Download citation
Download citation
link to html
In the isostructural title complexes, [M(C9H6N3O2)2(H2O)2] [M = CoII, (I), CdII, (II), and CuII, (III); the metal centres reside on a twofold axis in the space group C2/c for (I) and (II)], the metal centres are surrounded by four O atoms from two O,O′-bidentate carboxyl­ate groups and by two trans-coordinated aqua ligands, forming a distorted octa­hedral environment. The mol­ecules possess four hydrogen-bond donor (two aqua ligands) and four hydrogen-bond acceptor sites (two triazole groups), and aggregate by self-association, forming two-dimensional hydrogen-bonded frameworks [via O—H...N inter­actions; O...N = 2.749 (3)–2.872 (3) Å]. The layers are parallel and are tightly packed with short inter­layer distances of 4.93, 4.95 and 5.01 Å for (I), (II) and (III), respectively.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270107009080/gg3077sup1.cif
Contains datablocks global, I, II, III

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270107009080/gg3077Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270107009080/gg3077IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270107009080/gg3077IIIsup4.hkl
Contains datablock III

CCDC references: 645507; 645508; 645509

Computing details top

For all compounds, data collection: SMART-NT (Bruker, 1998). Cell refinement: SMART-NT or SAINT??? (Bruker, 1998) for (I), (III); SMART-NT or SAINT???? (Bruker, 1998) for (II). Data reduction: SMART-NT or SAINT??? for (I), (III); SMART-NT or SAINT???? for (II). For all compounds, program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: Diamond (Brandenburg, 1999); software used to prepare material for publication: WinGX (Version 1.700.00; Farrugia, 1999).

(I) Diaquabis[4-(4H-1,2,4-triazol-4-yl)benzoato-κ2O,O']cobalt(II) top
Crystal data top
[Co(C9H6N3O2)2(H2O)2]F(000) = 964
Mr = 471.30Dx = 1.753 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 13.5266 (9) ÅCell parameters from 7599 reflections
b = 9.8617 (7) Åθ = 2.6–27.6°
c = 14.4429 (9) ŵ = 1.02 mm1
β = 112.083 (3)°T = 213 K
V = 1785.3 (2) Å3Prism, pink
Z = 40.18 × 0.16 × 0.16 mm
Data collection top
Siemens SMART CCD
diffractometer
2057 independent reflections
Radiation source: fine-focus sealed tube1607 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.030
ω scansθmax = 27.6°, θmin = 2.6°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 1717
Tmin = 0.838, Tmax = 0.854k = 1212
7599 measured reflectionsl = 1818
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.028Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.068H-atom parameters constrained
S = 0.94 w = 1/[σ2(Fo2) + (0.043P)2]
where P = (Fo2 + 2Fc2)/3
