metal-organic compounds
Poly[[μ2-1,2-bis(4-pyridyl)ethene](μ3-1,3-phenylenediacetato)cadmium]
aCollege of Chemistry and Materials Science, Huaibei Normal University, Huaibei 235000, Anhui, People's Republic of China
*Correspondence e-mail: dongliu@chnu.edu.cn
In the title coordination polymer, [Cd(C10H8O4)(C12H10N2)]n, two centrosymmetrically related CdII atoms are bridged by two 1,3-phenylenediacetate ligands forming a chain along the [100] direction. The distorted pentagonal–bipyramidal coordination about each metal atom is completed by the N atoms of bridging 1,2-bis(4-pyridyl)ethene ligands, which link these one-dimensional chains into a two-dimensional net extending along the (101) plane.
Related literature
For two-dimensional nets constructed by CdII, dipyridyl ligands and dicarboxylate ligands, see: Tao et al. (2003); Tian et al. (2006); Wang et al. (2009).
Experimental
Crystal data
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Data collection: CrystalClear (Rigaku, 2001); cell CrystalClear; data reduction: CrystalStructure (Rigaku/MSC, 2004); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).
Supporting information
10.1107/S1600536811043467/bq2313sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811043467/bq2313Isup2.hkl
To a 25 ml Teflon-lined stainless steel autoclave was loaded Cd(NO3)2.4H2O (154 mg, 0.5 mmol), 1,3-phenylenediacetic acid (97 mg, 0.5 mmol), 1,2-bis(4-pyridyl)ethene (91 mg, 0.5 mmol), NaOH (40 mg, 1 mmol) and H2O (15 ml). The autoclave was sealed and heated in an oven to 433 K for three days, and then cooled to ambient temperature at the rate of 5 K/h to form yellow crystals. Yield: 180 mg (74% yield based on Cd). Anal. calcd. for C22H18CdN2O4: C, 54.28; H, 3.73; N, 5.75. Found: C, 53.96; H, 3.77; N, 6.03.
The C-bound H atoms were positioned geometrically, with C–H = 0.97 Å (methylene) or 0.94 Å (phenyl, pyridyl and vinyl), and refined as riding, with Uiso(H) = 1.5Ueq(C) for methylene groups or 1.2Ueq(C) otherwise.
Data collection: CrystalClear (Rigaku, 2001); cell
CrystalClear (Rigaku, 2001); data reduction: CrystalStructure (Rigaku/MSC, 2004); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).[Cd(C10H8O4)(C12H10N2)] | Z = 2 |
Mr = 486.79 | F(000) = 488 |
Triclinic, P1 | Dx = 1.702 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 9.4626 (19) Å | Cell parameters from 4814 reflections |
b = 10.113 (2) Å | θ = 3.2–27.5° |
c = 11.351 (2) Å | µ = 1.18 mm−1 |
α = 98.95 (3)° | T = 223 K |
β = 92.19 (3)° | Block, yellow |
γ = 116.88 (3)° | 0.40 × 0.30 × 0.25 mm |
V = 949.8 (3) Å3 |
Rigaku MercuryCCD area-detector diffractometer | 4256 independent reflections |
Radiation source: fine-focus sealed tube | 3630 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.029 |
ω scans | θmax = 27.5°, θmin = 3.2° |
