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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Mar 7;68(Pt 4):o969. doi: 10.1107/S1600536812009166

4-[(Z)-(n-Butyl­amino)(phenyl)methyl­idene]-3-methyl-1-phenyl-1H-pyrazol-5(4H)-one

Hai-Wen Wang a,*
PMCID: PMC3343944  PMID: 22590025

Abstract

The title compound, C21H23N3O, exists in an enamine–keto form with the amino group involved in an intra­molecular N—H⋯O hydrogen bond. The dihedral angle between the phenyl rings is 73.59 (6)°. The five-membered ring is nearly planar, the largest deviation being 0.0004 (7) Å, and makes dihedral angles of 4.81 (6) and 69.81 (5)° wth the phenyl rings. In the crystal, pairs of weak C—H⋯O inter­actions link the mol­ecules into centrosymmetric dimers.

Related literature  

For applications of Schiff bases derived from 4-acyl­pyrazolo­nes, see: Bernardino et al. (2006); Zhang et al. (2008). For related structures, see: Zhang et al. (2007); Chi et al. (2010); Zhen & Han (2005); Wang (2010).graphic file with name e-68-0o969-scheme1.jpg

Experimental  

Crystal data  

  • C21H23N3O

  • M r = 333.42

  • Monoclinic, Inline graphic

  • a = 9.5215 (9) Å

  • b = 14.7867 (14) Å

  • c = 12.8055 (12) Å

  • β = 100.645 (2)°

  • V = 1771.9 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 296 K

  • 0.28 × 0.20 × 0.16 mm

Data collection  

  • Bruker SMART 1000 CCD diffractometer

  • 16506 measured reflections

  • 4368 independent reflections

  • 3362 reflections with I > 2σ(I)

  • R int = 0.035

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.040

  • wR(F 2) = 0.103

  • S = 1.01

  • 4368 reflections

  • 232 parameters

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

  • Δρmax = 0.30 e Å−3

  • Δρmin = −0.20 e Å−3

Data collection: SMART (Bruker, 2001); cell refinement: SAINT-Plus (Bruker, 2003); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812009166/cv5252sup1.cif

e-68-0o969-sup1.cif (20.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812009166/cv5252Isup2.hkl

e-68-0o969-Isup2.hkl (214.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812009166/cv5252Isup3.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—H3A⋯O1 0.921 (16) 1.873 (16) 2.6704 (14) 143.5 (14)
C13—H13⋯O1i 0.93 2.39 3.3175 (15) 172

Symmetry code: (i) Inline graphic.

Acknowledgments

This work was supported by the College of Chemistry and Mol­ecular Engineering, East China University of Science and Technology.

supplementary crystallographic information

Comment

The Schiff bases derived from 4-acylpyrazolones have attracted much attention due to their applications in pharmaceutical and agrochemical fields (e.g. Bernardino et al., 2006; Zhang et al., 2008). In order to expand this field, we now report the synthesis and structure of the title compound, (I) (Fig. 1).

In (I), the Schiff base molecule adopts an E geometry with respect to the C=N bond (Fig. 1). All bond lengths and angles are comparable with those found in the related compounds (Chi et al., 2010; Wang et al., 2010; Zhen et al., 2005; Zhang et al.., 2007). The dihedral angle between the two phenyl rings is 73.59 (6)°. The five-membered ring of the title compound is nearly planar, with the largest deviation being 0.0004 (7)%A for atom N1. The dihedral angles between this mean plane and two benzene rings are 4.81 (6)° and 69.81 (5)%. Weak intermolecular C—H···O interactions (Table 1) link the molecules into centrosymmetric dimers.

Experimental

A mixture of a 10 ml HPMBP (2 mmol, 0.5566 g) anhydrous ethanol solution, and a 0.2 ml n-butylamine (2 mmol, 0.1463 g) solution was refluxed for ca 8 h, with addition of a few drops of glacial acetic acid as a catalyst. The ethanol was removed by evaporation and the resulting green precipitate formed was filtered off, washed with cold anhydrous ethanol and dried in air. Yellow block single crystals suitable for analysis were obtained by slow evaporation of a solution in anhydrous ethanol at room temperature for a few days.

