Abstract
In the title Schiff base complex, [Cu(C19H16Cl4N2O2)], the geometry around the CuII atom is distorted square-planar defined by the N2O2 donor atoms of the coordinated ligand. The dihedral angle between the substituted benzene rings is 29.95 (16)°. In the crystal, molecules are linked along the b axis, forming individual dimers through C—H⋯O interactions. The crystal structure is further stabilized by intermolecular π–π interactions [centroid–centroid distance = 3.6131 (17) Å].
Related literature
For standard values of bond lengths, see: Allen et al. (1987 ▶). For applications of Schiff bases in coordination chemistry, see, for example: Granovski et al. (1993 ▶); Blower (1998 ▶). For related structures see, for example: Ghaemi et al. (2011 ▶); Kargar et al. (2011 ▶, 2012 ▶).
Experimental
Crystal data
[Cu(C19H16Cl4N2O2)]
M r = 509.68
Monoclinic,
a = 12.4002 (10) Å
b = 8.4570 (7) Å
c = 20.0316 (19) Å
β = 97.278 (4)°
V = 2083.8 (3) Å3
Z = 4
Mo Kα radiation
μ = 1.58 mm−1
T = 291 K
0.25 × 0.18 × 0.09 mm
Data collection
Bruker SMART APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2005 ▶) T min = 0.694, T max = 0.871
18291 measured reflections
4988 independent reflections
2882 reflections with I > 2σ(I)
R int = 0.060
Refinement
R[F 2 > 2σ(F 2)] = 0.047
wR(F 2) = 0.105
S = 1.00
4988 reflections
255 parameters
H-atom parameters constrained
Δρmax = 0.38 e Å−3
Δρmin = −0.36 e Å−3
Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; 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 and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681200195X/hp2025sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681200195X/hp2025Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
---|---|---|---|---|
C8—H8A⋯O1i | 0.97 | 2.56 | 3.331 (4) | 136 |
Symmetry code: (i) .
Acknowledgments
HK and SA thank PNU for financial support. MNT thanks GC University of Sargodha, Pakistan for the research facilities.
supplementary crystallographic information
Comment
Schiff base complexes are one of the most important stereochemical models in transition metal coordination chemistry, with the ease of preparation and structural variations (Granovski et al., 1993; Blower et al., (1998). In continuation of our work on the crystal structure of Schiff base metal complexes (Kargar et al., 2012; Kargar et al., 2011; Ghaemi, et al., (2011), we determined the X-ray structure of the title compound.
The asymmetric unit of the title compound, Fig. 1, comprises a Schiff base complex. The bond lengths (Allen et al., 1987) and angles are within the normal ranges and are comparable to the related structure (Kargar et al., 2012; Kargar et al., 2011; Ghaemi, et al., (2011).
The geometry around CuII is a distorted square-planar which is supported by the N2O2 donor atoms of the coordinated Schiff base ligand. The dihedral angle between the substituted benzene rings is 29.95 (16)°. In the crystal structure the molecules are linked together along the b-axis, forming individual dimers through the intermolecular C—H···O interactions (Table 1, Fig. 2). The crystal structure is further stabilized by the intermolecular π-π interaction [Cg1···Cg1ii = 3.6131 (17)Å; (ii) 1 - X, 1- Y,-Z; Cg1 is the centroid of Cu(1)/O(2)/C(19)/C(14)/C(13)/N(2) ring].
Experimental
The title compound was synthesized by adding 3,5-dichloro-salicylaldehyde-2,2-dimethyl-1, 3-propanediamine (2 mmol) to a solution of CuCl2. 4H2O (2.1 mmol) in ethanol (30 ml). The mixture was refluxed with stirring for half an hour. The resultant solution was filtered. Dark-green single crystals of the title compound suitable for X-ray structure determination were recrystallized from ethanol by slow evaporation of the solvents at room temperature over several days.
Refinement
The H-atoms were included in calculated positions and treated as riding atoms: C—H = 0.93, 0.96 and 0.97 Å for CH, CH3 and CH2 H-atoms, respectively, with Uiso (H) = k x Ueq(C), where k = 1.5 for CH3 H-atoms, and k = 1.2 for all other H-atoms.
Figures
Fig. 1.
