Bruker (1999).SADABS, SMARTandSAINT. Bruker AXS Inc., Madison, Wisconsin, USA.
Chumakov, Yu. M., Antosyak, B. Ya., Mazus, M. D., Tsapkov, V. I. & Samus, N. N. (2000).Zh. Strukt. Khim.41, 1095±1997.
Farrugia, L. J. (1997).J. Appl. Cryst.30, 565. Farrugia, L. J. (1999).J. Appl. Cryst.32, 837±838.
Acta Cryst.(2002). E58, o1182±o1184 Yu, Wang and Miao C19H16F3N3O2S
o1183
organic papers
Figure 1
organic papers
o1184
Yu, Wang and Miao C19H16F3N3O2S Acta Cryst.(2002). E58, o1182±o1184 HoÈkelek, T., Isiklan, M. & Kilic, Z. (2001).Acta Cryst.C57, 117±119.Liu, L., Jia, D.-Z., Qiao, Y.-M. & Yu, K.-B. (2001).Acta Chim. Sin.59, 1495± 1501.
McLendon, G. & Martell, A. E. (1976).Coord. Chem. Rev.19, 1±39.
supporting information
sup-1 Acta Cryst. (2002). E58, o1182–o1184
supporting information
Acta Cryst. (2002). E58, o1182–o1184 [https://doi.org/10.1107/S1600536802017348]
1,5-Dimethyl-4-{[(
E
)-3-oxo-3-(2-thienyl)-1-(trifluoromethyl)-1-propenyl]amino}-2-phenyl-1,2-dihydro-3
H
-pyrazol-3-one
Ming Yu, Jin-Ling Wang and Fang-Ming Miao
(I)
Crystal data
C19H16F3N3O2S
Mr = 407.42
Triclinic, P1
a = 5.8063 (10) Å
b = 10.9254 (17) Å
c = 15.288 (2) Å
α = 74.790 (3)°
β = 97.463 (3)°
γ = 94.731 (4)°
V = 926.7 (2) Å3
Z = 2
F(000) = 420
Dx = 1.460 Mg m−3 Melting point: 161° K
Mo Kα radiation, λ = 0.71073 Å Cell parameters from 3101 reflections
θ = 1.5–25.1°
µ = 0.22 mm−1
T = 297 K Prism, yellow
0.35 × 0.30 × 0.25 mm
Data collection
Bruker SMART 1000 CCD diffractometer
Radiation source: fine-focus sealed tube Graphite monochromator
ω scans
Absorption correction: empirical (using intensity measurements)
(SADABS; Bruker, 1999)
Tmin = 0.926, Tmax = 0.946
3860 measured reflections 3245 independent reflections 2229 reflections with I > 2σ(I)
Rint = 0.018
θmax = 25.0°, θmin = 1.4°
h = −5→6
k = −12→8
l = −18→17
Refinement
Refinement on F2 Least-squares matrix: full
R[F2 > 2σ(F2)] = 0.057
wR(F2) = 0.173
S = 1.04 3245 reflections 286 parameters 338 restraints
Primary atom site location: structure-invariant direct methods
Secondary atom site location: difference Fourier map
Hydrogen site location: inferred from neighbouring sites
H-atom parameters constrained
w = 1/[σ2(F
o2) + (0.0983P)2 + 0.1991P] where P = (Fo2 + 2Fc2)/3
(Δ/σ)max = 0.002 Δρmax = 0.33 e Å−3 Δρmin = −0.45 e Å−3
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sup-2 Acta Cryst. (2002). E58, o1182–o1184
Special details
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)
S1 −0.23537 (16) 0.10275 (9) 0.21827 (6) 0.0521 (3) O1 0.5666 (4) −0.0983 (2) 0.44029 (16) 0.0470 (6) O2 0.3820 (4) 0.2882 (2) 0.18883 (17) 0.0534 (7) C6 0.1737 (5) −0.0213 (3) 0.2999 (2) 0.0341 (7) N1 −0.0231 (5) 0.3609 (2) 0.31225 (18) 0.0390 (6) N2 0.1358 (5) 0.3970 (2) 0.24688 (18) 0.0409 (7) N3 0.2464 (5) 0.0669 (2) 0.34539 (19) 0.0366 (6) H3 0.347 (6) 0.046 (3) 0.387 (2) 0.046 (10)* C8 0.4698 (6) −0.1652 (3) 0.3911 (2) 0.0377 (7) C9 0.5668 (7) −0.2959 (3) 0.4084 (3) 0.0571 (10)