Absorption correction: multi-scan (REQAB; Jacobson, 1998) | h = −12→11 |
Tmin = 0.649, Tmax = 0.757 | k = −12→12 |
8582 measured reflections | l = −11→14 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.033 | H-atom parameters constrained |
wR(F2) = 0.083 | w = 1/[σ2(Fo2) + (0.0352P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.09 | (Δ/σ)max = 0.001 |
4256 reflections | Δρmax = 1.16 e Å−3 |
263 parameters | Δρmin = −0.85 e Å−3 |
0 restraints | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.098 (3) |
[Cd(C10H8O4)(C12H10N2)] | γ = 116.88 (3)° |
Mr = 486.79 | V = 949.8 (3) Å3 |
Triclinic, P1 | Z = 2 |
a = 9.4626 (19) Å | Mo Kα radiation |
b = 10.113 (2) Å | µ = 1.18 mm−1 |
c = 11.351 (2) Å | T = 223 K |
α = 98.95 (3)° | 0.40 × 0.30 × 0.25 mm |
β = 92.19 (3)° |
Rigaku MercuryCCD area-detector diffractometer | 4256 independent reflections |
Absorption correction: multi-scan (REQAB; Jacobson, 1998) | 3630 reflections with I > 2σ(I) |
Tmin = 0.649, Tmax = 0.757 | Rint = 0.029 |
8582 measured reflections |
R[F2 > 2σ(F2)] = 0.033 | 0 restraints |
wR(F2) = 0.083 | H-atom parameters constrained |
S = 1.09 | Δρmax = 1.16 e Å−3 |
4256 reflections | Δρmin = −0.85 e Å−3 |
263 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cd1 | 0.16456 (3) | 0.49799 (2) | 0.10431 (2) | 0.02493 (12) | |
N1 | 0.1884 (3) | 0.3281 (3) | −0.0471 (3) | 0.0287 (6) | |
N2 | 0.1751 (3) | −0.3077 (3) | −0.7491 (2) | 0.0266 (6) | |
O1 | 0.1024 (3) | 0.3142 (3) | 0.2322 (2) | 0.0353 (6) | |
O2 | 0.3550 (3) | 0.4760 (2) | 0.2348 (2) | 0.0350 (6) | |
O3 | 0.8868 (3) | 0.3906 (3) | 0.0535 (2) | 0.0362 (6) | |
O4 | 0.6363 (3) | 0.2894 (3) | −0.0233 (2) | 0.0336 (6) | |
C1 | 0.2978 (4) | 0.3687 (4) | −0.1239 (3) | 0.0338 (8) | |
H1 | 0.3788 | 0.4693 | −0.1097 | 0.041* | |
C2 | 0.2974 (4) | 0.2702 (4) | −0.2224 (3) | 0.0325 (8) | |
H2 | 0.3759 | 0.3039 | −0.2745 | 0.039* | |
C3 | 0.1791 (4) | 0.1192 (3) | −0.2445 (3) | 0.0288 (7) | |
C4 | 0.0700 (4) | 0.0771 (4) | −0.1623 (3) | 0.0355 (8) | |
H4 | −0.0090 | −0.0239 | −0.1714 | 0.043* | |
C5 | 0.0775 (5) | 0.1841 (4) | −0.0670 (3) | 0.0365 (9) | |
H5 | 0.0006 | 0.1536 | −0.0135 | 0.044* | |
C6 | 0.1591 (4) | 0.0064 (4) | −0.3510 (3) | 0.0337 (8) | |
H6 | 0.0776 | −0.0924 | −0.3543 | 0.040* | |
C7 | 0.2438 (4) | 0.0293 (4) | −0.4427 (3) | 0.0320 (8) | |
H7 | 0.3282 | 0.1267 | −0.4391 | 0.038* | |
C8 | 0.2160 (4) | −0.0861 (3) | −0.5501 (3) | 0.0291 (7) | |
C9 | 0.3390 (4) | −0.0707 (4) | −0.6182 (3) | 0.0315 (8) | |
H9 | 0.4385 | 0.0162 | −0.5989 | 0.038* | |
C10 | 0.3148 (4) | −0.1832 (4) | −0.7145 (3) | 0.0315 (8) | |
H10 | 0.4008 | −0.1718 | −0.7580 | 0.038* | |
C11 | 0.0541 (4) | −0.3206 (4) | −0.6863 (3) | 0.0299 (7) | |
H11 | −0.0458 | −0.4061 | −0.7103 | 0.036* | |
C12 | 0.0698 (4) | −0.2139 (4) | −0.5878 (3) | 0.0331 (8) | |