2057 reflections(Δ/σ)max = 0.001
141 parametersΔρmax = 0.38 e Å3
0 restraintsΔρmin = 0.31 e Å3
Special details top

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) top
xyzUiso*/Ueq
Co10.00000.07711 (3)0.25000.01897 (11)
O10.14414 (9)0.03691 (12)0.29607 (10)0.0249 (3)
O20.14914 (9)0.18553 (11)0.30013 (9)0.0223 (3)
O30.00316 (10)0.10071 (15)0.39246 (10)0.0339 (3)
H10.05370.05560.43470.051*
H20.05710.08000.39440.051*
N10.80877 (11)0.01767 (16)0.45657 (12)0.0260 (3)
N20.80936 (11)0.11569 (15)0.42598 (12)0.0241 (3)
N30.64489 (10)0.06013 (13)0.40370 (10)0.0179 (3)
C10.71053 (14)0.04841 (17)0.44199 (14)0.0238 (4)
H1A0.68780.13340.45590.029*
C20.71094 (13)0.15929 (17)0.39482 (14)0.0218 (4)
H2A0.68880.24680.36980.026*
C30.53209 (12)0.06498 (16)0.37981 (12)0.0171 (3)
C40.47489 (13)0.05533 (16)0.35866 (14)0.0223 (4)
H4A0.50950.13800.35870.027*
C50.36607 (13)0.05241 (15)0.33750 (14)0.0215 (4)
H5A0.32690.13370.32410.026*
C60.31456 (12)0.07019 (17)0.33599 (12)0.0181 (3)
C70.37303 (13)0.19015 (16)0.35553 (14)0.0214 (4)
H7A0.33810.27330.35310.026*
C80.48238 (13)0.18840 (16)0.37852 (13)0.0217 (4)
H8A0.52200.26940.39290.026*
C90.19648 (12)0.07302 (16)0.30986 (12)0.0181 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co10.00907 (16)0.01947 (16)0.0285 (2)0.0000.00718 (14)0.000
O10.0121 (6)0.0215 (6)0.0410 (8)0.0024 (4)0.0099 (6)0.0014 (5)
O20.0125 (6)0.0207 (6)0.0332 (7)0.0014 (4)0.0080 (6)0.0005 (5)
O30.0137 (6)0.0605 (9)0.0287 (7)0.0091 (6)0.0091 (6)0.0097 (6)
N10.0143 (7)0.0334 (8)0.0293 (9)0.0055 (6)0.0071 (7)0.0010 (7)
N20.0120 (7)0.0344 (8)0.0258 (8)0.0009 (6)0.0070 (6)0.0004 (6)
N30.0097 (6)0.0233 (7)0.0207 (7)0.0011 (5)0.0057 (6)0.0002 (5)
C10.0164 (8)0.0262 (8)0.0283 (10)0.0046 (6)0.0078 (8)0.0043 (7)
C20.0140 (8)0.0262 (8)0.0259 (10)0.0017 (6)0.0081 (8)0.0001 (7)
C30.0093 (7)0.0235 (8)0.0188 (8)0.0006 (6)0.0057 (7)0.0006 (6)
C40.0146 (8)0.0201 (8)0.0337 (10)0.0023 (6)0.0108 (8)0.0002 (7)
C50.0142 (8)0.0185 (8)0.0328 (10)0.0020 (6)0.0102 (8)0.0008 (6)
C60.0110 (7)0.0227 (7)0.0206 (8)0.0002 (6)0.0060 (7)0.0006 (6)
C70.0131 (8)0.0197 (8)0.0314 (10)0.0014 (6)0.0085 (8)0.0026 (7)
C80.0130 (8)0.0201 (8)0.0308 (10)0.0028 (6)0.0071 (8)0.0043 (7)
C90.0108 (7)0.0225 (7)0.0214 (8)0.0003 (6)0.0065 (7)0.0005 (7)
Geometric parameters (Å, º) top
Co1—O12.1291 (12)C1—H1A0.9400
Co1—O22.1539 (11)C2—H2A0.9400
Co1—O32.0552 (13)C3—C41.386 (2)
O1—C91.269 (2)C3—C81.387 (2)
O2—C91.2622 (19)C4—C51.387 (2)
O3—H10.8500C4—H4A0.9400
O3—H20.8500C5—C61.391 (2)
N1—C11.301 (2)C5—H5A0.9400
N1—N21.388 (2)C6—C71.392 (2)
N2—C21.307 (2)C6—C91.497 (2)
N3—C21.363 (2)C7—C81.389 (2)
N3—C11.368 (2)C7—H7A0.9400
N3—C31.4330 (19)C8—H8A0.9400
O3—Co1—O3i166.99 (8)N2—C2—N3110.51 (15)
