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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jul 23;67(Pt 8):o2078. doi: 10.1107/S1600536811027930

6-Bromo-4-hydrazinyl­idene-1-methyl-3H-2λ6,1-benzothia­zine-2,2-dione

Muhammad Shafiq a, Islam Ullah Khan a, Muhammad Zia-ur-Rehman b, Muhammad Nadeem Arshad c,a,*, Abdullah M Asiri d
PMCID: PMC3213521  PMID: 22091100

Abstract

In the title mol­ecule, C9H10BrN3O2S, the thia­zine ring has an envelope conformation with the S atom at the flap. The geometry around the S atom is distorted tetra­hedral. In the crystal, inversion dimers linked by pairs of N—H⋯N hydrogen bonds occur, generating R 2 2(6) ring motifs. N—H⋯O hydrogen bonds and C—H⋯O inter­actions connect the dimers, forming a three-dimentional network structure.

Related literature

For the related structures of 6-bromo-1-methyl-1H-2,1-benzo­thia­zin-4(3H)-one 2,2-dioxide and 6-bromo-1-ethyl-1H-2,1-benzo­thia­zin-4(3H)-one 2,2-dioxide, see: Shafiq et al. (2009a ,b ), respectively. For the structures of other benzothia­zine derivatives, see: Shafiq et al. (2011); Arshad et al. (2011). For graph-set notation, see: Bernstein et al. (1995). For puckering parameters, see: Cremer & Pople (1975).graphic file with name e-67-o2078-scheme1.jpg

Experimental

Crystal data

  • C9H10BrN3O2S

  • M r = 304.17

  • Monoclinic, Inline graphic

  • a = 10.1483 (5) Å

  • b = 9.6375 (4) Å

  • c = 11.2118 (5) Å

  • β = 92.278 (2)°

  • V = 1095.69 (9) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 3.93 mm−1

  • T = 296 K

  • 0.21 × 0.09 × 0.07 mm

Data collection

  • Bruker Kappa APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2001) T min = 0.492, T max = 0.771

  • 12176 measured reflections

  • 2719 independent reflections

  • 1972 reflections with I > 2σ(I)

  • R int = 0.037

Refinement

  • R[F 2 > 2σ(F 2)] = 0.032

  • wR(F 2) = 0.079

  • S = 1.01

  • 2719 reflections

  • 152 parameters

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

  • Δρmax = 0.40 e Å−3

  • Δρmin = −0.35 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: WinGX (Farrugia, 1999) and PLATON.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811027930/su2288sup1.cif

e-67-o2078-sup1.cif (16.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811027930/su2288Isup2.hkl

e-67-o2078-Isup2.hkl (130.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811027930/su2288Isup3.cml

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
N3—H32⋯N2i 0.85 (4) 2.47 (4) 3.198 (4) 144 (3)
N3—H31⋯O1ii 0.90 (4) 2.38 (4) 3.252 (4) 162 (3)
C3—H3⋯O1iii 0.93 2.45 3.323 (3) 156

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

Acknowledgments

The authors acknowledge the Higher Education Commission of Pakistan for providing a grant for the project to strengthen the Materials Chemistry Laboratory at GC University, Lahore, Pakistan.

supplementary crystallographic information

Comment

Continuing our research on the synthesis (Shafiq et al., 2011; Arshad et al., 2011) and crystal structure studies of benzothiazine derivatives (Shafiq et al., 2009a), we present herein the crystal structure of the title compound, (I).

The molecular structure of the title molecule, (I), is illustrated in Fig. 1. The structure differs to a similar published compound, 6-Bromo-1-methyl-1H-2,1-benzothiazin-4(3H)-one 2,2-dioxide (II) [Shafiq et al., 2009a], in that the carbonyl group in (II) has been replaced with a hydrazide moiety in (I). The bond lengths and angles in the title compound are similar to those of (II) and in 6-Bromo-1-ethyl-1H-2,1-benzothiazin-4(3H)-one 2,2-dioxide (III) (Shafiq et al., 2009b). In (I) atom Br1, attached to the planar aromatic ring (C1—C6), lies out of the plane by 0.0547 (3) Å, while in (II) and (III) the deviations are slightly greater, i.e. 0.064 (4) and 0.073 (4) Å, respectively. The thiazine ring, (C1/C6/C7/C8/S1/N1), has an envelope conformation with atom S1 as the flap [puckering parameters: Q (puckering amplitude) = 0.5873 (18) Å, θ = 124.31 (19) °, and φ = 185.9 (3) ° (Cromer & Pople, 1975)].