H12 | −0.0183 | −0.2276 | −0.5462 | 0.040* | |
C13 | 0.4592 (4) | 0.2971 (3) | 0.3492 (3) | 0.0284 (7) | |
C14 | 0.5692 (4) | 0.3628 (4) | 0.4528 (3) | 0.0323 (8) | |
H14 | 0.5405 | 0.4004 | 0.5239 | 0.039* | |
C15 | 0.7199 (4) | 0.3733 (4) | 0.4519 (3) | 0.0358 (8) | |
H15 | 0.7939 | 0.4199 | 0.5218 | 0.043* | |
C16 | 0.7619 (4) | 0.3156 (4) | 0.3491 (3) | 0.0347 (8) | |
H16 | 0.8649 | 0.3239 | 0.3490 | 0.042* | |
C17 | 0.6528 (4) | 0.2449 (4) | 0.2447 (3) | 0.0301 (8) | |
C18 | 0.5032 (4) | 0.2396 (3) | 0.2462 (3) | 0.0305 (8) | |
H18 | 0.4304 | 0.1959 | 0.1757 | 0.037* | |
C19 | 0.2923 (4) | 0.2811 (4) | 0.3494 (3) | 0.0320 (8) | |
H19A | 0.2798 | 0.3177 | 0.4316 | 0.038* | |
H19B | 0.2160 | 0.1733 | 0.3279 | 0.038* | |
C20 | 0.2475 (4) | 0.3636 (3) | 0.2656 (3) | 0.0243 (7) | |
C21 | 0.6985 (4) | 0.1814 (4) | 0.1321 (3) | 0.0334 (8) | |
H21A | 0.6091 | 0.0842 | 0.0934 | 0.040* | |
H21B | 0.7899 | 0.1645 | 0.1525 | 0.040* | |
C22 | 0.7419 (4) | 0.2925 (3) | 0.0462 (3) | 0.0265 (7) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cd1 | 0.03223 (17) | 0.02483 (16) | 0.01910 (16) | 0.01568 (11) | 0.00324 (10) | 0.00013 (9) |
N1 | 0.0356 (15) | 0.0267 (14) | 0.0227 (16) | 0.0157 (12) | 0.0049 (13) | −0.0021 (11) |
N2 | 0.0348 (15) | 0.0267 (13) | 0.0190 (15) | 0.0167 (12) | 0.0024 (12) | −0.0013 (11) |
O1 | 0.0246 (12) | 0.0387 (13) | 0.0438 (17) | 0.0143 (10) | 0.0011 (11) | 0.0135 (11) |
O2 | 0.0269 (12) | 0.0334 (12) | 0.0422 (16) | 0.0094 (10) | 0.0020 (11) | 0.0162 (11) |
O3 | 0.0282 (13) | 0.0411 (14) | 0.0372 (16) | 0.0120 (11) | 0.0061 (11) | 0.0143 (12) |
O4 | 0.0324 (13) | 0.0397 (13) | 0.0278 (15) | 0.0161 (11) | 0.0016 (11) | 0.0067 (11) |
C1 | 0.0317 (18) | 0.0310 (17) | 0.033 (2) | 0.0129 (15) | 0.0063 (16) | −0.0055 (15) |
C2 | 0.0274 (17) | 0.0378 (18) | 0.028 (2) | 0.0147 (15) | 0.0067 (15) | −0.0035 (15) |
C3 | 0.0362 (18) | 0.0281 (16) | 0.026 (2) | 0.0199 (15) | 0.0030 (15) | −0.0008 (14) |
C4 | 0.047 (2) | 0.0230 (16) | 0.030 (2) | 0.0120 (15) | 0.0084 (17) | 0.0004 (14) |
C5 | 0.049 (2) | 0.0311 (18) | 0.027 (2) | 0.0164 (16) | 0.0148 (17) | 0.0029 (15) |
C6 | 0.039 (2) | 0.0275 (17) | 0.032 (2) | 0.0159 (15) | 0.0034 (16) | −0.0022 (14) |
C7 | 0.041 (2) | 0.0253 (16) | 0.029 (2) | 0.0159 (15) | 0.0035 (16) | 0.0020 (14) |
C8 | 0.043 (2) | 0.0264 (16) | 0.0231 (19) | 0.0208 (15) | 0.0025 (15) | 0.0031 (14) |
C9 | 0.042 (2) | 0.0247 (16) | 0.024 (2) | 0.0134 (15) | 0.0034 (16) | 0.0008 (14) |
C10 | 0.0374 (19) | 0.0318 (17) | 0.0236 (19) | 0.0159 (15) | 0.0063 (15) | 0.0007 (14) |
C11 | 0.0329 (18) | 0.0315 (17) | 0.0247 (19) | 0.0164 (15) | 0.0010 (15) | −0.0008 (14) |
C12 | 0.0355 (19) | 0.0428 (19) | 0.027 (2) | 0.0245 (16) | 0.0076 (16) | 0.0031 (15) |
C13 | 0.0299 (17) | 0.0306 (17) | 0.028 (2) | 0.0145 (14) | 0.0065 (15) | 0.0121 (15) |
