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Three new diclofenac-based copper(II) complexes, namely tetra­kis­{μ-2-[2-(2,6-di­chloro­anilino)phen­yl]acetato-κ2O:O′}bis­(methanol-κO)copper(II), [Cu2(μ-dicl)4(CH3OH)2] (1), bis­{2-[2-(2,6-di­chloro­anilino)phen­yl]acetato-κ2O,O′}bis­(1-vinyl-1H-imidazole-κN3)copper(II), [Cu(dicl)2(vim)2] (2), and bis­{2-[2-(2,6-di­chloro­anilino)phen­yl]acetato-κ2O,O′}bis­(1H-imidazole-κN3)copper(II), [Cu(dicl)2(im)2] (3) [dicl is diclofenac (C14H10Cl2NO2), vim is 1-vinyl­imidazole (C5H6N2) and im is imidazole (C3H4N2)], have been synthesized and char­ac­ter­ized by elemental analysis, FT–IR spectroscopy, thermal analysis and single-crystal X-ray diffraction. X-ray diffraction analysis shows that complex 1 consists of dimeric units in which the dicl ligand exhibits a bidentate syn,syn2 coordination mode linking two copper(II) centres. Complexes 2 and 3 have mononuclear units with the general formula [Cu(dicl)2L2] (L is vim or im) in which the CuII ions are octa­hedrally coordinated by two L and two dicl chelating ligands. The L and dicl ligands both occupy the trans positions of the coordination octa­hedron. The different coordination modes of dicl in the title complexes were revealed by Fourier transform IR (FT–IR) spectroscopy. The spin matching between the copper(II) centres in the dimeric [Cu2(μ-dicl)4(CH3OH)2] units was also confirmed by magnetic data to be lower than the spin-only value and electron paramagnetic resonance (EPR) spectra. The thermal properties of the complexes were investigated by thermogravimetric (TG) and differential thermal analysis (DTA) techniques.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229619001827/qf3021sup1.cif
Contains datablocks 1, 2, 3, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229619001827/qf30211sup2.hkl
Contains datablock 1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229619001827/qf30212sup3.hkl
Contains datablock 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229619001827/qf30213sup4.hkl
Contains datablock 3

CCDC references: 1558159; 1557904; 1555961

Computing details top

For all structures, data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA (Stoe & Cie, 2002); data reduction: X-RED32 (Stoe & Cie, 2002). Program(s) used to solve structure: SHELXT (Sheldrick, 2015a) for (1); SHELXT (Sheldrick, 2015b) for (2), (3). Program(s) used to refine structure: SHELXL (Sheldrick, 2015b) for (1); SHELXL (Sheldrick, 2015a) for (2), (3). For all structures, molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: WinGX (Farrugia, 2012) and PLATON (Spek, 2009).

Tetrakis{µ-2-[2-(2,6-dichloroanilino)phenyl]acetato-κ2O:O'}bis(methanol-κO)copper(II) (1) top
Crystal data top
[Cu2(C14H10Cl2NO2)4(CH4O)2]Z = 1
Mr = 1371.68F(000) = 698
Triclinic, P1Dx = 1.534 Mg m3
a = 10.5258 (5) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.9908 (6) ÅCell parameters from 18832 reflections
c = 13.0098 (7) Åθ = 1.7–27.6°
α = 113.097 (4)°µ = 1.14 mm1
β = 90.217 (4)°T = 296 K
γ = 99.529 (4)°Prism, blue
V = 1485.26 (14) Å30.62 × 0.48 × 0.24 mm
Data collection top
Stoe IPDS 2
diffractometer
6511 independent reflections
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus5112 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.049
Detector resolution: 6.67 pixels mm-1θmax = 27.0°, θmin = 1.7°
rotation method scansh = 1313
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
k = 1415
Tmin = 0.523, Tmax = 0.799l = 1616
17101 measured reflections
Refinement top
Refinement on F26 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.035H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.092 w = 1/[σ2(Fo2) + (0.0514P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.98(Δ/σ)max = 0.002
6511 reflectionsΔρmax = 0.37 e Å3