The ORTEP plot of the title compound, showing 40% probability displacement ellipsoids and the atomic numbering.
Fig. 2.
A part of the packing diagram of the title compound showing individual dimer formation through the intermolecular C—H···O intearctions (dashed lines). Only the H atoms involved in the interactions are shown.
Crystal data
[Cu(C19H16Cl4N2O2)] | F(000) = 1028 |
Mr = 509.68 | Dx = 1.625 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 2540 reflections |
a = 12.4002 (10) Å | θ = 2.5–27.4° |
b = 8.4570 (7) Å | µ = 1.58 mm−1 |
c = 20.0316 (19) Å | T = 291 K |
β = 97.278 (4)° | Block, dark-green |
V = 2083.8 (3) Å3 | 0.25 × 0.18 × 0.09 mm |
Z = 4 |
Data collection
Bruker SMART APEXII CCD area-detector diffractometer | 4988 independent reflections |
Radiation source: fine-focus sealed tube | 2882 reflections with I > 2σ(I) |
graphite | Rint = 0.060 |
φ and ω scans | θmax = 27.9°, θmin = 2.1° |
Absorption correction: multi-scan (SADABS; Bruker, 2005) | h = −16→14 |
Tmin = 0.694, Tmax = 0.871 | k = −9→11 |
18291 measured reflections | l = −26→26 |
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)] = 0.047 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.105 | H-atom parameters constrained |
S = 1.00 | w = 1/[σ2(Fo2) + (0.0376P)2] where P = (Fo2 + 2Fc2)/3 |
4988 reflections | (Δ/σ)max < 0.001 |
255 parameters | Δρmax = 0.38 e Å−3 |
0 restraints | Δρmin = −0.36 e Å−3 |
Special details
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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 | 0.5462 (3) | 0.8875 (4) | 0.14363 (17) | 0.0370 (8) | |
C2 | 0.6238 (3) | 0.9020 (4) | 0.20186 (18) | 0.0428 (9) | |
C3 | 0.6049 (3) | 0.9834 (4) | 0.25795 (18) | 0.0468 (9) | |
H3 | 0.6577 | 0.9874 | 0.2953 | 0.056* | |
C4 | 0.5058 (3) | 1.0605 (4) | 0.25883 (18) | 0.0486 (9) | |
C5 | 0.4286 (3) | 1.0532 (4) | 0.20422 (18) | 0.0430 (9) | |
H5 | 0.3629 | 1.1057 | 0.2051 | 0.052* | |
C6 | 0.4466 (3) | 0.9681 (4) | 0.14670 (17) | 0.0365 (8) | |
C7 | 0.3634 (3) | 0.9733 (4) | 0.08983 (17) | 0.0398 (8) | |
H7 | 0.3024 | 1.0343 | 0.0944 | 0.048* | |
C8 | 0.2764 (3) | 0.9331 (4) | −0.02093 (17) | 0.0442 (9) | |
H8A | 0.3077 | 0.9657 | −0.0607 | 0.053* | |
H8B | 0.2327 | 1.0201 | −0.0078 | 0.053* | |
C9 | 0.2022 (3) | 0.7905 (4) | −0.03888 (18) | 0.0414 (8) | |
C10 | 0.1184 (3) | 0.7758 (5) | 0.0105 (2) | 0.0725 (13) | |
H10A | 0.1548 | 0.7761 | 0.0557 | 0.109* | |
H10B | 0.0788 | 0.6788 | 0.0022 | 0.109* | |
H10C | 0.0689 | 0.8634 | 0.0045 | 0.109* | |
C11 | 0.1447 (3) | 0.8178 (5) | −0.1105 (2) | 0.0722 (13) | |
H11A | 0.0918 | 0.7361 | −0.1217 | 0.108* | |
H11B | 0.1973 | 0.8156 | −0.1418 | 0.108* | |
H11C | 0.1091 | 0.9188 | −0.1127 | 0.108* | |
C12 | 0.2678 (2) | 0.6363 (4) | −0.03537 (18) | 0.0436 (9) | |
H12A | 0.2730 | 0.5953 | 0.0101 | 0.052* | |
H12B | 0.2283 | 0.5593 | −0.0649 | 0.052* | |
C13 | 0.4035 (3) | 0.5747 (4) | −0.10521 (18) | 0.0411 (9) | |
H13 | 0.3483 | 0.5186 | −0.1305 | 0.049* | |
C14 | 0.5102 (3) | 0.5676 (4) | −0.12688 (18) | 0.0394 (8) | |
C15 | 0.5173 (3) | 0.4938 (4) | −0.18871 (19) | 0.0490 (10) | |
H15 | 0.4548 | 0.4545 | −0.2138 | 0.059* | |
C16 | 0.6153 (3) | 0.4793 (4) | −0.21236 (18) | 0.0505 (10) | |
C17 | 0.7093 (3) | 0.5351 (4) | −0.17506 (18) | 0.0464 (9) | |
H17 | 0.7761 | 0.5236 | −0.1910 | 0.056* | |
C18 | 0.7030 (2) | 0.6076 (4) | −0.11442 (17) | 0.0374 (8) | |
C19 | 0.6035 (2) | 0.6294 (4) | −0.08710 (17) | 0.0354 (8) | |
Cl1 | 0.74867 (8) | 0.80938 (13) | 0.20120 (6) | 0.0735 (4) | |
Cl2 | 0.48425 (9) | 1.16671 (15) | 0.33020 (6) | 0.0774 (4) | |
Cl3 | 0.62354 (9) | 0.38486 (16) | −0.28877 (6) | 0.0822 (4) | |
Cl4 | 0.82198 (6) | 0.67591 (10) | −0.06837 (5) | 0.0476 (2) | |
Cu1 | 0.48016 (3) | 0.76529 (5) | 0.01057 (2) | 0.03872 (14) | |
N1 | 0.3649 (2) | 0.9025 (3) | 0.03362 (14) | 0.0384 (7) | |
N2 | 0.37799 (19) | 0.6517 (3) | −0.05406 (14) | 0.0374 (7) | |
O1 | 0.57082 (17) | 0.8082 (3) | 0.09215 (12) | 0.0448 (6) | |
O2 | 0.60372 (17) | 0.6982 (3) | −0.02938 (12) | 0.0431 (6) |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0357 (19) | 0.035 (2) | 0.040 (2) | −0.0035 (15) | 0.0030 (16) | 0.0027 (16) |
C2 | 0.0335 (19) | 0.038 (2) | 0.055 (2) | 0.0000 (15) | −0.0015 (17) | 0.0029 (18) |
C3 | 0.048 (2) | 0.045 (2) | 0.045 (2) | −0.0118 (17) | −0.0026 (18) | 0.0024 (18) |
C4 | 0.050 (2) | 0.054 (2) | 0.042 (2) | −0.0112 (19) | 0.0095 (19) | −0.0025 (18) |
C5 | 0.040 (2) | 0.045 (2) | 0.045 (2) | 0.0019 (17) | 0.0106 (18) | 0.0005 (18) |
C6 | 0.0335 (19) | 0.036 (2) | 0.040 (2) | −0.0006 (15) | 0.0041 (16) | 0.0032 (16) |
C7 | 0.0345 (19) | 0.037 (2) | 0.049 (2) | 0.0021 (15) | 0.0108 (17) | 0.0023 (17) |
C8 | 0.046 (2) | 0.045 (2) | 0.040 (2) | 0.0141 (17) | −0.0017 (17) | 0.0079 (17) |
C9 | 0.0311 (18) | 0.047 (2) | 0.046 (2) | 0.0060 (15) | 0.0005 (16) | 0.0039 (17) |
C10 | 0.044 (2) | 0.084 (3) | 0.094 (4) | 0.007 (2) | 0.028 (2) | −0.004 (3) |
C11 | 0.070 (3) | 0.067 (3) | 0.070 (3) | 0.010 (2) | −0.027 (2) | −0.001 (2) |
C12 | 0.0301 (18) | 0.046 (2) | 0.055 (2) | −0.0014 (16) | 0.0085 (17) | 0.0046 (18) |
C13 | 0.0324 (19) | 0.036 (2) | 0.053 (2) | −0.0017 (15) | −0.0012 (17) | 0.0003 (17) |
C14 | 0.0326 (19) | 0.036 (2) | 0.049 (2) | 0.0016 (15) | 0.0036 (17) | −0.0009 (17) |
C15 | 0.040 (2) | 0.051 (2) | 0.055 (3) | −0.0033 (17) | 0.0005 (19) | −0.0141 (19) |
C16 | 0.044 (2) | 0.057 (2) | 0.052 (3) | −0.0002 (18) | 0.0116 (19) | −0.018 (2) |
C17 | 0.039 (2) | 0.048 (2) | 0.056 (2) | 0.0011 (17) | 0.0177 (19) | −0.0066 (19) |
C18 | 0.0329 (18) | 0.0348 (19) | 0.045 (2) | −0.0006 (14) | 0.0066 (16) | 0.0010 (16) |
C19 | 0.0337 (19) | 0.0294 (18) | 0.043 (2) | 0.0025 (14) | 0.0034 (16) | 0.0011 (16) |
Cl1 | 0.0471 (6) | 0.0767 (8) | 0.0895 (9) | 0.0202 (5) | −0.0185 (6) | −0.0163 (6) |
Cl2 | 0.0730 (8) | 0.1044 (9) | 0.0569 (7) | −0.0119 (7) | 0.0172 (6) | −0.0287 (6) |
Cl3 | 0.0600 (7) | 0.1171 (10) | 0.0709 (8) | −0.0016 (6) | 0.0130 (6) | −0.0493 (7) |
Cl4 | 0.0320 (5) | 0.0540 (6) | 0.0568 (6) | −0.0024 (4) | 0.0058 (4) | −0.0025 (5) |
Cu1 | 0.0315 (2) | 0.0416 (3) | 0.0435 (3) | 0.00221 (18) | 0.00652 (19) | −0.0001 (2) |
N1 | 0.0312 (15) | 0.0406 (17) | 0.0418 (18) | 0.0036 (12) | −0.0011 (13) | 0.0022 (14) |
N2 | 0.0293 (15) | 0.0356 (16) | 0.0481 (18) | −0.0012 (12) | 0.0086 (13) | 0.0008 (14) |
O1 | 0.0317 (13) | 0.0533 (15) | 0.0483 (16) | 0.0058 (11) | 0.0006 (11) | −0.0046 (12) |
O2 | 0.0321 (13) | 0.0509 (15) | 0.0469 (15) | −0.0002 (10) | 0.0073 (11) | −0.0083 (12) |
Geometric parameters (Å, °)
C1—O1 | 1.299 (4) | C11—H11A | 0.9600 |
C1—C6 | 1.418 (4) | C11—H11B | 0.9600 |
C1—C2 | 1.420 (4) | C11—H11C | 0.9600 |
C2—C3 | 1.362 (5) | C12—N2 | 1.467 (4) |
C2—Cl1 | 1.737 (3) | C12—H12A | 0.9700 |
C3—C4 | 1.394 (5) | C12—H12B | 0.9700 |
C3—H3 | 0.9300 | C13—N2 | 1.287 (4) |
C4—C5 | 1.360 (5) | C13—C14 | 1.444 (4) |
C4—Cl2 | 1.737 (4) | C13—H13 | 0.9300 |
C5—C6 | 1.400 (4) | C14—C15 | 1.399 (5) |
C5—H5 | 0.9300 | C14—C19 | 1.419 (4) |
C6—C7 | 1.437 (4) | C15—C16 | 1.365 (4) |
C7—N1 | 1.278 (4) | C15—H15 | 0.9300 |
C7—H7 | 0.9300 | C16—C17 | 1.385 (5) |
C8—N1 | 1.470 (4) | C16—Cl3 | 1.741 (3) |
