organic compounds
1-(4-Methylphenyl)-3-phenyl-1H-pyrazol-5-yl 4-nitrobenzenesulfonate
aCHEMSOL, 1 Harcourt Road, Aberdeen, AB15 5NY, Scotland, bDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia, and cCentro de Desenvolvimento Tecnológico em Saúde (CDTS), Fundação Oswaldo Cruz (FIOCRUZ), Casa Amarela, Campus de Manguinhos, Av. Brasil 4365, 21040-900 Rio de Janeiro, RJ, Brazil
*Correspondence e-mail: edward.tiekink@gmail.com
In the title molecule, C22H17N3O5S, the pyrazole ring is planar (r.m.s. deviation = 0.018 Å) and forms dihedral angles of 21.45 (10) and 6.96 (10)° with the N- and C-bound benzene rings, respectively. Supramolecular layers in the bc plane are formed in the crystal via C—H⋯O and π–π interactions involving the sulfonamide benzene ring interacting with the N- and C-bound benzene rings [centroid–centroid distances = 3.790 (2) and 3.730 (2) Å, respectively]. The crystal studied was found to be a twin (twin law 1 0 0.678, 0 -1 0, 0 0 -1), the fractional contribution of the minor component being approximately 36%.
Related literature
For related structures and background references to pyrazoles, see: Wardell et al. (2012); Baddeley et al. (2012). For the synthesis, see: Galoyan et al. (1969). For the treatment of twinned diffraction data, see: Spek (2009).
Experimental
Crystal data
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Refinement
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Data collection: COLLECT (Hooft, 1998); cell DENZO (Otwinowski & Minor, 1997) and COLLECT; data reduction: DENZO and COLLECT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
10.1107/S1600536812010598/hb6674sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812010598/hb6674Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812010598/hb6674Isup3.cml
A solution of 4-MeC6H4NHNH2.HCl (2 mmol) and PhCOCH2CONHPh (2 mmol) in Me2CO (20 ml) was refluxed for 1 h. A solution of 4-nitrobenzenesulfonyl chloride (2 mmol) in Me2CO (10 ml) was added and the reaction mixture was refluxed for 30 min, rotary evaporated and the residue was recrystallized twice from EtOH as yellow plates, M.pt: 445–447 K.
The C-bound H atoms were geometrically placed (C—H = 0.95–0.98 Å) and refined as riding with Uiso(H) = 1.2–1.5Ueq(C). Owing to poor agreement three reflections, i.e. (7 0 10), (7 1 13) and (12 5 13), were removed from the final cycles of The sample was a non-merohedral twin (twin law 1 0 0.678, 0 1 0, 0 0 1) and the fractional contribution of the minor component refined to 0.362 (2). The twin domains were separated by using the TwinRotMat routine in PLATON (Spek, 2009).
The structure of the title compound is now reported in continuation of related structural studies (Wardell et al. 2012; Baddeley et al., 2012).
In the title compound, Fig. 2, the pyrazole ring is planar with a r.m.s. deviation for the fitted atoms of 0.018 Å; the maximum deviations from this plane are 0.015 (1) Å (for the N1 atom) and -0.015 (1) Å (C8). The N– and C-bound benzene rings are inclined to this plane forming dihedral angles of 21.45 (10) and 6.96 (10)°, respectively; the dihedral angle between the benzene rings is 20.42 (10)° consistent with a non-planar molecule.
In the crystal, molecules are assembled into supramolecular layers in the bc plane via C—H···O, Table 1, and π—π interactions involving the sulfonamide benzene ring interacting with the N– and C-bound benzene rings {ring centroid···ring centroid distances = 3.790 (2) Å [angle of inclination = 0.96 (17)° for 1 - x, 1 - y, -z] and 3.730 (2) Å [angle of inclination = 10.02 (17)° for 1 - x, -1/2 + y, -1/2 - z], respectively}, Fig. 3. Layers stack along the a axis with no specific interactions between them, Fig. 4.
For related structures and background references to pyrazoles, see: Wardell et al. (2012); Baddeley et al. (2012). For the synthesis, see: Galoyan et al. (1969). For the treatment of twinned diffraction data, see: Spek (2009).