Refinement

The H3A atom bonded to N3 was located in a difference map and isotropically refined. C-bound H atoms were placed in calculated positions, with C—H = 0.93-0.97 Å, and refined as riding, with Uiso(H)=1.2-1.5 Ueq (C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing the atomic numbering and 30% probability displacement ellipsoids. Dashed line denotes hydrogen bond.

Crystal data

C21H23N3O F(000) = 712.0
Mr = 333.42 Dx = 1.250 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 3753 reflections
a = 9.5215 (9) Å θ = 2.6–28.1°
b = 14.7867 (14) Å µ = 0.08 mm1
c = 12.8055 (12) Å T = 296 K
β = 100.645 (2)° Block, yellow
V = 1771.9 (3) Å3 0.28 × 0.20 × 0.16 mm
Z = 4

Data collection

Bruker SMART 1000 CCD diffractometer 3362 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.035
Graphite monochromator θmax = 28.3°, θmin = 2.6°
phi and ω scans h = −12→12
16506 measured reflections k = −19→19
4368 independent reflections l = −17→16

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)] = 0.040 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103 H atoms treated by a mixture of independent and constrained refinement
S = 1.01 w = 1/[σ2(Fo2) + (0.0499P)2 + 0.4177P] where P = (Fo2 + 2Fc2)/3
4368 reflections (Δ/σ)max < 0.001
232 parameters Δρmax = 0.30 e Å3
0 restraints Δρmin = −0.20 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.
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)

