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

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6-Bromo-4-[2-(4-fluoro­benzyl­­idene)hydrazin-1-yl­­idene]-1-methyl-3,4-di­hydro-1H-2λ6,1-benzo­thia­zine-2,2-dione

aDepartment of Chemistry, Government College University, Faisalabad 38040, Pakistan, bMaterials Chemistry Laboratory, Department of Chemistry, Government College University, Lahore 54000, Pakistan, and cDepartment of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland
*Correspondence e-mail: hafizshafique@hotmail.com

(Received 4 August 2012; accepted 30 August 2012; online 5 September 2012)

In the title compound, C16H13BrFN3O2S, the dihedral angle between the aromatic rings is 2.55 (19)° and the C=N—N=C torsion angle is 178.9 (3)°. The conformation of the thia­zine ring is an envelope, with the S atom displaced by −0.811 (3) Å from the mean plane of the other five atoms (r.m.s. deviation = 0.042 Å). In the crystal, C—H⋯O inter­actions link the mol­ecules and weak aromatic ππ stacking between the fluoro­benzene and bromo­benzene rings [centroid–centroid separation = 3.720 (2) Å and inter­planar angle = 2.6 (2)°] is also observed.

Related literature

For the synthesis and for the biological activity of related materials, see: Shafiq, Zia-Ur-Rehman et al. (2011[Shafiq, M., Zia-Ur-Rehman, M., Khan, I. U., Arshad, M. N. & Khan, S. A. (2011). J. Chil. Chem. Soc. 56, 527-531.]). For a related structure, see: Shafiq, Khan et al. (2011[Shafiq, M., Khan, I. U., Zia-ur-Rehman, M., Arshad, M. N. & Asiri, A. M. (2011). Acta Cryst. E67, o2092.])

[Scheme 1]

Experimental

Crystal data
  • C16H13BrFN3O2S

  • Mr = 410.26

  • Triclinic, [P \overline 1]

  • a = 7.8996 (4) Å

  • b = 9.0070 (4) Å

  • c = 13.5057 (7) Å

  • α = 104.176 (3)°

  • β = 90.977 (3)°

  • γ = 113.466 (3)°

  • V = 847.51 (7) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 2.57 mm−1

  • T = 296 K

  • 0.37 × 0.16 × 0.14 mm

Data collection
  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2007[Bruker (2007). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.450, Tmax = 0.715

  • 17622 measured reflections

  • 4186 independent reflections

  • 2331 reflections with I > 2σ(I)

  • Rint = 0.038

Refinement
  • R[F2 > 2σ(F2)] = 0.043

  • wR(F2) = 0.118

  • S = 0.99

  • 4186 reflections

  • 218 parameters

  • H-atom parameters constrained

  • Δρmax = 0.58 e Å−3

  • Δρmin = −0.78 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C8—H8B⋯O2i 0.97 2.56 3.397 (4) 145
C9—H9⋯O1ii 0.93 2.39 3.292 (4) 163
Symmetry codes: (i) -x+1, -y+1, -z; (ii) x, y+1, z.

Data collection: APEX2 (Bruker, 2007[Bruker (2007). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2007[Bruker (2007). 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: ORTEP-3 (Farrugia, 1997[Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.]); software used to prepare material for publication: SHELXL97.

Supporting information


Related literature top

For the synthesis and for the biological activity of related materials, see: Shafiq, Zia-Ur-Rehman et al. (2011). For a related structure, see: Shafiq, Khan et al. (2011)

Experimental top

For the synthesis, see: Shafiq, Zia-Ur-Rehman et al. (2011). Yellow needles were recrystallized from ethylacetate under slow evaporation.

Refinement top

The H atoms were placed in calculated positions (C—H = 0.93–0.97 Å) and refined as riding. The methyl group was allowed to rotate, but not to tip, to best fit the electron density. The constraint Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C) was applied.

