Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803018622/ww6107sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536803018622/ww6107Isup2.hkl |
CCDC reference: 222832
Key indicators
- Single-crystal X-ray study
- T = 293 K
- Mean (C-C) = 0.006 Å
- R factor = 0.025
- wR factor = 0.065
- Data-to-parameter ratio = 13.6
checkCIF/PLATON results
No syntax errors found
Alert level B PLAT029_ALERT_3_B _diffrn_measured_fraction_theta_full Low ....... 0.98
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 0 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion
The hydrothermal reaction of cadmium chloride (0.06 g, 0.26 mmol), 2,2'-bipyridine (0.04 g, 0.25 mmol) and water (15.0 ml) was carried out at 433 K for 4 d. After cooling to room temperature at 5 K h−1, the crystalline complex, (I), was isolated in 63% yield (based on Cd). IR (KBr, ν, cm−1): 3417, 1604, 1558, 1439, 1375, 1171, 1016, 771, 735. Elemental analysis, calculated for C10H8N2CdCl2: C 35.38, H 2.38, N 8.25%; found: C 35.16, H 2.17, N 8.23%.
All H atoms were located in a difference Fourier map but were introduced in idealized positions (C—H = 0.93 Å) and treated as riding, with displacement parameters fixed at 120% of those of their parent atoms. The maximum residual electron-density peak is 0.84 Å from the Cd atom.
Data collection: SMART (Siemens, 1996); cell refinement: SMART; data reduction: SAINT (Siemens, 1994); program(s) used to solve structure: SHELXTL (Siemens, 1994); program(s) used to refine structure: SHELXTL; molecular graphics: XPREP (Bruker, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick 1997).
[CdCl2(C10H8N2)] | F(000) = 656 |
Mr = 339.49 | Dx = 2.058 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 35 reflections |
a = 17.5517 (6) Å | θ = 2.5–25.0° |
b = 9.3166 (6) Å | µ = 2.44 mm−1 |
c = 7.1710 (4) Å | T = 293 K |
β = 110.860 (2)° | Prism, colourless |
V = 1095.76 (10) Å3 | 0.56 × 0.22 × 0.20 mm |
Z = 4 |
Siemens SMART CCD area-detector diffractometer | 954 independent reflections |
Radiation source: fine-focus sealed tube | 885 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.019 |
ω scans | θmax = 25.0°, θmin = 2.5° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −20→10 |
Tmin = 0.494, Tmax = 0.613 | k = −11→6 |
1693 measured reflections | l = −8→8 |
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)] = 0.025 | H-atom parameters constrained |
wR(F2) = 0.065 | w = 1/[σ2(Fo2) + (0.0528P)2 + 0.4415P] where P = (Fo2 + 2Fc2)/3 |
S = 1.12 | (Δ/σ)max = 0.001 |
954 reflections | Δρmax = 0.43 e Å−3 |