In the crystal structure of compound (I) the functional hydrazide group is involved in the formation of inversion dimers, through N3—H32···N2 hydrogen bonding, and generates a six-membered R22(6) ring motif (Bernstein et al., 1995). These dimers are further connected through N—H···O hydrogen bonds and weak C—H···O interactions to form a three dimensional network structure (Table 1, Fig. 2).

Experimental

A mixture of 1-methyl-2,2-dioxo-2,3-dihydro-1H-2λ6-benzo [c][1,2]thiazin-4-one (10.60 g; 50.0 mmoles), hydrazine hydrate (85%) (5.0 ml) and ethanol (200 ml) was reacted at 318 K using an ultrasound reaction bath for about 35 mins. After completion of the reaction, excess hydrazine and solvent were removed under vacuum. The crude product obtained was washed with water and dried; Yield: 74%. Suitable crystals were produced through recrystalization in methanol under slow evaporation.

Refinement

The NH H-atom was located in a difference Fourier map and refined with Uiso(H)=1.2Ueq(N). The C-bound H-atoms were included in calculated positions and treated as riding atoms: C-H = 0.93, 0.96, and 0.97 Å for CH(aromatic), CH3 and CH2 H-atoms, respectively, with Uiso(H) = k × Ueq(parent C-atom), where k = 1.5 for CH3 H-atoms and k = 1.2 for all other H-atoms.

Figures

Fig. 1.

Fig. 1.

A view of the molecular structure of the title molecule, (I), showing the labelling scheme and 50% displacement ellipsoids.

Fig. 2.

Fig. 2.

A perspective view of the crystal packing of compound (I), showing the inversion dimers formed through N—H···N hydrogen bonds (dashed lines; see Table 1 for details).

Crystal data

C9H10BrN3O2S F(000) = 608
Mr = 304.17 Dx = 1.844 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 3531 reflections
a = 10.1483 (5) Å θ = 2.7–24.7°
b = 9.6375 (4) Å µ = 3.93 mm1
c = 11.2118 (5) Å T = 296 K
β = 92.278 (2)° Needle, yellow
V = 1095.69 (9) Å3 0.21 × 0.09 × 0.07 mm
Z = 4

Data collection

Bruker Kappa APEXII CCD diffractometer 2719 independent reflections
Radiation source: fine-focus sealed tube 1972 reflections with I > 2σ(I)
graphite Rint = 0.037
φ and ω scans θmax = 28.3°, θmin = 2.7°
Absorption correction: multi-scan (SADABS; Bruker, 2001) h = −13→13
Tmin = 0.492, Tmax = 0.771 k = −12→7
12176 measured reflections l = −14→14

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.032 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.079 H atoms treated by a mixture of independent and constrained refinement
S = 1.01 w = 1/[σ2(Fo2) + (0.0403P)2 + 0.1092P] where P = (Fo2 + 2Fc2)/3
2719 reflections (Δ/σ)max = 0.001
152 parameters Δρmax = 0.40 e Å3
0 restraints Δρmin = −0.35 e Å3

