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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 27;67(Pt 9):o2428. doi: 10.1107/S1600536811032879

4-(5-Oxo-3-phenyl-4,5-dihydro-1H-pyrazol-1-yl)benzene­sulfonamide

Abdulrahman O Al-Youbi a, Abdullah M Asiri a,b, Hassan M Faidallah a, Khalid A Alamry a, Seik Weng Ng c,a,*
PMCID: PMC3200779  PMID: 22064810

Abstract

With respect to the aliphatic planar five-membered ring (r.m.s. deviation = 0.011 Å) of the title compound, C15H13N3O2S, the phenyl ring is aligned at 6.9 (1)° and the phenyl­ene ring at 2.4 (1)°, so that the three rings are nearly coplanar. The amino group has the N atom in a pyramidal geometry; the group is a hydrogen-bond donor to the sulfonyl O atom of one mol­ecule and to the ketonic O atom of another mol­ecule, resulting in the formation of a layer parallel to the bc plane.

Related literature

For the synthesis, see: Casoni (1956); Itano (1955).graphic file with name e-67-o2428-scheme1.jpg

Experimental

Crystal data

  • C15H13N3O3S

  • M r = 315.34

  • Monoclinic, Inline graphic

  • a = 13.6794 (4) Å

  • b = 13.4304 (4) Å

  • c = 7.3678 (2) Å

  • β = 91.055 (3)°

  • V = 1353.38 (7) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 2.29 mm−1

  • T = 100 K

  • 0.30 × 0.05 × 0.05 mm

Data collection

  • Agilent SuperNova Dual diffractometer with an Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) T min = 0.546, T max = 0.894

  • 10404 measured reflections

  • 2731 independent reflections

  • 2444 reflections with I > 2σ(I)

  • R int = 0.041

Refinement

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.121

  • S = 1.06

  • 2731 reflections

  • 207 parameters

  • 2 restraints

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

  • Δρmax = 0.73 e Å−3

  • Δρmin = −0.51 e Å−3

Data collection: CrysAlis PRO (Agilent, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811032879/bt5611sup1.cif

e-67-o2428-sup1.cif (18.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811032879/bt5611Isup2.hkl

e-67-o2428-Isup2.hkl (134.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811032879/bt5611Isup3.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—H1⋯O3i 0.88 (1) 2.12 (1) 2.975 (2) 164 (2)
N3—H2⋯O2ii 0.87 (1) 2.12 (1) 2.978 (2) 168 (2)

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

Acknowledgments

We thank King Abdulaziz University and the University of Malaya for supporting this study.

supplementary crystallographic information

Comment

We are examining the medicinal properties of phenylpyrazolones of which the 4-benzenesulfamide derivative (Scheme I) is expected to show enhanced activity. The synthesis of the compound was reported a long time ago (Casoni, 1956; Itano, 1955). With respect to the aliphatic planar five-membered ring, the phenyl ring is aligned at 6.9 (1)° and the phenylene ring at 2.4 (1)°. The amino group is hydrogen bond donor to the sulfonyl O atom of one molecule and to the ketonic O atom of another molecule to result in the formation of a layer parallel to the bc plane.

Experimental

Ethyl benzoylacetate (10 mmol) and 4-hydrazinobenzenesulfonamide hydrochloride (10 mmol) were heated in ethanol (50 ml) for 4 h; water was added to precipitate the product, which was collected and recrystallized from ethanol as brownish-orange crystals; m.p. 510–511 K.

Refinement

Carbon bound H-atoms were placed in calculated positions [C–H 0.95 to 0.98 Å, Uiso(H) 1.2–1.5Ueq(C)] and were included in the refinement in the riding model approximation.

The amino H-atoms were located in a difference Fouier map and were refined with a distance restraint of N–H 0.88±0.01 Å; their isotropic displacement parameter were freely refined.

Figures

Fig. 1.

Fig. 1.

Anisotropic displacement ellipsoid plot (Barbour, 2001) of C15H13N3O2S at the 70% probability level; hydrogen atoms are drawn as spheres of arbitrary radius.

