Download citation
Download citation
link to html
The design and synthesis of new organic lgands is important to the rapid development of coordination polymers (CPs). However, CPs based on asym­metric ligands are still rare, mainly because such ligands are usually expensive and more difficult to synthesize. The new asymmetric ligand 4-[4-(1H-imidazol-1-yl)phen­yl]pyridine (IPP) has been used to construct the title one-dimensional coordination polymer, catena-poly[[[aqua­{4-[4-(1H-imidazol-1-yl-κN3)phen­yl]pyridine}­cadmium(II)]-μ-5-hy­droxy­benzene-1,3-di­carboxyl­ato-κ3O1,O1′:O3] monohydrate], {[Cd(C8H4O5)(C14H11N3)2(H2O)]·H2O}n, under hydro­thermal reaction of IPP with CdII in the presence of 5-hy­droxy­isophthalic acid (5-OH-H2bdc). The CdII cation is coordinated by two N atoms from two distinct IPP ligands, three carboxyl­ate O atoms from two different 5-OH-bdc2− dianionic ligands and one water O atom in a distorted octa­hedral geometry. The cationic [Cd(IPP)2]2+ nodes are linked by 5-OH-bdc2− ligands to generate a one-dimensional chain. These chains are extended into a two-dimensional layer structure via O—H...O and O—H...N hydrogen bonds and π–π inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229616004587/fn3215sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229616004587/fn3215Isup3.hkl
Contains datablock I

CCDC reference: 1469060

Introduction top

The design and synthesis of new organic lgands is extremely important to the rapid development of coordination polymers (CPs) (Almeida Paz et al., 2012). In recent decades, numerous symmetric organic ligands have been synthesized and employed to construct CPs with different structures and potential applications. Among them, two structurally similar ligands 1,4-bis­(imidazol-1-yl)benzene (bimb) and 1,4-bis­(4-pyridyl)­benzene (bpbenz) have been used widely in the synthesis of CPs as linear ditopic ligands. It has been reported that bimb reacts with Cd(BF4)2·6H2O (Li et al., 2010) to generate a double inter­penetrating α-Po network, while bpbenz reacts with Cd(NO3)2·6H2O to generate a three-dimensional pillar–layer framework (Guo et al., 2012). However, CPs based on asymmetric ligands are still rare. This is mainly because such ligands are usually expensive and more difficult to synthesize. As far as we know, there is some probability that the noncentrosymmetry of the asymmetric organic ligands could be transferred into the framework of the CPs and some symmetry-dependent properties such as piezoelectricity, pyroelectricity, ferroelectricity and second-order nonlinear optics (Zhang & Xiong, 2012) may thus occur in these noncentrosymmetric CPs. Therefore, we designed and synthesized a new asymmetric heterobifunctional organic ligand, 4-[4-(1H-imidazol-1-yl)phenyl]­pyridine (IPP), containing both pyridine and imidazole rings. Reacting IPP, we successfully obtained a new cadmium coordination polymer, {[Cd(5—OH-bdc)(IPP)2(H2O)]·H2O}n (I), the crystal structure of (I) we now report.

Experimental top

Synthesis and crystallization top

For the synthesis of IPP, a mixture of tetra­kis(tri­phenyl­phosphane)palladium (0.08 g, 0.05 mmol), 1,4-di­bromo­benzene (2.36 g, 10 mmol), (pyridin-4-yl)boronic acid (1.00 g, 7.5 mmol) and K2CO3 (5.52 g, 4.0 mmol) in anhydrous N,N-di­methyl­formamide (DMF, 30 ml) in a 100 ml two-necked round-bottomed flask under N2 was stirred at 363 K for 48 h. The reaction mixture was filtered and the collected solid was purified on a silica-gel column using petroleum ether and ethyl acetate (3:1 v/v) as eluent to afford the 4-pyridyl bromo­benzene [ambiguous, please clarify ]. A mixture of CuI (0.09 g, 0.5 mmol), 4-pyridyl bromo­benzene (2.46 g, 10 mmol), imidazole (1.36 g, 2.0 mmol) and K2CO3 (2.76 g, 2.0 mmol) in DMF (30 ml) in a 100 ml two-necked round-bottomed flask under a nitro­gen atmosphere was stirred at 423 K for 48 h. The reaction mixture was filtered and the filtrate was added to H2O (200 ml). The precipitate was filtered off and washed with water and dried in a vacuum to afford the product in 80% yield. 1H NMR (CDCl3, 400 Hz): δ 8.70 (d, J = 4.8 Hz, 2H), 7.76 (d, J = 7.2 Hz, 2H), 7.51–7.54 (m, 4H), 7.35 (s, 1H), 7.25–7.26 (m, 2H). Analysis calculated for C14H11N3: C 75.31, H 5.87, N 18.82%; found: C 75.48, H 5.94, N 18.72%.

For the synthesis of (I), a mixture of Cd(NO3)2.6H2O (172 mg, 0.5 mmol), 5-hy­droxy benzene-1,3-di­carb­oxy­lic acid (5-OH—H2bdc) (80 mg, 0.5 mmol), IPP (110 mg, 0.5 mmol), water (6 ml) and DMF (1 ml) was placed in a Teflon reactor (25 ml). The mixture was heated at 373 K for 3 d and then allowed to cool to room temperature. Colourless block-shaped crystals of (I) were obtained (yield 42%, based on Cd). Analysis calculated for C36H30CdN6O7: C 56.08, H 3.92, N 10.90%; found: C 55.99, H 3.97, N 10.92%. IR (KBr pellet, cm-1): 3414 (s), 3129 (s), 1606 (m), 1550 (m), 1396 (m),1303 (w), 1267 (w), 1124 (w), 1061 (m), 814 (m), 729 (m), 646 (w), 559 (w), 499 (w), 459 (w).

