organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890
Volume 71| Part 6| June 2015| Pages o383-o384

Crystal structure of (Z)-2-(5-fluoro-2-oxoindolin-3-yl­­idene)hydrazinecarbo­thio­amide

aEscola de Química e Alimentos, Universidade Federal do Rio Grande, Av. Itália km 08, Campus Carreiros, 96203-900 Rio Grande-RS, Brazil, bDepartamento de Química, Universidade Federal de Santa Maria, Av. Roraima s/n, Campus Universitário, 97105-900 Santa Maria-RS, Brazil, and cDepartamento de Química, Universidade Federal de Sergipe, Av. Marechal Rondon s/n, Campus Universitário, 49100-000 São Cristóvão-SE, Brazil
*Correspondence e-mail: vanessa.gervini@gmail.com

Edited by M. Lopez-Rodriguez, Universidad de La Laguna, Tenerife (Received 22 April 2015; accepted 3 May 2015; online 9 May 2015)

In the title compound, C9H7FN4OS, the mol­ecules are almost planar, with an r.m.s. deviation of 0.047 (3) Å from the mean plane defined by the non-H atoms and a maximum deviation of 0.123 (2) Å for the amine N atom. The torsion angle for the N—N—C—S unit is 176.57 (19)°. In the crystal, mol­ecules are linked into inversion dimers via pairs of N—H⋯F hydrogen bonds and, additionally, through N—H⋯O and N—H⋯S hydrogen bonds, building a two-dimensional hydrogen-bond network parallel to the (103) plane. An intra­molecular N—H⋯O inter­action is also observed.

1. Related literature

For one of the first reports of the synthesis of thio­semicarbazone derivatives, see: Freund & Schander (1902[Freund, M. & Schander, A. (1902). Chem. Ber. 35, 2602-2606.]). For the synthesis and crystal structure of a similar compound, namely (Z)-2-(5-fluoro-2-oxoindolin-3-yl­idene)-N-phenyl­hydrazinecarbo­thio­amide, see: Ali et al. (2012[Ali, A. Q., Eltayeb, N. E., Teoh, S. G., Salhin, A. & Fun, H.-K. (2012). Acta Cryst. E68, o285-o286.]). For a review on hydrogen bonding, see: Steiner (2002[Steiner, T. (2002). Angew. Chem. Int. Ed. 41, 48-76.]).

[Scheme 1]

2. Experimental

2.1. Crystal data

  • C9H7FN4OS

  • Mr = 238.25

  • Monoclinic, P 21 /n

  • a = 4.7151 (1) Å

  • b = 15.4517 (4) Å

  • c = 13.9645 (4) Å

  • β = 93.921 (2)°

  • V = 1015.02 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.32 mm−1

  • T = 293 K

  • 0.44 × 0.16 × 0.11 mm

2.2. Data collection

  • Bruker X8 Kappa APEXII diffractometer

  • Absorption correction: numerical (SADABS; Bruker 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.954, Tmax = 0.966

  • 12531 measured reflections

  • 2239 independent reflections

  • 1390 reflections with I > 2σ(I)

  • Rint = 0.064

2.3. Refinement

  • R[F2 > 2σ(F2)] = 0.049

  • wR(F2) = 0.140

  • S = 1.01

  • 2239 reflections

  • 145 parameters

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.29 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3⋯O1 0.86 2.12 2.781 (3) 133
N1—H1⋯S1i 0.86 2.55 3.367 (2) 158
N4—H4A⋯F1ii 0.86 2.24 2.956 (3) 140
N4—H4B⋯O1iii 0.86 2.03 2.879 (3) 171
Symmetry codes: (i) [-x+{\script{1\over 2}}, y+{\script{1\over 2}}, -z+{\script{3\over 2}}]; (ii) -x+2, -y, -z+1; (iii) [-x+{\script{1\over 2}}, y-{\script{1\over 2}}, -z+{\script{3\over 2}}].

Data collection: APEX2 (Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2009[Bruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; 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: DIAMOND (Brandenburg, 2006[Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany.]); software used to prepare material for publication: publCIF (Westrip, 2010[Westrip, S. P. (2010). J. Appl. Cryst. 43, 920-925.]).