C14 | 0.0363 (19) | 0.0346 (18) | 0.028 (2) | 0.0177 (15) | 0.0081 (16) | 0.0082 (15) |
C15 | 0.038 (2) | 0.0413 (19) | 0.030 (2) | 0.0211 (17) | −0.0032 (16) | 0.0042 (16) |
C16 | 0.0314 (18) | 0.0425 (19) | 0.039 (2) | 0.0221 (16) | 0.0070 (17) | 0.0140 (17) |
C17 | 0.0367 (19) | 0.0299 (17) | 0.030 (2) | 0.0175 (15) | 0.0113 (16) | 0.0138 (15) |
C18 | 0.0331 (18) | 0.0315 (17) | 0.026 (2) | 0.0135 (15) | 0.0033 (15) | 0.0097 (15) |
C19 | 0.0284 (17) | 0.0367 (18) | 0.031 (2) | 0.0137 (15) | 0.0060 (15) | 0.0119 (15) |
C20 | 0.0279 (17) | 0.0261 (15) | 0.0211 (18) | 0.0148 (14) | 0.0042 (14) | 0.0035 (13) |
C21 | 0.041 (2) | 0.0321 (17) | 0.031 (2) | 0.0188 (16) | 0.0109 (17) | 0.0094 (15) |
C22 | 0.0338 (18) | 0.0285 (16) | 0.0193 (18) | 0.0177 (15) | 0.0052 (15) | −0.0010 (13) |
Cd1—N1 | 2.327 (3) | C6—H6 | 0.9400 |
Cd1—N2i | 2.332 (3) | C7—C8 | 1.474 (5) |
Cd1—O3ii | 2.351 (2) | C7—H7 | 0.9400 |
Cd1—O2 | 2.398 (2) | C8—C9 | 1.386 (5) |
Cd1—O3iii | 2.402 (2) | C8—C12 | 1.390 (5) |
Cd1—O1 | 2.413 (2) | C9—C10 | 1.378 (5) |
Cd1—O4iii | 2.470 (2) | C9—H9 | 0.9400 |
Cd1—C20 | 2.729 (3) | C10—H10 | 0.9400 |
Cd1—C22iii | 2.781 (3) | C11—C12 | 1.380 (5) |
N1—C5 | 1.331 (4) | C11—H11 | 0.9400 |
N1—C1 | 1.340 (4) | C12—H12 | 0.9400 |
N2—C10 | 1.337 (4) | C13—C18 | 1.387 (5) |
N2—C11 | 1.338 (4) | C13—C14 | 1.395 (5) |
N2—Cd1iv | 2.331 (3) | C13—C19 | 1.513 (5) |
O1—C20 | 1.249 (4) | C14—C15 | 1.382 (5) |
O2—C20 | 1.247 (4) | C14—H14 | 0.9400 |
O3—C22 | 1.267 (4) | C15—C16 | 1.376 (5) |
O3—Cd1v | 2.351 (2) | C15—H15 | 0.9400 |
O3—Cd1iii | 2.402 (2) | C16—C17 | 1.399 (5) |
O4—C22 | 1.235 (4) | C16—H16 | 0.9400 |
O4—Cd1iii | 2.470 (2) | C17—C18 | 1.392 (5) |
C1—C2 | 1.376 (5) | C17—C21 | 1.507 (5) |
C1—H1 | 0.9400 | C18—H18 | 0.9400 |
C2—C3 | 1.400 (4) | C19—C20 | 1.522 (5) |
C2—H2 | 0.9400 | C19—H19A | 0.9800 |
C3—C4 | 1.385 (5) | C19—H19B | 0.9800 |
C3—C6 | 1.469 (5) | C21—C22 | 1.529 (5) |
C4—C5 | 1.380 (5) | C21—H21A | 0.9800 |
C4—H4 | 0.9400 | C21—H21B | 0.9800 |
C5—H5 | 0.9400 | C22—Cd1iii | 2.781 (3) |
C6—C7 | 1.323 (5) | ||
N1—Cd1—N2i | 172.12 (9) | C3—C4—H4 | 120.1 |
N1—Cd1—O3ii | 92.92 (10) | N1—C5—C4 | 123.3 (3) |
N2i—Cd1—O3ii | 93.60 (10) | N1—C5—H5 | 118.4 |
N1—Cd1—O2 | 88.91 (10) | C4—C5—H5 | 118.4 |
N2i—Cd1—O2 | 88.96 (10) | C7—C6—C3 | 126.8 (3) |
O3ii—Cd1—O2 | 139.86 (8) | C7—C6—H6 | 116.6 |
N1—Cd1—O3iii | 86.43 (9) | C3—C6—H6 | 116.6 |
N2i—Cd1—O3iii | 91.45 (9) | C6—C7—C8 | 125.0 (3) |
O3ii—Cd1—O3iii | 71.46 (9) | C6—C7—H7 | 117.5 |
O2—Cd1—O3iii | 148.59 (8) | C8—C7—H7 | 117.5 |
N1—Cd1—O1 | 88.59 (9) | C9—C8—C12 | 116.8 (3) |
N2i—Cd1—O1 | 96.33 (9) | C9—C8—C7 | 120.0 (3) |
O3ii—Cd1—O1 | 85.54 (8) | C12—C8—C7 | 123.1 (3) |
O2—Cd1—O1 | 54.39 (8) | C10—C9—C8 | 119.7 (3) |
O3iii—Cd1—O1 | 156.16 (8) | C10—C9—H9 | 120.1 |