Refinement top

Crystal data, data collection and structure refinement details are summarized in Table 1. The water H atoms were located in a difference Fourier map and included as riding atoms, with O—H = 0.85 and Uiso(H) = 1.5Ueq(O). The C-bound H atoms were placed in calculated positions and treated as riding, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C).

Results and discussion top

The title compound, (I), crystallizes in the centrosymmetric triclinic space group P1 with an asymmetric unit comprised of a bivalent CdII ion, two IPP ligands, one dianionic 5-OH-bdc2- ligand, one coordinated water molecule and one lattice water molecule (Fig. 1). The coordination environment of the CdII atom is best considered as a slightly distorted o­cta­hedral geometry. The equatorial plane is defined by three carboxyl­ate O atoms from two different 5-OH-bdc2- ligands and one O atom from a coordinated water molecule, while the apical positions are occupied by two N atoms from two different IPP ligands. The Cd—N bond lengths are 2.2626 (19) and 2.315 (2) Å, while the Cd—O bond lengths vary greatly, from 2.2330 (16) to 2.5081 (16) Å. The average Cd—O and Cd—N distances in (I) are comparable with those reported for other CdII compounds (Zhang et al., 2015; Yin et al., 2012). Each CdII cation is linked to a terminal water molecular and two IPP ligands to form a [Cd(IPP)2(H2O)]2+ unit. These units are then inter­connected by bridging 5-OH-bdc2- ligands in a κ2,κ12 coordination mode to generate a one-dimensional [Cd(5—OH-bdc)(IPP)2(H2O)]n chain along the b axis, with a Cd···Cd separation of 10.3722 (5) Å (Fig. 2). Only the imidazole ring of the IPP ligand coordinates to the CdII ion. As shown in Fig. 3, neighbouring chains in (I) are linked by ππ stacking inter­actions, leading to the formation of a two-dimensional layer structure. Moreover, there are five inter­molecular O—H···O and O—H···N hydrogen bonds (Table 2) involved in this two-dimensional layer structure, which further enchance the stability of the two-dimensional network. The first hydrogen bond is between the lattice water molecule and the carboxyl­ate O atom of the 5-OH-bdc2- ligand, the second is between the lattice water and the uncoordinated pyridine N atom of the IPP ligand, the third is between the hy­droxy group of 5-OH-bdc2- and the uncoordinated pyridine N atom of the IPP ligand, the fourth is between the coordinated water molecule and the carboxyl­ate O atoms of the 5-OH-bdc2- ligands, and the last is between the coordinated water molecular and the lattice water molecule. Thus, the combination of ππ inter­actions and extensive hydrogen bonds results in the formation of a two-dimensional network (Fig. 4).

In summary, a new asymmetric ditopic ligand, namely 4-[4-(1H-imidazol-1-yl)phenyl]­pyridine (IPP), has been synthesized and used to construct a one-dimensional cadmium(II) coordination polymer. The IPP ligand is coordinated to the CdII ion by an imidazole-ring N atom only, while the pyridine N atom remains uncoordinated and acts as a hydrogen-bond acceptor. Even though the IPP ligand does not expand the structure, the uncoordinated pyridine ring still plays an important role in the stabilization of the structure.

Structure description top

The design and synthesis of new organic lgands is extremely important to the rapid development of coordination polymers (CPs) (Almeida Paz et al., 2012). In recent decades, numerous symmetric organic ligands have been synthesized and employed to construct CPs with different structures and potential applications. Among them, two structurally similar ligands 1,4-bis­(imidazol-1-yl)benzene (bimb) and 1,4-bis­(4-pyridyl)­benzene (bpbenz) have been used widely in the synthesis of CPs as linear ditopic ligands. It has been reported that bimb reacts with Cd(BF4)2·6H2O (Li et al., 2010) to generate a double inter­penetrating α-Po network, while bpbenz reacts with Cd(NO3)2·6H2O to generate a three-dimensional pillar–layer framework (Guo et al., 2012). However, CPs based on asymmetric ligands are still rare. This is mainly because such ligands are usually expensive and more difficult to synthesize. As far as we know, there is some probability that the noncentrosymmetry of the asymmetric organic ligands could be transferred into the framework of the CPs and some symmetry-dependent properties such as piezoelectricity, pyroelectricity, ferroelectricity and second-order nonlinear optics (Zhang & Xiong, 2012) may thus occur in these noncentrosymmetric CPs. Therefore, we designed and synthesized a new asymmetric heterobifunctional organic ligand, 4-[4-(1H-imidazol-1-yl)phenyl]­pyridine (IPP), containing both pyridine and imidazole rings. Reacting IPP, we successfully obtained a new cadmium coordination polymer, {[Cd(5—OH-bdc)(IPP)2(H2O)]·H2O}n (I), the crystal structure of (I) we now report.

The title compound, (I), crystallizes in the centrosymmetric triclinic space group P1 with an asymmetric unit comprised of a bivalent CdII ion, two IPP ligands, one dianionic 5-OH-bdc2- ligand, one coordinated water molecule and one lattice water molecule (Fig. 1). The coordination environment of the CdII atom is best considered as a slightly distorted o­cta­hedral geometry. The equatorial plane is defined by three carboxyl­ate O atoms from two different 5-OH-bdc2- ligands and one O atom from a coordinated water molecule, while the apical positions are occupied by two N atoms from two different IPP ligands. The Cd—N bond lengths are 2.2626 (19) and 2.315 (2) Å, while the Cd—O bond lengths vary greatly, from 2.2330 (16) to 2.5081 (16) Å. The average Cd—O and Cd—N distances in (I) are comparable with those reported for other CdII compounds (Zhang et al., 2015; Yin et al., 2012). Each CdII cation is linked to a terminal water molecular and two IPP ligands to form a [Cd(IPP)2(H2O)]2+ unit. These units are then inter­connected by bridging 5-OH-bdc2- ligands in a κ2,κ12 coordination mode to generate a one-dimensional [Cd(5—OH-bdc)(IPP)2(H2O)]n chain along the b axis, with a Cd···Cd separation of 10.3722 (5) Å (Fig. 2). Only the imidazole ring of the IPP ligand coordinates to the CdII ion. As shown in Fig. 3, neighbouring chains in (I) are linked by ππ stacking inter­actions, leading to the formation of a two-dimensional layer structure. Moreover, there are five inter­molecular O—H···O and O—H···N hydrogen bonds (Table 2) involved in this two-dimensional layer structure, which further enchance the stability of the two-dimensional network. The first hydrogen bond is between the lattice water molecule and the carboxyl­ate O atom of the 5-OH-bdc2- ligand, the second is between the lattice water and the uncoordinated pyridine N atom of the IPP ligand, the third is between the hy­droxy group of 5-OH-bdc2- and the uncoordinated pyridine N atom of the IPP ligand, the fourth is between the coordinated water molecule and the carboxyl­ate O atoms of the 5-OH-bdc2- ligands, and the last is between the coordinated water molecular and the lattice water molecule. Thus, the combination of ππ inter­actions and extensive hydrogen bonds results in the formation of a two-dimensional network (Fig. 4).