x y z Uiso*/Ueq
C1 0.21783 (12) 0.26068 (9) 0.88837 (9) 0.0167 (2)
C2 0.10538 (13) 0.21696 (9) 0.92399 (9) 0.0204 (3)
H2 0.1013 0.1541 0.9255 0.024*
C3 −0.00037 (13) 0.26856 (9) 0.95714 (10) 0.0218 (3)
H3 −0.0742 0.2397 0.9824 0.026*
C4 0.00239 (13) 0.36198 (9) 0.95320 (9) 0.0218 (3)
H4 −0.0699 0.3957 0.9744 0.026*
C5 0.11413 (13) 0.40483 (9) 0.91726 (10) 0.0220 (3)
H5 0.1166 0.4676 0.9144 0.026*
C6 0.22209 (13) 0.35488 (9) 0.88561 (9) 0.0193 (3)
H6 0.2973 0.3842 0.8626 0.023*
C7 0.35303 (12) 0.11883 (8) 0.85902 (9) 0.0158 (2)
C8 0.48777 (12) 0.10785 (8) 0.82441 (9) 0.0159 (2)
C9 0.53156 (12) 0.19778 (8) 0.80232 (9) 0.0168 (2)
C10 0.66208 (13) 0.22991 (9) 0.76371 (10) 0.0217 (3)
H10A 0.6553 0.2136 0.6904 0.033*
H10B 0.7453 0.2023 0.8052 0.033*
H10C 0.6693 0.2945 0.7708 0.033*
C11 0.55372 (12) 0.02287 (8) 0.82705 (9) 0.0152 (2)
C12 0.69661 (12) 0.00963 (8) 0.79819 (9) 0.0153 (2)
C13 0.81099 (13) −0.01709 (9) 0.87666 (9) 0.0185 (3)
H13 0.7970 −0.0279 0.9456 0.022*
C14 0.94570 (13) −0.02752 (9) 0.85151 (10) 0.0221 (3)
H14 1.0223 −0.0446 0.9038 0.027*
C15 0.96628 (13) −0.01252 (9) 0.74855 (10) 0.0228 (3)
H15 1.0567 −0.0195 0.7319 0.027*
C16 0.85241 (14) 0.01285 (9) 0.67051 (10) 0.0212 (3)
H16 0.8663 0.0221 0.6013 0.025*
C17 0.71793 (13) 0.02451 (8) 0.69496 (9) 0.0179 (2)
H17 0.6419 0.0423 0.6425 0.021*
C18 0.53117 (13) −0.14295 (8) 0.85933 (9) 0.0177 (2)
H18A 0.6204 −0.1519 0.9088 0.021*
H18B 0.5456 −0.1600 0.7889 0.021*
C19 0.41494 (13) −0.20109 (8) 0.89147 (9) 0.0172 (2)
H19A 0.4043 −0.1852 0.9631 0.021*
H19B 0.3250 −0.1886 0.8444 0.021*
C20 0.44787 (13) −0.30125 (9) 0.88723 (10) 0.0197 (3)
H20A 0.5401 −0.3132 0.9316 0.024*
H20B 0.4540 −0.3177 0.8149 0.024*
C21 0.33508 (15) −0.35963 (9) 0.92449 (11) 0.0262 (3)
H21A 0.3317 −0.3456 0.9972 0.039*
H21B 0.3589 −0.4223 0.9188 0.039*
H21C 0.2435 −0.3478 0.8810 0.039*
H3A 0.4031 (17) −0.0341 (11) 0.8798 (12) 0.030 (4)*
N1 0.32840 (10) 0.21097 (7) 0.85512 (8) 0.0172 (2)
N2 0.43854 (10) 0.25859 (7) 0.82022 (8) 0.0182 (2)
N3 0.48854 (11) −0.04789 (7) 0.85966 (8) 0.0172 (2)
O1 0.27412 (9) 0.06007 (6) 0.88848 (7) 0.0195 (2)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0156 (5) 0.0187 (6) 0.0152 (5) 0.0023 (5) 0.0014 (4) −0.0004 (4)
C2 0.0197 (6) 0.0187 (6) 0.0231 (6) 0.0020 (5) 0.0050 (5) 0.0022 (5)
C3 0.0188 (6) 0.0255 (7) 0.0219 (6) 0.0013 (5) 0.0058 (5) 0.0014 (5)
C4 0.0203 (6) 0.0251 (7) 0.0204 (6) 0.0061 (5) 0.0048 (5) −0.0026 (5)
C5 0.0249 (6) 0.0175 (7) 0.0234 (6) 0.0020 (5) 0.0042 (5) −0.0032 (5)
C6 0.0189 (6) 0.0180 (6) 0.0209 (6) −0.0008 (5) 0.0034 (4) −0.0002 (5)
C7 0.0163 (5) 0.0158 (6) 0.0149 (5) −0.0001 (5) 0.0019 (4) 0.0002 (4)
C8 0.0150 (5) 0.0171 (6) 0.0157 (5) −0.0013 (4) 0.0034 (4) 0.0005 (4)
C9 0.0165 (5) 0.0171 (6) 0.0167 (5) −0.0003 (5) 0.0026 (4) 0.0004 (4)
C10 0.0200 (6) 0.0174 (6) 0.0293 (6) −0.0020 (5) 0.0088 (5) 0.0009 (5)
C11 0.0156 (5) 0.0171 (6) 0.0128 (5) −0.0014 (5) 0.0019 (4) 0.0000 (4)
C12 0.0154 (5) 0.0129 (6) 0.0184 (5) −0.0009 (4) 0.0050 (4) −0.0011 (4)
C13 0.0184 (6) 0.0186 (6) 0.0188 (5) −0.0011 (5) 0.0042 (4) 0.0005 (5)
C14 0.0162 (6) 0.0213 (7) 0.0282 (6) −0.0001 (5) 0.0024 (5) 0.0004 (5)
C15 0.0170 (6) 0.0209 (7) 0.0333 (7) −0.0030 (5) 0.0116 (5) −0.0056 (5)
C16 0.0261 (6) 0.0189 (6) 0.0208 (6) −0.0054 (5) 0.0106 (5) −0.0040 (5)
C17 0.0197 (6) 0.0159 (6) 0.0183 (5) −0.0023 (5) 0.0038 (4) −0.0010 (5)
C18 0.0181 (5) 0.0142 (6) 0.0216 (5) 0.0010 (5) 0.0055 (4) 0.0006 (5)
C19 0.0181 (5) 0.0159 (6) 0.0182 (5) −0.0007 (5) 0.0051 (4) 0.0012 (4)
C20 0.0218 (6) 0.0153 (6) 0.0224 (6) −0.0006 (5) 0.0047 (5) 0.0012 (5)
C21 0.0324 (7) 0.0190 (7) 0.0283 (6) −0.0056 (6) 0.0087 (5) 0.0008 (5)
N1 0.0159 (5) 0.0149 (5) 0.0218 (5) 0.0002 (4) 0.0064 (4) 0.0020 (4)
N2 0.0164 (5) 0.0168 (5) 0.0226 (5) −0.0020 (4) 0.0068 (4) 0.0016 (4)
N3 0.0165 (5) 0.0142 (5) 0.0224 (5) 0.0007 (4) 0.0073 (4) 0.0009 (4)
O1 0.0180 (4) 0.0168 (5) 0.0252 (4) −0.0018 (3) 0.0082 (3) 0.0018 (3)