381 parametersΔρmin = 0.31 e Å3
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cu10.62472 (2)0.52584 (2)1.00611 (2)0.03371 (8)
Cl40.83375 (8)0.08701 (8)0.89976 (7)0.0768 (2)
Cl30.85861 (10)0.30347 (8)0.78876 (8)0.0866 (3)
Cl20.16436 (11)0.59749 (10)0.76281 (7)0.0937 (3)
Cl10.35861 (10)0.36461 (9)0.36844 (8)0.0894 (3)
O40.62230 (15)0.36876 (14)1.01926 (13)0.0455 (4)
O30.40678 (15)0.32667 (14)1.01186 (14)0.0489 (4)
O20.60524 (15)0.43459 (15)0.84294 (12)0.0470 (4)
O10.38967 (15)0.39115 (15)0.83091 (12)0.0483 (4)
O50.83487 (16)0.5793 (2)1.01673 (17)0.0632 (5)
N20.73925 (19)0.1329 (2)0.89084 (18)0.0531 (5)
C140.4971 (2)0.3826 (2)0.79014 (17)0.0396 (5)
C150.5167 (2)0.30170 (19)1.01925 (16)0.0378 (4)
N10.3130 (2)0.4168 (2)0.6095 (2)0.0598 (6)
C170.5110 (2)0.07874 (19)0.90659 (18)0.0372 (4)
C160.5230 (2)0.1793 (2)1.02367 (18)0.0411 (5)
H16A0.4537540.1590351.0658350.049*
H16B0.6044800.1845191.0618920.049*
C230.8557 (2)0.1087 (2)0.84249 (19)0.0456 (5)
C220.6184 (2)0.0558 (2)0.84408 (18)0.0404 (5)
C120.3755 (2)0.2299 (2)0.60337 (17)0.0449 (5)
C180.3916 (2)0.0066 (2)0.8594 (2)0.0459 (5)
H180.3188170.0223340.8992590.055*
C70.2868 (2)0.2867 (2)0.57186 (18)0.0465 (5)
C130.5015 (2)0.3034 (2)0.66690 (18)0.0512 (6)
H13A0.5388080.3566210.6304940.061*
H13B0.5597610.2465670.6604370.061*
C280.9269 (2)0.1854 (2)0.7973 (2)0.0504 (5)
C190.3787 (2)0.0882 (2)0.7544 (2)0.0530 (6)
H190.2979050.1357460.7241020.064*
C50.1809 (3)0.5699 (3)0.6232 (2)0.0587 (6)
C60.2517 (2)0.4810 (2)0.5613 (2)0.0529 (6)
C210.6051 (2)0.0404 (2)0.7394 (2)0.0515 (6)
H210.6771870.0568970.6988580.062*
C261.1011 (2)0.0759 (3)0.7665 (2)0.0648 (8)
H261.1831820.0657560.7426380.078*
C80.1751 (3)0.2163 (3)0.5065 (2)0.0578 (6)
H80.1166840.2542850.4841930.069*
C110.3481 (3)0.1035 (2)0.5707 (2)0.0592 (7)
H110.4062410.0644570.5919200.071*
C240.9129 (2)0.0131 (2)0.8444 (2)0.0509 (6)
C251.0338 (3)0.0035 (3)0.8074 (2)0.0631 (7)
H251.0693560.0682780.8103270.076*
C200.4853 (2)0.1121 (2)0.6949 (2)0.0539 (6)
H200.4770390.1766260.6245570.065*
C100.2349 (3)0.0339 (3)0.5067 (2)0.0701 (9)
H100.2170880.0509500.4859630.084*
C90.1501 (3)0.0903 (3)0.4743 (2)0.0672 (8)
H90.0750180.0435750.4302260.081*
C40.1240 (3)0.6380 (3)0.5780 (3)0.0665 (7)
H40.0772150.6965160.6220450.080*
C20.2059 (3)0.5318 (3)0.4029 (3)0.0672 (7)
H2A0.2132370.5175110.3277710.081*
C271.0482 (2)0.1701 (3)0.7604 (2)0.0598 (7)
H271.0935330.2235000.7316720.072*
C10.2645 (3)0.4657 (3)0.4498 (2)0.0588 (6)
C30.1369 (3)0.6188 (3)0.4680 (3)0.0708 (8)
H30.0989570.6644780.4371150.085*
C290.8947 (3)0.6347 (4)0.9482 (3)0.0878 (11)
H29A0.9865900.6515990.9642860.132*
H29B0.8736670.5800210.8709470.132*
H29C0.8646630.7103740.9623410.132*
H50.8831 (14)0.547 (3)1.043 (3)0.132*
H20.736 (3)0.2071 (16)0.916 (2)0.052 (8)*
H10.331 (3)0.454 (3)0.6791 (15)0.077 (10)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.03398 (13)0.03066 (14)0.03555 (13)0.00819 (9)0.00045 (9)0.01130 (9)
Cl40.0804 (5)0.0800 (5)0.0909 (5)0.0253 (4)0.0235 (4)0.0519 (4)
Cl30.1045 (6)0.0685 (5)0.1028 (6)0.0282 (5)0.0185 (5)0.0461 (5)
Cl20.1157 (7)0.1037 (7)0.0583 (4)0.0344 (6)0.0115 (4)0.0229 (4)
Cl10.1132 (7)0.0830 (6)0.0783 (5)0.0383 (5)0.0316 (5)0.0307 (4)
O40.0436 (8)0.0412 (9)0.0582 (9)0.0112 (7)0.0043 (7)0.0254 (7)
O30.0452 (9)0.0382 (9)0.0683 (10)0.0124 (7)0.0058 (7)0.0246 (8)
O20.0437 (8)0.0525 (10)0.0386 (8)0.0105 (7)0.0010 (6)0.0109 (7)
O10.0447 (8)0.0552 (10)0.0356 (7)0.0105 (7)0.0000 (6)0.0076 (7)
O50.0385 (9)0.0749 (13)0.0740 (12)0.0005 (8)0.0022 (8)0.0313 (10)
N20.0361 (10)0.0439 (12)0.0644 (13)0.0075 (9)0.0095 (9)0.0057 (10)
C140.0476 (12)0.0379 (11)0.0350 (10)0.0125 (9)0.0000 (9)0.0145 (9)
C150.0480 (12)0.0335 (11)0.0345 (10)0.0139 (9)0.0059 (8)0.0138 (8)
N10.0709 (14)0.0472 (13)0.0554 (13)0.0080 (10)0.0193 (11)0.0153 (10)