Data collection: COLLECT (Hooft, 1998); cell
DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998); data reduction: DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).C22H17N3O5S | F(000) = 904 |
Mr = 435.46 | Dx = 1.472 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 67707 reflections |
a = 13.5339 (12) Å | θ = 2.9–27.5° |
b = 10.4827 (10) Å | µ = 0.21 mm−1 |
c = 14.9303 (13) Å | T = 120 K |
β = 111.975 (3)° | Plate, yellow |
V = 1964.3 (3) Å3 | 0.58 × 0.38 × 0.04 mm |
Z = 4 |
Rigaku Saturn724+ diffractometer | 4454 independent reflections |
Radiation source: Rotating Anode | 3951 reflections with I > 2σ(I) |
Confocal monochromator | Rint = 0.000 |
Detector resolution: 28.5714 pixels mm-1 | θmax = 27.5°, θmin = 3.2° |
profile data from ω–scans | h = −17→16 |
Absorption correction: multi-scan (SADABS; Sheldrick, 2007) | k = 0→13 |
Tmin = 0.620, Tmax = 0.746 | l = 0→19 |
4454 measured reflections |
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)] = 0.069 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.179 | H-atom parameters constrained |
S = 1.19 | w = 1/[σ2(Fo2) + (0.0562P)2 + 4.737P] where P = (Fo2 + 2Fc2)/3 |
4454 reflections | (Δ/σ)max < 0.001 |
282 parameters | Δρmax = 0.59 e Å−3 |
0 restraints | Δρmin = −0.62 e Å−3 |
C22H17N3O5S | V = 1964.3 (3) Å3 |
Mr = 435.46 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 13.5339 (12) Å | µ = 0.21 mm−1 |
b = 10.4827 (10) Å | T = 120 K |
c = 14.9303 (13) Å | 0.58 × 0.38 × 0.04 mm |
β = 111.975 (3)° |
Rigaku Saturn724+ diffractometer | 4454 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2007) | 3951 reflections with I > 2σ(I) |
Tmin = 0.620, Tmax = 0.746 | Rint = 0.000 |
4454 measured reflections |
R[F2 > 2σ(F2)] = 0.069 | 0 restraints |
wR(F2) = 0.179 | H-atom parameters constrained |
S = 1.19 | Δρmax = 0.59 e Å−3 |
4454 reflections | Δρmin = −0.62 e Å−3 |
282 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.47829 (6) | 0.20331 (9) | 0.00726 (6) | 0.0203 (2) | |
O1 | 0.51909 (18) | 0.3508 (3) | 0.01445 (17) | 0.0203 (5) | |
O2 | 0.5619 (2) | 0.1219 (3) | 0.0044 (2) | 0.0268 (6) | |
O3 | 0.4369 (2) | 0.1938 (3) | 0.08223 (19) | 0.0315 (7) | |
O4 | 0.1490 (2) | 0.2303 (3) | −0.4513 (2) | 0.0360 (7) | |
O5 | 0.0359 (2) | 0.2650 (3) | −0.3824 (2) | 0.0377 (8) | |
N1 | 0.7023 (2) | 0.4081 (3) | 0.0618 (2) | 0.0156 (6) | |
N2 | 0.7780 (2) | 0.4243 (3) | 0.0225 (2) | 0.0156 (6) | |
N3 | 0.1265 (2) | 0.2427 (3) | −0.3796 (2) | 0.0254 (7) | |
