research communications
Structure of a dinuclear cadmium complex with 2,2′-bipyridine, monodentate nitrate and 3-carboxy-6-methylpyridine-2-carboxylate ligands: intramolecular carbonyl(lone pair)⋯π(ring) and nitrate(π)⋯π(ring) interactions
aDepartamento de Ciencias Químicas y Recursos Naturales, Facultad de Ingeniería y Ciencias, Universidad de La Frontera, Casilla 54-D, Temuco, Chile, bDepartamento de Química Inorgánica, Analítica y Química Física, INQUIMAE-CONICET, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, Buenos Aires, Argentina, and cGerencia de Investigación y Aplicaciones, Centro Atómico Constituyentes, Comisión Nacional de Energía Atómica, Buenos Aires, Argentina
*Correspondence e-mail: juan.granifo@ufrontera.cl, baggio@cnea.gov.ar
The centrosymmetric dinuclear complex bis(μ-3-carboxy-6-methylpyridine-2-carboxylato)-κ3N,O2:O2;κ3O2:N,O2-bis[(2,2′-bipyridine-κ2N,N′)(nitrato-κO)cadmium] methanol monosolvate, [Cd2(C8H6NO4)2(NO3)2(C10H8N2)2]·CH3OH, was isolated as colourless crystals from the reaction of Cd(NO3)2·4H2O, 6-methylpyridine-2,3-dicarboxylic acid (mepydcH2) and 2,2′-bipyridine in methanol. The consists of a CdII cation bound to a μ-κ3N,O2:O2-mepydcH− anion, an N,N′-bidentate 2,2′-bipyridine group and an O-monodentate nitrate anion, and is completed with a methanol solvent molecule at half-occupancy. The Cd complex unit is linked to its centrosymmetric image through a bridging mepydcH− carboxylate O atom to complete the dinuclear complex molecule. Despite a significant variation in the coordination angles, indicating a considerable departure from octahedral coordination geometry about the CdII atom, the Cd—O and Cd—N distances in this complex are surprisingly similar. The consists of O—H⋯O hydrogen-bonded chains parallel to a, further bound by C—H⋯O contacts along b to form planar two-dimensional arrays parallel to (001). The juxtaposed planes form interstitial columnar voids that are filled by the methanol solvent molecules. These in turn interact with the complex molecules to further stabilize the structure. A search in the literature showed that complexes with the mepydcH− ligand are rare and complexes reported previously with this ligand do not adopt the μ-κ3 coordination mode found in the title compound.
Keywords: crystal structure; dinuclear Cd complex; intramolecular C—O⋯π(ring) and N—O⋯π(ring) interactions.
CCDC reference: 1409269
1. Chemical context
Pyridinedicarboxylate ligands derived from pyridine-2,3-dicarboxylic acid (pydcH2) have been extensively used in the construction of a large variety of structural motifs. The two deprotonated forms pydcH− and pydc2− have been shown to adopt a wide range of coordination modes through their carboxylate oxygen and pyridyl nitrogen atoms (Wang et al., 2009). A search in the CSD (Version 5.3; Groom & Allen, 2014) disclosed ca 200 complexes displaying diverse topologies, viz. monomers (Gao et al., 2010; Drew et al., 1971), dimers (Shankar et al., 2013), oligomers (Yu et al., 2003) as well as one-dimensional (Semerci et al., 2014), two-dimensional (Çolak et al., 2011) and three-dimensional (Kanoo et al., 2012) polymers. In the vast majority of cases the ligand adopts an N,O-chelating mode, although there are a few exceptions to this where the binding sites attach to different metal atoms (e.g. Wang et al., 2014). By contrast, when complexes containing similar ligands but with methyl substituents in the 6-position were sought, namely those generated from 6-methylpyridine-2,3-dicarboxylic acid (mepydcH2), only a single structure was found involving the monoanionic mepydcH− ligand similar to that reported here (Gurunatha & Maji, 2009). This unique structural motif appears in the form of three isostructural, monomeric MII (M = Fe, Co, Ni) complexes [M(bpee)2(mepydcH)2] (bpee = 1,2-bis(4-pyridyl)ethylene) with octahedral geometry around MII. Both mepydcH− fragments act in a simple κ2N,O2-chelating mode binding to a single nucleus while the two N-bound bpee ligands are trans-monodentate. The formation of these mononuclear complexes is unusual considering the obvious bridging potential of the bpee ligands. Mixed-ligand complexes based on non-methylated 2,3-pyridinedicarboxylate and 4,4′-bipyridine-like ligands usually generate stable polymeric structures with the exo-bidentate ligands adopting a bridging role (Kanoo et al., 2012; Wang et al., 2009; Maji et al., 2005).