N1—Cd1—O4iii | 89.83 (9) | C8—C9—H9 | 120.1 |
N2i—Cd1—O4iii | 82.82 (9) | N2—C10—C9 | 123.3 (3) |
O3ii—Cd1—O4iii | 124.49 (8) | N2—C10—H10 | 118.4 |
O2—Cd1—O4iii | 95.59 (8) | C9—C10—H10 | 118.4 |
O3iii—Cd1—O4iii | 53.40 (8) | N2—C11—C12 | 122.8 (3) |
O1—Cd1—O4iii | 149.96 (8) | N2—C11—H11 | 118.6 |
N1—Cd1—C20 | 87.53 (10) | C12—C11—H11 | 118.6 |
N2i—Cd1—C20 | 94.02 (10) | C11—C12—C8 | 120.0 (3) |
O3ii—Cd1—C20 | 112.79 (9) | C11—C12—H12 | 120.0 |
O2—Cd1—C20 | 27.18 (8) | C8—C12—H12 | 120.0 |
O3iii—Cd1—C20 | 172.80 (8) | C18—C13—C14 | 118.6 (3) |
O1—Cd1—C20 | 27.25 (8) | C18—C13—C19 | 120.1 (3) |
O4iii—Cd1—C20 | 122.72 (9) | C14—C13—C19 | 121.3 (3) |
N1—Cd1—C22iii | 88.67 (9) | C15—C14—C13 | 120.6 (3) |
N2i—Cd1—C22iii | 86.02 (9) | C15—C14—H14 | 119.7 |
O3ii—Cd1—C22iii | 98.26 (10) | C13—C14—H14 | 119.7 |
O2—Cd1—C22iii | 121.88 (9) | C16—C15—C14 | 120.2 (4) |
O3iii—Cd1—C22iii | 27.06 (9) | C16—C15—H15 | 119.9 |
O1—Cd1—C22iii | 175.42 (8) | C14—C15—H15 | 119.9 |
O4iii—Cd1—C22iii | 26.36 (9) | C15—C16—C17 | 120.6 (3) |
C20—Cd1—C22iii | 148.87 (10) | C15—C16—H16 | 119.7 |
N1—Cd1—Cd1vi | 89.56 (8) | C17—C16—H16 | 119.7 |
N2i—Cd1—Cd1vi | 93.09 (8) | C18—C17—C16 | 118.3 (3) |
O3ii—Cd1—Cd1vi | 36.17 (6) | C18—C17—C21 | 120.9 (3) |
O2—Cd1—Cd1vi | 175.62 (5) | C16—C17—C21 | 120.7 (3) |
O3iii—Cd1—Cd1vi | 35.29 (6) | C13—C18—C17 | 121.6 (3) |
O1—Cd1—Cd1vi | 121.47 (6) | C13—C18—H18 | 119.2 |
O4iii—Cd1—Cd1vi | 88.51 (6) | C17—C18—H18 | 119.2 |
C20—Cd1—Cd1vi | 148.61 (7) | C13—C19—C20 | 116.1 (3) |
C22iii—Cd1—Cd1vi | 62.17 (8) | C13—C19—H19A | 108.3 |
C5—N1—C1 | 117.3 (3) | C20—C19—H19A | 108.3 |
C5—N1—Cd1 | 118.4 (2) | C13—C19—H19B | 108.3 |
C1—N1—Cd1 | 124.0 (2) | C20—C19—H19B | 108.3 |
C10—N2—C11 | 117.2 (3) | H19A—C19—H19B | 107.4 |
C10—N2—Cd1iv | 118.7 (2) | O2—C20—O1 | 123.5 (3) |
C11—N2—Cd1iv | 123.5 (2) | O2—C20—C19 | 119.4 (3) |
C20—O1—Cd1 | 90.57 (19) | O1—C20—C19 | 117.1 (3) |
C20—O2—Cd1 | 91.3 (2) | O2—C20—Cd1 | 61.47 (17) |
C22—O3—Cd1v | 156.6 (2) | O1—C20—Cd1 | 62.18 (17) |
C22—O3—Cd1iii | 93.4 (2) | C19—C20—Cd1 | 176.6 (2) |
Cd1v—O3—Cd1iii | 108.54 (9) | C17—C21—C22 | 109.4 (3) |
C22—O4—Cd1iii | 91.02 (19) | C17—C21—H21A | 109.8 |
N1—C1—C2 | 123.2 (3) | C22—C21—H21A | 109.8 |
N1—C1—H1 | 118.4 | C17—C21—H21B | 109.8 |
C2—C1—H1 | 118.4 | C22—C21—H21B | 109.8 |
C1—C2—C3 | 119.4 (3) | H21A—C21—H21B | 108.2 |
C1—C2—H2 | 120.3 | O4—C22—O3 | 122.1 (3) |
C3—C2—H2 | 120.3 | O4—C22—C21 | 120.0 (3) |
C4—C3—C2 | 116.9 (3) | O3—C22—C21 | 117.7 (3) |
C4—C3—C6 | 118.5 (3) | O4—C22—Cd1iii | 62.63 (17) |
C2—C3—C6 | 124.5 (3) | O3—C22—Cd1iii | 59.56 (17) |
C5—C4—C3 | 119.8 (3) | C21—C22—Cd1iii | 177.3 (3) |
C5—C4—H4 | 120.1 |
Symmetry codes: (i) x, y+1, z+1; (ii) x−1, y, z; (iii) −x+1, −y+1, −z; (iv) x, y−1, z−1; (v) x+1, y, z; (vi) −x, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | [Cd(C10H8O4)(C12H10N2)] |