Supporting information


Structural commentary top

\ Concerning our inter­est on the study of the supra­molecular chemistry of thio­semicarbazone derivatives from natural products, we report herein the crystal structure of the (Z)-2-(5-fluoro-2-oxoindolin-3-yl­idene)-N-\ hydrazinecarbo­thio­amide, a thio­semicarbazone derivative from 5-fluorisatin (Fig. 1). The molecular structure of the title compound matches the asymmetric unit and itsn't planar. The maximum deviation from the mean plane of the non-H atoms amounts to 0.1229 (22) Å for N4 and the torsion angle for the N2–N3–C9–S1–entity amounts to 176.57 (19)°. All bond distances and angles are consistent with literature data of a similiar compound, (Z)-2-(5-fluoro-2-oxoindolin-3-yl­idene)-N-\ phenyl­hydrazinecarbo­thio­amide (Ali et al., 2012). In the crystal of the title compound, the molecules are linked into dimers via pairs of N4—H4A···F1 hydrogen bonds. The dimers are linked into a two dimensional hydrogen bonded network through the N1—H1···S1, O1···H4B—N4 and S1···H1—N1 hydrogen bonds. In addition, an intra­molecular N3—H3···O1 inter­action is also observed and the O1 atom builds a bifurcated hydrogen bonding with the H3 and H4B atoms (Table 1, Fig. 2 and Steiner, 2002). The 2-D H-bonded polymers are stacked along the a-axis without any strong or relevant inter­molecular inter­actions between themselves. The molecules of the title compound are also related by two fold screw axis parallel to the b-direction (Fig. 2)

Synthesis and crystallization top

Starting materials were commercially available and were used without further purification. The synthesis was adapted from a procedure reported previously (Freund & Schander, 1902). The hydro­chloric acid catalyzed reaction of 5-fluorisatin (8,83 mmol) and thio­semicarbazide (8,83 mmol) in ethanol (50 ml) was refluxed for 6 h. After cooling and filtering, the title compound was obtained. Crystals suitable for X-ray diffraction of title compound were obtained in ethanol by the slow evaporation of the solvent.

Refinement top

All aromatic H atoms were positioned with idealized geometry and were refined isotropic with Uiso(H) = 1.2 Ueq(C) using a riding model with C—H = 0.93 Å. The other H atoms were located in difference map but were positioned with idealized geometry and refined isotropic with Uiso(H) = 1.2 Ueq(N) using a riding model with N—H = 0.86 Å.

Related literature top

For one of the first reports of the synthesis of thiosemicarbazone derivatives, see: Freund & Schander (1902). For the synthesis and crystal structure of a similar compound, namely (Z)-2-(5-fluoro-2-oxoindolin-3-ylidene)-N-phenylhydrazinecarbothioamide, see: Ali et al. (2012). For a review on hydrogen bonding, see: Steiner (2002).