C8—C9 | 1.532 (4) | C17—C18 | 1.372 (4) |
C8—H8A | 0.9700 | C17—H17 | 0.9300 |
C8—H8B | 0.9700 | C18—C19 | 1.424 (4) |
C9—C10 | 1.528 (5) | C18—Cl4 | 1.737 (3) |
C9—C12 | 1.534 (4) | C19—O2 | 1.294 (4) |
C9—C11 | 1.537 (5) | Cu1—O1 | 1.898 (2) |
C10—H10A | 0.9600 | Cu1—O2 | 1.903 (2) |
C10—H10B | 0.9600 | Cu1—N1 | 1.942 (3) |
C10—H10C | 0.9600 | Cu1—N2 | 1.947 (3) |
O1—C1—C6 | 125.2 (3) | H11A—C11—H11C | 109.5 |
O1—C1—C2 | 119.6 (3) | H11B—C11—H11C | 109.5 |
C6—C1—C2 | 115.2 (3) | N2—C12—C9 | 114.7 (3) |
C3—C2—C1 | 123.5 (3) | N2—C12—H12A | 108.6 |
C3—C2—Cl1 | 118.7 (3) | C9—C12—H12A | 108.6 |
C1—C2—Cl1 | 117.8 (3) | N2—C12—H12B | 108.6 |
C2—C3—C4 | 119.3 (3) | C9—C12—H12B | 108.6 |
C2—C3—H3 | 120.3 | H12A—C12—H12B | 107.6 |
C4—C3—H3 | 120.3 | N2—C13—C14 | 126.0 (3) |
C5—C4—C3 | 120.0 (3) | N2—C13—H13 | 117.0 |
C5—C4—Cl2 | 121.3 (3) | C14—C13—H13 | 117.0 |
C3—C4—Cl2 | 118.7 (3) | C15—C14—C19 | 121.5 (3) |
C4—C5—C6 | 121.1 (3) | C15—C14—C13 | 116.6 (3) |
C4—C5—H5 | 119.5 | C19—C14—C13 | 121.9 (3) |
C6—C5—H5 | 119.5 | C16—C15—C14 | 120.4 (3) |
C5—C6—C1 | 120.8 (3) | C16—C15—H15 | 119.8 |
C5—C6—C7 | 117.6 (3) | C14—C15—H15 | 119.8 |
C1—C6—C7 | 121.5 (3) | C15—C16—C17 | 120.5 (3) |
N1—C7—C6 | 126.5 (3) | C15—C16—Cl3 | 120.0 (3) |
N1—C7—H7 | 116.7 | C17—C16—Cl3 | 119.5 (3) |
C6—C7—H7 | 116.7 | C18—C17—C16 | 119.4 (3) |
N1—C8—C9 | 113.9 (3) | C18—C17—H17 | 120.3 |
N1—C8—H8A | 108.8 | C16—C17—H17 | 120.3 |
C9—C8—H8A | 108.8 | C17—C18—C19 | 123.2 (3) |
N1—C8—H8B | 108.8 | C17—C18—Cl4 | 118.6 (2) |
C9—C8—H8B | 108.8 | C19—C18—Cl4 | 118.2 (3) |
H8A—C8—H8B | 107.7 | O2—C19—C14 | 125.2 (3) |
C10—C9—C8 | 110.5 (3) | O2—C19—C18 | 119.9 (3) |
C10—C9—C12 | 107.6 (3) | C14—C19—C18 | 114.9 (3) |
C8—C9—C12 | 111.1 (3) | O1—Cu1—O2 | 89.91 (10) |
C10—C9—C11 | 110.1 (3) | O1—Cu1—N1 | 93.14 (11) |
C8—C9—C11 | 107.1 (3) | O2—Cu1—N1 | 159.14 (11) |
C12—C9—C11 | 110.6 (3) | O1—Cu1—N2 | 158.73 (10) |
C9—C10—H10A | 109.5 | O2—Cu1—N2 | 93.67 (10) |
C9—C10—H10B | 109.5 | N1—Cu1—N2 | 90.94 (11) |
H10A—C10—H10B | 109.5 | C7—N1—C8 | 118.7 (3) |
C9—C10—H10C | 109.5 | C7—N1—Cu1 | 125.7 (2) |
H10A—C10—H10C | 109.5 | C8—N1—Cu1 | 115.6 (2) |
H10B—C10—H10C | 109.5 | C13—N2—C12 | 119.3 (3) |
C9—C11—H11A | 109.5 | C13—N2—Cu1 | 125.0 (2) |
C9—C11—H11B | 109.5 | C12—N2—Cu1 | 115.0 (2) |
H11A—C11—H11B | 109.5 | C1—O1—Cu1 | 127.5 (2) |
C9—C11—H11C | 109.5 | C19—O2—Cu1 | 126.8 (2) |