Crystal data

C15H13N3O3S F(000) = 656
Mr = 315.34 Dx = 1.548 Mg m3
Monoclinic, P21/c Cu Kα radiation, λ = 1.54184 Å
Hall symbol: -P 2ybc Cell parameters from 4563 reflections
a = 13.6794 (4) Å θ = 3.2–74.4°
b = 13.4304 (4) Å µ = 2.29 mm1
c = 7.3678 (2) Å T = 100 K
β = 91.055 (3)° Prism, brown orange
V = 1353.38 (7) Å3 0.30 × 0.05 × 0.05 mm
Z = 4

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector 2731 independent reflections
Radiation source: SuperNova (Cu) X-ray Source 2444 reflections with I > 2σ(I)
Mirror Rint = 0.041
Detector resolution: 10.4041 pixels mm-1 θmax = 74.5°, θmin = 3.2°
ω scan h = −17→16
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) k = −16→16
Tmin = 0.546, Tmax = 0.894 l = −5→9
10404 measured reflections

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)] = 0.041 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.121 H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0759P)2 + 0.5321P] where P = (Fo2 + 2Fc2)/3
2731 reflections (Δ/σ)max = 0.001
207 parameters Δρmax = 0.73 e Å3
2 restraints Δρmin = −0.51 e Å3

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
S1 0.91654 (3) 0.64477 (3) 0.49527 (6) 0.01653 (16)
O1 0.52785 (10) 0.32661 (11) 0.6467 (2) 0.0319 (4)
O2 0.90632 (9) 0.74972 (10) 0.46298 (18) 0.0220 (3)
O3 0.95114 (9) 0.58212 (10) 0.35168 (17) 0.0209 (3)
N2 0.46514 (11) 0.56244 (12) 0.8066 (2) 0.0203 (3)
N3 0.99249 (12) 0.63163 (12) 0.6642 (2) 0.0197 (3)
H1 1.0122 (17) 0.5704 (9) 0.682 (3) 0.028 (6)*
H2 0.9740 (16) 0.6620 (16) 0.763 (2) 0.023 (6)*
N1 0.52929 (11) 0.49471 (11) 0.7246 (2) 0.0197 (3)
C1 0.49011 (14) 0.39912 (14) 0.7147 (3) 0.0227 (4)
C2 0.39264 (14) 0.40640 (14) 0.8033 (3) 0.0224 (4)
H2A 0.3390 0.3864 0.7189 0.027*
H2B 0.3903 0.3645 0.9138 0.027*
C3 0.38673 (13) 0.51403 (14) 0.8491 (2) 0.0198 (4)
C4 0.30272 (13) 0.56293 (14) 0.9324 (2) 0.0205 (4)
C5 0.30792 (15) 0.66235 (15) 0.9877 (3) 0.0261 (4)
H5 0.3663 0.6993 0.9713 0.031*
C6 0.22764 (16) 0.70694 (16) 1.0664 (3) 0.0312 (5)
H6 0.2311 0.7745 1.1040 0.037*
C7 0.14192 (15) 0.65297 (16) 1.0905 (3) 0.0294 (5)
H7 0.0870 0.6837 1.1441 0.035*
C8 0.13695 (14) 0.55477 (17) 1.0363 (3) 0.0281 (5)