C1 | 0.6074 (2) | 0.3760 (3) | −0.0095 (2) | 0.0169 (7) | |
C2 | 0.7290 (2) | 0.4006 (3) | −0.0717 (2) | 0.0141 (6) | |
C3 | 0.6198 (3) | 0.3718 (3) | −0.0957 (2) | 0.0183 (7) | |
H3 | 0.5673 | 0.3539 | −0.1576 | 0.022* | |
C4 | 0.3726 (3) | 0.2062 (3) | −0.1065 (3) | 0.0185 (7) | |
C5 | 0.2715 (3) | 0.2430 (4) | −0.1110 (3) | 0.0206 (7) | |
H5 | 0.2587 | 0.2609 | −0.0539 | 0.025* | |
C6 | 0.1898 (3) | 0.2525 (4) | −0.2022 (3) | 0.0222 (7) | |
H6 | 0.1196 | 0.2749 | −0.2081 | 0.027* | |
C7 | 0.2126 (3) | 0.2292 (3) | −0.2831 (3) | 0.0199 (7) | |
C8 | 0.3132 (3) | 0.1929 (4) | −0.2796 (3) | 0.0220 (7) | |
H8 | 0.3262 | 0.1777 | −0.3370 | 0.026* | |
C9 | 0.3942 (3) | 0.1796 (3) | −0.1886 (3) | 0.0189 (7) | |
H9 | 0.4633 | 0.1527 | −0.1829 | 0.023* | |
C10 | 0.7302 (3) | 0.4228 (3) | 0.1639 (2) | 0.0152 (6) | |
C11 | 0.8359 (3) | 0.3992 (3) | 0.2245 (3) | 0.0181 (7) | |
H11 | 0.8871 | 0.3757 | 0.1980 | 0.022* | |
C12 | 0.8651 (3) | 0.4106 (3) | 0.3239 (2) | 0.0198 (7) | |
H12 | 0.9369 | 0.3951 | 0.3651 | 0.024* | |
C13 | 0.7909 (3) | 0.4445 (3) | 0.3644 (3) | 0.0210 (7) | |
C14 | 0.6856 (3) | 0.4686 (4) | 0.3023 (3) | 0.0211 (7) | |
H14 | 0.6343 | 0.4919 | 0.3287 | 0.025* | |
C15 | 0.6551 (3) | 0.4590 (3) | 0.2020 (3) | 0.0197 (7) | |
H15 | 0.5838 | 0.4770 | 0.1604 | 0.024* | |
C16 | 0.8218 (3) | 0.4510 (4) | 0.4733 (3) | 0.0307 (9) | |
H16A | 0.7642 | 0.4912 | 0.4879 | 0.046* | |
H16B | 0.8871 | 0.5014 | 0.5020 | 0.046* | |
H16C | 0.8341 | 0.3645 | 0.5002 | 0.046* | |
C17 | 0.7883 (3) | 0.4054 (3) | −0.1369 (2) | 0.0157 (6) | |
C18 | 0.7359 (3) | 0.3973 (3) | −0.2370 (2) | 0.0166 (6) | |
H18 | 0.6609 | 0.3851 | −0.2640 | 0.020* | |
C19 | 0.7925 (3) | 0.4068 (3) | −0.2978 (2) | 0.0191 (7) | |
H19 | 0.7563 | 0.4007 | −0.3658 | 0.023* | |
C20 | 0.9031 (3) | 0.4255 (4) | −0.2584 (3) | 0.0210 (7) | |
H20 | 0.9417 | 0.4348 | −0.2997 | 0.025* | |
C21 | 0.9563 (3) | 0.4303 (3) | −0.1586 (3) | 0.0194 (7) | |
H21 | 1.0315 | 0.4409 | −0.1319 | 0.023* | |
C22 | 0.8997 (3) | 0.4196 (3) | −0.0977 (2) | 0.0185 (7) | |
H22 | 0.9365 | 0.4218 | −0.0297 | 0.022* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0124 (4) | 0.0288 (5) | 0.0195 (4) | −0.0052 (3) | 0.0057 (3) | 0.0020 (4) |
O1 | 0.0110 (10) | 0.0319 (14) | 0.0212 (12) | −0.0056 (10) | 0.0097 (10) | −0.0077 (10) |
O2 | 0.0167 (12) | 0.0245 (14) | 0.0359 (15) | 0.0004 (10) | 0.0058 (11) | 0.0053 (12) |
O3 | 0.0206 (12) | 0.0545 (19) | 0.0206 (13) | −0.0108 (13) | 0.0090 (11) | 0.0067 (13) |
O4 | 0.0335 (15) | 0.0501 (19) | 0.0210 (14) | −0.0070 (14) | 0.0061 (12) | −0.0007 (13) |
O5 | 0.0202 (13) | 0.050 (2) | 0.0338 (16) | 0.0089 (13) | −0.0002 (12) | −0.0092 (14) |
N1 | 0.0106 (12) | 0.0238 (15) | 0.0136 (13) | −0.0030 (11) | 0.0057 (11) | 0.0008 (11) |
N2 | 0.0110 (12) | 0.0238 (15) | 0.0144 (13) | −0.0021 (11) | 0.0075 (11) | 0.0014 (11) |
N3 | 0.0230 (15) | 0.0232 (16) | 0.0244 (17) | −0.0028 (13) | 0.0024 (13) | −0.0025 (13) |
C1 | 0.0077 (13) | 0.0240 (17) | 0.0179 (15) | −0.0046 (12) | 0.0034 (12) | −0.0022 (14) |
C2 | 0.0113 (14) | 0.0175 (16) | 0.0127 (15) | −0.0014 (12) | 0.0034 (12) | −0.0004 (12) |
C3 | 0.0126 (14) | 0.0237 (18) | 0.0171 (16) | −0.0034 (13) | 0.0037 (12) | −0.0022 (13) |
C4 | 0.0124 (14) | 0.0224 (17) | 0.0190 (16) | −0.0046 (13) | 0.0040 (12) | −0.0001 (14) |
C5 | 0.0161 (15) | 0.0254 (18) | 0.0228 (18) | −0.0043 (14) | 0.0100 (13) | −0.0032 (14) |
C6 | 0.0139 (15) | 0.0242 (18) | 0.0274 (19) | −0.0010 (14) | 0.0066 (14) | −0.0014 (15) |
C7 | 0.0146 (15) | 0.0196 (17) | 0.0225 (17) | −0.0042 (13) | 0.0035 (13) | −0.0020 (14) |
C8 | 0.0190 (16) | 0.0241 (18) | 0.0227 (17) | −0.0044 (14) | 0.0077 (14) | −0.0029 (14) |
C9 | 0.0137 (14) | 0.0210 (17) | 0.0240 (18) | −0.0029 (13) | 0.0093 (13) | −0.0036 (14) |
C10 | 0.0163 (15) | 0.0177 (16) | 0.0104 (15) | −0.0014 (12) | 0.0036 (12) | −0.0001 (12) |
C11 | 0.0141 (15) | 0.0231 (17) | 0.0172 (16) | 0.0001 (13) | 0.0060 (13) | 0.0017 (13) |
C12 | 0.0174 (16) | 0.0220 (18) | 0.0172 (17) | −0.0024 (13) | 0.0034 (13) | 0.0007 (13) |
C13 | 0.0273 (18) | 0.0200 (17) | 0.0164 (16) | −0.0054 (14) | 0.0090 (14) | −0.0015 (14) |
C14 | 0.0214 (17) | 0.0235 (18) | 0.0225 (18) | −0.0019 (14) | 0.0130 (15) | −0.0020 (14) |
C15 | 0.0170 (15) | 0.0209 (16) | 0.0218 (17) | −0.0019 (13) | 0.0080 (14) | −0.0015 (14) |
C16 | 0.037 (2) | 0.039 (2) | 0.0143 (17) | −0.0007 (18) | 0.0082 (16) | 0.0005 (16) |
C17 | 0.0159 (15) | 0.0178 (16) | 0.0145 (15) | −0.0020 (12) | 0.0071 (13) | −0.0001 (12) |
C18 | 0.0159 (15) | 0.0189 (16) | 0.0137 (15) | −0.0007 (12) | 0.0040 (12) | −0.0002 (13) |
C19 | 0.0209 (16) | 0.0214 (17) | 0.0135 (16) | −0.0014 (13) | 0.0050 (13) | −0.0006 (13) |
C20 | 0.0217 (17) | 0.0263 (19) | 0.0220 (18) | −0.0007 (14) | 0.0163 (15) | −0.0008 (14) |
C21 | 0.0134 (15) | 0.0246 (18) | 0.0207 (17) | −0.0030 (13) | 0.0071 (13) | −0.0002 (14) |
C22 | 0.0161 (15) | 0.0248 (18) | 0.0135 (15) | −0.0007 (13) | 0.0045 (13) | −0.0001 (13) |
S1—O3 | 1.430 (3) | C10—C15 | 1.391 (5) |
S1—O2 | 1.431 (3) | C10—C11 | 1.399 (4) |
S1—O1 | 1.632 (3) | C11—C12 | 1.391 (5) |
S1—C4 | 1.765 (3) | C11—H11 | 0.9500 |
O1—C1 | 1.395 (4) | C12—C13 | 1.397 (5) |
O4—N3 | 1.225 (4) | C12—H12 | 0.9500 |
O5—N3 | 1.233 (4) | C13—C14 | 1.402 (5) |
N1—N2 | 1.366 (4) | C13—C16 | 1.522 (5) |
N1—C1 | 1.368 (4) | C14—C15 | 1.401 (5) |
N1—C10 | 1.435 (4) | C14—H14 | 0.9500 |
N2—C2 | 1.336 (4) | C15—H15 | 0.9500 |
N3—C7 | 1.482 (5) | C16—H16A | 0.9800 |
C1—C3 | 1.360 (5) | C16—H16B | 0.9800 |
C2—C3 | 1.417 (4) | C16—H16C | 0.9800 |
C2—C17 | 1.476 (4) | C17—C18 | 1.397 (5) |
C3—H3 | 0.9500 | C17—C22 | 1.406 (5) |
C4—C9 | 1.390 (5) | C18—C19 | 1.393 (5) |
C4—C5 | 1.399 (5) | C18—H18 | 0.9500 |
C5—C6 | 1.399 (5) | C19—C20 | 1.402 (5) |
C5—H5 | 0.9500 | C19—H19 | 0.9500 |
C6—C7 | 1.376 (5) | C20—C21 | 1.391 (5) |
C6—H6 | 0.9500 | C20—H20 | 0.9500 |
C7—C8 | 1.396 (5) | C21—C22 | 1.396 (5) |
C8—C9 | 1.397 (5) | C21—H21 | 0.9500 |
C8—H8 | 0.9500 | C22—H22 | 0.9500 |
C9—H9 | 0.9500 | ||
O3—S1—O2 | 121.83 (18) | C15—C10—N1 | 121.5 (3) |
O3—S1—O1 | 103.66 (16) | C11—C10—N1 | 117.8 (3) |
O2—S1—O1 | 108.38 (14) | C12—C11—C10 | 119.2 (3) |
O3—S1—C4 | 109.94 (16) | C12—C11—H11 | 120.4 |
O2—S1—C4 | 110.29 (17) | C10—C11—H11 | 120.4 |
O1—S1—C4 | 100.35 (15) | C11—C12—C13 | 121.4 (3) |
C1—O1—S1 | 117.6 (2) | C11—C12—H12 | 119.3 |
N2—N1—C1 | 109.5 (3) | C13—C12—H12 | 119.3 |
N2—N1—C10 | 120.0 (3) | C12—C13—C14 | 118.5 (3) |
C1—N1—C10 | 130.5 (3) | C12—C13—C16 | 121.3 (3) |
C2—N2—N1 | 105.8 (2) | C14—C13—C16 | 120.2 (3) |
O4—N3—O5 | 124.0 (3) | C15—C14—C13 | 120.9 (3) |
O4—N3—C7 | 118.5 (3) | C15—C14—H14 | 119.5 |
O5—N3—C7 | 117.4 (3) | C13—C14—H14 | 119.5 |
C3—C1—N1 | 109.4 (3) | C10—C15—C14 | 119.2 (3) |
C3—C1—O1 | 131.1 (3) | C10—C15—H15 | 120.4 |
N1—C1—O1 | 119.5 (3) | C14—C15—H15 | 120.4 |
N2—C2—C3 | 111.4 (3) | C13—C16—H16A | 109.5 |
N2—C2—C17 | 120.7 (3) | C13—C16—H16B | 109.5 |
C3—C2—C17 | 127.9 (3) | H16A—C16—H16B | 109.5 |
C1—C3—C2 | 103.9 (3) | C13—C16—H16C | 109.5 |
C1—C3—H3 | 128.0 | H16A—C16—H16C | 109.5 |
C2—C3—H3 | 128.0 | H16B—C16—H16C | 109.5 |
C9—C4—C5 | 122.5 (3) | C18—C17—C22 | 119.2 (3) |
C9—C4—S1 | 118.9 (3) | C18—C17—C2 | 121.3 (3) |
C5—C4—S1 | 118.5 (3) | C22—C17—C2 | 119.5 (3) |
C4—C5—C6 | 118.0 (3) | C19—C18—C17 | 120.7 (3) |
C4—C5—H5 | 121.0 | C19—C18—H18 | 119.7 |
C6—C5—H5 | 121.0 | C17—C18—H18 | 119.7 |
C7—C6—C5 | 119.1 (3) | C18—C19—C20 | 119.8 (3) |
C7—C6—H6 | 120.4 | C18—C19—H19 | 120.1 |
C5—C6—H6 | 120.4 | C20—C19—H19 | 120.1 |
C6—C7—C8 | 123.5 (3) | C21—C20—C19 | 119.9 (3) |
C6—C7—N3 | 118.9 (3) | C21—C20—H20 | 120.1 |
C8—C7—N3 | 117.6 (3) | C19—C20—H20 | 120.1 |
C7—C8—C9 | 117.5 (3) | C20—C21—C22 | 120.3 (3) |
C7—C8—H8 | 121.2 | C20—C21—H21 | 119.9 |
C9—C8—H8 | 121.2 | C22—C21—H21 | 119.9 |
C4—C9—C8 | 119.4 (3) | C21—C22—C17 | 120.1 (3) |
C4—C9—H9 | 120.3 | C21—C22—H22 | 119.9 |
C8—C9—H9 | 120.3 | C17—C22—H22 | 119.9 |
C15—C10—C11 | 120.7 (3) | ||
O3—S1—O1—C1 | 147.7 (2) | C6—C7—C8—C9 | 0.2 (6) |
O2—S1—O1—C1 | 17.0 (3) | N3—C7—C8—C9 | −179.7 (3) |
C4—S1—O1—C1 | −98.6 (2) | C5—C4—C9—C8 | 1.7 (5) |
C1—N1—N2—C2 | −0.7 (4) | S1—C4—C9—C8 | −174.2 (3) |
C10—N1—N2—C2 | 178.1 (3) | C7—C8—C9—C4 | −1.8 (5) |
N2—N1—C1—C3 | −0.5 (4) | N2—N1—C10—C15 | 153.3 (3) |
C10—N1—C1—C3 | −179.1 (3) | C1—N1—C10—C15 | −28.3 (6) |
N2—N1—C1—O1 | 178.0 (3) | N2—N1—C10—C11 | −26.9 (5) |
C10—N1—C1—O1 | −0.5 (6) | C1—N1—C10—C11 | 151.6 (4) |
S1—O1—C1—C3 | 69.1 (5) | C15—C10—C11—C12 | 0.9 (5) |
S1—O1—C1—N1 | −109.1 (3) | N1—C10—C11—C12 | −179.0 (3) |
N1—N2—C2—C3 | 1.5 (4) | C10—C11—C12—C13 | 0.4 (5) |
N1—N2—C2—C17 | −178.1 (3) | C11—C12—C13—C14 | −0.8 (5) |
N1—C1—C3—C2 | 1.3 (4) | C11—C12—C13—C16 | 177.2 (4) |
O1—C1—C3—C2 | −177.0 (4) | C12—C13—C14—C15 | 0.1 (5) |
N2—C2—C3—C1 | −1.8 (4) | C16—C13—C14—C15 | −177.9 (4) |
C17—C2—C3—C1 | 177.8 (3) | C11—C10—C15—C14 | −1.6 (5) |
O3—S1—C4—C9 | −162.3 (3) | N1—C10—C15—C14 | 178.2 (3) |
O2—S1—C4—C9 | −25.3 (3) | C13—C14—C15—C10 | 1.1 (5) |
O1—S1—C4—C9 | 88.9 (3) | N2—C2—C17—C18 | −171.6 (3) |
O3—S1—C4—C5 | 21.6 (4) | C3—C2—C17—C18 | 8.8 (5) |
O2—S1—C4—C5 | 158.7 (3) | N2—C2—C17—C22 | 7.8 (5) |
O1—S1—C4—C5 | −87.2 (3) | C3—C2—C17—C22 | −171.8 (3) |
C9—C4—C5—C6 | 0.2 (5) | C22—C17—C18—C19 | −1.9 (5) |
S1—C4—C5—C6 | 176.1 (3) | C2—C17—C18—C19 | 177.5 (3) |
C4—C5—C6—C7 | −1.8 (5) | C17—C18—C19—C20 | −0.4 (5) |
C5—C6—C7—C8 | 1.6 (6) | C18—C19—C20—C21 | 2.1 (6) |
C5—C6—C7—N3 | −178.4 (3) | C19—C20—C21—C22 | −1.5 (6) |
O4—N3—C7—C6 | 175.1 (4) | C20—C21—C22—C17 | −0.8 (5) |
O5—N3—C7—C6 | −5.4 (5) | C18—C17—C22—C21 | 2.5 (5) |
O4—N3—C7—C8 | −5.0 (5) | C2—C17—C22—C21 | −177.0 (3) |
O5—N3—C7—C8 | 174.5 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
C5—H5···O4i | 0.95 | 2.50 | 3.387 (5) | 155 |
Symmetry code: (i) x, −y+1/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C22H17N3O5S |
Mr | 435.46 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 120 |
a, b, c (Å) | 13.5339 (12), 10.4827 (10), 14.9303 (13) |
β (°) | 111.975 (3) |