In an attempt to understand the coordination behaviour of this unusual monoanionic mepydcH− ligand better, we report the structure of the dinuclear complex [Cd2(2,2′-bipyridine)2(mepydcH)2(NO3)2]·MeOH (I). The uncommon bridging-chelating μ2-(κ3N,O2:O2) coordination behaviour and the fact that the ligand is only singly deprotonated has no counterpart in complexes of the non-methylated ligands and makes this a genuinely novel structure. The closest relatives with 2,2′-bipyridine as the auxiliary ligand are found with di-anionic pydc2− ligands, but these are either mononuclear (Wang & Okabe, 2005) or form coordination polymers (Li et al., 2013; Yin & Liu, 2009; Zhang et al. 2013).
2. Structural commentary
The complex consists of a CdII cation to which a singly protonated 3-carboxy-6-methylpyridine-2-carboxylate ion (mepydcH−) chelates through the pyridine N and carboxylate O atoms. A chelating 2,2′-bipyridine that binds through both nitrogen atoms and a unidentate nitrate anion complete the coordination sphere; the also contains a non-coordinating half-occupancy methanol solvate. This five coordinate CdII unit, in turn, binds to its centrosymmetric image through the carboxylate oxygen atom of the mepydcH− ligand, forming a pair of Cd–O–Cd bridges. As a result, a dimeric unit forms (Fig. 1) with each CdII atom in a six-coordinate N3O3 ligand environment. The Cd—X (X = N or O) distances are reasonable, spanning the range 2.304 (2)–2.332 (3) Å. However, the coordination angles vary widely [X–Cd–X ranges: cis 71.15 (10)–115.79 (9)°; trans 142.36 (8)–159.48 (9)°]; the result is a rather distorted octahedral geometry around Cd1. Selected geometric parameters are shown in Table 1; the bridging Cd—O distances are the shortest in the coordination sphere, 2.304 (2) and 2.310 (2) Å, resulting in a Cd⋯Cd separation of 3.700 (3) Å. This value is slightly larger than the mean for similar environments found in the CSD (3.61 Å for 885 cases), though well within the sample standard deviation (0.22 Å).
3. Supramolecular features
The viz., hydrogen bonds (Table 2), C=O⋯π and nitrate(π)⋯π contacts (Table 3). These interactions can be clearly differentiated according to the that they support:
made up of isolated dimers, is sustained by three different types of non-covalent interaction,
|
a) Contacts #1 (Table 2) and #9, #10 (Table 3) are internal to the dinuclear motif, as shown in Fig. 1. The first one links the bipyridine C10A—H10A group with the coordinating nitrate oxygen O1C. Contact #9 is a typical lone pair–π interaction with a dihedral angle of 72.19° between the carboxylate and the ring plane, and a C—O⋯Cg2 angle of 126.63°. These values are close to those for the ideal geometry (90° and 120°, respectively) when a lone pair provided by a carbonyl oxygen points toward the centroid of an aromatic ring (Egli & Sarkhel, 2007). By contrast, in contact #10 the orientation of the nitrate plane is more or less parallel to the ring plane (6.84°), suggesting a π–π interaction with the π-orbitals of the nitrate fragment interacting with those of the aromatic ring. A similar argument has already been applied by Frontera et al. (2011) and García-Raso et al. (2009) when nitrate anions interact with pyrimidinium rings. These carbonyl(lone pair)⋯π(ring) (#9) and nitrate(π)⋯π(ring) (#10) interactions in (I) fulfill a relevant function, serving to strengthen the dimeric unit (Fig. 1).
b) Strong intermolecular O—H⋯O contacts #2 (Table 2) involving the hydrogen atom of the free carboxylic acid group of the mepydcH− ligand with a non-bonded oxygen atom of a nitrate ligand, has the pivotal action of linking the dimers along a, forming chains parallel to [100] (Fig. 2).
c) C—H⋯O interactions #3, #4 and #5 (Table 2), in turn, serve to link the above chains laterally along b, to form 2D substructures parallel to (001) (Fig. 3a). These planes juxtapose along [001] with rather weak direct interactions. In the process, however, significant columnar voids parallel to the chains are formed (with a volume 13% of the total cell volume, Fig. 3b) in which the partial occupancy methanol solvate molecules reside. These are not free, but enter instead into a number of weak C—H⋯O, O—H⋯O and C—H⋯π interactions (#6, #7 and #8 in Table 2) linking them to a framework of complex molecules, further stabilizing the structure.