In summary, a new asymmetric ditopic ligand, namely 4-[4-(1H-imidazol-1-yl)phenyl]­pyridine (IPP), has been synthesized and used to construct a one-dimensional cadmium(II) coordination polymer. The IPP ligand is coordinated to the CdII ion by an imidazole-ring N atom only, while the pyridine N atom remains uncoordinated and acts as a hydrogen-bond acceptor. Even though the IPP ligand does not expand the structure, the uncoordinated pyridine ring still plays an important role in the stabilization of the structure.

Synthesis and crystallization top

For the synthesis of IPP, a mixture of tetra­kis(tri­phenyl­phosphane)palladium (0.08 g, 0.05 mmol), 1,4-di­bromo­benzene (2.36 g, 10 mmol), (pyridin-4-yl)boronic acid (1.00 g, 7.5 mmol) and K2CO3 (5.52 g, 4.0 mmol) in anhydrous N,N-di­methyl­formamide (DMF, 30 ml) in a 100 ml two-necked round-bottomed flask under N2 was stirred at 363 K for 48 h. The reaction mixture was filtered and the collected solid was purified on a silica-gel column using petroleum ether and ethyl acetate (3:1 v/v) as eluent to afford the 4-pyridyl bromo­benzene [ambiguous, please clarify ]. A mixture of CuI (0.09 g, 0.5 mmol), 4-pyridyl bromo­benzene (2.46 g, 10 mmol), imidazole (1.36 g, 2.0 mmol) and K2CO3 (2.76 g, 2.0 mmol) in DMF (30 ml) in a 100 ml two-necked round-bottomed flask under a nitro­gen atmosphere was stirred at 423 K for 48 h. The reaction mixture was filtered and the filtrate was added to H2O (200 ml). The precipitate was filtered off and washed with water and dried in a vacuum to afford the product in 80% yield. 1H NMR (CDCl3, 400 Hz): δ 8.70 (d, J = 4.8 Hz, 2H), 7.76 (d, J = 7.2 Hz, 2H), 7.51–7.54 (m, 4H), 7.35 (s, 1H), 7.25–7.26 (m, 2H). Analysis calculated for C14H11N3: C 75.31, H 5.87, N 18.82%; found: C 75.48, H 5.94, N 18.72%.

For the synthesis of (I), a mixture of Cd(NO3)2.6H2O (172 mg, 0.5 mmol), 5-hy­droxy benzene-1,3-di­carb­oxy­lic acid (5-OH—H2bdc) (80 mg, 0.5 mmol), IPP (110 mg, 0.5 mmol), water (6 ml) and DMF (1 ml) was placed in a Teflon reactor (25 ml). The mixture was heated at 373 K for 3 d and then allowed to cool to room temperature. Colourless block-shaped crystals of (I) were obtained (yield 42%, based on Cd). Analysis calculated for C36H30CdN6O7: C 56.08, H 3.92, N 10.90%; found: C 55.99, H 3.97, N 10.92%. IR (KBr pellet, cm-1): 3414 (s), 3129 (s), 1606 (m), 1550 (m), 1396 (m),1303 (w), 1267 (w), 1124 (w), 1061 (m), 814 (m), 729 (m), 646 (w), 559 (w), 499 (w), 459 (w).