V (Å3) | 1964.3 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.21 |
Crystal size (mm) | 0.58 × 0.38 × 0.04 |
Data collection | |
Diffractometer | Rigaku Saturn724+ |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2007) |
Tmin, Tmax | 0.620, 0.746 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4454, 4454, 3951 |
Rint | 0.000 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.069, 0.179, 1.19 |
No. of reflections | 4454 |
No. of parameters | 282 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.59, −0.62 |
Computer programs: DENZO (Otwinowski & Minor, 1997) and COLLECT (Hooft, 1998), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006), publCIF (Westrip, 2010).
D—H···A | D—H | H···A | D···A | D—H···A |
C5—H5···O4i | 0.95 | 2.50 | 3.387 (5) | 155 |
Symmetry code: (i) x, −y+1/2, z+1/2. |
Footnotes
‡Additional correspondence author, e-mail: j.wardell@abdn.ac.uk.
Acknowledgements
The use of the EPSRC X-ray crystallographic service at the University of Southampton, England, and the valuable assistance of the staff there is gratefully acknowledged. JLW acknowledges support from CAPES (Brazil). Support from the Ministry of Higher Education, Malaysia, High-Impact Research scheme (UM.C/HIR/MOHE/SC/12) is gratefully acknowledged.
References
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The structure of the title compound is now reported in continuation of related structural studies (Wardell et al. 2012; Baddeley et al., 2012).
In the title compound, Fig. 2, the pyrazole ring is planar with a r.m.s. deviation for the fitted atoms of 0.018 Å; the maximum deviations from this plane are 0.015 (1) Å (for the N1 atom) and -0.015 (1) Å (C8). The N– and C-bound benzene rings are inclined to this plane forming dihedral angles of 21.45 (10) and 6.96 (10)°, respectively; the dihedral angle between the benzene rings is 20.42 (10)° consistent with a non-planar molecule.
In the crystal, molecules are assembled into supramolecular layers in the bc plane via C—H···O, Table 1, and π—π interactions involving the sulfonamide benzene ring interacting with the N– and C-bound benzene rings {ring centroid···ring centroid distances = 3.790 (2) Å [angle of inclination = 0.96 (17)° for symmetry operation 1 - x, 1 - y, -z] and 3.730 (2) Å [angle of inclination = 10.02 (17)° for symmetry operation 1 - x, -1/2 + y, -1/2 - z], respectively}, Fig. 3. Layers stack along the a axis with no specific interactions between them, Fig. 4.