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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2015 Jan 3;71(Pt 2):124–127. doi: 10.1107/S205698901402756X

Crystal structure of chlorido­{1-(2,3-dimethyl-5-oxido-1-phenyl-1H-pyrazol-2-ium-4-yl-κO)-2-[3-methyl-5-oxo-1-phenyl-4,5-di­hydro-1H-pyrazol-4-yl­idene-κO]hydrazin-1-ido-κN 1}copper(II) from laboratory X-ray powder data

Olga Kovalchukova a,*, Van Nguen a, Svetlana Strashnova a, Dmitry Kuznetsov b, Teimuraz Berikashvili c
PMCID: PMC4384589  PMID: 25878798

In the title copper(II) complex containing chloride and a derivative of 3-methyl-1-phenyl-4-hydrazopyrazolin-5-one, acting as a tridentate ligand, the CuII atom is in a slightly distorted square-planar coordination. Mol­ecules stack in columns along the c axis.

Keywords: crystal structure, azo­pyrazolone, copper complex, powder diffraction

Abstract

In the title compound, [Cu(C21H19N6O2)Cl], the CuII atom is in a slightly distorted square-planar coordination involving two O atoms from the pyrazolone rings [Cu—O = 2.088 (10) and 1.975 (10) Å], an N atom of the azo group [Cu—N = 2.048 (13) Å] and a chloride anion [Cu—Cl = 2.183 (5) Å]. The organic anions act as tridentate chelating ligands. The mol­ecules stack in columns along the c axis.

Chemical context  

Derivatives of 3-methyl-1-phenyl-4-hydrazopyrazolin-5-one and their metal complexes are well known dyes and possess a wide spectrum of biological activity (Wiley & Wiley, 2008; Liu et al., 2007; Hallas & Towns, 1996). Despite the fact that quite a number of metal complexes are known to exist, the determination of their crystal structures is rather problematic because of the high dispersity of azo-dyes. Only few of them have been structurally characterized (El-Hefnawy et al., 1992; Casas et al., 2007; Emeleus et al., 2001; Zaitseva et al., 1981; Kovalchukova et al., 2012; Bansse et al., 1997; Lalor et al., 1995). All of them show two similar coordination modes of the organic mol­ecules: bidentate chelating for those with no donating atoms in the aryl­azo fragment or tridentate chelating for ligands with an extra coordinating group.graphic file with name e-71-00124-scheme1.jpg

Structural commentary  

The central CuII atom is in a square-planar coordination (Fig. 1) by two O atoms from the pyrazolone rings, an N atom of the azo group, and a chloride anion. The coordination is slightly distorted in view of the two Cu—O bond lengths [2.088 (10) and 1.975 (10) Å], the Cu—Cl [2.183 (5) Å] and the Cu—N bond lengths [2.048 (13) Å]. The sum of the bond angles at the Cu atom [O10—Cu30—N15 = 90.9 (5), O10—Cu30—Cl31 94.0 (4), N15—Cu30—O20 = 83.0 (5), O20—Cu30—Cl31 92.0 (3)°] equals 359.9° which is indicative of the planarity of the CuII coordination. The organic anions act as tridentate chelating ligands. The N14—N15, N14—C13 and N15—C16 bond lengths [1.306 (17), 1.34 (2) and 1.39 (2) Å, respectively] are very close, thus indicating a strong conjunction of the two pyrazolone fragments which lie in one plane [maximum deviation 0.134 (13) Å for N14]. The benzene rings of the substituents are twisted around this plane by 83 (2) and 9(3)°.

Figure 1.

Figure 1

View of the title compound showing the atomic numbering. H atoms are omitted for clarity.

Supra­molecular features  

In the crystal, the mol­ecules are stacked in columns along the c axis in such a way that mol­ecules in neighboring columns at the same level are rotated by approximately 90° (Fig. 2). No Cu⋯Cu inter­actions between CuII atoms of neighboring mol­ecules are found.

Figure 2.

Figure 2

View of the crystal packing along the b axis.

Database survey  

The crystal structures of metal complexes with azo­pyrazolone derivatives are described by El–Hefnawy et al. (1992), Casas et al. (2007), Emeleus et al. (2001), Zaitseva et al. (1981), Kovalchukova et al. (2012), Bansse et al. (1997) and Lalor et al. (1995).

Synthesis and crystallization  

The title compound was prepared by mixing equimolar ethanol solutions of the organic ligand and copper(II) chloride. The reaction mixture was stirred under reflux for three hours. After cooling, fine brown needles of the title complex precipitated. These were then filtered off, washed using a small amount of ethanol and dried over P2O5.

Refinement details  

The X-ray powder diffraction data were collected using a Huber G670 Guinier camera (Cu-K α1 radiation, λ = 1.54059 Å) equipped with an image-plate detector. The monoclinic unit-cell dimensions were determined using three indexing programs: TREOR90 (Werner et al., 1985), ITO (Visser, 1969) and AUTOX (Zlokazov, 1992, 1995). Based on systematic extinctions, the space group was determined to be P21/c. The unit-cell parameters and space group were further tested using a Pawley (1981) fit and confirmed by the crystal structure solution.

The crystal structure was solved with the use of a simulated annealing technique (Zhukov et al., 2001). The initial mol­ecular model of the title complex was obtained using density functional theory (DFT) calculations in vacuo using the quantum-chemical code Priroda (Laikov, 1997, 2004, 2005; Laikov & Ustynyuk, 2005) employing the generalized-gradient approximation (GGA) and PBE exchange correlation function (Perdew et al., 1996). In simulated annealing runs (without H atoms), the total number of varied degrees of freedom (DOF) was eight: three translational, three orientational and two torsional ones for the rotation of the two phenyl rings. The solution was fitted with the program MRIA (Zlokazov & Chernyshev, 1992) in a bond-restrained Rietveld refinement using a split-type pseudo-Voigt peak-profile function (Toraya, 1986) and symmetrized harmonics expansion up to the 4th order (Ahtee et al., 1989; Järvinen, 1993) for the texture formalism. Restraints were applied to the intra­molecular bond lengths and contacts (< 2.8 Å) where the strength of the restraints was a function of inter­atomic separation and, for intra­molecular bond lengths, corresponded to an r.m.s. deviation of 0.02 Å. Additional restraints were applied to the planarity of aromatic rings with the attached atoms, with a maximum allowed deviation from the mean plane of 0.03 Å. All non-H atoms were refined isotropically. H atoms were positioned geometrically (C—H = 0.93–0.96 Å) and not refined. The experimental and calculated diffraction profile after the final bond-restrained Rietveld refinements is shown in Fig. 3. Crystal data, data collection and structure refinement details are summarized in Table 1.

Figure 3.

Figure 3

Final Rietveld plot. The experimental diffraction profile is indicated by black dots. The calculated diffraction profile is shown as the top red line, the difference profile is shown as the bottom blue line and the vertical green bars correspond to the positions of the Bragg reflections.

Table 1. Experimental details.

Crystal data
Chemical formula [Cu(C21H19N6O2)Cl]
M r 486.41
Crystal system, space group Monoclinic, P21/c
Temperature (K) 298
a, b, c () 15.1520(18), 22.1306(17), 6.7310(14)
() 101.80(2)
V (3) 2209.4(6)
Z 4
Radiation type Cu K 1, = 1.54059
(mm1) 2.76
Specimen shape, size (mm) Flat sheet, 15 1
 
Data collection
Diffractometer Guinier camera G670
Specimen mounting Thin layer in the specimen holder of the camera
Data collection mode Transmission
Scan method Continuous
2 values () 2min = 4.00, 2max = 75.00, 2step = 0.01
 
Refinement
R factors and goodness of fit R p = 0.019, R wp = 0.024, R exp = 0.019, R Bragg = 0.088, 2 = 1.734
No. of data points 7101
No. of parameters 155
No. of restraints 117
H-atom treatment H-atom parameters not refined

Computer programs: G670 Imaging Plate Guinier Camera Software (Huber, 2002), MRIA (Zlokazov Chernyshev, 1992), (Zhukov et al., 2001), PLATON (Spek, 2009), and SHELXL97 (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S205698901402756X/vn2088sup1.cif

e-71-00124-sup1.cif (272.5KB, cif)

Rietveld powder data: contains datablock(s) I. DOI: 10.1107/S205698901402756X/vn2088Isup2.rtv

e-71-00124-Isup2.rtv (236.1KB, rtv)

Supporting information file. DOI: 10.1107/S205698901402756X/vn2088Isup3.mol

Supporting information file. DOI: 10.1107/S205698901402756X/vn2088Isup4.mol

CCDC reference: 1040070

Additional supporting information: crystallographic information; 3D view; checkCIF report

Acknowledgments

The authors thank Dr V. V. Chernyshev (Lomonosov Moscow State University) for his kind assistance with the crystal structure determination. The research was supported by the Russian Foundation for Basic Research (grant 13–03–00079) and the Ministry of Education and Science of the Russian Federation (project 4.143.2014–K).

supplementary crystallographic information

Crystal data

[Cu(C21H19N6O2)Cl] F(000) = 996
Mr = 486.41 Dx = 1.462 Mg m3
Monoclinic, P21/c Cu Kα1 radiation, λ = 1.54059 Å
Hall symbol: -P 2ybc µ = 2.76 mm1
a = 15.1520 (18) Å T = 298 K
b = 22.1306 (17) Å Particle morphology: needle
c = 6.7310 (14) Å brown'
β = 101.80 (2)° flat sheet, 15 × 1 mm
V = 2209.4 (6) Å3 Specimen preparation: Prepared at 298 K and 101 kPa
Z = 4

Data collection

Guinier camera G670 diffractometer Data collection mode: transmission
Radiation source: line-focus sealed tube Scan method: continuous
Curved Germanium (111) monochromator min = 4.00°, 2θmax = 75.00°, 2θstep = 0.01°
Specimen mounting: thin layer in the specimen holder of the camera

Refinement

Refinement on Inet Profile function: split-type pseudo-Voigt (Toraya, 1986)
Least-squares matrix: full with fixed elements per cycle 155 parameters
Rp = 0.019 117 restraints
Rwp = 0.024 0 constraints
Rexp = 0.019 H-atom parameters not refined
RBragg = 0.088 Weighting scheme based on measured s.u.'s
χ2 = 1.734 (Δ/σ)max = 0.002
7101 data points Background function: Chebyshev polynomial up to the 5th order
Excluded region(s): none Preferred orientation correction: Symmetrized harmonics expansion up to the 4th order (Ahtee et al., 1989; Järvinen, 1993)

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
C1 0.5220 (10) 0.5094 (8) 0.264 (3) 0.094 (8)*
H1 0.4633 0.5001 0.2748 0.113*
C2 0.5471 (9) 0.5696 (8) 0.249 (3) 0.101 (9)*
H2 0.5048 0.6002 0.2453 0.121*
C3 0.5843 (10) 0.4630 (7) 0.262 (3) 0.103 (9)*
H3 0.5669 0.4228 0.2680 0.123*
C4 0.6367 (10) 0.5838 (8) 0.240 (3) 0.118 (9)*
C5 0.7003 (10) 0.5375 (7) 0.243 (3) 0.096 (8)*
H5 0.7599 0.5467 0.2398 0.115*
N6 0.6604 (8) 0.6455 (6) 0.225 (2) 0.105 (6)*
C7 0.7447 (11) 0.6707 (8) 0.238 (3) 0.107 (9)*
C8 0.6730 (9) 0.4775 (8) 0.252 (3) 0.098 (8)*
H8 0.7145 0.4466 0.2509 0.117*
N9 0.5931 (9) 0.6898 (6) 0.206 (2) 0.119 (7)*
O10 0.8175 (6) 0.6407 (5) 0.2551 (17) 0.087 (5)*
C11 0.6328 (11) 0.7427 (8) 0.206 (2) 0.110 (8)*
C12 0.5804 (10) 0.8000 (7) 0.191 (3) 0.091 (9)*
H12A 0.5176 0.7909 0.1805 0.136*
H12B 0.5882 0.8220 0.0731 0.136*
H12C 0.6015 0.8240 0.3102 0.136*
C13 0.7285 (10) 0.7352 (7) 0.224 (2) 0.093 (9)*
N14 0.7885 (8) 0.7798 (6) 0.226 (2) 0.089 (6)*
N15 0.8735 (8) 0.7646 (6) 0.2574 (19) 0.101 (7)*
C16 0.9368 (10) 0.8107 (8) 0.279 (3) 0.106 (9)*
C17 1.0271 (10) 0.7878 (7) 0.304 (3) 0.095 (9)*
C18 0.9411 (9) 0.8733 (8) 0.288 (3) 0.101 (9)*
N19 1.0839 (8) 0.8384 (6) 0.327 (2) 0.093 (7)*
O20 1.0518 (6) 0.7337 (5) 0.3047 (16) 0.094 (6)*
N21 1.0321 (8) 0.8895 (6) 0.319 (2) 0.104 (7)*
C22 0.8697 (10) 0.9203 (8) 0.268 (3) 0.099 (8)*
H22A 0.8971 0.9596 0.2829 0.149*
H22B 0.8354 0.9145 0.3720 0.149*
H22C 0.8306 0.9171 0.1373 0.149*
C23 1.1789 (10) 0.8343 (7) 0.394 (3) 0.106 (9)*
C24 1.2315 (10) 0.8204 (7) 0.251 (3) 0.097 (9)*
H24 1.2047 0.8152 0.1148 0.116*
C25 1.0666 (10) 0.9483 (7) 0.346 (3) 0.095 (9)*
H25A 1.1311 0.9470 0.3641 0.143*
H25B 1.0502 0.9661 0.4631 0.143*
H25C 1.0421 0.9720 0.2280 0.143*
C26 1.2192 (11) 0.8450 (7) 0.598 (3) 0.111 (9)*
H26 1.1841 0.8549 0.6911 0.133*
C27 1.3248 (10) 0.8145 (7) 0.316 (3) 0.098 (9)*
H27 1.3601 0.8038 0.2238 0.118*
C28 1.3126 (10) 0.8405 (7) 0.658 (3) 0.108 (9)*
H28 1.3400 0.8482 0.7924 0.130*
C29 1.3654 (11) 0.8246 (7) 0.519 (3) 0.110 (9)*
H29 1.4275 0.8207 0.5619 0.132*
Cu30 0.93520 (16) 0.68180 (13) 0.2845 (5) 0.0760 (14)*
Cl31 1.0116 (3) 0.5976 (2) 0.3067 (8) 0.084 (2)*

Geometric parameters (Å, º)

C1—C2 1.40 (2) C16—C17 1.44 (2)
C1—C3 1.40 (2) C17—O20 1.255 (19)
C1—H1 0.93 C17—N19 1.40 (2)
C2—C4 1.41 (2) C18—N21 1.398 (18)
C2—H2 0.93 C18—C22 1.49 (2)
C3—C8 1.40 (2) N19—N21 1.372 (18)
C3—H3 0.93 N19—C23 1.420 (19)
C4—C5 1.40 (2) O20—Cu30 2.088 (10)
C4—N6 1.42 (2) N21—C25 1.40 (2)
C5—C8 1.40 (2) C22—H22A 0.96
C5—H5 0.93 C22—H22B 0.96
N6—C7 1.38 (2) C22—H22C 0.96
N6—N9 1.401 (19) C23—C24 1.40 (3)
C7—O10 1.27 (2) C23—C26 1.40 (3)
C7—C13 1.45 (2) C24—C27 1.40 (2)
C8—H8 0.93 C24—H24 0.93
N9—C11 1.32 (2) C25—H25A 0.96
O10—Cu30 1.975 (10) C25—H25B 0.96
C11—C13 1.44 (2) C25—H25C 0.96
C11—C12 1.49 (2) C26—C28 1.39 (2)
C12—H12A 0.96 C26—H26 0.93
C12—H12B 0.96 C27—C29 1.40 (3)
C12—H12C 0.96 C27—H27 0.93
C13—N14 1.34 (2) C28—C29 1.39 (3)
N14—N15 1.306 (17) C28—H28 0.93
N15—C16 1.39 (2) C29—H29 0.93
N15—Cu30 2.048 (13) Cu30—Cl31 2.183 (5)
C16—C18 1.39 (2)
C2—C1—C3 120.5 (15) N19—C17—C16 106.3 (13)
C2—C1—H1 119.7 C16—C18—N21 107.4 (13)
C3—C1—H1 119.8 C16—C18—C22 131.9 (14)
C1—C2—C4 119.7 (15) N21—C18—C22 120.7 (14)
C1—C2—H2 120.1 N21—N19—C17 108.7 (12)
C4—C2—H2 120.1 N21—N19—C23 126.9 (12)
C1—C3—C8 119.4 (15) C17—N19—C23 122.9 (13)
C1—C3—H3 120.3 C17—O20—Cu30 106.1 (9)
C8—C3—H3 120.3 N19—N21—C18 109.5 (12)
C5—C4—C2 120.1 (16) N19—N21—C25 124.4 (12)
C5—C4—N6 121.3 (14) C18—N21—C25 126.1 (13)
C2—C4—N6 118.6 (15) C18—C22—H22A 109.5
C8—C5—C4 119.1 (15) C18—C22—H22B 109.5
C8—C5—H5 120.5 H22A—C22—H22B 109.4
C4—C5—H5 120.4 C18—C22—H22C 109.5
C7—N6—N9 111.7 (13) H22A—C22—H22C 109.5
C7—N6—C4 128.9 (13) H22B—C22—H22C 109.4
N9—N6—C4 119.3 (12) C24—C23—C26 120.8 (15)
O10—C7—N6 124.7 (15) C24—C23—N19 118.6 (15)
O10—C7—C13 130.7 (15) C26—C23—N19 120.6 (16)
N6—C7—C13 104.6 (13) C27—C24—C23 119.0 (17)
C5—C8—C3 121.1 (15) C27—C24—H24 120.5
C5—C8—H8 119.4 C23—C24—H24 120.5
C3—C8—H8 119.5 N21—C25—H25A 109.5
C11—N9—N6 107.4 (13) N21—C25—H25B 109.5
C7—O10—Cu30 121.1 (10) H25A—C25—H25B 109.5
N9—C11—C13 110.5 (15) N21—C25—H25C 109.5
N9—C11—C12 121.3 (14) H25A—C25—H25C 109.4
C13—C11—C12 128.2 (15) H25B—C25—H25C 109.5
C11—C12—H12A 109.5 C28—C26—C23 119.1 (17)
C11—C12—H12B 109.5 C28—C26—H26 120.4
H12A—C12—H12B 109.5 C23—C26—H26 120.5
C11—C12—H12C 109.5 C24—C27—C29 120.5 (18)
H12A—C12—H12C 109.5 C24—C27—H27 119.8
H12B—C12—H12C 109.5 C29—C27—H27 119.8
N14—C13—C11 125.8 (15) C29—C28—C26 120.7 (16)
N14—C13—C7 128.3 (14) C29—C28—H28 119.7
C11—C13—C7 105.9 (14) C26—C28—H28 119.7
N15—N14—C13 117.2 (13) C28—C29—C27 119.9 (14)
N14—N15—C16 117.7 (13) C28—C29—H29 120.1
N14—N15—Cu30 131.5 (10) C27—C29—H29 120.1
C16—N15—Cu30 110.8 (10) O10—Cu30—N15 90.9 (5)
N15—C16—C18 139.8 (15) O10—Cu30—O20 173.8 (4)
N15—C16—C17 112.0 (14) N15—Cu30—O20 83.0 (5)
C18—C16—C17 108.2 (14) O10—Cu30—Cl31 94.0 (4)
O20—C17—N19 125.9 (13) N15—Cu30—Cl31 174.8 (4)
O20—C17—C16 127.9 (14) O20—Cu30—Cl31 92.0 (3)

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) I, global. DOI: 10.1107/S205698901402756X/vn2088sup1.cif

e-71-00124-sup1.cif (272.5KB, cif)

Rietveld powder data: contains datablock(s) I. DOI: 10.1107/S205698901402756X/vn2088Isup2.rtv

e-71-00124-Isup2.rtv (236.1KB, rtv)

Supporting information file. DOI: 10.1107/S205698901402756X/vn2088Isup3.mol

Supporting information file. DOI: 10.1107/S205698901402756X/vn2088Isup4.mol

CCDC reference: 1040070

Additional supporting information: crystallographic information; 3D view; checkCIF report


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