Refinement details top

Crystal data, data collection and structure refinement details are summarized in Table 1. The water H atoms were located in a difference Fourier map and included as riding atoms, with O—H = 0.85 and Uiso(H) = 1.5Ueq(O). The C-bound H atoms were placed in calculated positions and treated as riding, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2003); data reduction: SAINT (Bruker, 2003); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2015); molecular graphics: SHELXTL (Sheldrick, 2008) and DIAMOND (Brandenburg, 2010); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. The coordination environment of the CdII atom in (I), shwon with 30% probability displacement ellipsoids. [Symmetry codes: (i) x, y - 1, z; (ii) x, y + 1, z.] [Please provide a fully labelled plot]
[Figure 2] Fig. 2. A view of the one-dimensional [Cd(5—OH-bdc)(IPP)2(H2O)]n chain of (I).
[Figure 3] Fig. 3. The ππ stacking interactions of (I).
[Figure 4] Fig. 4. The two-dimensional layer structure generated by hydrogen bonds and ππ stacking interactions.
catena-Poly[[[aqua{4-[4-(1H-imidazol-1-yl-κN3)phenyl]pyridine}cadmium(II)]-µ-5-hydroxybenzene-1,3-dicarboxylato-κ3O1,O1':O3] monohydrate] top
Crystal data top
[Cd(C8H4O5)(C14H12N3)2(H2O)]·H2OZ = 2
Mr = 771.06F(000) = 784
Triclinic, P1Dx = 1.597 Mg m3
a = 9.9863 (4) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.3722 (5) ÅCell parameters from 7368 reflections
c = 15.7502 (7) Åθ = 3.1–28.5°
α = 91.755 (4)°µ = 0.74 mm1
β = 99.029 (5)°T = 293 K
γ = 95.042 (3)°Block, clear light colourless
V = 1603.32 (13) Å30.37 × 0.35 × 0.32 mm
Data collection top
Agilent SuperNova Dual Source
diffractometer with an Eos detector
6291 independent reflections
Radiation source: SuperNova (Mo) X-ray Source5707 reflections with I > 2σ(I)
Detector resolution: 16.0733 pixels mm-1Rint = 0.031
ω scansθmax = 26.0°, θmin = 3.1°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1212
Tmin = 0.771, Tmax = 0.797k = 1212
11317 measured reflectionsl = 1918
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)] = 0.029Hydrogen site location: mixed
wR(F2) = 0.071H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0318P)2 + 0.3064P]
where P = (Fo2 + 2Fc2)/3
6291 reflections(Δ/σ)max = 0.001
455 parametersΔρmax = 0.40 e Å3
1 restraintΔρmin = 0.68 e Å3
Crystal data top
[Cd(C8H4O5)(C14H12N3)2(H2O)]·H2Oγ = 95.042 (3)°
Mr = 771.06V = 1603.32 (13) Å3
Triclinic, P1Z = 2
a = 9.9863 (4) ÅMo Kα radiation
b = 10.3722 (5) ŵ = 0.74 mm1
c = 15.7502 (7) ÅT = 293 K
α = 91.755 (4)°0.37 × 0.35 × 0.32 mm
β = 99.029 (5)°
Data collection top
Agilent SuperNova Dual Source
diffractometer with an Eos detector
6291 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
5707 reflections with I > 2σ(I)
Tmin = 0.771, Tmax = 0.797Rint = 0.031
11317 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0291 restraint
wR(F2) = 0.071H-atom parameters constrained
S = 1.05Δρmax = 0.40 e Å3
6291 reflectionsΔρmin = 0.68 e Å3
455 parameters
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.