Special details

Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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
Br1 0.94817 (3) 0.62148 (3) 1.15166 (3) 0.04753 (12)
S1 0.86913 (6) 1.05109 (6) 0.65175 (5) 0.03060 (16)
O1 0.81377 (18) 0.92236 (19) 0.60884 (16) 0.0413 (4)
O2 0.90132 (19) 1.15392 (19) 0.56664 (16) 0.0433 (5)
N1 1.00013 (19) 1.0224 (2) 0.73776 (18) 0.0321 (5)
N2 0.6567 (2) 1.0222 (2) 0.9307 (2) 0.0400 (5)
N3 0.5556 (3) 1.1148 (3) 0.9019 (3) 0.0551 (7)
H32 0.507 (4) 1.115 (3) 0.962 (3) 0.066*
H31 0.586 (3) 1.199 (4) 0.881 (3) 0.066*
C1 0.9838 (2) 0.9263 (2) 0.8314 (2) 0.0290 (5)
C2 1.0852 (3) 0.8338 (3) 0.8633 (2) 0.0363 (6)
H2 1.1616 0.8335 0.8202 0.044*
C3 1.0743 (3) 0.7436 (3) 0.9567 (2) 0.0377 (6)
H3 1.1427 0.6829 0.9774 0.045*
C4 0.9602 (3) 0.7443 (2) 1.0195 (2) 0.0341 (6)
C5 0.8576 (2) 0.8322 (2) 0.9895 (2) 0.0319 (6)
H5 0.7813 0.8299 1.0328 0.038*
C6 0.8669 (2) 0.9253 (2) 0.8943 (2) 0.0274 (5)
C7 0.7567 (2) 1.0212 (2) 0.8646 (2) 0.0290 (5)
C8 0.7637 (3) 1.1175 (2) 0.7582 (2) 0.0343 (6)
H8A 0.7954 1.2077 0.7848 0.041*
H8B 0.6761 1.1295 0.7219 0.041*
C9 1.1299 (3) 1.0488 (3) 0.6900 (3) 0.0457 (7)
H9A 1.1927 1.0658 0.7546 0.069*
H9B 1.1250 1.1284 0.6385 0.069*
H9C 1.1571 0.9694 0.6454 0.069*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.04682 (19) 0.04001 (17) 0.0552 (2) −0.00435 (13) −0.00552 (14) 0.01513 (13)
S1 0.0277 (3) 0.0349 (3) 0.0292 (3) 0.0003 (3) 0.0004 (3) 0.0005 (2)
O1 0.0432 (11) 0.0436 (10) 0.0366 (10) −0.0068 (9) −0.0041 (8) −0.0078 (8)
O2 0.0411 (11) 0.0484 (11) 0.0406 (11) 0.0029 (9) 0.0046 (9) 0.0129 (8)
N1 0.0234 (11) 0.0400 (11) 0.0330 (12) −0.0015 (9) 0.0008 (9) 0.0032 (9)
N2 0.0375 (13) 0.0384 (12) 0.0447 (14) 0.0089 (10) 0.0113 (11) 0.0073 (10)
N3 0.0439 (16) 0.0518 (16) 0.071 (2) 0.0180 (13) 0.0243 (14) 0.0177 (14)
C1 0.0265 (13) 0.0311 (12) 0.0290 (13) −0.0005 (10) −0.0034 (10) −0.0058 (10)
C2 0.0283 (14) 0.0411 (14) 0.0394 (16) 0.0041 (11) 0.0000 (12) −0.0047 (11)
C3 0.0337 (15) 0.0352 (13) 0.0436 (16) 0.0073 (11) −0.0062 (12) −0.0033 (11)
C4 0.0395 (15) 0.0257 (11) 0.0362 (14) −0.0052 (10) −0.0086 (12) −0.0002 (10)
C5 0.0300 (14) 0.0319 (12) 0.0335 (14) −0.0037 (10) −0.0015 (11) −0.0033 (10)
C6 0.0283 (13) 0.0259 (11) 0.0279 (13) −0.0023 (10) −0.0021 (10) −0.0050 (9)
C7 0.0276 (13) 0.0293 (12) 0.0302 (13) −0.0001 (10) 0.0022 (10) −0.0035 (10)
C8 0.0322 (14) 0.0348 (13) 0.0360 (14) 0.0045 (11) 0.0028 (11) 0.0017 (11)
C9 0.0265 (14) 0.0676 (19) 0.0432 (16) −0.0013 (13) 0.0049 (12) 0.0035 (14)

Geometric parameters (Å, °)