O3—Co1—O1i92.56 (5)N2—C2—H2A124.7
O3—Co1—O194.30 (5)N3—C2—H2A124.7
O3i—Co1—O192.56 (5)C4—C3—C8121.36 (14)
O1i—Co1—O1116.25 (6)C4—C3—N3118.69 (13)
O3—Co1—O286.73 (5)C8—C3—N3119.95 (14)
O3i—Co1—O286.82 (5)C3—C4—C5119.28 (14)
O1i—Co1—O2177.69 (5)C3—C4—H4A120.4
O1—Co1—O261.65 (4)C5—C4—H4A120.4
O3—Co1—O2i86.82 (5)C4—C5—C6120.35 (15)
O1—Co1—O2i177.69 (5)C4—C5—H5A119.8
O2—Co1—O2i120.47 (6)C6—C5—H5A119.8
C9—O1—Co189.38 (9)C5—C6—C7119.50 (14)
C9—O2—Co188.45 (9)C5—C6—C9120.04 (15)
Co1—O3—H1111.5C7—C6—C9120.43 (14)
Co1—O3—H2110.3C8—C7—C6120.72 (14)
H1—O3—H2111.9C8—C7—H7A119.6
C1—N1—N2107.28 (14)C6—C7—H7A119.6
C2—N2—N1107.11 (13)C3—C8—C7118.77 (14)
C2—N3—C1104.53 (14)C3—C8—H8A120.6
C2—N3—C3129.03 (14)C7—C8—H8A120.6
C1—N3—C3126.44 (14)O2—C9—O1120.25 (14)
N1—C1—N3110.57 (15)O2—C9—C6119.54 (14)
N1—C1—H1A124.7O1—C9—C6120.20 (14)
N3—C1—H1A124.7
O3—Co1—O1—C986.93 (10)C8—C3—C4—C51.1 (3)
O3i—Co1—O1—C982.01 (10)N3—C3—C4—C5178.65 (15)
O1i—Co1—O1—C9178.08 (11)C3—C4—C5—C61.0 (3)
O2—Co1—O1—C92.99 (9)C4—C5—C6—C70.2 (3)
O3—Co1—O2—C999.68 (10)C4—C5—C6—C9178.03 (15)
O3i—Co1—O2—C991.62 (10)C5—C6—C7—C81.4 (3)
O1—Co1—O2—C93.01 (9)C9—C6—C7—C8179.14 (16)
O2i—Co1—O2—C9175.94 (10)C4—C3—C8—C70.0 (3)
C1—N1—N2—C20.36 (19)N3—C3—C8—C7179.74 (15)
N2—N1—C1—N30.7 (2)C6—C7—C8—C31.2 (3)
C2—N3—C1—N10.8 (2)Co1—O2—C9—O15.15 (15)
C3—N3—C1—N1178.84 (15)Co1—O2—C9—C6173.77 (14)
N1—N2—C2—N30.12 (19)Co1—O1—C9—O25.21 (16)
C1—N3—C2—N20.53 (19)Co1—O1—C9—C6173.70 (14)
C3—N3—C2—N2179.06 (15)C5—C6—C9—O2173.83 (15)
C2—N3—C3—C4155.98 (17)C7—C6—C9—O23.9 (2)
C1—N3—C3—C424.5 (3)C5—C6—C9—O15.1 (3)
C2—N3—C3—C824.2 (3)C7—C6—C9—O1177.14 (15)
C1—N3—C3—C8155.29 (17)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H1···N1ii0.851.972.780 (2)159
O3—H2···N2iii0.852.052.843 (2)154
C4—H4A···O3iv0.942.633.428 (2)143
Symmetry codes: (ii) x+1, y, z+1; (iii) x1, y, z; (iv) x+1/2, y1/2, z.
(II) Diaquabis[4-(4H-1,2,4-triazol-4-yl)benzoato-κ2O,O']cadmium(II) top
Crystal data top
[Cd(C9H6N3O2)2(H2O)2]F(000) = 1048
Mr = 524.77Dx = 1.870 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 13.7301 (6) ÅCell parameters from 6196 reflections
b = 9.8915 (5) Åθ = 2.6–27.9°
c = 14.8111 (10) ŵ = 1.23 mm1
β = 112.063 (3)°T = 296 K
V = 1864.21 (18) Å3Prism, colorless
Z = 40.18 × 0.16 × 0.16 mm
Data collection top
Siemens SMART CCD
diffractometer
2213 independent reflections
Radiation source: fine-focus sealed tube1941 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.021
ω scansθmax = 27.9°, θmin = 2.6°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 1812
Tmin = 0.810, Tmax = 0.828k = 1112
6196 measured reflectionsl = 1819
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.086H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0474P)2 + 1.5785P]