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) top
xyzUiso*/Ueq
C10.8071 (2)0.2728 (2)0.90705 (15)0.0330 (5)
H10.80860.32530.86030.040*
C20.9156 (2)0.2549 (2)0.96616 (15)0.0322 (5)
H21.00470.29070.96760.039*
C30.7338 (2)0.1437 (2)0.99689 (15)0.0295 (5)
H30.67740.08951.02480.035*
C40.1449 (3)0.2412 (2)0.78415 (16)0.0370 (6)
H40.11740.22610.83700.044*
C50.0615 (2)0.2658 (3)0.71204 (16)0.0368 (6)
H50.03200.27100.70590.044*
C60.2706 (3)0.2665 (3)0.68687 (16)0.0377 (6)
H60.34580.27280.65860.045*
C71.2812 (3)0.0029 (3)1.47052 (16)0.0406 (6)
H71.28550.03321.52580.049*
C81.1981 (3)0.0484 (3)1.40408 (16)0.0384 (6)
H81.14710.11611.41510.046*
C91.1913 (2)0.0019 (2)1.32065 (15)0.0299 (5)
C101.2711 (2)0.1024 (3)1.30983 (15)0.0343 (6)
H101.27180.13841.25510.041*
C111.3484 (2)0.1481 (3)1.37969 (15)0.0364 (6)
H111.39950.21661.37060.044*
C120.0179 (3)0.4426 (2)0.15817 (16)0.0364 (6)
H120.08070.45000.12040.044*
C130.0637 (2)0.4141 (2)0.24226 (16)0.0340 (6)
H130.15550.40480.26020.041*
C140.0281 (2)0.3993 (2)0.29992 (15)0.0294 (5)
C150.1633 (2)0.4139 (2)0.26798 (15)0.0330 (5)
H150.22940.40290.30340.040*
C160.1992 (2)0.4447 (2)0.18335 (15)0.0350 (6)
H160.29010.45560.16360.042*
C170.0161 (2)0.3685 (2)0.39079 (15)0.0307 (5)
C180.1464 (2)0.4107 (3)0.43354 (16)0.0383 (6)
H180.20650.45810.40420.046*
C190.1882 (2)0.3836 (3)0.51815 (16)0.0398 (6)
H190.27510.41390.54570.048*
C200.1009 (2)0.3116 (2)0.56174 (15)0.0320 (5)
C210.0285 (2)0.2682 (3)0.52087 (16)0.0369 (6)
H210.08760.21930.55020.044*
C220.0699 (2)0.2973 (3)0.43654 (16)0.0356 (6)
H220.15760.26850.40980.043*
C230.9476 (2)0.1282 (2)1.09904 (14)0.0276 (5)
C241.0810 (2)0.1036 (3)1.09647 (15)0.0339 (6)
H241.11800.11461.04620.041*
C251.1582 (2)0.0629 (3)1.16904 (15)0.0352 (6)
H251.24770.04601.16730.042*
C261.1055 (2)0.0462 (2)1.24510 (15)0.0303 (5)
C270.9714 (2)0.0714 (2)1.24604 (15)0.0310 (5)
H270.93440.06141.29640.037*
C280.8922 (2)0.1110 (2)1.17361 (15)0.0312 (5)
H280.80210.12601.17480.037*
C290.5459 (2)0.4491 (2)0.79281 (15)0.0267 (5)
C300.5340 (2)0.5771 (2)0.75120 (13)0.0233 (5)
C310.5242 (2)0.5830 (2)0.66271 (14)0.0272 (5)
H310.53430.50970.62970.033*
C320.4995 (2)0.6981 (2)0.62325 (14)0.0286 (5)
C330.4868 (2)0.0752 (2)0.81420 (14)0.0256 (5)
C340.4870 (2)0.1921 (2)0.67279 (14)0.0277 (5)
H340.47070.11490.64630.033*
C350.4984 (2)0.1965 (2)0.76162 (13)0.0227 (4)
C360.5216 (2)0.3125 (2)0.80058 (14)0.0239 (5)
H360.52890.31640.86000.029*
Cd10.47879 (2)0.20674 (2)0.85471 (2)0.02486 (6)
N10.69323 (19)0.20182 (19)0.92609 (12)0.0304 (4)
N20.86848 (18)0.17278 (19)1.02407 (12)0.0278 (4)
N31.3554 (2)0.1008 (2)1.46020 (13)0.0354 (5)
N40.2763 (2)0.2415 (2)0.76850 (13)0.0358 (5)
N50.14254 (19)0.2819 (2)0.64895 (12)0.0323 (5)
N60.1111 (2)0.4599 (2)0.12818 (13)0.0354 (5)
O10.56899 (17)0.35329 (15)0.74880 (10)0.0349 (4)
O20.52448 (17)0.44150 (16)0.86949 (10)0.0350 (4)
O30.46282 (18)0.02488 (16)0.77267 (11)0.0382 (4)
O40.50274 (17)0.07717 (16)0.89424 (10)0.0353 (4)
O50.36295 (17)0.19246 (17)0.96874 (10)0.0377 (4)
H5A0.34120.26600.98330.056*
H5B0.40420.16361.01540.056*
O440.4871 (2)0.69915 (18)0.53596 (10)0.0465 (5)
H440.45640.76640.51930.070*
O1W0.25935 (19)0.41602 (18)0.01315 (12)0.0424 (4)
H1WA0.32830.46230.04010.064*
H1WB0.21510.46110.02370.064*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0399 (13)0.0305 (14)0.0279 (12)0.0008 (11)0.0047 (10)0.0051 (10)
C20.0307 (12)0.0345 (14)0.0309 (13)0.0021 (10)0.0051 (10)0.0056 (10)
C30.0273 (11)0.0307 (13)0.0298 (12)0.0026 (10)0.0013 (9)0.0069 (10)
C40.0414 (14)0.0338 (15)0.0352 (14)0.0001 (11)0.0060 (11)0.0013 (11)
C50.0318 (13)0.0402 (16)0.0374 (14)0.0007 (11)0.0038 (11)0.0033 (11)
C60.0344 (13)0.0488 (17)0.0295 (14)0.0124 (12)0.0003 (10)0.0012 (11)
C70.0556 (16)0.0394 (16)0.0250 (13)0.0099 (13)0.0014 (11)0.0031 (11)
C80.0473 (15)0.0323 (14)0.0344 (14)0.0133 (12)0.0010 (11)0.0041 (11)
C90.0284 (12)0.0306 (13)0.0292 (12)0.0013 (10)0.0005 (9)0.0028 (10)
C100.0341 (13)0.0420 (15)0.0273 (13)0.0091 (11)0.0038 (10)0.0006 (10)
C110.0357 (13)0.0402 (15)0.0340 (14)0.0117 (11)0.0037 (10)0.0029 (11)
C120.0398 (14)0.0333 (14)0.0376 (14)0.0003 (11)0.0129 (11)0.0007 (11)
C130.0263 (12)0.0356 (14)0.0396 (14)0.0014 (10)0.0044 (10)0.0012 (11)
C140.0276 (11)0.0278 (13)0.0318 (13)0.0036 (10)0.0020 (9)0.0005 (10)
C150.0300 (12)0.0338 (14)0.0358 (14)0.0044 (10)0.0063 (10)0.0029 (10)
C160.0322 (12)0.0366 (15)0.0354 (14)0.0051 (11)0.0017 (10)0.0026 (11)
C170.0272 (12)0.0325 (14)0.0320 (13)0.0053 (10)0.0024 (10)0.0015 (10)
C180.0313 (13)0.0439 (16)0.0383 (14)0.0028 (11)0.0044 (11)0.0041 (11)