H8 0.0784 0.5181 1.0528 0.034*
C9 0.21695 (13) 0.50911 (15) 0.9577 (3) 0.0235 (4)
H9 0.2132 0.4413 0.9213 0.028*
C10 0.62051 (12) 0.52987 (13) 0.6675 (2) 0.0178 (4)
C11 0.68801 (13) 0.46447 (14) 0.5912 (2) 0.0197 (4)
H11 0.6720 0.3961 0.5759 0.024*
C12 0.77831 (13) 0.49990 (13) 0.5381 (2) 0.0184 (4)
H12 0.8246 0.4557 0.4875 0.022*
C13 0.80101 (13) 0.60030 (13) 0.5590 (2) 0.0175 (4)
C14 0.73339 (14) 0.66554 (14) 0.6338 (3) 0.0201 (4)
H14 0.7495 0.7339 0.6481 0.024*
C15 0.64299 (14) 0.63125 (14) 0.6873 (3) 0.0200 (4)
H15 0.5967 0.6759 0.7369 0.024*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0140 (2) 0.0175 (3) 0.0182 (3) −0.00041 (14) 0.00381 (17) 0.00075 (14)
O1 0.0230 (7) 0.0225 (7) 0.0506 (9) −0.0015 (6) 0.0103 (7) −0.0049 (6)
O2 0.0202 (6) 0.0184 (7) 0.0276 (7) −0.0010 (5) 0.0052 (5) 0.0040 (5)
O3 0.0194 (6) 0.0241 (7) 0.0194 (6) −0.0005 (5) 0.0061 (5) −0.0021 (5)
N2 0.0148 (7) 0.0241 (8) 0.0221 (8) 0.0014 (6) 0.0047 (6) −0.0003 (6)
N3 0.0180 (8) 0.0205 (8) 0.0208 (8) 0.0015 (6) 0.0012 (6) −0.0009 (6)
N1 0.0161 (7) 0.0206 (8) 0.0226 (8) −0.0004 (6) 0.0050 (6) −0.0023 (6)
C1 0.0194 (9) 0.0227 (10) 0.0259 (9) −0.0017 (7) 0.0013 (7) 0.0021 (7)
C2 0.0179 (9) 0.0251 (10) 0.0242 (9) −0.0018 (7) 0.0024 (7) 0.0015 (7)
C3 0.0168 (9) 0.0248 (9) 0.0178 (8) −0.0014 (7) 0.0008 (7) 0.0022 (7)
C4 0.0162 (9) 0.0274 (9) 0.0179 (8) 0.0009 (7) 0.0022 (7) 0.0049 (7)
C5 0.0236 (10) 0.0259 (10) 0.0290 (10) 0.0004 (8) 0.0083 (8) 0.0056 (8)
C6 0.0326 (11) 0.0261 (10) 0.0353 (11) 0.0068 (8) 0.0120 (9) 0.0078 (8)
C7 0.0220 (10) 0.0400 (12) 0.0266 (10) 0.0123 (8) 0.0080 (8) 0.0114 (8)
C8 0.0153 (9) 0.0450 (12) 0.0241 (10) −0.0017 (8) 0.0019 (7) 0.0068 (8)
C9 0.0180 (9) 0.0329 (10) 0.0195 (9) −0.0034 (8) 0.0007 (7) 0.0007 (7)
C10 0.0146 (8) 0.0220 (9) 0.0170 (8) −0.0006 (7) 0.0012 (6) 0.0019 (7)
C11 0.0190 (9) 0.0203 (9) 0.0200 (8) −0.0009 (7) 0.0019 (7) −0.0004 (7)
C12 0.0161 (8) 0.0193 (8) 0.0199 (9) 0.0024 (7) 0.0029 (7) 0.0004 (6)
C13 0.0141 (8) 0.0208 (9) 0.0178 (8) −0.0012 (7) 0.0015 (6) 0.0019 (6)
C14 0.0195 (9) 0.0171 (8) 0.0240 (9) −0.0002 (7) 0.0033 (7) 0.0000 (7)
C15 0.0177 (9) 0.0211 (9) 0.0213 (9) 0.0017 (7) 0.0029 (7) −0.0007 (7)