Structure description top

For the synthesis and for the biological activity of related materials, see: Shafiq, Zia-Ur-Rehman et al. (2011). For a related structure, see: Shafiq, Khan et al. (2011)

Computing details top

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

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, showing displacement ellipsoids at the 50% probability level.
6-Bromo-4-[2-(4-fluorobenzylidene)hydrazin-1-ylidene]-1-methyl- 3,4-dihydro-1H-2λ6,1-benzothiazine-2,2-dione top
Crystal data top
C16H13BrFN3O2SZ = 2
Mr = 410.26F(000) = 412
Triclinic, P1Dx = 1.608 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.8996 (4) ÅCell parameters from 4416 reflections
b = 9.0070 (4) Åθ = 2.6–22.8°
c = 13.5057 (7) ŵ = 2.57 mm1
α = 104.176 (3)°T = 296 K
β = 90.977 (3)°Needle, yellow
γ = 113.466 (3)°0.37 × 0.16 × 0.14 mm
V = 847.51 (7) Å3
Data collection top
Bruker APEXII CCD
diffractometer
4186 independent reflections
Radiation source: fine-focus sealed tube2331 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
ω scansθmax = 28.3°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
h = 1010
Tmin = 0.450, Tmax = 0.715k = 1212
17622 measured reflectionsl = 1717
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)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118H-atom parameters constrained
S = 0.99 w = 1/[σ2(Fo2) + (0.0479P)2 + 0.5245P]
where P = (Fo2 + 2Fc2)/3
4186 reflections(Δ/σ)max = 0.001
218 parametersΔρmax = 0.58 e Å3
0 restraintsΔρmin = 0.78 e Å3
Crystal data top
C16H13BrFN3O2Sγ = 113.466 (3)°
Mr = 410.26V = 847.51 (7) Å3
Triclinic, P1Z = 2
a = 7.8996 (4) ÅMo Kα radiation
b = 9.0070 (4) ŵ = 2.57 mm1
c = 13.5057 (7) ÅT = 296 K
α = 104.176 (3)°0.37 × 0.16 × 0.14 mm
β = 90.977 (3)°
Data collection top
Bruker APEXII CCD
diffractometer
4186 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2007)
2331 reflections with I > 2σ(I)
Tmin = 0.450, Tmax = 0.715Rint = 0.038
17622 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.118H-atom parameters constrained
S = 0.99Δρmax = 0.58 e Å3
4186 reflectionsΔρmin = 0.78 e Å3
218 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
C10.9739 (4)0.8291 (4)0.2392 (2)0.0408 (7)
C21.0591 (5)0.8914 (4)0.3410 (2)0.0515 (8)
H21.08040.81940.37340.062*
C31.1121 (5)1.0568 (4)0.3941 (2)0.0535 (9)
H31.17201.09730.46120.064*
C41.0757 (5)1.1622 (4)0.3472 (2)0.0512 (8)
C50.9894 (4)1.1042 (4)0.2476 (2)0.0432 (7)
H50.96541.17710.21720.052*
C60.9377 (4)0.9379 (3)0.1919 (2)0.0354 (6)
C70.8470 (4)0.8820 (3)0.0850 (2)0.0345 (6)
C80.8201 (5)0.7111 (3)0.0194 (2)0.0458 (8)
H8A0.93510.71730.00750.055*
H8B0.72480.67430.03840.055*
C90.6595 (4)1.0158 (4)0.0800 (2)0.0379 (7)
H90.68181.11940.03440.045*