C190.0255 (12)0.0526 (17)0.0370 (14)0.0039 (11)0.0034 (10)0.0005 (12)
C200.0307 (12)0.0337 (14)0.0306 (13)0.0085 (10)0.0007 (10)0.0002 (10)
C210.0306 (12)0.0393 (15)0.0387 (14)0.0020 (11)0.0011 (11)0.0063 (11)
C220.0249 (12)0.0442 (16)0.0350 (14)0.0011 (11)0.0016 (10)0.0045 (11)
C230.0266 (11)0.0282 (13)0.0259 (12)0.0010 (9)0.0021 (9)0.0027 (9)
C240.0294 (12)0.0456 (16)0.0276 (13)0.0066 (11)0.0044 (10)0.0045 (11)
C250.0250 (12)0.0453 (16)0.0355 (14)0.0068 (11)0.0032 (10)0.0046 (11)
C260.0309 (12)0.0282 (13)0.0301 (13)0.0027 (10)0.0001 (10)0.0000 (9)
C270.0341 (12)0.0322 (14)0.0276 (12)0.0050 (10)0.0063 (10)0.0040 (10)
C280.0263 (11)0.0317 (14)0.0364 (14)0.0064 (10)0.0051 (10)0.0033 (10)
C290.0272 (11)0.0190 (12)0.0324 (13)0.0053 (9)0.0021 (9)0.0017 (9)
C300.0233 (10)0.0183 (11)0.0277 (12)0.0035 (8)0.0010 (9)0.0030 (9)
C310.0307 (12)0.0221 (12)0.0290 (12)0.0069 (9)0.0033 (9)0.0024 (9)
C320.0350 (12)0.0295 (13)0.0223 (12)0.0085 (10)0.0035 (9)0.0043 (9)
C330.0221 (11)0.0219 (12)0.0329 (13)0.0020 (9)0.0052 (9)0.0008 (9)
C340.0328 (12)0.0201 (12)0.0305 (12)0.0053 (9)0.0037 (10)0.0064 (9)
C350.0217 (10)0.0197 (11)0.0265 (11)0.0023 (8)0.0030 (8)0.0014 (8)
C360.0274 (11)0.0204 (11)0.0227 (11)0.0013 (9)0.0012 (9)0.0006 (8)
Cd10.03083 (10)0.02039 (10)0.02260 (10)0.00547 (7)0.00001 (7)0.00232 (6)
N10.0310 (10)0.0277 (11)0.0311 (11)0.0024 (8)0.0003 (8)0.0061 (8)
N20.0263 (9)0.0292 (11)0.0270 (10)0.0036 (8)0.0006 (8)0.0043 (8)
N30.0390 (11)0.0370 (12)0.0292 (11)0.0073 (9)0.0001 (9)0.0036 (9)
N40.0385 (11)0.0370 (13)0.0304 (11)0.0111 (9)0.0027 (9)0.0029 (9)
N50.0292 (10)0.0365 (12)0.0287 (11)0.0045 (9)0.0028 (8)0.0016 (8)
N60.0440 (12)0.0303 (12)0.0314 (11)0.0041 (9)0.0047 (9)0.0018 (9)
O10.0518 (10)0.0207 (9)0.0334 (9)0.0111 (7)0.0055 (7)0.0029 (6)
O20.0538 (10)0.0235 (9)0.0278 (9)0.0068 (8)0.0046 (8)0.0067 (7)
O30.0580 (11)0.0206 (9)0.0353 (10)0.0121 (8)0.0009 (8)0.0007 (7)
O40.0489 (10)0.0309 (10)0.0277 (9)0.0067 (8)0.0097 (8)0.0005 (7)
O50.0512 (10)0.0377 (10)0.0268 (9)0.0137 (8)0.0090 (8)0.0032 (7)
O440.0800 (14)0.0374 (11)0.0247 (9)0.0226 (10)0.0058 (9)0.0052 (8)
O1W0.0483 (11)0.0400 (11)0.0375 (11)0.0079 (9)0.0002 (8)0.0041 (8)
Geometric parameters (Å, º) top
C1—C21.344 (3)C20—N51.423 (3)
C1—N11.378 (3)C21—C221.379 (3)
C1—H10.9300C21—H210.9300
C2—N21.375 (3)C22—H220.9300
C2—H20.9300C23—C241.385 (3)
C3—N11.309 (3)C23—C281.384 (3)
C3—N21.350 (3)C23—N21.427 (3)
C3—H30.9300C24—C251.375 (3)
C4—C51.344 (3)C24—H240.9300
C4—N41.373 (3)C25—C261.391 (3)
C4—H40.9300C25—H250.9300
C5—N51.382 (3)C26—C271.390 (3)
C5—H50.9300C27—C281.377 (3)
C6—N41.313 (3)C27—H270.9300
C6—N51.349 (3)C28—H280.9300
C6—H60.9300C29—O11.252 (3)
C7—N31.329 (3)C29—O21.263 (3)
C7—C81.381 (4)C29—C301.504 (3)
C7—H70.9300C30—C311.386 (3)
C8—C91.389 (3)C30—C36i1.390 (3)
C8—H80.9300C31—C321.385 (3)
C9—C101.388 (3)C31—H310.9300
C9—C261.480 (3)C32—O441.361 (3)
C10—C111.364 (3)C32—C34i1.387 (3)
C10—H100.9300C33—O41.247 (3)
C11—N31.335 (3)C33—O31.264 (3)
C11—H110.9300C33—C351.508 (3)
C12—N61.330 (3)C34—C32ii1.387 (3)
C12—C131.381 (3)C34—C351.388 (3)
C12—H120.9300C34—H340.9300
C13—C141.391 (3)C35—C361.389 (3)
C13—H130.9300C36—C30ii1.390 (3)
C14—C151.388 (3)C36—H360.9300
C14—C171.483 (3)Cd1—O32.2330 (16)
C15—C161.380 (3)Cd1—N12.2626 (19)
C15—H150.9300Cd1—O52.2857 (15)
C16—N61.333 (3)Cd1—N42.315 (2)
C16—H160.9300Cd1—O22.4348 (16)
C17—C221.385 (3)Cd1—O12.5081 (16)
C17—C181.394 (3)O5—H5A0.8458
C18—C191.377 (3)O5—H5B0.8601
C18—H180.9300O44—H440.8200
C19—C201.377 (3)O1W—H1WA0.8500
C19—H190.9300O1W—H1WB0.8500
C20—C211.380 (3)
C2—C1—N1109.8 (2)C24—C25—H25119.2
C2—C1—H1125.1C26—C25—H25119.2
N1—C1—H1125.1C27—C26—C25118.2 (2)
C1—C2—N2106.2 (2)C27—C26—C9122.3 (2)
C1—C2—H2126.9C25—C26—C9119.4 (2)
N2—C2—H2126.9C28—C27—C26121.0 (2)
N1—C3—N2111.1 (2)C28—C27—H27119.5
N1—C3—H3124.4C26—C27—H27119.5
N2—C3—H3124.4C27—C28—C23119.7 (2)
C5—C4—N4110.2 (2)C27—C28—H28120.2
C5—C4—H4124.9C23—C28—H28120.2
N4—C4—H4124.9O1—C29—O2122.8 (2)
C4—C5—N5106.3 (2)O1—C29—C30118.9 (2)
C4—C5—H5126.9O2—C29—C30118.1 (2)
N5—C5—H5126.9C31—C30—C36i119.8 (2)
N4—C6—N5111.9 (2)C31—C30—C29120.0 (2)
N4—C6—H6124.0C36i—C30—C29119.98 (19)
N5—C6—H6124.0C30—C31—C32120.2 (2)
N3—C7—C8123.9 (2)C30—C31—H31119.9
N3—C7—H7118.0C32—C31—H31119.9
C8—C7—H7118.0O44—C32—C31118.4 (2)
C7—C8—C9119.4 (2)O44—C32—C34i121.8 (2)
C7—C8—H8120.3C31—C32—C34i119.8 (2)
C9—C8—H8120.3O4—C33—O3123.8 (2)
C10—C9—C8116.6 (2)O4—C33—C35119.8 (2)
C10—C9—C26119.9 (2)O3—C33—C35116.4 (2)
C8—C9—C26123.5 (2)C32ii—C34—C35120.6 (2)
C11—C10—C9119.8 (2)C32ii—C34—H34119.7