4. ATR (attenuated total reflectance) FT–IR spectroscopy
The IR spectra of mepydcH2, 2.2′-bipyridine and (I) were recorded on an Agilent Cary 630 FT–IR spectrometer with Varian Resolutions Pro software, using a Diamond ATR accessory. The FT–IR spectrum of (I) (Fig. 4) was recorded in the 4000–600 cm−1 range, and confirms the structural data indicating the presence of the coordinating nitrate and mepydcH− anions. Bands due to the unidentate NO3− group were found at 1478 and 1298 cm−1 and appear due to the νasym(ONO) and νsym(ONO) vibrations, with a shoulder at 1010 cm−1 due to the ν(NO) stretching modes of nitrate groups (Nakamoto, 1997). The carboxylic acid group (COOH) of the mepydcH− ligand in complex (I) is identified by a weak band at 3083 cm−1, ν(OH) stretching for a hydrogen-bonded system (Alisir et al., 2013), and a very strong band at 1738 cm−1, ν(C=O) stretch. The deprotonated carboxylate (COO−) is characterized by the asymmetric and symmetric stretching modes νas at 1593 cm−1 and νs at 1322 cm−1. This confirms the unidentate coordination of the carboxylate O atom, with the difference between these frequencies being > 200 cm−1(Δ = νas − νs = 271 cm−1) (Deacon & Phillips, 1980). Finally, around 1400 cm−1, a set of three bands appears (1412, 1391 and 1369 cm−1) of almost equal intensity due to the ν(C=C) + ν(C=N) vibrations from the coordinating 2,2′-bipyridine ligand (Yan et al., 2011).
5. Synthesis and crystallization
Solid 2,2′-bipyridine (0.031 g, 0.20 mmol) was added to a solution prepared by disolving Cd(NO3)·4H2O (0.062 g, 0.20 mmol) and mepydcH2 (0.036 g, 0.20 mmol) in MeOH (4.0 mL). The mixture was stirred to dissolve the 2,2′-bipyridine and was then allowed to stand undisturbed at room temperature in an uncovered 10 mL beaker. Colourless single crystals of compound (I) suitable for X-ray diffraction were obtained within 8 h. The crystals were separated by filtration, washed with MeOH (2 x 2 mL) and diethyl ether (2 x 3 mL) (yield: 0.045 g, 44%).
6. Refinement
Relevant crystallographic data for (I) as well as pertinent experimental details are provided in Table 4. H atoms bonded to C were found in a difference Fourier map, but were then idealized and refined as riding atoms; C—Harom: 0.93 Å, Ueq(H) = 1.2Ueq(C); C—Hmethyl: 0.97 Å, Ueq(H) = 1.5Ueq(C). The O—H hydrogen atom was refined with a restrained O—H distance [0.85 (1)Å], and with U(H) = 1.2Ueq(O). The methanol solvate was refined at half occupancy.
|
Supporting information
CCDC reference: 1409269
https://doi.org/10.1107/S2056989015012384/sj5468sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989015012384/sj5468Isup2.hkl
Data collection: CrysAlis PRO (Oxford Diffraction, 2009); cell
CrysAlis PRO (Oxford Diffraction, 2009); data reduction: CrysAlis PRO (Oxford Diffraction, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL2014 (Sheldrick, 2015) and PLATON (Spek, 2009).[Cd2(C8H6NO4)2(NO3)2(C10H8N2)2]·CH4O | Z = 1 |