where P = (Fo2 + 2Fc2)/3
2213 reflections(Δ/σ)max < 0.001
141 parametersΔρmax = 0.67 e Å3
0 restraintsΔρmin = 0.33 e Å3
Special details top

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) top
xyzUiso*/Ueq
Cd10.00000.08044 (3)0.25000.03738 (12)
O10.15745 (14)0.0332 (2)0.29622 (16)0.0412 (5)
O20.16224 (13)0.18906 (19)0.30451 (14)0.0376 (4)
O30.00698 (16)0.1188 (3)0.40408 (15)0.0520 (6)
H10.05760.07370.44630.078*
H20.05330.09810.40600.078*
N10.80989 (17)0.0116 (3)0.45761 (18)0.0420 (6)
N20.81063 (17)0.1206 (3)0.42637 (17)0.0378 (5)
N30.64934 (16)0.0651 (2)0.40523 (15)0.0278 (4)
C10.7141 (2)0.0411 (3)0.4444 (2)0.0394 (6)
H1A0.69230.12410.45970.047*
C20.71409 (19)0.1627 (3)0.39526 (19)0.0331 (6)
H2A0.69220.24820.36960.040*
C30.53806 (18)0.0699 (2)0.38105 (18)0.0262 (5)
C40.4824 (2)0.0497 (3)0.3619 (2)0.0356 (6)
H4A0.51650.13140.36370.043*
C50.3752 (2)0.0466 (3)0.3400 (2)0.0353 (6)
H5A0.33720.12690.32710.042*
C60.32420 (19)0.0742 (2)0.33720 (18)0.0286 (5)
C70.38106 (18)0.1938 (3)0.35575 (19)0.0326 (5)
H7A0.34670.27570.35270.039*
C80.48841 (19)0.1924 (3)0.37879 (19)0.0327 (6)
H8A0.52670.27250.39260.039*
C90.20695 (19)0.0769 (2)0.31081 (19)0.0295 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cd10.01693 (15)0.0448 (2)0.0498 (2)0.0000.01183 (12)0.000
O10.0192 (9)0.0345 (10)0.0689 (14)0.0015 (8)0.0156 (9)0.0021 (9)
O20.0176 (8)0.0346 (10)0.0593 (12)0.0008 (7)0.0130 (8)0.0003 (9)
O30.0238 (10)0.0874 (16)0.0461 (12)0.0141 (10)0.0147 (9)0.0154 (11)
N10.0220 (11)0.0523 (15)0.0499 (14)0.0106 (10)0.0115 (10)0.0063 (12)
N20.0199 (10)0.0511 (14)0.0422 (12)0.0020 (10)0.0115 (9)0.0002 (11)
N30.0160 (9)0.0357 (12)0.0325 (11)0.0026 (8)0.0098 (8)0.0014 (8)
C10.0249 (13)0.0403 (15)0.0526 (17)0.0084 (11)0.0139 (12)0.0093 (13)
C20.0207 (11)0.0389 (15)0.0407 (14)0.0011 (10)0.0127 (10)0.0023 (11)
C30.0149 (10)0.0357 (13)0.0286 (11)0.0025 (9)0.0087 (9)0.0018 (9)
C40.0232 (12)0.0272 (13)0.0581 (17)0.0028 (10)0.0171 (12)0.0007 (11)
C50.0226 (12)0.0275 (13)0.0579 (17)0.0043 (10)0.0177 (12)0.0016 (11)
C60.0181 (11)0.0348 (14)0.0344 (13)0.0008 (9)0.0115 (10)0.0009 (10)
C70.0178 (11)0.0300 (13)0.0483 (15)0.0016 (10)0.0106 (10)0.0033 (11)
C80.0202 (11)0.0312 (13)0.0451 (14)0.0035 (10)0.0104 (10)0.0052 (11)
C90.0168 (11)0.0352 (14)0.0367 (13)0.0009 (10)0.0102 (10)0.0007 (10)
Geometric parameters (Å, º) top
Cd1—O12.3008 (19)C1—H1A0.9300
Cd1—O22.3275 (17)C2—H2A0.9300
Cd1—O32.280 (2)C3—C41.379 (4)
O1—C91.258 (3)C3—C81.384 (3)
O2—C91.255 (3)C4—C51.383 (3)
O3—H10.8640C4—H4A0.9300
O3—H20.8630C5—C61.378 (4)
N1—C11.288 (4)C5—H5A0.9300
N1—N21.388 (4)C6—C71.387 (3)
N2—C21.298 (3)C6—C91.507 (3)
N3—C21.357 (3)C7—C81.383 (3)