C11—C10—H10120.1C35—C34—H34119.7
C9—C10—H10120.1C34—C35—C36119.3 (2)
N3—C11—C10124.1 (2)C34—C35—C33119.6 (2)
N3—C11—H11117.9C36—C35—C33121.15 (19)
C10—C11—H11117.9C30ii—C36—C35120.3 (2)
N6—C12—C13123.7 (2)C30ii—C36—H36119.8
N6—C12—H12118.2C35—C36—H36119.8
C13—C12—H12118.2O3—Cd1—N199.32 (7)
C12—C13—C14119.7 (2)O3—Cd1—O5114.82 (6)
C12—C13—H13120.2N1—Cd1—O599.12 (6)
C14—C13—H13120.2O3—Cd1—N483.79 (7)
C15—C14—C13116.6 (2)N1—Cd1—N4169.72 (7)
C15—C14—C17121.7 (2)O5—Cd1—N488.32 (7)
C13—C14—C17121.7 (2)O3—Cd1—O2148.76 (6)
C16—C15—C14119.6 (2)N1—Cd1—O285.67 (6)
C16—C15—H15120.2O5—Cd1—O294.49 (6)
C14—C15—H15120.2N4—Cd1—O286.68 (7)
N6—C16—C15123.8 (2)O3—Cd1—O195.95 (6)
N6—C16—H16118.1N1—Cd1—O189.59 (6)
C15—C16—H16118.1O5—Cd1—O1145.86 (6)
C22—C17—C18117.4 (2)N4—Cd1—O180.32 (7)
C22—C17—C14121.6 (2)O2—Cd1—O153.05 (5)
C18—C17—C14121.1 (2)C3—N1—C1105.88 (19)
C19—C18—C17121.6 (2)C3—N1—Cd1128.52 (15)
C19—C18—H18119.2C1—N1—Cd1125.30 (16)
C17—C18—H18119.2C3—N2—C2107.05 (19)
C20—C19—C18119.7 (2)C3—N2—C23126.84 (19)
C20—C19—H19120.1C2—N2—C23126.11 (19)
C18—C19—H19120.1C7—N3—C11116.2 (2)
C19—C20—C21119.9 (2)C6—N4—C4105.4 (2)
C19—C20—N5120.5 (2)C6—N4—Cd1121.94 (16)
C21—C20—N5119.6 (2)C4—N4—Cd1132.70 (17)
C22—C21—C20119.9 (2)C6—N5—C5106.3 (2)
C22—C21—H21120.1C6—N5—C20126.5 (2)
C20—C21—H21120.1C5—N5—C20127.2 (2)
C21—C22—C17121.5 (2)C12—N6—C16116.6 (2)
C21—C22—H22119.2C29—O1—Cd189.25 (13)
C17—C22—H22119.2C29—O2—Cd192.37 (13)
C24—C23—C28120.4 (2)C33—O3—Cd1114.28 (15)
C24—C23—N2119.1 (2)Cd1—O5—H5A110.8
C28—C23—N2120.5 (2)Cd1—O5—H5B117.3
C25—C24—C23119.2 (2)H5A—O5—H5B104.9
C25—C24—H24120.4C32—O44—H44109.5
C23—C24—H24120.4H1WA—O1W—H1WB109.5
C24—C25—C26121.5 (2)
N1—C1—C2—N21.0 (3)C36i—C30—C31—C321.3 (3)
N4—C4—C5—N50.1 (3)C29—C30—C31—C32173.5 (2)
N3—C7—C8—C91.1 (4)C30—C31—C32—O44178.3 (2)
C7—C8—C9—C100.3 (4)C30—C31—C32—C34i1.2 (3)
C7—C8—C9—C26180.0 (2)C32ii—C34—C35—C360.5 (3)
C8—C9—C10—C111.3 (4)C32ii—C34—C35—C33178.96 (19)
C26—C9—C10—C11178.9 (2)O4—C33—C35—C34176.96 (19)
C9—C10—C11—N31.2 (4)O3—C33—C35—C342.0 (3)
N6—C12—C13—C141.5 (4)O4—C33—C35—C362.5 (3)
C12—C13—C14—C150.4 (4)O3—C33—C35—C36178.58 (19)
C12—C13—C14—C17179.9 (2)C34—C35—C36—C30ii0.4 (3)
C13—C14—C15—C161.6 (3)C33—C35—C36—C30ii179.08 (18)
C17—C14—C15—C16178.9 (2)N2—C3—N1—C10.5 (3)
C14—C15—C16—N61.2 (4)N2—C3—N1—Cd1174.36 (15)
C15—C14—C17—C2229.9 (4)C2—C1—N1—C30.9 (3)
C13—C14—C17—C22149.6 (3)C2—C1—N1—Cd1175.03 (16)
C15—C14—C17—C18150.0 (2)N1—C3—N2—C20.1 (3)
C13—C14—C17—C1830.5 (4)N1—C3—N2—C23179.4 (2)
C22—C17—C18—C190.5 (4)C1—C2—N2—C30.6 (3)
C14—C17—C18—C19179.4 (2)C1—C2—N2—C23178.8 (2)
C17—C18—C19—C201.1 (4)C24—C23—N2—C3144.9 (2)
C18—C19—C20—C210.8 (4)C28—C23—N2—C335.7 (4)
C18—C19—C20—N5179.5 (2)C24—C23—N2—C235.7 (3)
C19—C20—C21—C220.1 (4)C28—C23—N2—C2143.7 (2)
N5—C20—C21—C22179.6 (2)C8—C7—N3—C111.3 (4)
C20—C21—C22—C170.8 (4)C10—C11—N3—C70.1 (4)
C18—C17—C22—C210.5 (4)N5—C6—N4—C40.2 (3)
C14—C17—C22—C21179.7 (2)N5—C6—N4—Cd1179.33 (16)
C28—C23—C24—C250.5 (4)C5—C4—N4—C60.0 (3)
N2—C23—C24—C25178.9 (2)C5—C4—N4—Cd1179.41 (18)
C23—C24—C25—C260.2 (4)N4—C6—N5—C50.3 (3)
C24—C25—C26—C270.3 (4)N4—C6—N5—C20179.1 (2)
C24—C25—C26—C9178.0 (2)C4—C5—N5—C60.2 (3)
C10—C9—C26—C27135.3 (3)C4—C5—N5—C20179.0 (2)
C8—C9—C26—C2745.0 (3)C19—C20—N5—C630.1 (4)
C10—C9—C26—C2542.3 (3)C21—C20—N5—C6150.2 (3)
C8—C9—C26—C25137.4 (3)C19—C20—N5—C5148.5 (3)
C25—C26—C27—C280.4 (4)C21—C20—N5—C531.2 (4)
C9—C26—C27—C28177.2 (2)C13—C12—N6—C162.0 (4)
C26—C27—C28—C231.2 (4)C15—C16—N6—C120.6 (4)
C24—C23—C28—C271.2 (4)O2—C29—O1—Cd116.1 (2)
N2—C23—C28—C27178.2 (2)C30—C29—O1—Cd1159.74 (17)
O1—C29—C30—C3111.5 (3)O1—C29—O2—Cd116.7 (2)
O2—C29—C30—C31164.6 (2)C30—C29—O2—Cd1159.25 (17)
O1—C29—C30—C36i173.8 (2)O4—C33—O3—Cd17.9 (3)
O2—C29—C30—C36i10.2 (3)C35—C33—O3—Cd1171.02 (13)
Symmetry codes: (i) x, y+1, z; (ii) x, y1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1W—H1WB···N6iii0.852.042.877 (3)169
O1W—H1WA···O2iv0.852.052.878 (2)166
O44—H44···N3v0.821.952.757 (3)167
O5—H5B···O4vi0.861.872.724 (2)171
O5—H5A···O1Wvii0.851.902.736 (3)170
C16—H16···O2viii0.932.643.539 (3)162
C11—H11···O1ix0.932.403.142 (3)137
C6—H6···O10.932.513.034 (3)116
C3—H3···O4vi0.932.363.171 (3)146
C3—H3···O4vi0.932.363.171 (3)146
C6—H6···O10.932.513.034 (3)116
C11—H11···O1ix0.932.403.142 (3)137
C16—H16···O2viii0.932.643.539 (3)162
O5—H5A···O1Wvii0.851.902.736 (3)170
O5—H5B···O4vi0.861.872.724 (2)171
O44—H44···N3v0.821.952.757 (3)167
Symmetry codes: (iii) x, y+1, z; (iv) x+1, y+1, z+1; (v) x1, y+1, z1; (vi) x+1, y, z+2; (vii) x, y, z+1; (viii) x, y+1, z+1; (ix) x+2, y, z+2.