C170.0393 (10)0.0313 (11)0.0477 (11)0.0117 (8)0.0046 (8)0.0208 (9)
C160.0487 (12)0.0379 (12)0.0449 (11)0.0146 (9)0.0098 (9)0.0224 (9)
C230.0335 (10)0.0512 (14)0.0456 (12)0.0073 (9)0.0025 (9)0.0126 (10)
C220.0353 (10)0.0394 (12)0.0490 (12)0.0107 (8)0.0048 (9)0.0186 (9)
C120.0544 (13)0.0484 (14)0.0293 (10)0.0114 (10)0.0067 (9)0.0120 (9)
C180.0370 (11)0.0439 (13)0.0615 (14)0.0111 (9)0.0069 (10)0.0245 (11)
C70.0509 (13)0.0460 (13)0.0364 (11)0.0026 (10)0.0003 (9)0.0123 (9)
C130.0507 (13)0.0593 (15)0.0365 (11)0.0160 (11)0.0016 (9)0.0092 (10)
C280.0482 (13)0.0500 (14)0.0471 (12)0.0042 (10)0.0011 (10)0.0149 (10)
C190.0419 (12)0.0467 (14)0.0656 (15)0.0043 (10)0.0077 (11)0.0189 (12)
C50.0548 (14)0.0571 (16)0.0571 (15)0.0049 (12)0.0042 (11)0.0172 (12)
C60.0513 (13)0.0453 (14)0.0575 (14)0.0023 (10)0.0104 (11)0.0183 (11)
C210.0488 (13)0.0506 (14)0.0505 (13)0.0149 (11)0.0098 (10)0.0128 (11)
C260.0381 (12)0.101 (2)0.0523 (14)0.0188 (14)0.0104 (11)0.0254 (15)
C80.0516 (14)0.0666 (17)0.0464 (13)0.0000 (12)0.0052 (10)0.0176 (12)
C110.0881 (19)0.0490 (15)0.0388 (12)0.0160 (13)0.0077 (12)0.0142 (10)
C240.0475 (12)0.0590 (15)0.0493 (13)0.0159 (11)0.0077 (10)0.0225 (11)
C250.0524 (14)0.086 (2)0.0571 (15)0.0340 (14)0.0074 (12)0.0262 (14)
C200.0578 (14)0.0459 (14)0.0488 (13)0.0129 (11)0.0042 (11)0.0078 (11)
C100.105 (2)0.0441 (15)0.0469 (14)0.0068 (15)0.0107 (15)0.0107 (12)
C90.0717 (18)0.0671 (19)0.0435 (13)0.0172 (15)0.0014 (12)0.0133 (13)
C40.0573 (16)0.0557 (17)0.081 (2)0.0137 (13)0.0056 (14)0.0207 (14)
C20.0735 (18)0.0695 (19)0.0615 (16)0.0029 (15)0.0080 (14)0.0332 (14)
C270.0485 (13)0.0768 (19)0.0476 (13)0.0029 (13)0.0061 (11)0.0235 (13)
C10.0620 (16)0.0539 (16)0.0586 (15)0.0072 (12)0.0007 (12)0.0215 (12)
C30.0716 (19)0.068 (2)0.082 (2)0.0105 (15)0.0123 (16)0.0405 (16)
C290.076 (2)0.091 (3)0.078 (2)0.0196 (18)0.0110 (17)0.0284 (18)
Geometric parameters (Å, º) top
Cu1—O3i1.9519 (16)C18—H180.9300
Cu1—O41.9532 (15)C7—C81.385 (3)
Cu1—O21.9610 (15)C13—H13A0.9700
Cu1—O1i1.9764 (15)C13—H13B0.9700
Cu1—O52.1866 (17)C28—C271.380 (4)
Cu1—Cu1i2.5854 (5)C19—C201.371 (4)
Cl4—C241.734 (3)C19—H190.9300
Cl3—C281.729 (3)C5—C41.381 (4)
Cl2—C51.729 (3)C5—C61.390 (4)
Cl1—C11.723 (3)C6—C11.399 (4)
O4—C151.260 (3)C21—C201.381 (4)
O3—C151.254 (3)C21—H210.9300
O2—C141.256 (3)C26—C251.366 (4)
O1—C141.254 (3)C26—C271.368 (4)
O5—C291.401 (4)C26—H260.9300
O5—H50.829 (9)C8—C91.378 (4)
N2—C231.401 (3)C8—H80.9300
N2—C221.417 (3)C11—C101.388 (4)
N2—H20.824 (17)C11—H110.9300
C14—C131.515 (3)C24—C251.380 (3)
C15—C161.503 (3)C25—H250.9300
N1—C61.393 (3)C20—H200.9300
N1—C71.417 (3)C10—C91.360 (5)
N1—H10.842 (17)C10—H100.9300
C17—C181.387 (3)C9—H90.9300
C17—C221.396 (3)C4—C31.369 (4)
C17—C161.516 (3)C4—H40.9300
C16—H16A0.9700C2—C31.376 (4)
C16—H16B0.9700C2—C11.386 (4)
C23—C241.388 (3)C2—H2A0.9300
C23—C281.398 (3)C27—H270.9300
C22—C211.385 (3)C3—H30.9300
C12—C111.383 (4)C29—H29A0.9600
C12—C71.389 (3)C29—H29B0.9600
C12—C131.501 (3)C29—H29C0.9600
C18—C191.381 (3)
O3i—Cu1—O4169.60 (6)C14—C13—H13B108.1
O3i—Cu1—O290.02 (7)H13A—C13—H13B107.3
O4—Cu1—O287.92 (7)C27—C28—C23122.4 (2)
O3i—Cu1—O1i89.46 (7)C27—C28—Cl3119.8 (2)
O4—Cu1—O1i90.76 (7)C23—C28—Cl3117.78 (19)
O2—Cu1—O1i169.70 (6)C20—C19—C18119.9 (2)
O3i—Cu1—O593.77 (7)C20—C19—H19120.1
O4—Cu1—O596.57 (7)C18—C19—H19120.1
O2—Cu1—O595.55 (7)C4—C5—C6122.7 (3)
O1i—Cu1—O594.74 (7)C4—C5—Cl2118.5 (2)
O3i—Cu1—Cu1i83.20 (5)C6—C5—Cl2118.8 (2)
O4—Cu1—Cu1i86.46 (5)C5—C6—N1121.9 (2)
O2—Cu1—Cu1i84.89 (5)C5—C6—C1116.0 (2)
O1i—Cu1—Cu1i84.84 (5)N1—C6—C1122.0 (3)
O5—Cu1—Cu1i176.95 (6)C20—C21—C22120.4 (2)
C15—O4—Cu1120.47 (14)C20—C21—H21119.8
C15—O3—Cu1i124.41 (15)C22—C21—H21119.8
C14—O2—Cu1122.47 (14)C25—C26—C27120.3 (2)
C14—O1—Cu1i121.76 (13)C25—C26—H26119.9
C29—O5—Cu1121.02 (19)C27—C26—H26119.9
C29—O5—H5114.2 (12)C9—C8—C7120.4 (3)
Cu1—O5—H5121.4 (12)C9—C8—H8119.8