N3—C11.358 (3)C7—H7A0.9300
N3—C31.433 (3)C8—H8A0.9300
O3—Cd1—O3i160.83 (12)N2—C2—N3110.9 (2)
O3—Cd1—O1i93.48 (8)N2—C2—H2A124.6
O3—Cd1—O195.85 (7)N3—C2—H2A124.6
O3i—Cd1—O193.48 (8)C4—C3—C8121.0 (2)
O1i—Cd1—O1121.51 (10)C4—C3—N3118.7 (2)
O3—Cd1—O284.32 (7)C8—C3—N3120.3 (2)
O3i—Cd1—O286.86 (7)C3—C4—C5119.3 (2)
O1i—Cd1—O2176.96 (7)C3—C4—H4A120.4
O1—Cd1—O256.80 (7)C5—C4—H4A120.4
O3—Cd1—O2i86.86 (7)C6—C5—C4120.6 (2)
O1—Cd1—O2i176.96 (7)C6—C5—H5A119.7
O2—Cd1—O2i125.02 (9)C4—C5—H5A119.7
C9—O1—Cd190.85 (15)C5—C6—C7119.5 (2)
C9—O2—Cd189.73 (14)C5—C6—C9120.3 (2)
Cd1—O3—H1111.0C7—C6—C9120.2 (2)
Cd1—O3—H2108.3C8—C7—C6120.6 (2)
H1—O3—H2111.9C8—C7—H7A119.7
C1—N1—N2107.3 (2)C6—C7—H7A119.7
C2—N2—N1106.6 (2)C7—C8—C3119.0 (2)
C2—N3—C1104.3 (2)C7—C8—H8A120.5
C2—N3—C3129.0 (2)C3—C8—H8A120.5
C1—N3—C3126.7 (2)O2—C9—O1122.3 (2)
N1—C1—N3110.9 (3)O2—C9—C6118.7 (2)
N1—C1—H1A124.6O1—C9—C6119.0 (2)
N3—C1—H1A124.6
C1—N1—N2—C20.5 (3)C4—C5—C6—C9178.4 (3)
N2—N1—C1—N30.2 (3)C5—C6—C7—C81.2 (4)
C2—N3—C1—N10.1 (3)C9—C6—C7—C8179.2 (2)
C3—N3—C1—N1179.6 (2)C6—C7—C8—C31.4 (4)
N1—N2—C2—N30.6 (3)C4—C3—C8—C70.8 (4)
C1—N3—C2—N20.5 (3)N3—C3—C8—C7179.6 (2)
C3—N3—C2—N2179.3 (2)Cd1—O2—C9—O15.4 (3)
C2—N3—C3—C4155.6 (3)Cd1—O2—C9—C6174.9 (2)
C1—N3—C3—C424.6 (4)Cd1—O1—C9—O25.4 (3)
C2—N3—C3—C825.5 (4)Cd1—O1—C9—C6174.8 (2)
C1—N3—C3—C8154.2 (3)C5—C6—C9—O2176.8 (3)
C8—C3—C4—C50.1 (4)C7—C6—C9—O21.2 (4)
N3—C3—C4—C5179.0 (2)C5—C6—C9—O13.5 (4)
C3—C4—C5—C60.1 (5)C7—C6—C9—O1178.6 (2)
C4—C5—C6—C70.5 (4)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H1···N1ii0.861.942.788 (2)166
O3—H2···N2iii0.862.012.836 (2)159
C4—H4A···O3iv0.932.563.331 (2)141
Symmetry codes: (ii) x+1, y, z+1; (iii) x1, y, z; (iv) x+1/2, y1/2, z.
(III) Diaquabis[4-(4H-1,2,4-triazol-4-yl)benzoato-κ2O,O']copper(II) top
Crystal data top
[Cu(C9H6N3O2)2(H2O)2]F(000) = 972
Mr = 475.91Dx = 1.746 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 13.4483 (4) ÅCell parameters from 4301 reflections
b = 10.0101 (3) Åθ = 2.5–27.9°
c = 14.4749 (5) ŵ = 1.26 mm1
β = 111.674 (2)°T = 296 K
V = 1810.83 (10) Å3Prism, green
Z = 40.50 × 0.20 × 0.20 mm
Data collection top
Siemens SMART CCD
diffractometer
4301 independent reflections
Radiation source: fine-focus sealed tube3232 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.036
ω scansθmax = 27.9°, θmin = 2.5°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 1617
Tmin = 0.571, Tmax = 0.787k = 1013
13821 measured reflectionsl = 1919
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.105H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0483P)2 + 0.7524P]
where P = (Fo2 + 2Fc2)/3
4301 reflections(Δ/σ)max = 0.001
280 parametersΔρmax = 0.39 e Å3
0 restraintsΔρmin = 0.55 e Å3
Special details top