70 parameters | Δρmin = −0.53 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0037 (4) |
[CdCl2(C10H8N2)] | V = 1095.76 (10) Å3 |
Mr = 339.49 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 17.5517 (6) Å | µ = 2.44 mm−1 |
b = 9.3166 (6) Å | T = 293 K |
c = 7.1710 (4) Å | 0.56 × 0.22 × 0.20 mm |
β = 110.860 (2)° |
Siemens SMART CCD area-detector diffractometer | 954 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 885 reflections with I > 2σ(I) |
Tmin = 0.494, Tmax = 0.613 | Rint = 0.019 |
1693 measured reflections |
R[F2 > 2σ(F2)] = 0.025 | 0 restraints |
wR(F2) = 0.065 | H-atom parameters constrained |
S = 1.12 | Δρmax = 0.43 e Å−3 |
954 reflections | Δρmin = −0.53 e Å−3 |
70 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 | ||
Cd | 0.5000 | 0.58652 (3) | 0.7500 | 0.03294 (18) | |
Cl | 0.59307 (5) | 0.41676 (9) | 1.01188 (13) | 0.0381 (2) | |
C1 | 0.3487 (2) | 0.7879 (5) | 0.4744 (6) | 0.0440 (9) | |
H1A | 0.3263 | 0.6989 | 0.4264 | 0.053* | |
C2 | 0.3018 (2) | 0.9094 (5) | 0.4072 (6) | 0.0504 (11) | |
H2A | 0.2486 | 0.9023 | 0.3172 | 0.060* | |
C3 | 0.3354 (3) | 1.0404 (5) | 0.4758 (6) | 0.0526 (11) | |
H3A | 0.3051 | 1.1238 | 0.4319 | 0.063* | |
C4 | 0.4139 (3) | 1.0482 (4) | 0.6096 (6) | 0.0427 (9) | |
H4A | 0.4377 | 1.1366 | 0.6560 | 0.051* | |
C5 | 0.4574 (2) | 0.9218 (3) | 0.6747 (5) | 0.0309 (7) | |
N | 0.42536 (16) | 0.7934 (3) | 0.6064 (4) | 0.0335 (6) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cd | 0.0349 (3) | 0.0249 (2) | 0.0302 (2) | 0.000 | 0.00078 (15) | 0.000 |
Cl | 0.0374 (5) | 0.0361 (5) | 0.0362 (5) | 0.0098 (3) | 0.0073 (4) | 0.0075 (3) |
C1 | 0.0324 (18) | 0.047 (2) | 0.046 (2) | −0.0018 (16) | 0.0052 (16) | 0.0092 (17) |
C2 | 0.031 (2) | 0.068 (3) | 0.047 (2) | 0.0070 (19) | 0.0070 (17) | 0.020 (2) |
C3 | 0.056 (3) | 0.056 (3) | 0.050 (2) | 0.024 (2) | 0.023 (2) | 0.021 (2) |
C4 | 0.055 (2) | 0.0303 (18) | 0.046 (2) | 0.0075 (17) | 0.0225 (19) | 0.0080 (16) |
C5 | 0.0347 (19) | 0.0278 (17) | 0.0335 (17) | 0.0011 (14) | 0.0162 (15) | 0.0030 (13) |
N | 0.0283 (14) | 0.0347 (16) | 0.0344 (15) | −0.0014 (12) | 0.0075 (12) | 0.0052 (12) |
Cd—Ni | 2.352 (3) | C1—H1A | 0.9300 |
Cd—N | 2.352 (3) | C2—C3 | 1.368 (7) |
Cd—Cli | 2.5519 (8) | C2—H2A | 0.9300 |
Cd—Cl | 2.5519 (8) | C3—C4 | 1.373 (6) |
Cd—Clii | 2.7517 (9) | C3—H3A | 0.9300 |
Cd—Cliii | 2.7517 (9) | C4—C5 | 1.390 (5) |
Cl—Cdii | 2.7517 (9) | C4—H4A | 0.9300 |
C1—N | 1.342 (4) | C5—N | 1.338 (4) |
C1—C2 | 1.381 (6) | C5—C5i | 1.502 (7) |
Ni—Cd—N | 69.93 (14) | N—C1—H1A | 118.7 |
Ni—Cd—Cli | 160.22 (7) | C2—C1—H1A | 118.7 |