Mr = 1053.50 | F(000) = 526 |
Triclinic, P1 | Dx = 1.746 Mg m−3 |
a = 8.4096 (5) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 10.9626 (6) Å | Cell parameters from 2675 reflections |
c = 11.5056 (4) Å | θ = 3.8–28.8° |
α = 71.241 (4)° | µ = 1.14 mm−1 |
β = 86.537 (4)° | T = 295 K |
γ = 86.803 (5)° | Block, colourless |
V = 1001.79 (9) Å3 | 0.36 × 0.14 × 0.10 mm |
Oxford Diffraction Gemini CCD S Ultra diffractometer | 4155 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.057 |
ω scans, thick slices | θmax = 29.1°, θmin = 3.6° |
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | h = −11→11 |
k = −14→14 | |
21744 measured reflections | l = −15→15 |
4819 independent reflections |
Refinement on F2 | 4 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.036 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.092 | w = 1/[σ2(Fo2) + (0.0394P)2 + 1.5425P] where P = (Fo2 + 2Fc2)/3 |
S = 1.01 | (Δ/σ)max < 0.001 |
4819 reflections | Δρmax = 1.07 e Å−3 |
298 parameters | Δρmin = −0.74 e Å−3 |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Cd1 | 0.47993 (3) | 0.63548 (2) | 0.35527 (2) | 0.01961 (9) | |
N1A | 0.6981 (3) | 0.7364 (3) | 0.3922 (3) | 0.0229 (6) | |
N2A | 0.4198 (3) | 0.8540 (3) | 0.3047 (2) | 0.0223 (6) | |
C1A | 0.8378 (4) | 0.6740 (4) | 0.4272 (3) | 0.0279 (7) | |
H1A | 0.8516 | 0.5882 | 0.4306 | 0.033* | |
C2A | 0.9614 (4) | 0.7331 (4) | 0.4581 (3) | 0.0292 (8) | |
H2A | 1.0575 | 0.6883 | 0.4821 | 0.035* | |
C3A | 0.9393 (4) | 0.8601 (4) | 0.4526 (3) | 0.0312 (8) | |
H3A | 1.0204 | 0.9020 | 0.4740 | 0.037* | |
C4A | 0.7968 (4) | 0.9252 (4) | 0.4152 (3) | 0.0286 (7) | |
H4A | 0.7812 | 1.0114 | 0.4104 | 0.034* | |
C5A | 0.6771 (4) | 0.8603 (3) | 0.3851 (3) | 0.0196 (6) | |
C6A | 0.5211 (4) | 0.9244 (3) | 0.3409 (3) | 0.0201 (6) | |
C7A | 0.4801 (4) | 1.0501 (3) | 0.3369 (3) | 0.0263 (7) | |
H7A | 0.5504 | 1.0976 | 0.3629 | 0.032* | |
C8A | 0.3343 (4) | 1.1041 (3) | 0.2940 (3) | 0.0286 (8) | |
H8A | 0.3048 | 1.1877 | 0.2920 | 0.034* | |
C9A | 0.2327 (4) | 1.0328 (3) | 0.2540 (3) | 0.0303 (8) | |
H9A | 0.1348 | 1.0679 | 0.2230 | 0.036* | |
C10A | 0.2801 (4) | 0.9084 (3) | 0.2614 (3) | 0.0280 (7) | |
H10A | 0.2116 | 0.8599 | 0.2351 | 0.034* | |
O1B | 0.6097 (3) | 0.4384 (2) | 0.44192 (19) | 0.0216 (5) | |
O2B | 0.7028 (3) | 0.2598 (2) | 0.4031 (2) | 0.0256 (5) | |
O3B | 0.8147 (3) | 0.1816 (3) | 0.1644 (3) | 0.0390 (6) | |
O4B | 0.9923 (3) | 0.2717 (3) | 0.2400 (3) | 0.0340 (6) | |
H4BO | 1.004 (6) | 0.344 (2) | 0.248 (4) | 0.051 (14)* | |
N1B | 0.5964 (3) | 0.5661 (3) | 0.1972 (2) | 0.0200 (5) | |
C1B | 0.6745 (4) | 0.4503 (3) | 0.2349 (3) | 0.0185 (6) | |
C2B | 0.7605 (4) | 0.3994 (3) | 0.1523 (3) | 0.0226 (7) | |
C3B | 0.7607 (5) | 0.4714 (4) | 0.0288 (3) | 0.0316 (8) | |
H3B | 0.8164 | 0.4402 | −0.0288 | 0.038* | |
C4B | 0.6796 (5) | 0.5880 (4) | −0.0090 (3) | 0.0343 (9) | |
H4B | 0.6799 | 0.6361 | −0.0919 | 0.041* | |
C5B | 0.5963 (4) | 0.6345 (3) | 0.0780 (3) | 0.0255 (7) | |
C6B | 0.6608 (4) | 0.3736 (3) | 0.3714 (3) | 0.0185 (6) | |
C7B | 0.8543 (4) | 0.2739 (3) | 0.1893 (3) | 0.0265 (7) | |
C8B | 0.5036 (5) | 0.7606 (4) | 0.0418 (3) | 0.0376 (9) | |
H8BA | 0.5131 | 0.7999 | −0.0457 | 0.056* | |
H8BB | 0.3934 | 0.7462 | 0.0669 | 0.056* | |
H8BC | 0.5448 | 0.8166 | 0.0811 | 0.056* | |
N1C | 0.1872 (3) | 0.5118 (3) | 0.2872 (2) | 0.0248 (6) | |
O1C | 0.2228 (3) | 0.6168 (3) | 0.3000 (3) | 0.0350 (6) | |
O2C | 0.2871 (3) | 0.4227 (3) | 0.2993 (3) | 0.0341 (6) | |
O3C | 0.0460 (3) | 0.5009 (3) | 0.2619 (3) | 0.0374 (6) | |
O1M | 0.7710 (10) | 0.9624 (9) | 0.0748 (8) | 0.072 (2) | 0.5 |
H1M | 0.816 (4) | 1.0346 (13) | 0.046 (17) | 0.18 (9)* | 0.5 |
C1M | 0.8993 (11) | 0.8676 (10) | 0.0932 (8) | 0.060 (3) | 0.5 |
H1M1 | 0.9936 | 0.9068 | 0.0490 | 0.090* | 0.5 |
H1M2 | 0.8713 | 0.7994 | 0.0637 | 0.090* | 0.5 |
H1M3 | 0.9189 | 0.8331 | 0.1792 | 0.090* | 0.5 |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cd1 | 0.02114 (13) | 0.01596 (13) | 0.02201 (13) | 0.00148 (9) | −0.00289 (9) | −0.00650 (9) |
N1A | 0.0207 (14) | 0.0214 (14) | 0.0274 (14) | −0.0001 (11) | −0.0030 (11) | −0.0087 (11) |
N2A | 0.0226 (14) | 0.0178 (14) | 0.0259 (14) | 0.0016 (11) | −0.0031 (11) | −0.0062 (11) |
C1A | 0.0255 (17) | 0.0252 (18) | 0.0331 (18) | 0.0027 (14) | −0.0037 (14) | −0.0095 (15) |
C2A | 0.0201 (16) | 0.038 (2) | 0.0293 (18) | −0.0008 (15) | −0.0038 (14) | −0.0105 (16) |
C3A | 0.0261 (18) | 0.040 (2) | 0.0324 (19) | −0.0088 (16) | −0.0041 (15) | −0.0166 (16) |
C4A | 0.0336 (19) | 0.0228 (18) | 0.0327 (18) | −0.0046 (15) | −0.0020 (15) | −0.0129 (15) |
C5A | 0.0216 (15) | 0.0188 (16) | 0.0192 (14) | −0.0028 (12) | 0.0002 (12) | −0.0069 (12) |
C6A | 0.0231 (16) | 0.0182 (16) | 0.0181 (14) | −0.0022 (13) | 0.0004 (12) | −0.0048 (12) |
C7A | 0.0312 (18) | 0.0193 (17) | 0.0279 (17) | −0.0039 (14) | 0.0003 (14) | −0.0069 (14) |
C8A | 0.036 (2) | 0.0169 (17) | 0.0293 (18) | 0.0031 (14) | 0.0055 (15) | −0.0043 (14) |
C9A | 0.0277 (18) | 0.0239 (18) | 0.0374 (19) | 0.0089 (15) | −0.0044 (15) | −0.0083 (15) |
C10A | 0.0248 (17) | 0.0228 (18) | 0.0363 (19) | 0.0030 (14) | −0.0067 (14) | −0.0089 (15) |
O1B | 0.0278 (12) | 0.0180 (11) | 0.0185 (11) | 0.0049 (9) | 0.0004 (9) | −0.0062 (9) |
O2B | 0.0328 (13) | 0.0168 (12) | 0.0271 (12) | 0.0025 (10) | −0.0033 (10) | −0.0073 (10) |
O3B | 0.0471 (17) | 0.0307 (15) | 0.0461 (16) | 0.0020 (12) | −0.0037 (13) | −0.0221 (13) |
O4B | 0.0265 (13) | 0.0314 (15) | 0.0481 (16) | 0.0076 (11) | −0.0078 (11) | −0.0182 (13) |
N1B | 0.0196 (13) | 0.0185 (14) | 0.0216 (13) | −0.0010 (11) | −0.0033 (10) | −0.0055 (11) |
C1B | 0.0173 (14) | 0.0193 (16) | 0.0208 (15) | −0.0016 (12) | −0.0047 (12) | −0.0082 (12) |
C2B | 0.0197 (16) | 0.0245 (17) | 0.0259 (16) | −0.0017 (13) | −0.0012 (13) | −0.0110 (14) |
C3B | 0.038 (2) | 0.035 (2) | 0.0234 (17) | 0.0039 (16) | 0.0038 (15) | −0.0126 (15) |
C4B | 0.047 (2) | 0.032 (2) | 0.0203 (16) | 0.0064 (17) | −0.0004 (15) | −0.0051 (15) |
C5B | 0.0295 (18) | 0.0226 (17) | 0.0234 (16) | 0.0013 (14) | −0.0052 (13) | −0.0055 (13) |
C6B | 0.0156 (14) | 0.0181 (16) | 0.0237 (15) | −0.0006 (12) | −0.0029 (12) | −0.0088 (12) |
C7B | 0.0265 (17) | 0.0270 (19) | 0.0283 (17) | 0.0012 (14) | 0.0046 (14) | −0.0135 (15) |
C8B | 0.051 (2) | 0.032 (2) | 0.0256 (18) | 0.0103 (18) | −0.0058 (17) | −0.0053 (16) |
N1C | 0.0250 (15) | 0.0292 (16) | 0.0218 (13) | −0.0013 (12) | −0.0019 (11) | −0.0104 (12) |
O1C | 0.0264 (13) | 0.0315 (15) | 0.0561 (17) | 0.0001 (11) | −0.0092 (12) | −0.0254 (13) |
O2C | 0.0268 (13) | 0.0282 (14) | 0.0484 (16) | 0.0019 (11) | −0.0004 (11) | −0.0143 (12) |
O3C | 0.0253 (13) | 0.0381 (16) | 0.0555 (17) | −0.0034 (11) | −0.0108 (12) | −0.0224 (14) |
O1M | 0.078 (6) | 0.075 (6) | 0.077 (5) | −0.016 (5) | −0.010 (4) | −0.039 (5) |
C1M | 0.052 (6) | 0.097 (9) | 0.036 (5) | −0.018 (6) | −0.010 (4) | −0.023 (5) |
Cd1—O1Bi | 2.304 (2) | O1B—C6B | 1.281 (4) |
Cd1—O1B | 2.310 (2) | O2B—C6B | 1.220 (4) |
Cd1—N2A | 2.310 (3) | O3B—C7B | 1.205 (4) |
Cd1—N1A | 2.323 (3) | O4B—C7B | 1.326 (4) |
Cd1—O1C | 2.329 (2) | O4B—H4BO | 0.845 (10) |
Cd1—N1B | 2.332 (3) | N1B—C5B | 1.336 (4) |
N1A—C5A | 1.336 (4) | N1B—C1B | 1.348 (4) |
N1A—C1A | 1.342 (4) | C1B—C2B | 1.397 (4) |
N2A—C10A | 1.336 (4) | C1B—C6B | 1.525 (4) |
N2A—C6A | 1.349 (4) | C2B—C3B | 1.386 (5) |
C1A—C2A | 1.377 (5) | C2B—C7B | 1.496 (5) |
C1A—H1A | 0.9300 | C3B—C4B | 1.367 (5) |
C2A—C3A | 1.375 (5) | C3B—H3B | 0.9300 |
C2A—H2A | 0.9300 | C4B—C5B | 1.398 (5) |
C3A—C4A | 1.378 (5) | C4B—H4B | 0.9300 |
C3A—H3A | 0.9300 | C5B—C8B | 1.497 (5) |
C4A—C5A | 1.387 (5) | C8B—H8BA | 0.9600 |
C4A—H4A | 0.9300 | C8B—H8BB | 0.9600 |
C5A—C6A | 1.490 (4) | C8B—H8BC | 0.9600 |
C6A—C7A | 1.389 (5) | N1C—O2C | 1.230 (4) |
C7A—C8A | 1.379 (5) | N1C—O3C | 1.260 (4) |
C7A—H7A | 0.9300 | N1C—O1C | 1.261 (4) |
C8A—C9A | 1.380 (5) | O1M—C1M | 1.431 (8) |
C8A—H8A | 0.9300 | O1M—H1M | 0.855 (10) |
C9A—C10A | 1.377 (5) | C1M—H1M1 | 0.9600 |
C9A—H9A | 0.9300 | C1M—H1M2 | 0.9600 |
C10A—H10A | 0.9300 | C1M—H1M3 | 0.9600 |
O1Bi—Cd1—O1B | 73.38 (8) | N2A—C10A—C9A | 123.1 (3) |
O1Bi—Cd1—N2A | 101.83 (9) | N2A—C10A—H10A | 118.4 |
O1B—Cd1—N2A | 159.48 (9) | C9A—C10A—H10A | 118.4 |
O1Bi—Cd1—N1A | 94.90 (9) | C6B—O1B—Cd1i | 128.9 (2) |
O1B—Cd1—N1A | 89.17 (9) | C6B—O1B—Cd1 | 118.42 (19) |
N2A—Cd1—N1A | 71.15 (10) | Cd1i—O1B—Cd1 | 106.62 (8) |
O1Bi—Cd1—O1C | 88.36 (9) | C7B—O4B—H4BO | 109 (3) |
O1B—Cd1—O1C | 112.97 (9) | C5B—N1B—C1B | 120.4 (3) |
N2A—Cd1—O1C | 86.44 (9) | C5B—N1B—Cd1 | 124.9 (2) |
N1A—Cd1—O1C | 157.56 (10) | C1B—N1B—Cd1 | 114.7 (2) |
O1Bi—Cd1—N1B | 142.36 (8) | N1B—C1B—C2B | 121.7 (3) |
O1B—Cd1—N1B | 71.66 (8) | N1B—C1B—C6B | 117.5 (3) |
N2A—Cd1—N1B | 115.79 (9) | C2B—C1B—C6B | 120.7 (3) |
N1A—Cd1—N1B | 98.09 (9) | C3B—C2B—C1B | 117.6 (3) |
O1C—Cd1—N1B | 92.65 (9) | C3B—C2B—C7B | 118.4 (3) |
C5A—N1A—C1A | 119.8 (3) | C1B—C2B—C7B | 124.1 (3) |
C5A—N1A—Cd1 | 117.1 (2) | C4B—C3B—C2B | 120.4 (3) |
C1A—N1A—Cd1 | 123.0 (2) | C4B—C3B—H3B | 119.8 |
C10A—N2A—C6A | 118.9 (3) | C2B—C3B—H3B | 119.8 |
C10A—N2A—Cd1 | 123.4 (2) | C3B—C4B—C5B | 119.6 (3) |
C6A—N2A—Cd1 | 116.7 (2) | C3B—C4B—H4B | 120.2 |
N1A—C1A—C2A | 122.1 (3) | C5B—C4B—H4B | 120.2 |
N1A—C1A—H1A | 119.0 | N1B—C5B—C4B | 120.4 (3) |
C2A—C1A—H1A | 119.0 | N1B—C5B—C8B | 117.7 (3) |
C3A—C2A—C1A | 118.3 (3) | C4B—C5B—C8B | 121.9 (3) |
C3A—C2A—H2A | 120.9 | O2B—C6B—O1B | 126.7 (3) |
C1A—C2A—H2A | 120.9 | O2B—C6B—C1B | 118.0 (3) |
C2A—C3A—C4A | 119.9 (3) | O1B—C6B—C1B | 115.3 (3) |
C2A—C3A—H3A | 120.0 | O3B—C7B—O4B | 120.6 (3) |
C4A—C3A—H3A | 120.0 | O3B—C7B—C2B | 122.0 (3) |
C3A—C4A—C5A | 118.9 (3) | O4B—C7B—C2B | 117.1 (3) |
C3A—C4A—H4A | 120.5 | C5B—C8B—H8BA | 109.5 |
C5A—C4A—H4A | 120.5 | C5B—C8B—H8BB | 109.5 |
N1A—C5A—C4A | 121.0 (3) | H8BA—C8B—H8BB | 109.5 |
N1A—C5A—C6A | 116.7 (3) | C5B—C8B—H8BC | 109.5 |
C4A—C5A—C6A | 122.3 (3) | H8BA—C8B—H8BC | 109.5 |
N2A—C6A—C7A | 121.0 (3) | H8BB—C8B—H8BC | 109.5 |
N2A—C6A—C5A | 116.6 (3) | O2C—N1C—O3C | 121.1 (3) |
C7A—C6A—C5A | 122.4 (3) | O2C—N1C—O1C | 121.0 (3) |
C8A—C7A—C6A | 119.4 (3) | O3C—N1C—O1C | 117.9 (3) |
C8A—C7A—H7A | 120.3 | N1C—O1C—Cd1 | 118.4 (2) |
C6A—C7A—H7A | 120.3 | C1M—O1M—H1M | 104.7 (13) |
C7A—C8A—C9A | 119.4 (3) | O1M—C1M—H1M1 | 109.5 |
C7A—C8A—H8A | 120.3 | O1M—C1M—H1M2 | 109.5 |
C9A—C8A—H8A | 120.3 | H1M1—C1M—H1M2 | 109.5 |
C10A—C9A—C8A | 118.2 (3) | O1M—C1M—H1M3 | 109.5 |
C10A—C9A—H9A | 120.9 | H1M1—C1M—H1M3 | 109.5 |
C8A—C9A—H9A | 120.9 | H1M2—C1M—H1M3 | 109.5 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
Cg1 is the centroid of the N1A/C1A–C5A ring. |
Int.# | D—H···A | D—H | H···A | D···A | D—H···A |
#1 | C10A—H10A···O1C | 0.93 | 2.52 | 3.143 (5) | 124 |
#2 | O4B—H4BO···O3Cii | 0.84 (3) | 1.83 (3) | 2.670 (5) | 176 (6) |
#3 | C7A—H7A···O2Biii | 0.93 | 2.42 | 3.339 (4) | 168 |
#4 | C8A—H8A···O2Ciii | 0.93 | 2.59 | 3.51 (4) | 167 |
#5 | C9A—H9A···O4Biv | 0.93 | 2.53 | 3.186 (5) | 127 |
#6 | C8B—H8BC···O1M | 0.960 | 2.54 | 3.361 (8) | 144 |
#7 | O1M—H1M···O3Biii | 0.85 (5) | 2.42 (9) | 2.951 (9) | 121 (9) |
#8 | C1M—H1M3···Cg1 | 0.96 | 2.78 | 3.640 | 149 |
Symmetry codes: (ii) 1 + x, y, z; (iii) x, 1 + y, z; (iv) -1 + x, 1 + y, z. |
Cg1 is the centroid of the N1A/C1A–C5A ring and Cg2 is the centroid of the N2A/C6A–C10A ring. |
Int.# | X—O···Cg | O···Cg | X—O···Cg |
#9 | C6B-O2B···Cg2i | 3.637 (3) | 126.6 (2) |
#10 | N1C-O2C···Cg1i | 3.442 (4) | 104.2 (2) |
Symmetry code: (i) 1 - x, 1 - y, 1 - z. |
Acknowledgements
The authors acknowledge the Universidad de La Frontera (Proyecto DIUFRO DI15–0027) and ANPCyT (project No. PME 2006–01113) for the purchase of the Oxford Gemini CCD diffractometer.