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) top
xyzUiso*/Ueq
Cu10.245975 (19)0.66068 (3)0.24870 (2)0.02728 (11)
O10.39100 (12)0.72780 (17)0.28705 (13)0.0348 (4)
O20.41565 (13)0.51206 (18)0.31827 (15)0.0444 (5)
O30.09854 (11)0.60241 (16)0.20779 (12)0.0300 (4)
O40.08660 (13)0.82128 (16)0.19047 (15)0.0418 (5)
O50.23969 (13)0.6187 (2)0.11294 (13)0.0415 (4)
H10.30010.62970.10790.062*
H20.19300.66590.06950.062*
O60.25190 (14)0.6661 (2)0.38628 (14)0.0508 (6)
H30.19050.67760.38910.076*
H40.29470.72580.42040.076*
N11.05531 (15)0.7948 (2)0.45891 (15)0.0339 (5)
N21.06570 (15)0.6653 (2)0.42989 (15)0.0329 (5)
N30.89811 (13)0.69928 (19)0.40789 (13)0.0252 (4)
N40.57351 (15)0.7263 (2)0.03454 (16)0.0398 (5)
N50.56489 (15)0.6002 (2)0.07641 (15)0.0373 (5)
N60.40455 (14)0.67049 (18)0.09400 (14)0.0264 (4)
C10.95508 (18)0.8121 (2)0.44445 (18)0.0325 (5)
H1A0.92620.89100.45740.039*
C20.97164 (17)0.6107 (2)0.40034 (17)0.0293 (5)
H2A0.95650.52350.37730.035*
C30.78610 (16)0.6788 (2)0.38397 (16)0.0245 (5)
C40.71836 (17)0.7872 (2)0.35558 (18)0.0305 (5)
H4A0.74540.87150.35110.037*
C50.60993 (17)0.7702 (2)0.33377 (18)0.0305 (5)
H5A0.56430.84340.31530.037*
C60.56891 (17)0.6446 (2)0.33925 (17)0.0268 (5)
C70.63819 (18)0.5365 (2)0.36612 (19)0.0329 (5)
H7A0.61120.45170.36890.039*
C80.74681 (18)0.5527 (2)0.38885 (19)0.0326 (5)
H8A0.79270.47960.40720.039*
C90.45090 (17)0.6253 (2)0.31374 (17)0.0286 (5)
C100.47793 (18)0.7655 (3)0.04653 (18)0.0351 (6)
H10A0.46160.84750.02550.042*
C110.46379 (18)0.5702 (3)0.11054 (18)0.0333 (5)
H11A0.43560.49030.14220.040*
C120.29169 (16)0.6793 (2)0.11892 (16)0.0243 (5)
C130.24369 (18)0.8039 (2)0.13370 (18)0.0311 (5)
H13A0.28430.88050.12910.037*
C140.13485 (18)0.8134 (2)0.15541 (18)0.0304 (5)
H14A0.10260.89710.16430.036*
C150.07326 (16)0.6996 (2)0.16412 (16)0.0251 (5)
C160.12287 (17)0.5747 (2)0.15096 (18)0.0284 (5)
H16A0.08200.49780.15800.034*
C170.23173 (18)0.5640 (2)0.12766 (18)0.0306 (5)
H17A0.26440.48060.11790.037*
C180.04455 (16)0.7110 (2)0.18885 (16)0.0258 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.01299 (15)0.03152 (18)0.03728 (18)0.00017 (10)0.00922 (12)0.00061 (12)
O10.0154 (8)0.0384 (10)0.0504 (11)0.0003 (7)0.0120 (7)0.0022 (8)
O20.0239 (9)0.0382 (10)0.0712 (13)0.0057 (8)0.0176 (9)0.0044 (9)
O30.0139 (7)0.0310 (9)0.0437 (10)0.0002 (6)0.0091 (7)0.0005 (7)
O40.0230 (9)0.0307 (10)0.0722 (13)0.0036 (7)0.0182 (9)0.0018 (8)
O50.0198 (8)0.0676 (12)0.0379 (10)0.0105 (8)0.0118 (8)0.0090 (9)
O60.0209 (9)0.0921 (17)0.0417 (11)0.0145 (9)0.0143 (8)0.0165 (10)
N10.0187 (9)0.0417 (12)0.0396 (12)0.0073 (8)0.0088 (9)0.0032 (9)
N20.0176 (9)0.0458 (13)0.0353 (11)0.0004 (8)0.0098 (8)0.0002 (9)
N30.0144 (9)0.0311 (10)0.0301 (10)0.0015 (7)0.0082 (8)0.0016 (8)