N—Cd—Cli | 94.29 (7) | C3—C2—C1 | 118.6 (4) |
Ni—Cd—Cl | 94.29 (7) | C3—C2—H2A | 120.7 |
N—Cd—Cl | 160.22 (7) | C1—C2—H2A | 120.7 |
Cli—Cd—Cl | 103.40 (4) | C2—C3—C4 | 119.7 (4) |
Ni—Cd—Clii | 95.66 (7) | C2—C3—H3A | 120.2 |
N—Cd—Clii | 85.39 (7) | C4—C3—H3A | 120.2 |
Cli—Cd—Clii | 94.81 (3) | C3—C4—C5 | 118.9 (4) |
Cl—Cd—Clii | 84.40 (3) | C3—C4—H4A | 120.5 |
Ni—Cd—Cliii | 85.39 (7) | C5—C4—H4A | 120.5 |
N—Cd—Cliii | 95.66 (7) | N—C5—C4 | 121.7 (4) |
Cli—Cd—Cliii | 84.40 (3) | N—C5—C5i | 116.37 (19) |
Cl—Cd—Cliii | 94.81 (3) | C4—C5—C5i | 121.9 (2) |
Clii—Cd—Cliii | 178.73 (4) | C5—N—C1 | 118.5 (3) |
Cd—Cl—Cdii | 95.60 (3) | C5—N—Cd | 118.5 (2) |
N—C1—C2 | 122.6 (4) | C1—N—Cd | 122.7 (3) |
Ni—Cd—Cl—Cdii | 95.28 (7) | C5i—C5—N—Cd | 5.7 (5) |
N—Cd—Cl—Cdii | 59.2 (2) | C2—C1—N—C5 | −0.1 (6) |
Cli—Cd—Cl—Cdii | −93.63 (3) | C2—C1—N—Cd | 172.6 (3) |
Clii—Cd—Cl—Cdii | 0.0 | Ni—Cd—N—C5 | −2.15 (18) |
Cliii—Cd—Cl—Cdii | −179.00 (3) | Cli—Cd—N—C5 | −169.9 (2) |
N—C1—C2—C3 | 1.0 (6) | Cl—Cd—N—C5 | 36.5 (4) |
C1—C2—C3—C4 | −0.5 (6) | Clii—Cd—N—C5 | 95.6 (2) |
C2—C3—C4—C5 | −0.9 (6) | Cliii—Cd—N—C5 | −85.1 (2) |
C3—C4—C5—N | 1.8 (5) | Ni—Cd—N—C1 | −174.9 (4) |
C3—C4—C5—C5i | −178.3 (4) | Cli—Cd—N—C1 | 17.4 (3) |
C4—C5—N—C1 | −1.3 (5) | Cl—Cd—N—C1 | −136.2 (3) |
C5i—C5—N—C1 | 178.8 (4) | Clii—Cd—N—C1 | −77.1 (3) |
C4—C5—N—Cd | −174.3 (3) | Cliii—Cd—N—C1 | 102.1 (3) |
Symmetry codes: (i) −x+1, y, −z+3/2; (ii) −x+1, −y+1, −z+2; (iii) x, −y+1, z−1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H2A···Cliv | 0.93 | 2.83 | 3.751 (5) | 171 |
C4—H4A···Clv | 0.93 | 2.84 | 3.534 (5) | 132 |
Symmetry codes: (iv) x−1/2, y+1/2, z−1; (v) −x+1, y+1, −z+3/2. |
Experimental details
Crystal data | |
Chemical formula | [CdCl2(C10H8N2)] |
Mr | 339.49 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 293 |
a, b, c (Å) | 17.5517 (6), 9.3166 (6), 7.1710 (4) |
β (°) | 110.860 (2) |
V (Å3) | 1095.76 (10) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 2.44 |
Crystal size (mm) | 0.56 × 0.22 × 0.20 |
Data collection | |
Diffractometer | Siemens SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.494, 0.613 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 1693, 954, 885 |
Rint | 0.019 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.025, 0.065, 1.12 |
No. of reflections | 954 |
No. of parameters | 70 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.43, −0.53 |
Computer programs: SMART (Siemens, 1996), SMART, SAINT (Siemens, 1994), SHELXTL (Siemens, 1994), SHELXTL, XPREP (Bruker, 1997), SHELXL97 (Sheldrick 1997).
Cd—Ni | 2.352 (3) | C2—C3 | 1.368 (7) |
Cd—Cl | 2.5519 (8) | C3—C4 | 1.373 (6) |
Cd—Clii | 2.7517 (9) | C4—C5 | 1.390 (5) |
C1—N | 1.342 (4) | C5—N | 1.338 (4) |
C1—C2 | 1.381 (6) | C5—C5i | 1.502 (7) |
Ni—Cd—N | 69.93 (14) | Cl—Cd—Clii | 84.40 (3) |
Ni—Cd—Cli | 160.22 (7) | Clii—Cd—Cliii | 178.73 (4) |
N—Cd—Cli | 94.29 (7) | Cd—Cl—Cdii | 95.60 (3) |
N—Cd—Cl | 160.22 (7) | N—C1—C2 | 122.6 (4) |
Cli—Cd—Cl | 103.40 (4) | C3—C2—C1 | 118.6 (4) |
Ni—Cd—Clii | 95.66 (7) | C2—C3—C4 | 119.7 (4) |
N—Cd—Clii | 85.39 (7) | C3—C4—C5 | 118.9 (4) |
Cli—Cd—Clii | 94.81 (3) | N—C5—C4 | 121.7 (4) |
Symmetry codes: (i) −x+1, y, −z+3/2; (ii) −x+1, −y+1, −z+2; (iii) x, −y+1, z−1/2. |
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Polynuclear d10 metal complexes have been found to exhibit intriguing structural and photoluminescent properties. Chloride-bridged cadmium(II) polymeric complexes are of considerable interest, because they may act as photoactive materials. Structural studies of chloride-bridged CdII polymeric complexes are common (Bell et al., 1982; Griffith et al., 1982; Bigoli et al., 1983; Huang et al., 1998). However, CdII polymeric complexes with a CdCl2N2 coordination polydedron have rarely been reported (Bonomo et al., 1989). We have introduced 2,2'-bipyridine as a terminal ligand which favours crystal growth of the product. Through a hydrothermal reaction, we have successfully synthesized the title crystalline chloride-bridged Cd complex [CdCl2(bpy)]n (bpy is 2,2'-bipyridine), (I).
Single crystal X-ray diffraction analysis reveals that compound (I) crystallizes in space group C2/c and consists of one-dimensional chains along the c axis. It is isostructural with an analogous bromide-bridged CuII complex (Garland et al., 1988). The CdII ion is positioned on the 21 axis, so the primarily monomeric unit is generated by symmetry (Fig. 1).
The CdII ion in (I) is coordinated by two N atoms from one chelating bpy ligand and by four Cl atoms, to furnish a distorted coordination octahedron, as depicted in Fig. 2. The basal plane is formed by the two cis N atoms from the bpy ligand [Cd—N 2.352 (3) Å] and the two cis Cl atoms [Cd—Cl 2.5519 (8) Å]. The axial positions of the octahedron are occupied by Cl atoms from neighbouring monomeric units [Cd—Cl 2.7517 (9) Å]. Adjacent Cd coordination octahedra share Cl—Cl edges, thus forming a one-dimensional chain along the c axis. All bpy ligands are coordinated in a chelating mode and they lie on alternate sides of the chain. The Cd···Cd distance between neighbouring CdII ions in the chain is 3.931 (9) Å, which is shorter than that of the CuII isomorph [3.974 (1) Å]. The closest distance between the pyridyl rings of two bpy ligands in neighbouring chains is 3.342 (3) Å, indicating the existence of π–π interactions between the adjacent chains. Thus the chains are connected to each other via π–π interactions to form two-dimensional layers parallel to the bc plane.
The packing of (I) (Fig. 3) is determined by van der Waals interactions and possible hydrogen bonds involving the C atoms of the bpy ligand and Cl atoms of the same [C4—H4A···Cli 3.534 (5) Å] or adjacent [C2—H2A···Clii 3.751 (5) Å] chains [symmetry codes: (i) 1 − x, 1 + y, 3/2 − z; (ii) x − 1/2, 1/2 + y, z − 1].