C23—N2—C22122.94 (19)C7—C8—H8119.8
C23—N2—H2111.7 (19)C12—C11—C10120.9 (3)
C22—N2—H2113.6 (19)C12—C11—H11119.5
O1—C14—O2125.66 (19)C10—C11—H11119.5
O1—C14—C13119.10 (19)C25—C24—C23122.6 (2)
O2—C14—C13115.24 (19)C25—C24—Cl4117.8 (2)
O3—C15—O4125.4 (2)C23—C24—Cl4119.54 (18)
O3—C15—C16117.42 (19)C26—C25—C24119.6 (3)
O4—C15—C16117.11 (19)C26—C25—H25120.2
C6—N1—C7123.4 (2)C24—C25—H25120.2
C6—N1—H1115 (2)C19—C20—C21120.0 (2)
C7—N1—H1113 (2)C19—C20—H20120.0
C18—C17—C22118.5 (2)C21—C20—H20120.0
C18—C17—C16120.05 (19)C9—C10—C11119.8 (3)
C22—C17—C16121.48 (19)C9—C10—H10120.1
C15—C16—C17110.75 (17)C11—C10—H10120.1
C15—C16—H16A109.5C10—C9—C8120.2 (3)
C17—C16—H16A109.5C10—C9—H9119.9
C15—C16—H16B109.5C8—C9—H9119.9
C17—C16—H16B109.5C3—C4—C5119.6 (3)
H16A—C16—H16B108.1C3—C4—H4120.2
C24—C23—C28115.6 (2)C5—C4—H4120.2
C24—C23—N2122.3 (2)C3—C2—C1119.8 (3)
C28—C23—N2121.9 (2)C3—C2—H2A120.1
C21—C22—C17120.0 (2)C1—C2—H2A120.1
C21—C22—N2121.8 (2)C26—C27—C28119.5 (3)
C17—C22—N2118.24 (19)C26—C27—H27120.3
C11—C12—C7118.7 (2)C28—C27—H27120.3
C11—C12—C13120.5 (2)C2—C1—C6121.8 (3)
C7—C12—C13120.7 (2)C2—C1—Cl1118.6 (2)
C19—C18—C17121.2 (2)C6—C1—Cl1119.6 (2)
C19—C18—H18119.4C4—C3—C2120.0 (3)
C17—C18—H18119.4C4—C3—H3120.0
C8—C7—C12120.0 (2)C2—C3—H3120.0
C8—C7—N1121.6 (2)O5—C29—H29A109.5
C12—C7—N1118.4 (2)O5—C29—H29B109.5
C12—C13—C14116.90 (19)H29A—C29—H29B109.5
C12—C13—H13A108.1O5—C29—H29C109.5
C14—C13—H13A108.1H29A—C29—H29C109.5
C12—C13—H13B108.1H29B—C29—H29C109.5
Cu1i—O1—C14—O27.9 (3)C4—C5—C6—N1177.3 (3)
Cu1i—O1—C14—C13171.88 (16)Cl2—C5—C6—N12.2 (4)
Cu1—O2—C14—O17.0 (3)C4—C5—C6—C11.2 (4)
Cu1—O2—C14—C13172.79 (16)Cl2—C5—C6—C1178.2 (2)
Cu1i—O3—C15—O42.0 (3)C7—N1—C6—C5121.3 (3)
Cu1i—O3—C15—C16175.29 (13)C7—N1—C6—C162.9 (4)
Cu1—O4—C15—O30.4 (3)C17—C22—C21—C201.8 (4)
Cu1—O4—C15—C16176.91 (13)N2—C22—C21—C20178.4 (2)
O3—C15—C16—C1784.8 (2)C12—C7—C8—C91.3 (4)
O4—C15—C16—C1792.8 (2)N1—C7—C8—C9177.8 (2)
C18—C17—C16—C1595.1 (2)C7—C12—C11—C100.7 (4)
C22—C17—C16—C1585.2 (2)C13—C12—C11—C10176.5 (2)
C22—N2—C23—C2471.7 (3)C28—C23—C24—C251.9 (4)
C22—N2—C23—C28113.5 (3)N2—C23—C24—C25173.1 (2)
C18—C17—C22—C212.6 (3)C28—C23—C24—Cl4179.45 (17)
C16—C17—C22—C21177.0 (2)N2—C23—C24—Cl44.4 (3)
C18—C17—C22—N2177.5 (2)C27—C26—C25—C241.0 (4)
C16—C17—C22—N22.8 (3)C23—C24—C25—C260.4 (4)
C23—N2—C22—C218.4 (4)Cl4—C24—C25—C26177.9 (2)
C23—N2—C22—C17171.4 (2)C18—C19—C20—C210.8 (4)
C22—C17—C18—C191.8 (3)C22—C21—C20—C190.0 (4)
C16—C17—C18—C19177.9 (2)C12—C11—C10—C90.7 (4)
C11—C12—C7—C81.7 (3)C11—C10—C9—C81.2 (4)
C13—C12—C7—C8175.4 (2)C7—C8—C9—C100.1 (4)
C11—C12—C7—N1177.5 (2)C6—C5—C4—C30.1 (4)
C13—C12—C7—N15.4 (3)Cl2—C5—C4—C3179.3 (2)
C6—N1—C7—C818.3 (4)C25—C26—C27—C280.8 (4)
C6—N1—C7—C12162.5 (2)C23—C28—C27—C260.9 (4)
C11—C12—C13—C14107.3 (3)Cl3—C28—C27—C26179.4 (2)
C7—C12—C13—C1475.6 (3)C3—C2—C1—C62.5 (5)
O1—C14—C13—C125.7 (3)C3—C2—C1—Cl1176.0 (2)
O2—C14—C13—C12174.2 (2)C5—C6—C1—C22.4 (4)
C24—C23—C28—C272.2 (3)N1—C6—C1—C2178.4 (3)
N2—C23—C28—C27172.9 (2)C5—C6—C1—Cl1176.1 (2)
C24—C23—C28—Cl3178.11 (18)N1—C6—C1—Cl10.0 (4)
N2—C23—C28—Cl36.8 (3)C5—C4—C3—C20.2 (5)
C17—C18—C19—C200.1 (4)C1—C2—C3—C41.3 (5)
Symmetry code: (i) x+1, y+1, z+2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C29—H29A···Cl2ii0.963.153.701 (3)119
N2—H2···O40.82 (2)2.40 (2)3.125 (3)148 (2)
N1—H1···O10.84 (2)2.48 (3)3.132 (3)135 (3)
Symmetry code: (ii) x+1, y, z.
Bis{2-[2-(2,6-dichloroanilino)phenyl]acetato-κ2O,O'}bis(1-vinyl-1H-imidazole-κN3)copper(II) (2) top
Crystal data top
[Cu(C14H10Cl2NO2)2(C5H6N2)2]F(000) = 862
Mr = 842.03Dx = 1.441 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 15.1741 (7) ÅCell parameters from 12318 reflections
b = 7.9241 (2) Åθ = 1.7–27.1°
c = 16.3037 (8) ŵ = 0.89 mm1
β = 98.073 (4)°T = 296 K
V = 1940.95 (14) Å3Prism, blue
Z = 20.37 × 0.28 × 0.17 mm