References
Alisir, S. H., Sariboga, B., Topcu, Y. & Yang, S.-Y. (2013). J. Inorg. Organomet. Polym. 23, 1061–1067. Web of Science CSD CrossRef CAS Google Scholar
Çolak, A. T., Pamuk, G., Yeşilel, O. K. & Yüksel, F. (2011). Solid State Sci. 13, 2100–2104. Google Scholar
Deacon, G. B. & Phillips, R. J. (1980). Coord. Chem. Rev. 33, 227–250. CrossRef CAS Web of Science Google Scholar
Drew, M. G. B., Matthews, R. W. & Walton, R. A. (1971). J. Chem. Soc. A, pp. 2959–2962. CSD CrossRef Web of Science Google Scholar
Egli, M. & Sarkhel, S. (2007). Acc. Chem. Res. 40, 197–205. Web of Science CrossRef PubMed CAS Google Scholar
Frontera, A., Gamez, P., Mascal, M., Mooibroek, T. J. & Reedijk, J. (2011). Angew. Chem. Int. Ed. 50, 9564–9583. Web of Science CrossRef CAS Google Scholar
Gao, E.-J., Zhu, M.-C., Huang, Y., Liu, L., Liu, H.-Y., Liu, F.-C., Ma, S. & Shi, C.-Y. (2010). Eur. J. Med. Chem. 45, 1034–1041. Web of Science CSD CrossRef CAS PubMed Google Scholar
García-Raso, A., Albertí, F. M., Fiol, J. J., Tasada, A., Barceló-Oliver, M., Molins, E., Estarellas, C., Frontera, A., Quiñonero, D. & Deyà, P. M. (2009). Cryst. Growth Des. 9, 2363–2376. Google Scholar
Groom, C. R. & Allen, F. H. (2014). Angew. Chem. Int. Ed. 53, 662–671. Web of Science CSD CrossRef CAS Google Scholar
Gurunatha, K. L. & Maji, T. K. (2009). Inorg. Chim. Acta, 362, 1541–1545. Web of Science CSD CrossRef CAS Google Scholar
Kanoo, P., Matsuda, R., Kitaura, R., Kitagawa, S. & Maji, T. K. (2012). Inorg. Chem. 51, 9141–9143. Web of Science CSD CrossRef CAS PubMed Google Scholar
Li, W., Li, C.-H., Li, H.-F., Xu, J.-S. & Li, L. (2013). Jiegou Huaxue, 32, 1567–1571. CAS Google Scholar
Maji, T. K., Mostafa, G., Matsuda, R. & Kitagawa, S. (2005). J. Am. Chem. Soc. 127, 17152–17153. Web of Science CSD CrossRef PubMed CAS Google Scholar
Nakamoto, K. (1997). Infrared and Raman Spectra of Inorganic and Coordination Compounds, 5th ed. New York: Wiley & Sons. Google Scholar
Oxford Diffraction (2009). CrysAlis PRO. Oxford Diffraction Ltd, Abingdon, England. Google Scholar
Semerci, F., Yeşilel, O. Z., Ölmez, H. & Büyükgüngör, O. (2014). Inorg. Chim. Acta, 409, 407–417. Web of Science CSD CrossRef CAS Google Scholar
Shankar, K., Das, B. & Baruah, J. B. (2013). Eur. J. Inorg. Chem. pp. 6147–6155. Web of Science CSD CrossRef Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Sheldrick, G. M. (2015). Acta Cryst. C71, 3–8. Web of Science CrossRef IUCr Journals Google Scholar
Spek, A. L. (2009). Acta Cryst. D65, 148–155. Web of Science CrossRef CAS IUCr Journals Google Scholar
Wang, G.-H., Li, Z.-G., Jia, H.-Q., Hu, N.-H. & Xu, J.-W. (2009). CrystEngComm, 11, 292–297. Web of Science CSD CrossRef CAS Google Scholar
Wang, Y. & Okabe, N. (2005). Chem. Pharm. Bull. 53, 366–373. Web of Science CSD CrossRef PubMed CAS Google Scholar
Wang, D.-F., Wang, Z.-H., Zhang, T., Huang, R.-B. & Zheng, L.-S. (2014). J. Mol. Struct. 1068, 210–215. Web of Science CSD CrossRef CAS Google Scholar
Yan, B., Hodsdon, S. A., Li, Y.-F., Carmichael, C. N., Cao, Y. & Pan, W.-P. (2011). J. Solid State Chem. 184, 3179–3184. Web of Science CSD CrossRef CAS Google Scholar
Yin, H. & Liu, S.-X. (2009). J. Mol. Struct. 918, 165–173. Web of Science CSD CrossRef CAS Google Scholar
Yu, Z.-T., Li, G.-H., Jiang, Y.-S., Xu, J.-J. & Chen, J.-S. (2003). Dalton Trans. pp. 4219–4220. Web of Science CSD CrossRef Google Scholar
Zhang, C., Zhang, L.-Y., Wang, S.-L. & Huang, Q. (2013). Z. Kristallogr. New Cryst. Struct. 228, 265–266. CAS Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.