supplementary materials


zq2060 scheme

Acta Cryst. (2010). E66, o2707    [ doi:10.1107/S1600536810038274 ]

3-(6-Fluoro-4-oxo-4H-chromen-3-yl)-3,4-dihydro-2H-1,2,4-benzothiadiazine-1,1-dione

M. al-Rashida, S. A. Nagra, I. U. Khan, G. Kostakis and G. Abbas

Abstract top

In the title compound, C16H11FN2O4S, the mean planes of the bicyclic chromone system and of the benzene ring of the benzothiadiazine derivative make a dihedral angle of 54.28 (5)°. An intramolecular N-H...O hydrogen bond occurs. In the crystal, molecules are linked into layers by N-H...O and C-H...O hydrogen bonds, generating an infinite two-dimensional network.

Comment top

The 1,2,4-benzothiadiazine-1,1-dioxide ring system has attained considerable importance in pharmaceutical and medicinal chemistry mainly due to the compounds such as chlorothiazide and diazoxide (Zhu et al., 2005; Kamal et al., 2007a). The sulfonamide group is an active pharmacophore which is responsible for many biological activities (Weisman & Brown, 1964). The crystal structure of the condensation product of 4-aminobenzenesulfonamide with 4-oxo-4H-1-benzopyran-3-carboxaldehyde has previously been reported (al-Rashida et al., 2009). Herein, we report the crystal structure of the condensation product of 2-aminobenzenesulfonamide with 6-fluoro-4-oxo-4H-1-benzopyran-3-carboxaldehyde.

In the molecule of the title compound (Fig. 1), the two rings of the chromone system (F1, O1, O4, C2—C10) are coplanar, making a dihedral angle of 0.55 (19)°. The carbon atom C11 deviates only by 0.034 (5) Å from the mean plane of the chromone. The phenyl ring (C12—C17) and the atoms N4, S1 and C11 are coplanar as well (rms deviation = 0.033) and make a dihedral angle of 54.28 (5)° with the mean plane of the chromone system.

The crystal structure is stabilized by intra- and intermolecular N—H···O and C—H···O hydrogen bonds which link the molecules into an infinite two-dimensional network (Fig. 2).

Related literature top

For background to the importance of the 1,2,4-benzothiadiazine-1,1-dioxide ring system in pharmaceutical and medicinal chemistry, see: Zhu et al. (2005); Kamal et al. (2007a). For a survey on the antimicrobial activity of benzothiadiazine derivatives, see: Di Bella et al. (1983); Kamal et al. (2007a,b). The sulfonamide group is an active pharmacophore which is responsible for many biological activities, see: Weisman & Brown (1964). For a related structure, see: Mariya-al-Rashida et al. (2009);

Experimental top

A solution of 2-aminobenzenesulfonamide (1.0 mmol) in 10 ml ethanol was slowly added to the stirred solution of 6-fluoro-4-oxo-4H-1-benzopyran-3-carboxaldehyde (1.0 mmol) containing a catalytic amount of p-toluene sulfonic acid (p-TsOH) and refluxed for 3 hrs. The resulting product was isolated by filtration, washed with ethanol, dried and recrystallized from hot ethanol and acetone (1:1) (yield 81%, m.p. 472 K).

Refinement top

The H atoms attached to N were located in a difference Fourier map and their coordinates were refined, with Uiso(H) = 1.2Ueq(N). The remaining H atoms were positioned geometrically with C-H = 0.93 and 0.98 Å for aromatic and methine H atoms, respectively, and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C).

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 for Windows (Farrugia, 1997) and Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title molecule, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. A packing diagram of the title compound showing hydrogen bonds as dashed lines.
3-(6-Fluoro-4-oxo-4H-chromen-3-yl)-3,4-dihydro-2H-1,2,4- benzothiadiazine-1,1-dione top
Crystal data top
C16H11FN2O4SF(000) = 712
Mr = 346.34Dx = 1.567 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 1626 reflections
a = 7.0739 (3) Åθ = 3.3–22.0°
b = 8.2861 (4) ŵ = 0.26 mm1
c = 25.0456 (12) ÅT = 296 K
V = 1468.05 (12) Å3Needle, orange
Z = 40.31 × 0.06 × 0.05 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1993 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.056
graphiteθmax = 28.3°, θmin = 3.0°
phi and ω scansh = 99
9538 measured reflectionsk = 1010
3453 independent reflectionsl = 3324
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.052H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.093 w = 1/[σ2(Fo2) + (0.0318P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.97(Δ/σ)max < 0.001
3453 reflectionsΔρmax = 0.23 e Å3
223 parametersΔρmin = 0.28 e Å3
3 restraintsAbsolute structure: Flack (1983), 1345 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.01 (9)
Crystal data top
C16H11FN2O4SV = 1468.05 (12) Å3
Mr = 346.34Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 7.0739 (3) ŵ = 0.26 mm1
b = 8.2861 (4) ÅT = 296 K
c = 25.0456 (12) Å0.31 × 0.06 × 0.05 mm
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1993 reflections with I > 2σ(I)
9538 measured reflectionsRint = 0.056
3453 independent reflectionsθmax = 28.3°
Refinement top
R[F2 > 2σ(F2)] = 0.052H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.093Δρmax = 0.23 e Å3
S = 0.97Δρmin = 0.28 e Å3
3453 reflectionsAbsolute structure: Flack (1983), 1345 Friedel pairs
223 parametersFlack parameter: 0.01 (9)
3 restraints
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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
S10.05991 (10)0.79823 (11)0.18441 (3)0.0371 (2)
O20.0424 (3)0.9692 (3)0.18575 (10)0.0520 (6)
O30.1066 (2)0.7017 (3)0.18043 (9)0.0481 (6)
N40.4758 (3)0.7352 (4)0.19622 (11)0.0431 (8)
H4A0.593 (4)0.736 (4)0.2026 (12)0.052*
N20.1714 (3)0.7397 (3)0.23806 (11)0.0315 (7)
H2A0.167 (4)0.634 (4)0.2387 (11)0.038*
C170.2141 (4)0.7419 (4)0.13334 (13)0.0342 (8)
C160.1469 (4)0.7134 (5)0.08251 (14)0.0469 (9)
H160.01940.72950.07530.056*
C150.2643 (5)0.6619 (4)0.04245 (14)0.0551 (10)
H150.21870.64460.00810.066*
C140.4523 (5)0.6364 (5)0.05458 (13)0.0499 (10)
H140.53350.60020.02790.060*
C130.5222 (4)0.6627 (4)0.10455 (13)0.0453 (10)
H130.64960.64400.11130.054*
C120.4050 (4)0.7178 (4)0.14604 (12)0.0338 (8)
C110.3657 (4)0.8018 (4)0.24047 (12)0.0334 (7)
H110.36290.91970.23740.040*
C30.4590 (4)0.7558 (4)0.29238 (12)0.0323 (8)