N40.0190 (10)0.0576 (15)0.0413 (12)0.0058 (9)0.0092 (9)0.0017 (11)
N50.0185 (10)0.0568 (14)0.0367 (12)0.0040 (9)0.0104 (9)0.0032 (10)
N60.0155 (9)0.0355 (11)0.0278 (10)0.0015 (7)0.0076 (8)0.0007 (8)
C10.0231 (11)0.0327 (13)0.0426 (14)0.0049 (9)0.0130 (11)0.0049 (10)
C20.0175 (11)0.0354 (13)0.0353 (13)0.0019 (9)0.0102 (10)0.0004 (10)
C30.0134 (10)0.0334 (12)0.0269 (11)0.0006 (8)0.0076 (9)0.0004 (9)
C40.0208 (11)0.0265 (11)0.0454 (14)0.0020 (9)0.0136 (10)0.0013 (10)
C50.0204 (11)0.0285 (12)0.0438 (14)0.0034 (9)0.0134 (10)0.0004 (10)
C60.0158 (10)0.0370 (13)0.0283 (12)0.0013 (9)0.0089 (9)0.0004 (9)
C70.0211 (11)0.0290 (12)0.0482 (15)0.0026 (9)0.0124 (11)0.0059 (11)
C80.0189 (11)0.0287 (12)0.0483 (15)0.0032 (9)0.0104 (11)0.0069 (10)
C90.0164 (11)0.0390 (13)0.0312 (12)0.0029 (9)0.0098 (10)0.0035 (10)
C100.0199 (11)0.0451 (15)0.0385 (14)0.0052 (10)0.0086 (10)0.0029 (11)
C110.0223 (11)0.0436 (14)0.0341 (13)0.0052 (10)0.0107 (10)0.0012 (11)
C120.0136 (10)0.0353 (12)0.0244 (11)0.0002 (8)0.0074 (9)0.0008 (9)
C130.0225 (11)0.0271 (12)0.0446 (14)0.0051 (9)0.0136 (11)0.0005 (10)
C140.0221 (11)0.0257 (12)0.0451 (14)0.0026 (9)0.0145 (10)0.0012 (10)
C150.0153 (10)0.0311 (11)0.0286 (11)0.0002 (8)0.0079 (9)0.0007 (9)
C160.0193 (11)0.0262 (11)0.0395 (13)0.0027 (9)0.0106 (10)0.0013 (10)
C170.0205 (11)0.0288 (12)0.0418 (14)0.0027 (9)0.0109 (10)0.0035 (10)
C180.0172 (10)0.0300 (11)0.0316 (12)0.0013 (9)0.0104 (9)0.0011 (10)
Geometric parameters (Å, º) top
Cu1—O11.9400 (15)C2—H2A0.9300
Cu1—O31.9377 (14)C3—C41.378 (3)
Cu1—O51.9806 (17)C3—C81.381 (3)
Cu1—O61.9642 (18)C4—C51.384 (3)
O1—C91.273 (3)C4—H4A0.9300
O2—C91.240 (3)C5—C61.387 (3)
O3—C181.279 (3)C5—H5A0.9300
O4—C181.237 (3)C6—C71.387 (3)
O5—H10.8500C6—C91.503 (3)
O5—H20.8500C7—C81.383 (3)
O6—H30.8500C7—H7A0.9300
O6—H40.8500C8—H8A0.9300
N1—C11.297 (3)C10—H10A0.9300
N1—N21.386 (3)C11—H11A0.9300
N2—C21.297 (3)C12—C131.384 (3)
N3—C11.357 (3)C12—C171.387 (3)
N3—C21.362 (3)C13—C141.382 (3)
N3—C31.430 (3)C13—H13A0.9300
N4—C101.293 (3)C14—C151.387 (3)
N4—N51.386 (3)C14—H14A0.9300
N5—C111.299 (3)C15—C161.396 (3)
N6—C111.357 (3)C15—C181.494 (3)
N6—C101.360 (3)C16—C171.380 (3)
N6—C121.427 (3)C16—H16A0.9300
C1—H1A0.9300C17—H17A0.9300
O3—Cu1—O1177.14 (6)C5—C6—C7118.9 (2)
O3—Cu1—O688.40 (7)C5—C6—C9120.6 (2)
O1—Cu1—O692.31 (7)C7—C6—C9120.5 (2)
O3—Cu1—O588.22 (7)C8—C7—C6121.1 (2)
O1—Cu1—O591.57 (7)C8—C7—H7A119.4
O6—Cu1—O5169.33 (8)C6—C7—H7A119.4
C9—O1—Cu1105.33 (14)C3—C8—C7119.0 (2)
C18—O3—Cu1104.21 (13)C3—C8—H8A120.5
Cu1—O5—H1111.5C7—C8—H8A120.5
Cu1—O5—H2111.5O2—C9—O1122.8 (2)
H1—O5—H2109.4O2—C9—C6119.6 (2)
Cu1—O6—H3112.1O1—C9—C6117.6 (2)
Cu1—O6—H4112.0N4—C10—N6110.8 (2)
H3—O6—H4109.9N4—C10—H10A124.6