Geometric parameters (Å, °)

S1—O2 1.4358 (13) C5—H5 0.9500
S1—O3 1.4386 (13) C6—C7 1.393 (3)
S1—N3 1.6160 (17) C6—H6 0.9500
S1—C13 1.7611 (18) C7—C8 1.379 (3)
O1—C1 1.215 (2) C7—H7 0.9500
N2—C3 1.298 (2) C8—C9 1.390 (3)
N2—N1 1.408 (2) C8—H8 0.9500
N3—H1 0.875 (10) C9—H9 0.9500
N3—H2 0.873 (10) C10—C11 1.400 (2)
N1—C1 1.393 (2) C10—C15 1.403 (3)
N1—C10 1.406 (2) C11—C12 1.387 (3)
C1—C2 1.499 (3) C11—H11 0.9500
C2—C3 1.487 (3) C12—C13 1.392 (2)
C2—H2A 0.9900 C12—H12 0.9500
C2—H2B 0.9900 C13—C14 1.395 (2)
C3—C4 1.468 (2) C14—C15 1.384 (3)
C4—C9 1.393 (3) C14—H14 0.9500
C4—C5 1.397 (3) C15—H15 0.9500
C5—C6 1.387 (3)
O2—S1—O3 119.00 (8) C5—C6—C7 120.2 (2)
O2—S1—N3 107.10 (8) C5—C6—H6 119.9
O3—S1—N3 106.67 (8) C7—C6—H6 119.9
O2—S1—C13 106.97 (8) C8—C7—C6 119.86 (19)
O3—S1—C13 107.85 (8) C8—C7—H7 120.1
N3—S1—C13 108.97 (8) C6—C7—H7 120.1
C3—N2—N1 107.72 (15) C7—C8—C9 120.49 (19)
S1—N3—H1 114.1 (16) C7—C8—H8 119.8
S1—N3—H2 113.3 (16) C9—C8—H8 119.8
H1—N3—H2 114 (2) C8—C9—C4 119.88 (19)
C1—N1—C10 129.54 (15) C8—C9—H9 120.1
C1—N1—N2 112.08 (14) C4—C9—H9 120.1
C10—N1—N2 118.38 (14) C11—C10—N1 120.35 (16)
O1—C1—N1 126.49 (17) C11—C10—C15 120.39 (16)
O1—C1—C2 128.35 (18) N1—C10—C15 119.26 (16)
N1—C1—C2 105.17 (16) C12—C11—C10 119.71 (17)
C3—C2—C1 102.40 (15) C12—C11—H11 120.1
C3—C2—H2A 111.3 C10—C11—H11 120.1
C1—C2—H2A 111.3 C11—C12—C13 119.97 (16)
C3—C2—H2B 111.3 C11—C12—H12 120.0
C1—C2—H2B 111.3 C13—C12—H12 120.0
H2A—C2—H2B 109.2 C12—C13—C14 120.26 (16)
N2—C3—C4 122.26 (17) C12—C13—S1 119.91 (13)
N2—C3—C2 112.57 (16) C14—C13—S1 119.81 (14)
C4—C3—C2 125.17 (16) C15—C14—C13 120.41 (17)
C9—C4—C5 119.68 (17) C15—C14—H14 119.8
C9—C4—C3 119.44 (17) C13—C14—H14 119.8
C5—C4—C3 120.88 (17) C14—C15—C10 119.25 (17)
C6—C5—C4 119.85 (19) C14—C15—H15 120.4
C6—C5—H5 120.1 C10—C15—H15 120.4
C4—C5—H5 120.1
C3—N2—N1—C1 −0.1 (2) C5—C4—C9—C8 0.5 (3)
C3—N2—N1—C10 −179.52 (16) C3—C4—C9—C8 −179.92 (17)
C10—N1—C1—O1 −2.7 (3) C1—N1—C10—C11 −1.6 (3)
N2—N1—C1—O1 177.9 (2) N2—N1—C10—C11 177.72 (15)
C10—N1—C1—C2 177.83 (17) C1—N1—C10—C15 178.21 (18)
N2—N1—C1—C2 −1.6 (2) N2—N1—C10—C15 −2.4 (2)
O1—C1—C2—C3 −177.1 (2) N1—C10—C11—C12 −178.97 (16)
N1—C1—C2—C3 2.34 (19) C15—C10—C11—C12 1.2 (3)
N1—N2—C3—C4 −178.03 (16) C10—C11—C12—C13 −0.7 (3)
N1—N2—C3—C2 1.7 (2) C11—C12—C13—C14 0.2 (3)
C1—C2—C3—N2 −2.6 (2) C11—C12—C13—S1 178.85 (14)
C1—C2—C3—C4 177.17 (17) O2—S1—C13—C12 157.60 (15)
N2—C3—C4—C9 173.44 (17) O3—S1—C13—C12 28.50 (17)
C2—C3—C4—C9 −6.3 (3) N3—S1—C13—C12 −86.93 (16)
N2—C3—C4—C5 −7.0 (3) O2—S1—C13—C14 −23.78 (17)
C2—C3—C4—C5 173.27 (18) O3—S1—C13—C14 −152.88 (15)
C9—C4—C5—C6 −0.3 (3) N3—S1—C13—C14 91.69 (16)
C3—C4—C5—C6 −179.88 (18) C12—C13—C14—C15 −0.3 (3)
C4—C5—C6—C7 0.0 (3) S1—C13—C14—C15 −178.89 (14)
C5—C6—C7—C8 0.2 (3) C13—C14—C15—C10 0.8 (3)
C6—C7—C8—C9 0.0 (3) C11—C10—C15—C14 −1.2 (3)
C7—C8—C9—C4 −0.4 (3) N1—C10—C15—C14 178.94 (16)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N3—H1···O3i 0.88 (1) 2.12 (1) 2.975 (2) 164 (2)
N3—H2···O2ii 0.87 (1) 2.12 (1) 2.978 (2) 168 (2)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5611).

References

  1. Agilent (2010). CrysAlis PRO Agilent Technologies, Yarnton, Oxfordshire, England.
  2. Barbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.
  3. Casoni, D. (1956). Boll. Sci. Fac. Chim. Ind. Bologna, 14, 22–30.
  4. Itano, K. (1955). Yakugaku Zasshi, 5, 441–444.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

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) global, I. DOI: 10.1107/S1600536811032879/bt5611sup1.cif

e-67-o2428-sup1.cif (18.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811032879/bt5611Isup2.hkl

e-67-o2428-Isup2.hkl (134.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811032879/bt5611Isup3.cml

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


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