Data collection top
Stoe IPDS 2
diffractometer
3803 independent reflections
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus2650 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.037
Detector resolution: 6.67 pixels mm-1θmax = 26.0°, θmin = 2.5°
rotation method scansh = 1818
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
k = 99
Tmin = 0.740, Tmax = 0.876l = 2020
12278 measured reflections
Refinement top
Refinement on F22 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.056H-atom parameters constrained
wR(F2) = 0.171 w = 1/[σ2(Fo2) + (0.1109P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
3803 reflectionsΔρmax = 1.06 e Å3
241 parametersΔρmin = 0.60 e Å3
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cu10.5000000.5000000.5000000.0522 (2)
Cl10.07722 (9)1.00235 (15)0.41883 (10)0.0884 (4)
Cl20.21990 (10)0.38030 (16)0.43961 (10)0.1029 (5)
O10.40382 (15)0.6691 (3)0.48896 (15)0.0590 (6)
O20.51228 (16)0.8041 (4)0.56651 (16)0.0728 (8)
N10.21950 (18)0.7502 (4)0.47099 (18)0.0575 (7)
H10.2672060.7469930.4481110.069*
N20.4652 (2)0.4225 (4)0.60695 (18)0.0600 (8)
N30.3973 (3)0.4041 (5)0.7157 (2)0.0832 (11)
C120.2980 (2)0.9128 (5)0.5830 (2)0.0562 (8)
C70.2238 (2)0.8204 (4)0.5506 (2)0.0518 (8)
C140.4354 (2)0.8003 (5)0.5302 (2)0.0564 (9)
C60.1412 (2)0.6857 (5)0.4276 (2)0.0572 (9)
C130.3731 (3)0.9477 (5)0.5322 (3)0.0649 (10)
H13A0.3475580.9757290.4759800.078*
H13B0.4067251.0447560.5554240.078*
C10.0683 (2)0.7884 (5)0.4005 (3)0.0663 (10)
C80.1548 (2)0.7984 (5)0.5978 (2)0.0614 (9)
H80.1043350.7377150.5762210.074*
C110.3030 (3)0.9775 (5)0.6618 (3)0.0736 (11)
H110.3532641.0376700.6843120.088*
C150.3926 (3)0.4632 (5)0.6379 (3)0.0705 (11)
H150.3450740.5239230.6100740.085*
C170.5169 (3)0.3344 (7)0.6679 (2)0.0799 (13)
H170.5728930.2908330.6632840.096*
C90.1608 (3)0.8656 (6)0.6758 (3)0.0764 (12)
H90.1144000.8502070.7066790.092*
C50.1319 (3)0.5149 (5)0.4065 (3)0.0696 (10)
C20.0084 (3)0.7249 (7)0.3561 (3)0.0866 (14)
H20.0566620.7955820.3397910.104*
C160.4759 (4)0.3193 (8)0.7351 (3)0.0927 (14)
H160.4964890.2634650.7842430.111*
C30.0132 (4)0.5551 (8)0.3358 (4)0.0971 (17)
H30.0646880.5121520.3052260.117*
C40.0565 (4)0.4508 (7)0.3603 (3)0.0907 (15)
H40.0532430.3371690.3460200.109*
C100.2337 (3)0.9541 (7)0.7084 (3)0.0834 (13)
H100.2374640.9989980.7614470.100*
C180.3407 (4)0.4116 (9)0.7772 (4)0.1093 (19)
H180.3575680.3604910.8283860.131*
C190.2648 (6)0.4901 (10)0.7624 (6)0.148 (3)
H19A0.2478800.5411870.7112850.178*
H19B0.2274360.4950940.8029780.178*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0397 (3)0.0731 (4)0.0447 (3)0.0038 (3)0.0091 (2)0.0047 (3)
Cl10.0769 (7)0.0682 (7)0.1199 (10)0.0141 (5)0.0127 (7)0.0139 (6)
Cl20.1121 (10)0.0646 (7)0.1226 (11)0.0153 (7)0.0160 (8)0.0044 (7)
O10.0446 (12)0.0736 (17)0.0590 (14)0.0022 (11)0.0081 (10)0.0084 (13)
O20.0480 (14)0.105 (2)0.0650 (15)0.0126 (14)0.0061 (12)0.0039 (15)
N10.0443 (14)0.0676 (19)0.0624 (17)0.0042 (14)0.0131 (12)0.0056 (15)
N20.0539 (16)0.077 (2)0.0514 (16)0.0054 (15)0.0154 (13)0.0019 (16)
N30.105 (3)0.088 (3)0.067 (2)0.027 (2)0.047 (2)0.0161 (19)
C120.0499 (18)0.049 (2)0.072 (2)0.0024 (15)0.0153 (16)0.0083 (18)
C70.0455 (17)0.0485 (18)0.063 (2)0.0039 (14)0.0140 (14)0.0021 (16)
C140.0478 (18)0.073 (2)0.0515 (18)0.0068 (17)0.0186 (15)0.0012 (18)
C60.0511 (19)0.064 (2)0.057 (2)0.0052 (16)0.0085 (15)0.0030 (18)
C130.056 (2)0.058 (2)0.085 (3)0.0103 (17)0.0237 (19)0.0003 (19)
C10.053 (2)0.069 (2)0.077 (2)0.0015 (18)0.0092 (18)0.013 (2)
C80.0510 (19)0.067 (2)0.069 (2)0.0014 (17)0.0187 (16)0.0022 (19)
C110.068 (2)0.070 (3)0.085 (3)0.0048 (19)0.016 (2)0.017 (2)
C150.071 (2)0.073 (3)0.071 (2)0.002 (2)0.026 (2)0.005 (2)
C170.072 (3)0.116 (4)0.051 (2)0.003 (3)0.0055 (18)0.007 (2)
C90.064 (2)0.095 (3)0.075 (3)0.004 (2)0.027 (2)0.001 (2)
C50.076 (3)0.061 (2)0.068 (2)0.0087 (19)0.0003 (19)0.006 (2)
C20.059 (2)0.097 (4)0.100 (3)0.008 (2)0.003 (2)0.029 (3)
C160.106 (3)0.121 (4)0.052 (2)0.011 (3)0.014 (2)0.002 (3)
C30.079 (3)0.109 (4)0.095 (4)0.029 (3)0.019 (3)0.022 (3)
C40.106 (4)0.075 (3)0.086 (3)0.026 (3)0.006 (3)0.006 (3)
C100.085 (3)0.099 (3)0.070 (3)0.007 (3)0.023 (2)0.023 (2)
C180.115 (5)0.125 (5)0.097 (4)0.008 (4)0.047 (4)0.011 (4)
C190.135 (7)0.174 (8)0.136 (7)0.019 (6)0.018 (5)0.022 (5)
Geometric parameters (Å, º) top
Cu1—O11.971 (2)C13—H13A0.9700
Cu1—O1i1.971 (2)C13—H13B0.9700
Cu1—N21.989 (3)C1—C21.377 (6)
Cu1—N2i1.989 (3)C8—C91.369 (6)
Cu1—O22.639 (1)C8—H80.9300
Cu1—O2i2.6385 (1)C11—C101.393 (7)
Cl1—C11.724 (5)C11—H110.9300
Cl2—C51.735 (5)C15—H150.9300
O1—C141.294 (5)C17—C161.338 (6)
O2—C141.232 (4)C17—H170.9300
N1—C61.392 (4)C9—C101.353 (7)
N1—C71.405 (4)C9—H90.9300
N1—H10.8600C5—C41.376 (7)
N2—C151.314 (5)C2—C31.385 (8)
N2—C171.368 (5)C2—H20.9300
N3—C151.345 (6)C16—H160.9300
N3—C161.367 (7)C3—C41.357 (8)
N3—C181.412 (6)C3—H30.9300
C12—C111.376 (6)C4—H40.9300
C12—C71.384 (5)C10—H100.9300
C12—C131.524 (5)C18—C191.301 (7)
C7—C81.395 (5)C18—H180.9300
C14—C131.506 (5)C19—H19A0.9300
C6—C11.394 (5)C19—H19B0.9300
C6—C51.399 (6)
O1—Cu1—O1i180.0C9—C8—C7120.4 (4)
O1—Cu1—N290.31 (12)C9—C8—H8119.8
O1—Cu1—O254.92 (12)C7—C8—H8119.8
O2—Cu1—N286.21 (12)C12—C11—C10120.8 (4)
O1i—Cu1—N289.69 (11)C12—C11—H11119.6
O1i—Cu1—O2125.08 (11)C10—C11—H11119.6
O1—Cu1—N2i89.69 (11)N2—C15—N3109.9 (4)
O1i—Cu1—N2i90.31 (12)N2—C15—H15125.1
N2—Cu1—N2i180.00 (19)N3—C15—H15125.1
C14—O1—Cu1106.5 (2)C16—C17—N2110.8 (4)
C6—N1—C7122.7 (3)C16—C17—H17124.6
C6—N1—H1118.7N2—C17—H17124.6
C7—N1—H1118.7C10—C9—C8120.7 (4)
C15—N2—C17105.8 (3)C10—C9—H9119.6
C15—N2—Cu1126.9 (3)C8—C9—H9119.6
C17—N2—Cu1126.8 (3)C4—C5—C6122.6 (5)
C15—N3—C16108.6 (4)C4—C5—Cl2119.2 (4)
C15—N3—C18134.4 (5)C6—C5—Cl2118.2 (3)
C16—N3—C18117.0 (5)C1—C2—C3119.5 (5)
C11—C12—C7119.3 (3)C1—C2—H2120.3
C11—C12—C13119.5 (4)C3—C2—H2120.3
C7—C12—C13121.3 (3)C17—C16—N3104.9 (4)
C12—C7—C8119.3 (3)C17—C16—H16127.6
C12—C7—N1119.4 (3)N3—C16—H16127.6
C8—C7—N1121.3 (3)C4—C3—C2120.6 (5)
O2—C14—O1121.8 (4)C4—C3—H3119.7
O2—C14—C13121.7 (4)C2—C3—H3119.7
O1—C14—C13116.5 (3)C3—C4—C5119.4 (5)
N1—C6—C1122.0 (4)C3—C4—H4120.3
N1—C6—C5122.0 (4)C5—C4—H4120.3
C1—C6—C5116.0 (4)C9—C10—C11119.5 (4)
C14—C13—C12113.0 (3)C9—C10—H10120.2
C14—C13—H13A109.0C11—C10—H10120.2
C12—C13—H13A109.0C19—C18—N3120.0 (7)
C14—C13—H13B109.0C19—C18—H18120.0
C12—C13—H13B109.0N3—C18—H18120.0
H13A—C13—H13B107.8C18—C19—H19A120.0
C2—C1—C6121.9 (4)C18—C19—H19B120.0
C2—C1—Cl1119.3 (4)H19A—C19—H19B120.0
C6—C1—Cl1118.7 (3)
C11—C12—C7—C81.5 (6)Cu1—N2—C15—N3172.2 (3)
C13—C12—C7—C8177.0 (3)C16—N3—C15—N20.9 (5)
C11—C12—C7—N1178.3 (4)C18—N3—C15—N2179.1 (5)
C13—C12—C7—N13.2 (5)C15—N2—C17—C160.8 (6)
C6—N1—C7—C12166.7 (4)Cu1—N2—C17—C16173.1 (4)
C6—N1—C7—C813.4 (5)C7—C8—C9—C100.1 (7)
Cu1—O1—C14—O20.4 (4)N1—C6—C5—C4176.9 (4)
Cu1—O1—C14—C13179.0 (2)C1—C6—C5—C41.1 (6)
C7—N1—C6—C165.9 (5)N1—C6—C5—Cl22.7 (5)
C7—N1—C6—C5116.2 (4)C1—C6—C5—Cl2179.2 (3)
O2—C14—C13—C12110.0 (4)C6—C1—C2—C31.6 (7)
O1—C14—C13—C1269.4 (5)Cl1—C1—C2—C3175.2 (4)
C11—C12—C13—C14101.9 (4)N2—C17—C16—N31.3 (6)
C7—C12—C13—C1479.6 (5)C15—N3—C16—C171.4 (6)
N1—C6—C1—C2178.6 (4)C18—N3—C16—C17178.7 (5)
C5—C6—C1—C20.6 (6)C1—C2—C3—C40.9 (8)
N1—C6—C1—Cl11.8 (5)C2—C3—C4—C50.8 (9)
C5—C6—C1—Cl1176.2 (3)C6—C5—C4—C31.8 (8)
C12—C7—C8—C90.8 (6)Cl2—C5—C4—C3178.6 (4)
N1—C7—C8—C9179.0 (4)C8—C9—C10—C110.3 (8)
C7—C12—C11—C101.4 (6)C12—C11—C10—C90.5 (8)
C13—C12—C11—C10177.2 (4)C15—N3—C18—C190.1 (11)
C17—N2—C15—N30.1 (5)C16—N3—C18—C19179.8 (7)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.862.182.845 (4)134
C16—H16···O2ii0.932.483.217 (5)137
C4—H4···Cl1iii0.932.913.682 (5)142
C18—H18···O2ii0.932.473.255 (8)143
Symmetry codes: (ii) x+1, y1/2, z+3/2; (iii) x, y1, z.