C100.5657 (4)0.9726 (4)0.1840 (2)0.0409 (7)
C110.5109 (5)0.8138 (4)0.2507 (2)0.0552 (9)
H110.53090.73070.22960.066*
C120.4260 (5)0.7788 (6)0.3493 (3)0.0735 (12)
H120.38770.67220.39480.088*
C130.3996 (5)0.9026 (7)0.3781 (3)0.0741 (13)
C140.4504 (5)1.0597 (6)0.3152 (3)0.0725 (12)
H140.43001.14160.33770.087*
C150.5335 (5)1.0944 (5)0.2165 (3)0.0564 (9)
H150.56821.20090.17130.068*
C160.9850 (6)0.5539 (5)0.2319 (3)0.0817 (13)
H16A1.11670.60670.25350.122*
H16B0.95310.44690.18270.122*
H16C0.92020.53780.29060.122*
S10.75433 (14)0.56638 (10)0.09239 (7)0.0548 (3)
N10.9317 (4)0.6609 (3)0.1849 (2)0.0542 (7)
N20.7961 (3)0.9817 (3)0.05209 (17)0.0383 (6)
N30.7109 (3)0.9153 (3)0.05055 (17)0.0407 (6)
O10.7609 (4)0.4128 (3)0.0372 (2)0.0824 (9)
O20.5862 (3)0.5604 (3)0.1320 (2)0.0672 (7)
F10.3170 (4)0.8672 (4)0.47568 (18)0.1185 (11)
Br11.14956 (8)1.39006 (5)0.42019 (3)0.0926 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0408 (18)0.0441 (16)0.0416 (17)0.0197 (15)0.0030 (14)0.0151 (13)
C20.054 (2)0.064 (2)0.0436 (18)0.0272 (18)0.0006 (15)0.0233 (16)
C30.057 (2)0.069 (2)0.0319 (17)0.0243 (18)0.0045 (15)0.0115 (15)
C40.060 (2)0.0507 (18)0.0361 (17)0.0231 (17)0.0059 (15)0.0009 (14)
C50.0503 (19)0.0433 (16)0.0337 (15)0.0197 (15)0.0039 (14)0.0066 (13)
C60.0375 (17)0.0377 (14)0.0306 (14)0.0149 (13)0.0023 (12)0.0099 (12)
C70.0352 (16)0.0314 (13)0.0329 (15)0.0100 (13)0.0015 (12)0.0086 (11)
C80.056 (2)0.0360 (15)0.0395 (17)0.0171 (15)0.0020 (15)0.0041 (13)
C90.0393 (17)0.0373 (15)0.0335 (15)0.0142 (13)0.0010 (13)0.0068 (12)
C100.0352 (17)0.0536 (18)0.0359 (16)0.0182 (15)0.0000 (13)0.0164 (13)
C110.056 (2)0.057 (2)0.0431 (19)0.0166 (18)0.0090 (16)0.0091 (15)
C120.064 (3)0.089 (3)0.041 (2)0.015 (2)0.0131 (18)0.004 (2)
C130.050 (2)0.129 (4)0.043 (2)0.031 (3)0.0069 (17)0.034 (2)
C140.065 (3)0.116 (4)0.065 (3)0.050 (3)0.009 (2)0.052 (3)
C150.054 (2)0.075 (2)0.052 (2)0.0337 (19)0.0086 (17)0.0260 (18)
C160.102 (3)0.059 (2)0.096 (3)0.042 (2)0.015 (3)0.030 (2)
S10.0655 (6)0.0316 (4)0.0608 (5)0.0150 (4)0.0081 (4)0.0115 (4)
N10.0662 (19)0.0447 (15)0.0571 (17)0.0273 (14)0.0093 (14)0.0170 (13)
N20.0437 (15)0.0375 (12)0.0291 (12)0.0151 (12)0.0052 (10)0.0048 (10)
N30.0495 (15)0.0401 (13)0.0294 (12)0.0173 (12)0.0045 (11)0.0070 (10)
O10.113 (2)0.0376 (13)0.090 (2)0.0338 (14)0.0166 (17)0.0037 (12)
O20.0524 (16)0.0561 (15)0.0801 (18)0.0050 (12)0.0048 (13)0.0266 (13)
F10.0919 (18)0.199 (3)0.0528 (14)0.043 (2)0.0233 (13)0.0460 (18)
Br10.1381 (5)0.0639 (3)0.0568 (3)0.0455 (3)0.0405 (3)0.01902 (18)
Geometric parameters (Å, º) top
C1—C21.395 (4)C10—C111.381 (4)
C1—C61.405 (4)C10—C151.385 (4)
C1—N11.411 (4)C11—C121.384 (5)
C2—C31.370 (5)C11—H110.9300
C2—H20.9300C12—C131.355 (6)