Geometric parameters (Å, º)

C1—C6 1.3942 (18) C12—C13 1.3956 (16)
C1—C2 1.3975 (17) C13—C14 1.3876 (17)
C1—N1 1.4125 (15) C13—H13 0.9300
C2—C3 1.3906 (18) C14—C15 1.3861 (18)
C2—H2 0.9300 C14—H14 0.9300
C3—C4 1.3827 (19) C15—C16 1.3838 (18)
C3—H3 0.9300 C15—H15 0.9300
C4—C5 1.3879 (19) C16—C17 1.3840 (17)
C4—H4 0.9300 C16—H16 0.9300
C5—C6 1.3858 (18) C17—H17 0.9300
C5—H5 0.9300 C18—N3 1.4633 (16)
C6—H6 0.9300 C18—C19 1.5171 (16)
C7—O1 1.2516 (15) C18—H18A 0.9700
C7—N1 1.3819 (16) C18—H18B 0.9700
C7—C8 1.4418 (16) C19—C20 1.5169 (17)
C8—C11 1.4023 (17) C19—H19A 0.9700
C8—C9 1.4373 (17) C19—H19B 0.9700
C9—N2 1.3117 (16) C20—C21 1.5218 (18)
C9—C10 1.4971 (16) C20—H20A 0.9700
C10—H10A 0.9600 C20—H20B 0.9700
C10—H10B 0.9600 C21—H21A 0.9600
C10—H10C 0.9600 C21—H21B 0.9600
C11—N3 1.3230 (15) C21—H21C 0.9600
C11—C12 1.4872 (16) N1—N2 1.4030 (14)
C12—C17 1.3914 (16) N3—H3A 0.921 (16)
C6—C1—C2 119.87 (11) C15—C14—H14 119.9
C6—C1—N1 119.04 (11) C13—C14—H14 119.9
C2—C1—N1 121.09 (11) C16—C15—C14 120.05 (11)
C3—C2—C1 119.18 (13) C16—C15—H15 120.0
C3—C2—H2 120.4 C14—C15—H15 120.0
C1—C2—H2 120.4 C15—C16—C17 120.31 (11)
C4—C3—C2 121.15 (12) C15—C16—H16 119.8
C4—C3—H3 119.4 C17—C16—H16 119.8
C2—C3—H3 119.4 C16—C17—C12 119.91 (11)
C3—C4—C5 119.28 (12) C16—C17—H17 120.0
C3—C4—H4 120.4 C12—C17—H17 120.0
C5—C4—H4 120.4 N3—C18—C19 109.09 (10)
C6—C5—C4 120.60 (13) N3—C18—H18A 109.9
C6—C5—H5 119.7 C19—C18—H18A 109.9
C4—C5—H5 119.7 N3—C18—H18B 109.9
C5—C6—C1 119.90 (12) C19—C18—H18B 109.9
C5—C6—H6 120.0 H18A—C18—H18B 108.3
C1—C6—H6 120.0 C20—C19—C18 112.19 (10)
O1—C7—N1 126.02 (11) C20—C19—H19A 109.2
O1—C7—C8 129.22 (12) C18—C19—H19A 109.2
N1—C7—C8 104.75 (10) C20—C19—H19B 109.2
C11—C8—C9 133.54 (11) C18—C19—H19B 109.2
C11—C8—C7 120.89 (11) H19A—C19—H19B 107.9
C9—C8—C7 105.26 (10) C19—C20—C21 112.34 (11)
N2—C9—C8 111.72 (11) C19—C20—H20A 109.1
N2—C9—C10 117.95 (11) C21—C20—H20A 109.1
C8—C9—C10 130.33 (11) C19—C20—H20B 109.1
C9—C10—H10A 109.5 C21—C20—H20B 109.1
C9—C10—H10B 109.5 H20A—C20—H20B 107.9
H10A—C10—H10B 109.5 C20—C21—H21A 109.5
C9—C10—H10C 109.5 C20—C21—H21B 109.5
H10A—C10—H10C 109.5 H21A—C21—H21B 109.5
H10B—C10—H10C 109.5 C20—C21—H21C 109.5
N3—C11—C8 118.83 (11) H21A—C21—H21C 109.5
N3—C11—C12 118.58 (11) H21B—C21—H21C 109.5
C8—C11—C12 122.56 (11) C7—N1—N2 111.99 (9)
C17—C12—C13 119.83 (11) C7—N1—C1 129.28 (10)
C17—C12—C11 121.06 (10) N2—N1—C1 118.52 (10)
C13—C12—C11 119.10 (10) C9—N2—N1 106.27 (10)
C14—C13—C12 119.75 (11) C11—N3—C18 127.75 (10)
C14—C13—H13 120.1 C11—N3—H3A 113.8 (10)
C12—C13—H13 120.1 C18—N3—H3A 118.3 (10)
C15—C14—C13 120.14 (11)
C6—C1—C2—C3 −0.55 (16) C11—C12—C13—C14 −178.40 (11)
N1—C1—C2—C3 179.27 (10) C12—C13—C14—C15 −0.77 (19)
C1—C2—C3—C4 1.43 (17) C13—C14—C15—C16 0.0 (2)
C2—C3—C4—C5 −1.14 (18) C14—C15—C16—C17 0.8 (2)
C3—C4—C5—C6 −0.03 (18) C15—C16—C17—C12 −0.76 (19)
C4—C5—C6—C1 0.89 (17) C13—C12—C17—C16 −0.06 (18)
C2—C1—C6—C5 −0.60 (17) C11—C12—C17—C16 179.14 (11)
N1—C1—C6—C5 179.59 (10) N3—C18—C19—C20 176.92 (9)
O1—C7—C8—C11 −4.43 (18) C18—C19—C20—C21 177.25 (10)
N1—C7—C8—C11 174.38 (10) O1—C7—N1—N2 178.95 (10)
O1—C7—C8—C9 −178.92 (11) C8—C7—N1—N2 0.09 (12)
N1—C7—C8—C9 −0.11 (11) O1—C7—N1—C1 4.41 (19)
C11—C8—C9—N2 −173.37 (12) C8—C7—N1—C1 −174.45 (10)
C7—C8—C9—N2 0.10 (13) C6—C1—N1—C7 174.10 (11)
C11—C8—C9—C10 6.6 (2) C2—C1—N1—C7 −5.72 (17)
C7—C8—C9—C10 −179.93 (11) C6—C1—N1—N2 −0.14 (15)
C9—C8—C11—N3 174.20 (12) C2—C1—N1—N2 −179.96 (10)
C7—C8—C11—N3 1.54 (16) C8—C9—N2—N1 −0.04 (12)
C9—C8—C11—C12 −3.62 (19) C10—C9—N2—N1 179.98 (9)
C7—C8—C11—C12 −176.27 (10) C7—N1—N2—C9 −0.03 (12)
N3—C11—C12—C17 116.65 (13) C1—N1—N2—C9 175.16 (9)
C8—C11—C12—C17 −65.53 (16) C8—C11—N3—C18 173.83 (11)
N3—C11—C12—C13 −64.14 (15) C12—C11—N3—C18 −8.27 (17)
C8—C11—C12—C13 113.67 (13) C19—C18—N3—C11 −173.20 (11)
C17—C12—C13—C14 0.82 (18)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N3—H3A···O1 0.921 (16) 1.873 (16) 2.6704 (14) 143.5 (14)
C13—H13···O1i 0.93 2.39 3.3175 (15) 172

Symmetry code: (i) −x+1, −y, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV5252).

References

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  3. Bruker (2003). SAINT-Plus Bruker AXS Inc., Madison, Wisconsin, USA.
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  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
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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) I, global. DOI: 10.1107/S1600536812009166/cv5252sup1.cif

e-68-0o969-sup1.cif (20.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812009166/cv5252Isup2.hkl

e-68-0o969-Isup2.hkl (214.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812009166/cv5252Isup3.cml

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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