Br1—C4 1.904 (2) C2—H2 0.9300
S1—O2 1.4228 (19) C3—C4 1.380 (4)
S1—O1 1.4369 (19) C3—H3 0.9300
S1—N1 1.635 (2) C4—C5 1.374 (3)
S1—C8 1.755 (3) C5—C6 1.400 (3)
N1—C1 1.415 (3) C5—H5 0.9300
N1—C9 1.464 (3) C6—C7 1.479 (3)
N2—C7 1.280 (3) C7—C8 1.515 (3)
N2—N3 1.388 (3) C8—H8A 0.9700
N3—H32 0.85 (4) C8—H8B 0.9700
N3—H31 0.90 (4) C9—H9A 0.9600
C1—C2 1.397 (4) C9—H9B 0.9600
C1—C6 1.404 (3) C9—H9C 0.9600
C2—C3 1.369 (4)
O2—S1—O1 118.29 (11) C5—C4—Br1 120.2 (2)
O2—S1—N1 108.09 (11) C3—C4—Br1 118.40 (19)
O1—S1—N1 110.45 (11) C4—C5—C6 120.6 (2)
O2—S1—C8 111.38 (11) C4—C5—H5 119.7
O1—S1—C8 107.55 (12) C6—C5—H5 119.7
N1—S1—C8 99.44 (11) C5—C6—C1 118.1 (2)
C1—N1—C9 121.3 (2) C5—C6—C7 120.0 (2)
C1—N1—S1 115.59 (16) C1—C6—C7 121.9 (2)
C9—N1—S1 118.49 (17) N2—C7—C6 118.9 (2)
C7—N2—N3 117.8 (2) N2—C7—C8 120.9 (2)
N2—N3—H32 105 (2) C6—C7—C8 120.1 (2)
N2—N3—H31 112 (2) C7—C8—S1 111.17 (16)
H32—N3—H31 115 (3) C7—C8—H8A 109.4
C2—C1—C6 119.7 (2) S1—C8—H8A 109.4
C2—C1—N1 120.0 (2) C7—C8—H8B 109.4
C6—C1—N1 120.2 (2) S1—C8—H8B 109.4
C3—C2—C1 121.4 (2) H8A—C8—H8B 108.0
C3—C2—H2 119.3 N1—C9—H9A 109.5
C1—C2—H2 119.3 N1—C9—H9B 109.5
C2—C3—C4 118.8 (2) H9A—C9—H9B 109.5
C2—C3—H3 120.6 N1—C9—H9C 109.5
C4—C3—H3 120.6 H9A—C9—H9C 109.5
C5—C4—C3 121.4 (2) H9B—C9—H9C 109.5
O2—S1—N1—C1 177.43 (17) C4—C5—C6—C1 −0.3 (3)
O1—S1—N1—C1 −51.7 (2) C4—C5—C6—C7 −178.8 (2)
C8—S1—N1—C1 61.13 (19) C2—C1—C6—C5 1.4 (3)
O2—S1—N1—C9 −26.3 (2) N1—C1—C6—C5 −177.3 (2)
O1—S1—N1—C9 104.5 (2) C2—C1—C6—C7 179.8 (2)
C8—S1—N1—C9 −142.6 (2) N1—C1—C6—C7 1.1 (3)
C9—N1—C1—C2 −13.4 (3) N3—N2—C7—C6 179.0 (2)
S1—N1—C1—C2 142.1 (2) N3—N2—C7—C8 −0.3 (4)
C9—N1—C1—C6 165.3 (2) C5—C6—C7—N2 3.4 (3)
S1—N1—C1—C6 −39.2 (3) C1—C6—C7—N2 −174.9 (2)
C6—C1—C2—C3 −1.4 (4) C5—C6—C7—C8 −177.2 (2)
N1—C1—C2—C3 177.3 (2) C1—C6—C7—C8 4.4 (3)
C1—C2—C3—C4 0.4 (4) N2—C7—C8—S1 −155.8 (2)
C2—C3—C4—C5 0.6 (4) C6—C7—C8—S1 24.9 (3)
C2—C3—C4—Br1 −178.47 (19) O2—S1—C8—C7 −165.88 (17)
C3—C4—C5—C6 −0.7 (4) O1—S1—C8—C7 63.0 (2)
Br1—C4—C5—C6 178.42 (17) N1—S1—C8—C7 −52.11 (19)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N3—H32···N2i 0.85 (4) 2.47 (4) 3.198 (4) 144 (3)
N3—H31···O1ii 0.90 (4) 2.38 (4) 3.252 (4) 162 (3)
C3—H3···O1iii 0.93 2.45 3.323 (3) 156.

Symmetry codes: (i) −x+1, −y+2, −z+2; (ii) −x+3/2, y+1/2, −z+3/2; (iii) x+1/2, −y+3/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2288).

References

  1. Arshad, M. N., Khan, I. U., Zia-ur-Rehman, M. & Shafiq, M. (2011). Asian J. Chem. 23, 2801–2805.
  2. Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555–1573.
  3. Bruker (2001). SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  5. Cremer, D. & Pople, J. A. (1975). J. Am. Chem. Soc. 97, 1354–1358.
  6. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  7. Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
  8. Shafiq, M., Khan, I. U., Arshad, M. N. & Siddiqui, W. A. (2011). Asian J. Chem. 23, 2101–2105.
  9. Shafiq, M., Tahir, M. N., Khan, I. U., Arshad, M. N. & Asghar, M. N. (2009a). Acta Cryst. E65, o1182. [DOI] [PMC free article] [PubMed]
  10. Shafiq, M., Tahir, M. N., Khan, I. U., Arshad, M. N. & Safdar, M. (2009b). Acta Cryst. E65, o393. [DOI] [PMC free article] [PubMed]
  11. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  12. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [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/S1600536811027930/su2288sup1.cif

e-67-o2078-sup1.cif (16.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811027930/su2288Isup2.hkl

e-67-o2078-Isup2.hkl (130.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811027930/su2288Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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