C3—C41.375 (5)C12—H120.9300
C3—H30.9300C13—C141.354 (6)
C4—C51.373 (4)C13—F11.365 (4)
C4—Br11.887 (3)C14—C151.382 (5)
C5—C61.388 (4)C14—H140.9300
C5—H50.9300C15—H150.9300
C6—C71.475 (4)C16—N11.457 (4)
C7—N21.281 (3)C16—H16A0.9600
C7—C81.505 (4)C16—H16B0.9600
C8—S11.746 (3)C16—H16C0.9600
C8—H8A0.9700S1—O11.423 (3)
C8—H8B0.9700S1—O21.426 (3)
C9—N31.268 (3)S1—N11.649 (3)
C9—C101.463 (4)N2—N31.405 (3)
C9—H90.9300
C2—C1—C6118.9 (3)C10—C11—C12119.8 (3)
C2—C1—N1119.7 (3)C10—C11—H11120.1
C6—C1—N1121.3 (3)C12—C11—H11120.1
C3—C2—C1121.3 (3)C13—C12—C11118.8 (4)
C3—C2—H2119.4C13—C12—H12120.6
C1—C2—H2119.4C11—C12—H12120.6
C2—C3—C4119.4 (3)C14—C13—C12123.5 (3)
C2—C3—H3120.3C14—C13—F1118.2 (4)
C4—C3—H3120.3C12—C13—F1118.4 (4)
C5—C4—C3120.8 (3)C13—C14—C15117.8 (4)
C5—C4—Br1119.9 (2)C13—C14—H14121.1
C3—C4—Br1119.3 (2)C15—C14—H14121.1
C4—C5—C6120.7 (3)C14—C15—C10120.8 (4)
C4—C5—H5119.7C14—C15—H15119.6
C6—C5—H5119.7C10—C15—H15119.6
C5—C6—C1118.9 (3)N1—C16—H16A109.5
C5—C6—C7118.7 (2)N1—C16—H16B109.5
C1—C6—C7122.4 (2)H16A—C16—H16B109.5
N2—C7—C6118.5 (2)N1—C16—H16C109.5
N2—C7—C8123.1 (2)H16A—C16—H16C109.5
C6—C7—C8118.4 (2)H16B—C16—H16C109.5
C7—C8—S1110.0 (2)O1—S1—O2118.54 (17)
C7—C8—H8A109.7O1—S1—N1107.04 (16)
S1—C8—H8A109.7O2—S1—N1110.83 (16)
C7—C8—H8B109.7O1—S1—C8110.49 (17)
S1—C8—H8B109.7O2—S1—C8108.71 (16)
H8A—C8—H8B108.2N1—S1—C899.57 (14)
N3—C9—C10121.5 (3)C1—N1—C16120.7 (3)
N3—C9—H9119.2C1—N1—S1117.5 (2)
C10—C9—H9119.2C16—N1—S1117.2 (2)
C11—C10—C15119.4 (3)C7—N2—N3113.6 (2)
C11—C10—C9121.5 (3)C9—N3—N2111.9 (2)
C15—C10—C9119.1 (3)
C6—C1—C2—C31.7 (5)C11—C12—C13—C140.7 (6)
N1—C1—C2—C3176.1 (3)C11—C12—C13—F1179.5 (3)
C1—C2—C3—C41.9 (5)C12—C13—C14—C150.0 (6)
C2—C3—C4—C50.9 (5)F1—C13—C14—C15179.8 (3)
C2—C3—C4—Br1179.8 (3)C13—C14—C15—C100.9 (6)
C3—C4—C5—C60.3 (5)C11—C10—C15—C141.2 (5)
Br1—C4—C5—C6178.6 (2)C9—C10—C15—C14178.1 (3)
C4—C5—C6—C10.4 (5)C7—C8—S1—O1169.6 (2)
C4—C5—C6—C7179.4 (3)C7—C8—S1—O258.7 (3)
C2—C1—C6—C50.6 (4)C7—C8—S1—N157.2 (2)
N1—C1—C6—C5177.2 (3)C2—C1—N1—C163.3 (5)
C2—C1—C6—C7179.6 (3)C6—C1—N1—C16174.5 (3)
N1—C1—C6—C72.6 (5)C2—C1—N1—S1152.0 (3)
C5—C6—C7—N29.5 (4)C6—C1—N1—S130.2 (4)
C1—C6—C7—N2170.6 (3)O1—S1—N1—C1169.3 (3)
C5—C6—C7—C8170.0 (3)O2—S1—N1—C160.1 (3)
C1—C6—C7—C89.8 (4)C8—S1—N1—C154.3 (3)
N2—C7—C8—S1140.5 (3)O1—S1—N1—C1634.5 (3)
C6—C7—C8—S140.0 (3)O2—S1—N1—C1696.1 (3)
N3—C9—C10—C117.3 (5)C8—S1—N1—C16149.5 (3)
N3—C9—C10—C15171.9 (3)C6—C7—N2—N3179.8 (2)
C15—C10—C11—C120.5 (5)C8—C7—N2—N30.7 (4)
C9—C10—C11—C12178.7 (3)C10—C9—N3—N2179.4 (3)
C10—C11—C12—C130.4 (6)C7—N2—N3—C9178.9 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8B···O2i0.972.563.397 (4)145
C9—H9···O1ii0.932.393.292 (4)163
Symmetry codes: (i) x+1, y+1, z; (ii) x, y+1, z.