Mr | 486.79 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 223 |
a, b, c (Å) | 9.4626 (19), 10.113 (2), 11.351 (2) |
α, β, γ (°) | 98.95 (3), 92.19 (3), 116.88 (3) |
V (Å3) | 949.8 (3) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 1.18 |
Crystal size (mm) | 0.40 × 0.30 × 0.25 |
Data collection | |
Diffractometer | Rigaku MercuryCCD area-detector diffractometer |
Absorption correction | Multi-scan (REQAB; Jacobson, 1998) |
Tmin, Tmax | 0.649, 0.757 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8582, 4256, 3630 |
Rint | 0.029 |
(sin θ/λ)max (Å−1) | 0.649 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.033, 0.083, 1.09 |
No. of reflections | 4256 |
No. of parameters | 263 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.16, −0.85 |
Computer programs: CrystalClear (Rigaku, 2001), CrystalStructure (Rigaku/MSC, 2004), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).
Acknowledgements
This work was supported by the Research Start-Up Fund for New Staff of Huaibei Normal University (grant No. 600581).
References
Jacobson, R. (1998). REQAB. Private communication to Rigaku Corporation, Tokyo, Japan. Google Scholar
Rigaku (2001). CrystalClear. Rigaku Corporation, Tokyo, Japan. Google Scholar
Rigaku/MSC (2004). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Spek, A. L. (2009). Acta Cryst. D65, 148–155. Web of Science CrossRef CAS IUCr Journals Google Scholar
Tao, J., Chen, X.-M., Huang, R.-B. & Zheng, L.-S. (2003). J. Solid State Chem. 170, 130–134. Web of Science CSD CrossRef CAS Google Scholar
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In recent years, particular attention has been devoted to coordination polymers because of their undisputed beauty and potential applications as materials for adsorption, separation, and catalysis (Tao et al., 2003; Tian et al., 2006; Wang et al., 2009). Conformationally flexible dicarboxylate ligands, showing varied geometries, are often featured in these new classes of compounds (Wang et al., 2009).
In this work, the reaction between Cd(NO3)2, 1,3-phenylenediacetic acid (1,3-H2pda) and 1,2-bis(4-pyridyl)ethene (bpe) afforded the title coordination polymer, [Cd(C12H10N2)(C10H8O4)]n (I). In (I), each CdII atom is located in a pentagonal bipyramidally environment, coordinated by five O atoms from three different 1,3-pda ligands at the basal positions and two N atom from two different bpe ligands at the apical position (Fig. 1). Two centrosymmetrically related CdII atoms are linked by two 1,3-pda ligands to form a one-dimensional chain along the a axis (Fig. 2). Such a chain is connected to its adjacent ones via pairs of bpe ligands to form a two-dimensional net extending along the ac plane (Fig. 3).