O1—C1—C2—C3 | 179.8 (3) | C15—C14—C19—C18 | −1.1 (5) |
C6—C1—C2—C3 | 1.6 (5) | C13—C14—C19—C18 | 177.7 (3) |
O1—C1—C2—Cl1 | −0.7 (4) | C17—C18—C19—O2 | 179.7 (3) |
C6—C1—C2—Cl1 | −178.9 (2) | Cl4—C18—C19—O2 | −0.1 (4) |
C1—C2—C3—C4 | −1.5 (5) | C17—C18—C19—C14 | 1.1 (5) |
Cl1—C2—C3—C4 | 179.0 (3) | Cl4—C18—C19—C14 | −178.7 (2) |
C2—C3—C4—C5 | 0.4 (5) | C6—C7—N1—C8 | −174.7 (3) |
C2—C3—C4—Cl2 | −178.8 (3) | C6—C7—N1—Cu1 | 1.0 (5) |
C3—C4—C5—C6 | 0.5 (5) | C9—C8—N1—C7 | −112.5 (3) |
Cl2—C4—C5—C6 | 179.7 (3) | C9—C8—N1—Cu1 | 71.4 (3) |
C4—C5—C6—C1 | −0.3 (5) | O1—Cu1—N1—C7 | −5.6 (3) |
C4—C5—C6—C7 | −176.7 (3) | O2—Cu1—N1—C7 | −103.6 (4) |
O1—C1—C6—C5 | −178.7 (3) | N2—Cu1—N1—C7 | 153.5 (3) |
C2—C1—C6—C5 | −0.6 (5) | O1—Cu1—N1—C8 | 170.2 (2) |
O1—C1—C6—C7 | −2.5 (5) | O2—Cu1—N1—C8 | 72.2 (4) |
C2—C1—C6—C7 | 175.6 (3) | N2—Cu1—N1—C8 | −30.7 (2) |
C5—C6—C7—N1 | −179.3 (3) | C14—C13—N2—C12 | −174.9 (3) |
C1—C6—C7—N1 | 4.3 (5) | C14—C13—N2—Cu1 | −4.7 (5) |
N1—C8—C9—C10 | 81.1 (4) | C9—C12—N2—C13 | −118.0 (3) |
N1—C8—C9—C12 | −38.1 (4) | C9—C12—N2—Cu1 | 70.9 (3) |
N1—C8—C9—C11 | −159.0 (3) | O1—Cu1—N2—C13 | −103.4 (3) |
C10—C9—C12—N2 | −153.9 (3) | O2—Cu1—N2—C13 | −4.1 (3) |
C8—C9—C12—N2 | −33.0 (4) | N1—Cu1—N2—C13 | 155.5 (3) |
C11—C9—C12—N2 | 85.8 (4) | O1—Cu1—N2—C12 | 67.2 (4) |
N2—C13—C14—C15 | −172.0 (3) | O2—Cu1—N2—C12 | 166.4 (2) |
N2—C13—C14—C19 | 9.1 (5) | N1—Cu1—N2—C12 | −33.9 (2) |
C19—C14—C15—C16 | 0.1 (5) | C6—C1—O1—Cu1 | −4.6 (5) |
C13—C14—C15—C16 | −178.7 (3) | C2—C1—O1—Cu1 | 177.4 (2) |
C14—C15—C16—C17 | 1.0 (6) | O2—Cu1—O1—C1 | 166.7 (3) |
C14—C15—C16—Cl3 | 179.1 (3) | N1—Cu1—O1—C1 | 7.4 (3) |
C15—C16—C17—C18 | −1.0 (6) | N2—Cu1—O1—C1 | −93.3 (4) |
Cl3—C16—C17—C18 | −179.1 (3) | C14—C19—O2—Cu1 | −10.9 (5) |
C16—C17—C18—C19 | −0.1 (5) | C18—C19—O2—Cu1 | 170.7 (2) |
C16—C17—C18—Cl4 | 179.7 (3) | O1—Cu1—O2—C19 | 170.8 (3) |
C15—C14—C19—O2 | −179.6 (3) | N1—Cu1—O2—C19 | −90.6 (4) |
C13—C14—C19—O2 | −0.8 (5) | N2—Cu1—O2—C19 | 11.8 (3) |
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
C8—H8A···O1i | 0.97 | 2.56 | 3.331 (4) | 136 |
Symmetry codes: (i) −x+1, −y+2, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HP2025).
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/S160053681200195X/hp2025sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681200195X/hp2025Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report