C40.6462 (4)0.8218 (4)0.30203 (12)0.0297 (7)
O40.7261 (3)0.9080 (3)0.26942 (8)0.0382 (6)
C100.7285 (4)0.7785 (4)0.35354 (12)0.0314 (7)
C50.9080 (4)0.8345 (4)0.36782 (12)0.0396 (9)
H50.97780.89980.34490.048*
C60.9767 (5)0.7904 (5)0.41614 (15)0.0516 (11)
F11.1503 (3)0.8486 (3)0.43125 (8)0.0783 (8)
C70.8798 (5)0.6941 (5)0.45116 (15)0.0598 (11)
H70.93140.66900.48430.072*
C80.7072 (5)0.6355 (4)0.43699 (13)0.0539 (10)
H80.64060.56700.45960.065*
C90.6331 (4)0.6803 (4)0.38801 (13)0.0401 (8)
O10.4555 (3)0.6203 (3)0.37625 (9)0.0471 (6)
C20.3784 (4)0.6620 (4)0.32923 (13)0.0429 (9)
H20.25840.62210.32170.051*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0215 (3)0.0401 (5)0.0498 (5)0.0054 (4)0.0011 (4)0.0013 (5)
O20.0419 (12)0.0430 (15)0.0711 (17)0.0132 (11)0.0049 (13)0.0072 (15)
O30.0186 (10)0.0601 (16)0.0658 (16)0.0026 (10)0.0003 (10)0.0045 (14)
N40.0170 (12)0.075 (2)0.0377 (18)0.0037 (14)0.0000 (11)0.0042 (15)
N20.0221 (12)0.0295 (17)0.0430 (17)0.0023 (11)0.0036 (11)0.0033 (13)
C170.0262 (15)0.038 (2)0.039 (2)0.0004 (14)0.0012 (13)0.0021 (16)
C160.0346 (16)0.060 (3)0.046 (2)0.0012 (18)0.0116 (16)0.007 (2)
C150.056 (2)0.074 (3)0.035 (2)0.007 (2)0.0062 (19)0.000 (2)
C140.049 (2)0.063 (3)0.038 (2)0.001 (2)0.0073 (18)0.005 (2)
C130.0280 (17)0.063 (3)0.044 (2)0.0004 (16)0.0028 (15)0.002 (2)
C120.0215 (15)0.041 (2)0.039 (2)0.0034 (14)0.0012 (13)0.0002 (18)
C110.0238 (14)0.038 (2)0.0387 (19)0.0060 (15)0.0045 (13)0.0012 (17)
C30.0282 (14)0.035 (2)0.0341 (19)0.0021 (15)0.0062 (14)0.0030 (16)
C40.0302 (15)0.0255 (19)0.0332 (19)0.0013 (14)0.0044 (13)0.0031 (16)
O40.0351 (11)0.0418 (15)0.0376 (13)0.0113 (11)0.0007 (10)0.0056 (11)
C100.0374 (16)0.026 (2)0.0307 (18)0.0027 (16)0.0000 (14)0.0034 (16)
C50.0404 (19)0.039 (2)0.039 (2)0.0019 (15)0.0028 (15)0.0014 (17)
C60.046 (2)0.060 (3)0.048 (2)0.000 (2)0.0181 (18)0.004 (2)
F10.0598 (13)0.108 (2)0.0671 (16)0.0153 (13)0.0323 (11)0.0078 (14)
C70.077 (3)0.062 (3)0.041 (2)0.001 (2)0.016 (2)0.006 (2)
C80.075 (3)0.051 (3)0.036 (2)0.003 (2)0.0002 (19)0.0075 (19)
C90.0470 (18)0.036 (2)0.038 (2)0.0005 (17)0.0016 (17)0.0016 (19)
O10.0512 (13)0.0521 (16)0.0381 (14)0.0150 (13)0.0022 (11)0.0119 (12)
C20.0349 (16)0.048 (3)0.045 (2)0.0079 (16)0.0031 (16)0.0028 (19)
Geometric parameters (Å, °) top
S1—O21.422 (2)C11—C31.507 (4)
S1—O31.427 (2)C11—H110.9800
S1—N21.632 (3)C3—C21.335 (4)
S1—C171.745 (3)C3—C41.453 (4)
N4—C121.360 (4)C4—O41.224 (3)
N4—C111.463 (4)C4—C101.460 (4)
N4—H4A0.85 (3)C10—C91.364 (4)
N2—C111.469 (3)C10—C51.398 (4)
N2—H2A0.88 (3)C5—C61.354 (4)
C17—C161.379 (4)C5—H50.9300
C17—C121.402 (4)C6—C71.370 (5)
C16—C151.370 (5)C6—F11.373 (3)
C16—H160.9300C7—C81.361 (5)
C15—C141.380 (4)C7—H70.9300
C15—H150.9300C8—C91.385 (4)
C14—C131.363 (4)C8—H80.9300
C14—H140.9300C9—O11.383 (4)
C13—C121.406 (4)O1—C21.343 (3)
C13—H130.9300C2—H20.9300
O2—S1—O3119.19 (14)N2—C11—C3110.9 (2)
O2—S1—N2108.60 (15)N4—C11—H11109.1