Computing details top

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. : The molecular structure of the title compound with labeling and displacement ellipsoids drawn at the 40% probability level. H atoms are drawn isotropically.
[Figure 2] Fig. 2. : A view, down the c axis, of the packing of the title compound showing the two dimensional hydrogen-bond network. Hydrogen bonds are shown as dashed lines.
(Z)-2-(5-Fluoro-2-oxoindolin-3-ylidene)hydrazinecarbothioamide top
Crystal data top
C9H7FN4OSF(000) = 488
Mr = 238.25Dx = 1.559 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 1744 reflections
a = 4.7151 (1) Åθ = 2.6–22.4°
b = 15.4517 (4) ŵ = 0.32 mm1
c = 13.9645 (4) ÅT = 293 K
β = 93.921 (2)°Block, orange
V = 1015.02 (4) Å30.44 × 0.16 × 0.11 mm
Z = 4
Data collection top
Bruker X8 Kappa APEXII
diffractometer
2239 independent reflections
Radiation source: fine-focus sealed tube, Bruker X8 Kappa APEX II1390 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.064
Detector resolution: 8.3333 pixels mm-1θmax = 27.2°, θmin = 2.0°
0.5 ° ω & ϕ scansh = 36
Absorption correction: numerical
(SADABS; Bruker 2009)
k = 1919
Tmin = 0.954, Tmax = 0.966l = 1717
12531 measured reflections
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)] = 0.049Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.140H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.0642P)2 + 0.1779P]
where P = (Fo2 + 2Fc2)/3
2239 reflections(Δ/σ)max < 0.001
145 parametersΔρmax = 0.20 e Å3
0 restraintsΔρmin = 0.29 e Å3
Crystal data top
C9H7FN4OSV = 1015.02 (4) Å3
Mr = 238.25Z = 4
Monoclinic, P21/nMo Kα radiation
a = 4.7151 (1) ŵ = 0.32 mm1
b = 15.4517 (4) ÅT = 293 K
c = 13.9645 (4) Å0.44 × 0.16 × 0.11 mm
β = 93.921 (2)°
Data collection top
Bruker X8 Kappa APEXII
diffractometer
2239 independent reflections
Absorption correction: numerical
(SADABS; Bruker 2009)
1390 reflections with I > 2σ(I)
Tmin = 0.954, Tmax = 0.966Rint = 0.064
12531 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.140H-atom parameters constrained
S = 1.01Δρmax = 0.20 e Å3
2239 reflectionsΔρmin = 0.29 e Å3
145 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
S10.02917 (16)0.03364 (5)0.86791 (6)0.0558 (3)
O10.3669 (4)0.28879 (12)0.73620 (14)0.0506 (5)
F11.2874 (4)0.11434 (14)0.40106 (15)0.0840 (7)
N30.3467 (4)0.10914 (14)0.74614 (16)0.0452 (6)
H30.29580.15720.77080.054*
N10.6921 (4)0.32661 (14)0.62633 (16)0.0472 (6)
H10.68640.38200.63190.057*
N20.5310 (4)0.10861 (14)0.67623 (16)0.0433 (5)
N40.3217 (5)0.03703 (14)0.73181 (19)0.0587 (7)
H4A0.43270.03220.68570.070*
H4B0.26280.08720.74810.070*
C10.8212 (5)0.19327 (16)0.57361 (19)0.0411 (6)
C80.6233 (5)0.18194 (16)0.64722 (19)0.0402 (6)
C70.5406 (5)0.27122 (16)0.67762 (19)0.0413 (6)
C60.8603 (5)0.28250 (17)0.56272 (19)0.0412 (6)
C51.0436 (6)0.31552 (19)0.4996 (2)0.0502 (7)
H51.07060.37480.49360.060*
C31.1423 (6)0.1702 (2)0.4555 (2)0.0549 (8)
C20.9634 (5)0.13570 (19)0.5189 (2)0.0507 (7)
H20.93930.07620.52460.061*
C90.2420 (5)0.03249 (16)0.7774 (2)0.0431 (6)
C41.1869 (6)0.2569 (2)0.4450 (2)0.0553 (8)
H41.31290.27660.40150.066*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0683 (5)0.0365 (4)0.0666 (5)0.0055 (3)0.0331 (4)0.0047 (3)
O10.0629 (11)0.0349 (10)0.0560 (12)0.0082 (9)0.0181 (10)0.0011 (9)
F10.0816 (12)0.0853 (15)0.0906 (15)0.0084 (11)0.0470 (11)0.0180 (12)
N30.0534 (12)0.0273 (11)0.0571 (15)0.0001 (9)0.0209 (11)0.0011 (10)
N10.0558 (13)0.0259 (11)0.0614 (15)0.0024 (9)0.0153 (12)0.0024 (10)
N20.0457 (11)0.0331 (12)0.0526 (14)0.0004 (9)0.0150 (10)0.0001 (10)
N40.0721 (15)0.0292 (12)0.0798 (18)0.0060 (11)0.0412 (14)0.0022 (12)