F1 0.4504 (6) −0.3742 (3) 0.3645 (3) 0.0903 (11) 0.90 F2 0.7836 (5) −0.2878 (3) 0.3908 (3) 0.1076 (13) 0.90 F3 0.5826 (9) −0.3552 (3) 0.4969 (2) 0.1119 (14) 0.90 F1A 0.626 (2) −0.3133 (15) 0.3328 (10) 0.097 (8) 0.10 F2A 0.750 (2) −0.3093 (18) 0.4663 (9) 0.084 (8) 0.10 F3A 0.418 (3) −0.3858 (14) 0.4452 (9) 0.095 (8) 0.10 C1 0.2518 (5) 0.2906 (3) 0.2455 (2) 0.0368 (7)
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sup-3 Acta Cryst. (2002). E58, o1182–o1184
H14 −0.5341 0.0847 0.1028 0.081* C21 0.0796 (6) 0.4990 (3) 0.1676 (2) 0.0390 (7) C22 −0.1366 (6) 0.5035 (3) 0.1193 (3) 0.0492 (9) H22 −0.2541 0.4400 0.1388 0.074* C23 −0.1829 (7) 0.6016 (4) 0.0415 (3) 0.0580 (10) H23 −0.3323 0.6056 0.0074 0.087* C24 −0.0117 (8) 0.6924 (4) 0.0143 (3) 0.0601 (10) H24 −0.0433 0.7598 −0.0387 0.090* C25 0.2025 (8) 0.6872 (4) 0.0622 (3) 0.0622 (11) H25 0.3199 0.7504 0.0420 0.093* C26 0.2522 (7) 0.5907 (3) 0.1405 (3) 0.0522 (9) H26 0.4015 0.5878 0.1746 0.078*
Atomic displacement parameters (Å2)
U11 U22 U33 U12 U13 U23
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sup-4 Acta Cryst. (2002). E58, o1182–o1184
Geometric parameters (Å, º)
S1—C14 1.682 (4) C4—H4A 0.980 S1—C11 1.723 (3) C4—H4B 0.980 O1—C8 1.235 (4) C4—H4C 0.980 O2—C1 1.228 (4) C5—H5A 0.980 C6—N3 1.340 (4) C5—H5B 0.980 C6—C7 1.401 (4) C5—H5C 0.980 C6—C11 1.458 (4) C7—H7 0.950 N1—C3 1.343 (4) C11—C12 1.447 (5) N1—N2 1.406 (4) C12—C13 1.453 (5) N1—C5 1.455 (4) C12—H12 0.950 N2—C1 1.397 (4) C13—C14 1.346 (6) N2—C21 1.437 (4) C13—H13 0.950 N3—C2 1.416 (4) C14—H14 0.950 N3—H3 0.81 (4) C21—C22 1.369 (5) C8—C7 1.396 (4) C21—C26 1.380 (5) C8—C9 1.524 (5) C22—C23 1.390 (5) C9—F2A 1.285 (13) C22—H22 0.950 C9—F1A 1.311 (13) C23—C24 1.369 (6) C9—F2 1.312 (5) C23—H23 0.950 C9—F3A 1.314 (13) C24—C25 1.357 (6) C9—F1 1.315 (4) C24—H24 0.950 C9—F3 1.333 (5) C25—C26 1.388 (5) C1—C2 1.438 (4) C25—H25 0.950 C2—C3 1.356 (4) C26—H26 0.950 C3—C4 1.494 (4)
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sup-5 Acta Cryst. (2002). E58, o1182–o1184
F2—C9—F3 102.5 (4) C13—C14—S1 113.1 (3) F1—C9—F3 106.8 (4) C13—C14—H14 123.5 F2A—C9—C8 112.0 (9) S1—C14—H14 123.5 F1A—C9—C8 110.6 (8) C22—C21—C26 121.0 (3) F2—C9—C8 111.7 (3) C22—C21—N2 121.1 (3) F3A—C9—C8 111.0 (9) C26—C21—N2 117.9 (3) F1—C9—C8 116.4 (3) C21—C22—C23 119.6 (3) F3—C9—C8 110.8 (3) C21—C22—H22 120.2 O2—C1—N2 124.6 (3) C23—C22—H22 120.2 O2—C1—C2 131.6 (3) C24—C23—C22 119.5 (4) N2—C1—C2 103.8 (3) C24—C23—H23 120.2 C3—C2—N3 126.8 (3) C22—C23—H23 120.2 C3—C2—C1 109.1 (3) C25—C24—C23 120.7 (3) N3—C2—C1 123.9 (3) C25—C24—H24 119.7 N1—C3—C2 109.8 (3) C23—C24—H24 119.7 N1—C3—C4 121.1 (3) C24—C25—C26 120.8 (4) C2—C3—C4 129.0 (3) C24—C25—H25 119.6 C3—C4—H4A 109.5 C26—C25—H25 119.6 C3—C4—H4B 109.5 C21—C26—C25 118.4 (4) H4A—C4—H4B 109.5 C21—C26—H26 120.8 C3—C4—H4C 109.5 C25—C26—H26 120.8
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sup-6 Acta Cryst. (2002). E58, o1182–o1184
O2—C1—C2—N3 0.4 (6) C22—C23—C24—C25 0.3 (6) N2—C1—C2—N3 178.8 (3) C23—C24—C25—C26 −0.8 (7) N2—N1—C3—C2 −6.2 (4) C22—C21—C26—C25 −0.7 (6) C5—N1—C3—C2 −154.6 (3) N2—C21—C26—C25 177.8 (3) N2—N1—C3—C4 176.6 (3) C24—C25—C26—C21 1.0 (6) C5—N1—C3—C4 28.1 (5)
Hydrogen-bond geometry (Å, º)
D—H···A D—H H···A D···A D—H···A