Experimental details

Crystal data
Chemical formulaC16H13BrFN3O2S
Mr410.26
Crystal system, space groupTriclinic, P1
Temperature (K)296
a, b, c (Å)7.8996 (4), 9.0070 (4), 13.5057 (7)
α, β, γ (°)104.176 (3), 90.977 (3), 113.466 (3)
V3)847.51 (7)
Z2
Radiation typeMo Kα
µ (mm1)2.57
Crystal size (mm)0.37 × 0.16 × 0.14
Data collection
DiffractometerBruker APEXII CCD
Absorption correctionMulti-scan
(SADABS; Bruker, 2007)
Tmin, Tmax0.450, 0.715
No. of measured, independent and
observed [I > 2σ(I)] reflections
17622, 4186, 2331
Rint0.038
(sin θ/λ)max1)0.668
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.118, 0.99
No. of reflections4186
No. of parameters218
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.58, 0.78

Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8B···O2i0.972.563.397 (4)145
C9—H9···O1ii0.932.393.292 (4)163
Symmetry codes: (i) x+1, y+1, z; (ii) x, y+1, z.
 

Acknowledgements

MS acknowledges the Higher Education Commission of Pakistan for financial support, GC University Lahore, Pakistan, for laboratory facilities during his PhD studies and Dr Michael Harmata for guidance during his stay at the Department of Chemistry, University of Missouri, USA.

References

First citationBruker (2007). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationFarrugia, L. J. (1997). J. Appl. Cryst. 30, 565.  CrossRef IUCr Journals Google Scholar
First citationShafiq, M., Khan, I. U., Zia-ur-Rehman, M., Arshad, M. N. & Asiri, A. M. (2011). Acta Cryst. E67, o2092.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationShafiq, M., Zia-Ur-Rehman, M., Khan, I. U., Arshad, M. N. & Khan, S. A. (2011). J. Chil. Chem. Soc. 56, 527–531.  CSD CrossRef CAS 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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