C10.0408 (13)0.0347 (14)0.0484 (16)0.0003 (11)0.0082 (12)0.0001 (11)
C80.0407 (13)0.0317 (14)0.0486 (16)0.0020 (11)0.0064 (12)0.0014 (11)
C70.0489 (14)0.0289 (13)0.0466 (15)0.0025 (11)0.0062 (12)0.0000 (11)
C60.0422 (13)0.0339 (14)0.0478 (16)0.0016 (11)0.0037 (12)0.0036 (11)
C50.0495 (15)0.0470 (17)0.0544 (18)0.0081 (13)0.0065 (13)0.0096 (14)
C30.0513 (16)0.060 (2)0.0551 (19)0.0032 (14)0.0170 (14)0.0062 (15)
C20.0497 (14)0.0437 (16)0.0604 (19)0.0022 (13)0.0157 (13)0.0020 (14)
C90.0452 (14)0.0314 (13)0.0537 (17)0.0003 (11)0.0106 (12)0.0004 (12)
C40.0484 (15)0.068 (2)0.0514 (18)0.0079 (14)0.0127 (14)0.0075 (15)
Geometric parameters (Å, º) top
S1—C91.667 (3)C1—C21.377 (4)
O1—C71.227 (3)C1—C61.401 (4)
F1—C31.365 (3)C1—C81.446 (3)
N3—N21.351 (3)C8—C71.503 (3)
N3—C91.366 (3)C7—O11.227 (3)
N3—H30.8600C6—C51.374 (3)
N1—C71.351 (3)C5—C41.388 (4)
N1—C61.407 (3)C5—H50.9300
N1—H10.8600C3—C41.365 (4)
N2—C81.289 (3)C3—C21.371 (4)
N4—C91.316 (3)C2—H20.9300
N4—H4A0.8600C4—H40.9300
N4—H4B0.8600
N2—N3—C9119.3 (2)C5—C6—C1121.9 (2)
N2—N3—H3120.3C5—C6—N1129.2 (3)
C9—N3—H3120.3C1—C6—N1108.9 (2)
C7—N1—C6111.7 (2)C6—C5—C4117.4 (3)
C7—N1—H1124.2C6—C5—H5121.3
C6—N1—H1124.2C4—C5—H5121.3
C8—N2—N3118.0 (2)F1—C3—C4118.3 (3)
C9—N4—H4A120.0F1—C3—C2117.9 (3)
C9—N4—H4B120.0C4—C3—C2123.8 (3)
H4A—N4—H4B120.0C3—C2—C1116.8 (3)
C2—C1—C6120.2 (2)C3—C2—H2121.6
C2—C1—C8132.8 (2)C1—C2—H2121.6
C6—C1—C8107.0 (2)N4—C9—N3115.6 (2)
N2—C8—C1125.3 (2)N4—C9—S1125.6 (2)
N2—C8—C7128.2 (2)N3—C9—S1118.83 (19)
C1—C8—C7106.4 (2)C3—C4—C5119.8 (3)
O1—C7—N1127.9 (2)C3—C4—H4120.1
O1—C7—C8126.1 (2)C5—C4—H4120.1
N1—C7—C8106.0 (2)
C9—N3—N2—C8179.0 (2)C2—C1—C6—N1179.9 (2)
N3—N2—C8—C1179.8 (2)C8—C1—C6—N10.5 (3)
N3—N2—C8—C73.6 (4)C7—N1—C6—C5179.5 (3)
C2—C1—C8—N21.7 (5)C7—N1—C6—C11.0 (3)
C6—C1—C8—N2178.8 (3)C1—C6—C5—C41.1 (4)
C2—C1—C8—C7178.9 (3)N1—C6—C5—C4179.5 (3)
C6—C1—C8—C71.5 (3)F1—C3—C2—C1179.4 (3)
C6—N1—C7—O1177.1 (3)C4—C3—C2—C10.6 (5)
C6—N1—C7—C81.9 (3)C6—C1—C2—C30.5 (4)
N2—C8—C7—O10.2 (5)C8—C1—C2—C3178.9 (3)
C1—C8—C7—O1176.9 (3)N2—N3—C9—N43.3 (4)
N2—C8—C7—N1179.2 (3)N2—N3—C9—S1176.57 (19)
C1—C8—C7—N12.1 (3)F1—C3—C4—C5179.8 (3)
C2—C1—C6—C51.4 (4)C2—C3—C4—C50.9 (5)
C8—C1—C6—C5178.2 (2)C6—C5—C4—C30.0 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3···O10.862.122.781 (3)133
N1—H1···S1i0.862.553.367 (2)158
N4—H4A···F1ii0.862.242.956 (3)140
N4—H4B···O1iii0.862.032.879 (3)171
Symmetry codes: (i) x+1/2, y+1/2, z+3/2; (ii) x+2, y, z+1; (iii) x+1/2, y1/2, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3···O10.862.122.781 (3)133.2
N1—H1···S1i0.862.553.367 (2)158.1
N4—H4A···F1ii0.862.242.956 (3)140.0
N4—H4B···O1iii0.862.032.879 (3)170.5
Symmetry codes: (i) x+1/2, y+1/2, z+3/2; (ii) x+2, y, z+1; (iii) x+1/2, y1/2, z+3/2.
 

Acknowledgements

We gratefully thank Professor Dr Manfredo Hörner (Federal University of Santa Maria, Brazil) for his help and support with the X-ray measurements.

References

First citationAli, A. Q., Eltayeb, N. E., Teoh, S. G., Salhin, A. & Fun, H.-K. (2012). Acta Cryst. E68, o285–o286.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationBrandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany.  Google Scholar
First citationBruker (2009). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationFreund, M. & Schander, A. (1902). Chem. Ber. 35, 2602–2606.  CrossRef CAS Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSteiner, T. (2002). Angew. Chem. Int. Ed. 41, 48–76.  Web of Science CrossRef CAS Google Scholar
First citationWestrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Volume 71| Part 6| June 2015| Pages o383-o384
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