O3—S1—N2106.84 (13)N2—C11—H11109.1
O2—S1—C17109.76 (14)C3—C11—H11109.1
O3—S1—C17108.36 (14)C2—C3—C4119.6 (3)
N2—S1—C17102.83 (13)C2—C3—C11123.8 (3)
C12—N4—C11122.9 (2)C4—C3—C11116.6 (3)
C12—N4—H4A122 (2)O4—C4—C3122.0 (3)
C11—N4—H4A112 (2)O4—C4—C10123.3 (3)
C11—N2—S1112.4 (2)C3—C4—C10114.7 (3)
C11—N2—H2A112.3 (19)C9—C10—C5119.0 (3)
S1—N2—H2A107.2 (19)C9—C10—C4120.5 (3)
C16—C17—C12121.1 (3)C5—C10—C4120.4 (3)
C16—C17—S1120.5 (2)C6—C5—C10117.7 (3)
C12—C17—S1118.3 (2)C6—C5—H5121.1
C15—C16—C17121.4 (3)C10—C5—H5121.1
C15—C16—H16119.3C5—C6—C7123.3 (3)
C17—C16—H16119.3C5—C6—F1118.2 (4)
C16—C15—C14118.0 (3)C7—C6—F1118.4 (3)
C16—C15—H15121.0C8—C7—C6119.3 (3)
C14—C15—H15121.0C8—C7—H7120.3
C13—C14—C15121.8 (3)C6—C7—H7120.3
C13—C14—H14119.1C7—C8—C9118.3 (3)
C15—C14—H14119.1C7—C8—H8120.8
C14—C13—C12121.1 (3)C9—C8—H8120.8
C14—C13—H13119.4C10—C9—O1121.9 (3)
C12—C13—H13119.4C10—C9—C8122.2 (3)
N4—C12—C17123.3 (3)O1—C9—C8115.8 (3)
N4—C12—C13120.0 (2)C2—O1—C9117.6 (3)
C17—C12—C13116.5 (3)C3—C2—O1125.6 (3)
N4—C11—N2109.6 (3)C3—C2—H2117.2
N4—C11—C3109.0 (2)O1—C2—H2117.2
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N4—H4A···O3i0.85 (3)2.21 (3)2.993 (3)153 (3)
N4—H4A···O40.85 (3)2.39 (3)2.924 (3)121 (3)
N2—H2A···O4ii0.88 (3)2.03 (3)2.848 (3)155 (3)
C2—H2···O2iii0.932.483.399 (4)168
C13—H13···O3i0.932.493.258 (3)140
Symmetry codes: (i) x+1, y, z; (ii) −x+1, y−1/2, −z+1/2; (iii) −x, y−1/2, −z+1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N4—H4A···O3i0.85 (3)2.21 (3)2.993 (3)153 (3)
N4—H4A···O40.85 (3)2.39 (3)2.924 (3)121 (3)
N2—H2A···O4ii0.88 (3)2.03 (3)2.848 (3)155 (3)
C2—H2···O2iii0.932.483.399 (4)168
C13—H13···O3i0.932.493.258 (3)140
Symmetry codes: (i) x+1, y, z; (ii) −x+1, y−1/2, −z+1/2; (iii) −x, y−1/2, −z+1/2.
Acknowledgements top

The authors acknowledge the Higher Education Commission, Islamabad, Pakistan, for financial and GCU Lahore for technical support.

references
References top

Mariya-al-Rashida, Tahir, M. N., Nagra, S. A., Imran, M. & Iqbal, J. (2009). Acta Cryst. E65, o1818–o1819.

Bruker (2007). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.

Di Bella, M., Monzani, A., Andrisano, M. G., Fabio, U. & Quaglio, G. P. (1983). Farmaco, 38, 466–472.

Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

Kamal, A., Ahmed, S. K., Reddy, K. S., Khan, M. N. A., Shetty, R. V. C. R. N. C., Siddhardha, B., Murty, U. S. N., China, A. & Nagaraja, V. (2007a). Lett. Drug Des. Discov. 4, 550–556.

Kamal, A., Khan, M. N. A., Reddy, K. S., Rohini, K., Sastry, G. N., Sateesh, B. & Sridhar, B. (2007b). Bioorg. Med. Chem. Lett. 17, 5400–5405.

Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Weisman, R. A. & Brown, G. M. (1964). J. Biol. Chem. 239, 326–331.

Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

Zhu, Z., Zhu, S., Liu, D., Cao, T., Wang, L. & Tepel, M. (2005). Hypertension, 45, 233–239.