Bis{2-[2-(2,6-dichloroanilino)phenyl]acetato-κ2O,O'}bis(1H-imidazole-κN3)copper(II) (3) top
Crystal data top
[Cu(C14H10Cl2NO2)2(C3H4N2)2]F(000) = 806
Mr = 789.96Dx = 1.470 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 7.6526 (4) ÅCell parameters from 12783 reflections
b = 7.5494 (5) Åθ = 1.3–25.9°
c = 31.071 (2) ŵ = 0.96 mm1
β = 96.277 (5)°T = 296 K
V = 1784.30 (19) Å3Prism, purple
Z = 20.39 × 0.29 × 0.24 mm
Data collection top
Stoe IPDS 2
diffractometer
3220 independent reflections
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus2070 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.107
Detector resolution: 6.67 pixels mm-1θmax = 25.4°, θmin = 1.3°
rotation method scansh = 99
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
k = 89
Tmin = 0.799, Tmax = 0.883l = 3737
10926 measured reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.062H-atom parameters constrained
wR(F2) = 0.185 w = 1/[σ2(Fo2) + (0.1024P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
3220 reflectionsΔρmax = 0.37 e Å3
223 parametersΔρmin = 0.75 e Å3
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cu10.5000000.5000000.5000000.0550 (3)
Cl21.02616 (19)0.5077 (2)0.71892 (5)0.0912 (5)
Cl10.39903 (19)0.5993 (2)0.62379 (7)0.1116 (6)
O20.6983 (4)0.5035 (4)0.54546 (10)0.0631 (8)
O10.8236 (4)0.3301 (5)0.49987 (11)0.0726 (9)
N20.5843 (4)0.7264 (5)0.47819 (12)0.0579 (9)
N10.7736 (5)0.4806 (5)0.63882 (12)0.0585 (9)
H10.7811940.5488840.6169460.070*
N30.6974 (5)0.9915 (5)0.47797 (15)0.0676 (10)
H30.7561001.0844370.4865920.081*
C70.8318 (5)0.3037 (6)0.63700 (14)0.0548 (10)
C120.9300 (5)0.2545 (6)0.60321 (15)0.0568 (11)
C80.7926 (6)0.1775 (7)0.66655 (15)0.0650 (12)
H80.7306870.2109030.6893730.078*
C140.8258 (6)0.4059 (7)0.53456 (15)0.0625 (12)
C130.9795 (5)0.3849 (7)0.57013 (15)0.0635 (12)
H13A1.0826850.3432120.5576180.076*
H13B1.0072750.4984400.5838100.076*
C60.7047 (6)0.5473 (6)0.67496 (16)0.0607 (12)
C170.6833 (6)0.8445 (7)0.50064 (16)0.0628 (11)
H170.7362760.8269610.5287060.075*
C160.6031 (7)0.9697 (7)0.43888 (18)0.0735 (14)
H160.5888301.0517110.4164330.088*
C90.8423 (8)0.0047 (7)0.66325 (18)0.0773 (14)
H90.8135220.0775890.6835940.093*
C150.5341 (6)0.8054 (7)0.43898 (16)0.0683 (12)
H150.4636530.7536580.4160960.082*
C110.9771 (7)0.0779 (8)0.60042 (18)0.0751 (14)
H111.0394890.0422090.5778710.090*
C50.8043 (7)0.5670 (7)0.71466 (17)0.0721 (13)
C100.9341 (8)0.0474 (7)0.6302 (2)0.0835 (16)
H100.9673050.1651040.6276970.100*
C10.5347 (7)0.6140 (7)0.6728 (2)0.0786 (15)
C40.7404 (9)0.6360 (8)0.7508 (2)0.0924 (18)
H40.8105870.6396680.7771820.111*
C20.4669 (8)0.6918 (9)0.7080 (3)0.102 (2)
H20.3535900.7381200.7053340.123*
C30.5730 (11)0.6985 (10)0.7473 (3)0.116 (3)
H3A0.5287690.7463150.7715170.139*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0502 (4)0.0567 (5)0.0573 (4)0.0036 (4)0.0024 (3)0.0003 (4)
Cl20.0846 (9)0.0994 (11)0.0849 (10)0.0075 (8)0.0125 (7)0.0113 (8)
Cl10.0633 (8)0.0947 (12)0.1711 (17)0.0110 (8)0.0133 (9)0.0066 (11)
O20.0573 (17)0.072 (2)0.0589 (17)0.0011 (17)0.0010 (13)0.0031 (15)
O10.081 (2)0.072 (2)0.065 (2)0.0185 (19)0.0097 (16)0.0040 (18)
N20.0481 (18)0.059 (2)0.066 (2)0.0052 (17)0.0072 (16)0.0004 (18)
N10.068 (2)0.050 (2)0.059 (2)0.0025 (18)0.0128 (17)0.0048 (17)
N30.062 (2)0.055 (2)0.088 (3)0.009 (2)0.022 (2)0.005 (2)
C70.046 (2)0.055 (3)0.063 (2)0.002 (2)0.0034 (18)0.003 (2)
C120.044 (2)0.062 (3)0.065 (3)0.002 (2)0.0066 (18)0.001 (2)
C80.073 (3)0.059 (3)0.064 (3)0.005 (2)0.012 (2)0.002 (2)
C140.063 (3)0.066 (3)0.058 (3)0.017 (2)0.006 (2)0.008 (2)
C130.046 (2)0.076 (3)0.069 (3)0.002 (2)0.009 (2)0.004 (2)
C60.062 (3)0.045 (2)0.078 (3)0.004 (2)0.019 (2)0.002 (2)
C170.057 (2)0.063 (3)0.071 (3)0.005 (2)0.014 (2)0.005 (2)
C160.063 (3)0.077 (4)0.080 (3)0.005 (3)0.009 (2)0.021 (3)
C90.104 (4)0.053 (3)0.073 (3)0.010 (3)0.006 (3)0.008 (3)
C150.061 (3)0.072 (3)0.074 (3)0.008 (3)0.011 (2)0.009 (3)
C110.065 (3)0.080 (4)0.081 (3)0.015 (3)0.013 (2)0.006 (3)
C50.080 (3)0.065 (3)0.073 (3)0.007 (3)0.015 (3)0.008 (3)
C100.099 (4)0.059 (3)0.092 (4)0.017 (3)0.006 (3)0.002 (3)
C10.061 (3)0.060 (3)0.116 (4)0.007 (2)0.016 (3)0.014 (3)
C40.115 (5)0.080 (4)0.089 (4)0.023 (4)0.038 (3)0.020 (3)
C20.070 (4)0.081 (4)0.163 (7)0.003 (3)0.048 (4)0.023 (4)