C1—N1—N2106.90 (19)N6—C10—H10A124.6
C2—N2—N1107.38 (19)N5—C11—N6111.2 (2)
C1—N3—C2104.52 (18)N5—C11—H11A124.4
C1—N3—C3127.30 (19)N6—C11—H11A124.4
C2—N3—C3128.18 (19)C13—C12—C17120.9 (2)
C10—N4—N5107.4 (2)C13—C12—N6119.10 (19)
C11—N5—N4106.47 (19)C17—C12—N6120.01 (19)
C11—N6—C10104.05 (19)C14—C13—C12119.5 (2)
C11—N6—C12129.78 (19)C14—C13—H13A120.3
C10—N6—C12126.17 (19)C12—C13—H13A120.3
N1—C1—N3110.8 (2)C13—C14—C15120.7 (2)
N1—C1—H1A124.6C13—C14—H14A119.7
N3—C1—H1A124.6C15—C14—H14A119.7
N2—C2—N3110.4 (2)C14—C15—C16118.93 (19)
N2—C2—H2A124.8C14—C15—C18120.3 (2)
N3—C2—H2A124.8C16—C15—C18120.8 (2)
C4—C3—C8120.8 (2)C17—C16—C15120.9 (2)
C4—C3—N3118.71 (19)C17—C16—H16A119.5
C8—C3—N3120.5 (2)C15—C16—H16A119.5
C3—C4—C5119.7 (2)C16—C17—C12119.1 (2)
C3—C4—H4A120.1C16—C17—H17A120.5
C5—C4—H4A120.1C12—C17—H17A120.5
C4—C5—C6120.4 (2)O4—C18—O3122.34 (19)
C4—C5—H5A119.8O4—C18—C15120.6 (2)
C6—C5—H5A119.8O3—C18—C15117.01 (19)
O6—Cu1—O1—C985.23 (16)C7—C6—C9—O21.1 (3)
O5—Cu1—O1—C984.83 (15)C5—C6—C9—O10.1 (3)
O6—Cu1—O3—C1890.46 (15)C7—C6—C9—O1178.1 (2)
O5—Cu1—O3—C1899.66 (14)N5—N4—C10—N60.7 (3)
C1—N1—N2—C20.6 (3)C11—N6—C10—N40.4 (3)
C10—N4—N5—C110.6 (3)C12—N6—C10—N4179.5 (2)
N2—N1—C1—N30.6 (3)N4—N5—C11—N60.4 (3)
C2—N3—C1—N10.4 (3)C10—N6—C11—N50.0 (3)
C3—N3—C1—N1179.0 (2)C12—N6—C11—N5179.9 (2)
N1—N2—C2—N30.4 (3)C11—N6—C12—C13153.1 (2)
C1—N3—C2—N20.0 (3)C10—N6—C12—C1326.9 (3)
C3—N3—C2—N2179.4 (2)C11—N6—C12—C1727.1 (3)
C1—N3—C3—C428.3 (3)C10—N6—C12—C17152.8 (2)
C2—N3—C3—C4152.4 (2)C17—C12—C13—C141.4 (4)
C1—N3—C3—C8151.9 (2)N6—C12—C13—C14178.4 (2)
C2—N3—C3—C827.3 (3)C12—C13—C14—C151.1 (4)
C8—C3—C4—C51.4 (4)C13—C14—C15—C160.2 (3)
N3—C3—C4—C5178.9 (2)C13—C14—C15—C18179.2 (2)
C3—C4—C5—C60.7 (4)C14—C15—C16—C171.3 (3)
C4—C5—C6—C70.5 (4)C18—C15—C16—C17179.7 (2)
C4—C5—C6—C9178.8 (2)C15—C16—C17—C121.0 (4)
C5—C6—C7—C81.1 (4)C13—C12—C17—C160.3 (3)
C9—C6—C7—C8179.4 (2)N6—C12—C17—C16179.4 (2)
C4—C3—C8—C70.9 (4)Cu1—O3—C18—O45.7 (3)
N3—C3—C8—C7179.4 (2)Cu1—O3—C18—C15174.38 (15)
C6—C7—C8—C30.4 (4)C14—C15—C18—O48.5 (3)
Cu1—O1—C9—O24.6 (3)C16—C15—C18—O4172.6 (2)
Cu1—O1—C9—C6174.65 (16)C14—C15—C18—O3171.6 (2)
C5—C6—C9—O2179.4 (2)C16—C15—C18—O37.3 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O5—H1···N5i0.852.052.872 (3)163
O5—H2···N1ii0.851.992.790 (3)157
O6—H3···N2iii0.851.982.799 (3)162
O6—H4···N4iv0.851.982.749 (3)149
C2—H2A···O4v0.932.233.158 (3)175
C4—H4A···O5vi0.932.523.368 (3)152
C13—H13A···O2vii0.932.543.371 (3)150
Symmetry codes: (i) x+1, y, z; (ii) x1, y+3/2, z1/2; (iii) x1, y, z; (iv) x+1, y+3/2, z+1/2; (v) x+1, y1/2, z+1/2; (vi) x+1, y+1/2, z+1/2; (vii) x, y+1/2, z+1/2.
 

Follow Acta Cryst. C
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds