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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Mar 17;68(Pt 4):o1086–o1087. doi: 10.1107/S1600536812010598

1-(4-Methyl­phen­yl)-3-phenyl-1H-pyrazol-5-yl 4-nitro­benzene­sulfonate

Solange M S V Wardell a, Edward R T Tiekink b,*, James L Wardell c,
PMCID: PMC3344041  PMID: 22589950

Abstract

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 merohedral 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).graphic file with name e-68-o1086-scheme1.jpg

Experimental  

Crystal data  

  • C22H17N3O5S

  • M r = 435.46

  • Monoclinic, Inline graphic

  • a = 13.5339 (12) Å

  • b = 10.4827 (10) Å

  • c = 14.9303 (13) Å

  • β = 111.975 (3)°

  • V = 1964.3 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.21 mm−1

  • T = 120 K

  • 0.58 × 0.38 × 0.04 mm

Data collection  

  • Rigaku Saturn724+ diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2007) T min = 0.620, T max = 0.746

  • 4454 measured reflections

  • 4454 independent reflections

  • 3951 reflections with I > 2σ(I)

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.069

  • wR(F 2) = 0.179

  • S = 1.19

  • 4454 reflections

  • 282 parameters

  • H-atom parameters constrained

  • Δρmax = 0.59 e Å−3

  • Δρmin = −0.62 e Å−3

Data collection: COLLECT (Hooft, 1998); cell refinement: 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).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812010598/hb6674sup1.cif

e-68-o1086-sup1.cif (21.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812010598/hb6674Isup2.hkl

e-68-o1086-Isup2.hkl (213.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812010598/hb6674Isup3.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
C5—H5⋯O4i 0.95 2.50 3.387 (5) 155

Symmetry code: (i) Inline graphic.

Acknowledgments

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.

supplementary crystallographic information

Comment

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.

Experimental

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.

Refinement

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 refinement. 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).

Figures

Fig. 1.

Fig. 1.

Reaction scheme. For further details see Baddeley et al. (2012).

Fig. 2.

Fig. 2.

The molecular structure of (I) showing displacement ellipsoids at the 50% probability level.

Fig. 3.

Fig. 3.

Supramolecular layer in the bc plane in (I) sustained by C—H···O and π—π interactions shown as orange and purple dashed lines, respectively.

Fig. 4.

Fig. 4.

A view in projection down the c axis of the crystal packing in (I) showing the stacking of layers. The C—H···O, and π—π interactions are shown as orange and purple dashed lines, respectively.

Crystal data

C22H17N3O5S F(000) = 904
Mr = 435.46 Dx = 1.472 Mg m3
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 mm1
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

Data collection

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

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 Å3
0 restraints Δρmin = −0.62 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
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*

Atomic displacement parameters (Å2)

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)

Geometric parameters (Å, º)

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)

Hydrogen-bond geometry (Å, º)

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

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB6674).

References

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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/S1600536812010598/hb6674sup1.cif

e-68-o1086-sup1.cif (21.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812010598/hb6674Isup2.hkl

e-68-o1086-Isup2.hkl (213.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812010598/hb6674Isup3.cml

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


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