Experimental details

Crystal data
Chemical formula[Cd(C8H4O5)(C14H12N3)2(H2O)]·H2O
Mr771.06
Crystal system, space groupTriclinic, P1
Temperature (K)293
a, b, c (Å)9.9863 (4), 10.3722 (5), 15.7502 (7)
α, β, γ (°)91.755 (4), 99.029 (5), 95.042 (3)
V3)1603.32 (13)
Z2
Radiation typeMo Kα
µ (mm1)0.74
Crystal size (mm)0.37 × 0.35 × 0.32
Data collection
DiffractometerAgilent SuperNova Dual Source
diffractometer with an Eos detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.771, 0.797
No. of measured, independent and
observed [I > 2σ(I)] reflections
11317, 6291, 5707
Rint0.031
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.029, 0.071, 1.05
No. of reflections6291
No. of parameters455
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.40, 0.68

Computer programs: APEX2 (Bruker, 2005), SAINT (Bruker, 2003), SHELXS97 (Sheldrick, 2008), SHELXL2013 (Sheldrick, 2015), SHELXTL (Sheldrick, 2008) and DIAMOND (Brandenburg, 2010), SHELXTL (Sheldrick, 2008) and publCIF (Westrip, 2010).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1W—H1WB···N6i0.852.042.877 (3)168.9
O1W—H1WA···O2ii0.852.052.878 (2)166.1
O44—H44···N3iii0.821.952.757 (3)166.7
O5—H5B···O4iv0.861.872.724 (2)170.7
O5—H5A···O1Wv0.851.902.736 (3)169.5
C16—H16···O2vi0.932.643.539 (3)162.1
C11—H11···O1vii0.932.403.142 (3)136.9
C6—H6···O10.932.513.034 (3)116.1
C3—H3···O4iv0.932.363.171 (3)145.7
C3—H3···O4iv0.932.363.171 (3)145.7
C6—H6···O10.932.513.034 (3)116.1
C11—H11···O1vii0.932.403.142 (3)136.9
C16—H16···O2vi0.932.643.539 (3)162.1
O5—H5A···O1Wv0.851.902.736 (3)169.5
O5—H5B···O4iv0.861.872.724 (2)170.7
O44—H44···N3iii0.821.952.757 (3)166.7
Symmetry codes: (i) x, y+1, z; (ii) x+1, y+1, z+1; (iii) x1, y+1, z1; (iv) x+1, y, z+2; (v) x, y, z+1; (vi) x, y+1, z+1; (vii) x+2, y, z+2.
 

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