C30.126 (6)0.093 (5)0.141 (7)0.029 (5)0.076 (5)0.039 (5)
Geometric parameters (Å, º) top
Cu1—O2i1.957 (3)C8—H80.9300
Cu1—O21.957 (3)C14—C131.532 (6)
Cu1—O12.789 (3)C13—H13A0.9700
Cu1—N2i1.973 (4)C13—H13B0.9700
Cu1—N21.973 (4)C6—C51.385 (7)
Cl2—C51.747 (6)C6—C11.390 (7)
Cl1—C11.749 (6)C17—H170.9300
O2—C141.297 (6)C16—C151.349 (7)
O1—C141.219 (5)C16—H160.9300
N2—C171.319 (6)C9—C101.363 (8)
N2—C151.373 (6)C9—H90.9300
N1—C61.386 (6)C15—H150.9300
N1—C71.411 (6)C11—C101.388 (8)
N1—H10.8600C11—H110.9300
N3—C171.325 (6)C5—C41.375 (7)
N3—C161.353 (7)C10—H100.9300
N3—H30.8600C1—C21.392 (8)
C7—C81.379 (6)C4—C31.358 (10)
C7—C121.406 (6)C4—H40.9300
C12—C111.386 (7)C2—C31.393 (10)
C12—C131.502 (6)C2—H20.9300
C8—C91.365 (7)C3—H3A0.9300
O2i—Cu1—O2180.0C5—C6—N1122.6 (4)
O2i—Cu1—N2i88.81 (14)C5—C6—C1115.2 (5)
O2—Cu1—N2i91.19 (14)N1—C6—C1121.9 (5)
O2—Cu1—N288.81 (14)N2—C17—N3111.1 (4)
N2i—Cu1—N2180.0 (2)N2—C17—H17124.4
O1—Cu1—O252.32 (12)N3—C17—H17124.4
O1i—Cu1—O2127.68 (12)C15—C16—N3106.3 (5)
N2i—Cu1—O185.76 (2)C15—C16—H16126.9
C14—O2—Cu1110.5 (3)N3—C16—H16126.9
C17—N2—C15105.3 (4)C10—C9—C8120.2 (5)
C17—N2—Cu1126.5 (3)C10—C9—H9119.9
C15—N2—Cu1127.6 (3)C8—C9—H9119.9
C6—N1—C7121.7 (4)C16—C15—N2109.3 (5)
C6—N1—H1119.1C16—C15—H15125.4
C7—N1—H1119.1N2—C15—H15125.4
C17—N3—C16108.0 (4)C12—C11—C10122.1 (5)
C17—N3—H3126.0C12—C11—H11119.0
C16—N3—H3126.0C10—C11—H11119.0
C8—C7—C12119.2 (4)C4—C5—C6123.9 (6)
C8—C7—N1122.4 (4)C4—C5—Cl2117.7 (5)
C12—C7—N1118.5 (4)C6—C5—Cl2118.4 (4)
C11—C12—C7117.7 (4)C9—C10—C11119.0 (5)
C11—C12—C13120.1 (4)C9—C10—H10120.5
C7—C12—C13122.2 (4)C11—C10—H10120.5
C9—C8—C7121.8 (5)C6—C1—C2122.8 (6)
C9—C8—H8119.1C6—C1—Cl1118.9 (4)
C7—C8—H8119.1C2—C1—Cl1118.3 (5)
O1—C14—O2124.0 (4)C3—C4—C5118.9 (7)
O1—C14—C13121.7 (5)C3—C4—H4120.5
O2—C14—C13114.3 (4)C5—C4—H4120.5
C12—C13—C14109.3 (4)C1—C2—C3118.3 (6)
C12—C13—H13A109.8C1—C2—H2120.9
C14—C13—H13A109.8C3—C2—H2120.9
C12—C13—H13B109.8C4—C3—C2120.8 (6)
C14—C13—H13B109.8C4—C3—H3A119.6
H13A—C13—H13B108.3C2—C3—H3A119.6
C6—N1—C7—C813.2 (7)N3—C16—C15—N20.5 (6)
C6—N1—C7—C12168.1 (4)C17—N2—C15—C160.4 (5)
C8—C7—C12—C112.4 (6)Cu1—N2—C15—C16171.4 (3)
N1—C7—C12—C11176.3 (4)C7—C12—C11—C101.6 (7)
C8—C7—C12—C13179.3 (4)C13—C12—C11—C10179.9 (5)
N1—C7—C12—C132.0 (6)N1—C6—C5—C4178.7 (5)
C12—C7—C8—C91.9 (7)C1—C6—C5—C44.3 (8)
N1—C7—C8—C9176.8 (5)N1—C6—C5—Cl20.8 (7)
Cu1—O2—C14—O13.1 (6)C1—C6—C5—Cl2173.6 (4)
Cu1—O2—C14—C13174.0 (3)C8—C9—C10—C110.6 (9)
C11—C12—C13—C1495.2 (5)C12—C11—C10—C90.1 (9)
C7—C12—C13—C1483.1 (6)C5—C6—C1—C21.3 (8)
O1—C14—C13—C12100.3 (5)N1—C6—C1—C2175.8 (5)
O2—C14—C13—C1276.9 (5)C5—C6—C1—Cl1178.9 (4)
C7—N1—C6—C566.0 (6)N1—C6—C1—Cl14.5 (7)
C7—N1—C6—C1119.9 (5)C6—C5—C4—C34.0 (9)
C15—N2—C17—N30.1 (5)Cl2—C5—C4—C3173.9 (5)
Cu1—N2—C17—N3171.8 (3)C6—C1—C2—C31.7 (10)
C16—N3—C17—N20.2 (5)Cl1—C1—C2—C3178.0 (5)
C17—N3—C16—C150.4 (5)C5—C4—C3—C20.6 (10)
C7—C8—C9—C100.3 (8)C1—C2—C3—C42.2 (11)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O20.862.272.900 (5)130
N3—H3···O1ii0.861.962.791 (5)163
C16—H16···Cl1iii0.932.923.791 (6)156
Symmetry codes: (ii) x, y+1, z; (iii) x+1, y+2, z+1.
Table S1. Selected IR spectral data for the dicl ligands 1, 2 and 3 top
AssignmentNadicl123
ν(NH)3250 (m)3326 (w)3232 (w)3259 (w), 3140 (w)
ν(O—H)3554 (w)
νar(C—H)3060 (vw)3066 (vw)3140 (w), 3112 (vw)3075 (w)
νas(COO)1572 (s)1577 (s)1561 (s)1560 (s)
νs(COO)1402 (w)1416 (m)1453 (m)1451 (m)
Δν171161108109
Note: (*) Frequencies in cm-1; w = weak; m = medium; s = strong; vs = very strong. Nadicl is sodium 2-[2-(2,6-dichloroanilino)phenyl]acetate.
Table S2. Comparative structural parameters for binuclear copper (II) carboxylates containing the [Cu2(syn,syn2-O2CR)4] core. top
ComplexCu···Cu (Å)ΔCu (Å)Cu—O(axial) (Å)Cu—O(basal) (Å)**Bridge length (Å)***
[Cu2(OCOCH3)4(DMF)2]2.614 (1)0.202.163 (3)1.964 (3)6.42
[Cu2(OCOCH3)4(MeOH)2]2.596 (1)0.182.160 (3)1.967 (2)6.46
[Cu2(dicl)4(DMF)2]2.627 (1)0.2032.122 (2)1.967 (2)6.42
[Cu2(dicl)4(acetone)2]2.610 (1)0.1912.177 (2)1.970 (2)6.45
[Cu2(dicl)4(MeOH)2]2.585 (1)0.1762.187 (1)1.961 (2)6.45
Note: (*) deviation of copper from the basal plane; (**) average distance; (***) sum of Cu—O–C—O—Cu.

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