supplementary materials


cv2561 scheme

Acta Cryst. (2009). E65, m693    [ doi:10.1107/S1600536809019266 ]

Dibromido(2,2':6',2''-terpyridine-[kappa]3N,N',N'')zinc(II)

Q.-L. Zhao and G.-P. Li

Abstract top

In the title compound, [ZnBr2(C15H11N3)], the ZnII ion is five-coordinated by the three N atoms from a 2,2':6',2''-terpyridine ligand (terpy) and two bromide anions in a distorted trigonal bipyramidal configuration. Each molecule is situated on a twofold rotational axis that passes through the ZnII ion and the central ring of the terpy ligand. In the crystal structure, aromatic [pi]-[pi] interactions between terpy ligands [centroid-centroid distances = 3.6265 (9) Å] link molecules into stacks propagated in the [001] direction.

Comment top

As a contribution to structural characterization of 2,2':6',2''-terpyridine complexes (Alizadeh et al., 2009; Huang et al., 2009; Ma et al., 2009; Bai et al., 2009) we present here the title complex (I).

In (I) (Fig. 1), the ZnII ion is five-coordinated in a distorted trigonal bipyramidal configuration by three N atoms from a 2,2':6',2''-terpyridine ligand and by two Br anions. The Zn–Br and Zn–N bond lengths are within normal ranges (Mahmoudi et al., 2009).

In the crystal structure, the ππ stacking interactions between aromatic rings of Cg1 and Cg2 [Cg1 and Cg2 are (N1, C6 — C8, C7i, C6i) and (N2, C1 — C5) ring centroids, respectively, symmetry code: (i) -x + 1, y, -z + 1/2] are observed, with a centroid–centroid distances of 3.6265 (9) Å.

Related literature top

For related structures, see: Alizadeh et al. (2009); Mahmoudi et al. (2009); Huang et al. (2009); Ma et al. (2009); Bai et al. (2009).

Experimental top

The title compound was synthesized hydrothermally in a Teflon-lined autoclave (25 mL) by heating a mixture of 2,2':6',2''-terpyridine (0.2 mmol), ZnBr2 (0.2 mmol) and one drop of Et3N (pH 8–9) in water (10 mL) at 393 K for 3 d. Crystals suitable for X-ray analysis were obtained.

Refinement top

All H atoms were included in calculated positions, with C—H distances fixed to 0.93 Å and were refined in the riding-model approximation, with Uiso(H) = 1.2 Ueq (C).

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT (Bruker, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with the atom-labelling scheme [symmetry code: (A) -x, + 1, y, -z + 1/2]. Displacement ellipsoids are drawn at the 50% probability level. H atoms are presented as small spheres of arbitrary radius.
[Figure 2] Fig. 2. A portion of the crystal packing showing the ππ interactions (dashed lines) between the aromatic rings.
Dibromido(2,2':6',2''-terpyridine-κ3N,N',N'')zinc(II) top
Crystal data top
[ZnBr2(C15H11N3)]F000 = 888
Mr = 458.46Dx = 2.042 Mg m3
Monoclinic, C2/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 1580 reflections
a = 17.0972 (5) Åθ = 2.5–26.3º
b = 9.3528 (3) ŵ = 7.00 mm1
c = 11.5334 (4) ÅT = 296 K
β = 126.0510 (10)ºBlock, colourless
V = 1491.08 (8) Å30.20 × 0.18 × 0.16 mm
Z = 4
Data collection top
Bruker SMART APEXII CCD
diffractometer
1457 independent reflections
Radiation source: fine-focus sealed tube1371 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.019
T = 296 Kθmax = 26.0º
φ and ω scansθmin = 2.6º
Absorption correction: multi-scan
(SADABS; Bruker, 2005)
h = 21→21
Tmin = 0.335, Tmax = 0.401k = 11→11
9665 measured reflectionsl = 14→14
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.015H-atom parameters constrained
wR(F2) = 0.039  w = 1/[σ2(Fo2) + (0.0184P)2 + 1.2604P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
1457 reflectionsΔρmax = 0.27 e Å3
97 parametersΔρmin = 0.29 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
[ZnBr2(C15H11N3)]V = 1491.08 (8) Å3
Mr = 458.46Z = 4
Monoclinic, C2/cMo Kα
a = 17.0972 (5) ŵ = 7.00 mm1
b = 9.3528 (3) ÅT = 296 K
c = 11.5334 (4) Å0.20 × 0.18 × 0.16 mm
β = 126.0510 (10)º
Data collection top
Bruker SMART APEXII CCD
diffractometer
1457 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2005)
1371 reflections with I > 2σ(I)
Tmin = 0.335, Tmax = 0.401Rint = 0.019
9665 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.01597 parameters
wR(F2) = 0.039H-atom parameters constrained
S = 1.08Δρmax = 0.27 e Å3
1457 reflectionsΔρmin = 0.29 e Å3
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br10.380531 (15)0.11870 (2)0.03979 (2)0.04022 (8)
Zn10.50000.25499 (3)0.25000.02736 (8)
N10.50000.4802 (2)0.25000.0253 (4)
N20.58982 (11)0.31649 (16)0.18054 (15)0.0288 (3)
C10.63375 (14)0.2248 (2)0.1474 (2)0.0352 (4)
H10.62560.12720.15250.042*
C20.69093 (14)0.2696 (2)0.1056 (2)0.0392 (4)
H20.72100.20330.08380.047*
C30.70254 (14)0.4137 (2)0.0970 (2)0.0394 (4)
H30.74110.44610.07000.047*
C40.65606 (13)0.5102 (2)0.12890 (18)0.0346 (4)
H40.66200.60810.12190.042*
C50.60056 (12)0.45792 (18)0.17152 (16)0.0268 (4)
C60.54892 (12)0.55136 (18)0.21013 (16)0.0263 (3)
C70.54910 (13)0.69976 (19)0.20701 (19)0.0337 (4)
H70.58150.74850.17670.040*
C80.50000.7736 (3)0.25000.0367 (6)
H80.50000.87300.25000.044*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.04910 (14)0.03300 (12)0.03959 (12)0.01116 (8)0.02667 (10)0.00711 (7)
Zn10.03545 (17)0.01984 (14)0.03395 (16)0.0000.02441 (14)0.000
N10.0293 (10)0.0231 (10)0.0253 (9)0.0000.0170 (9)0.000
N20.0322 (8)0.0264 (8)0.0335 (7)0.0007 (6)0.0224 (7)0.0004 (6)
C10.0407 (11)0.0311 (10)0.0417 (10)0.0025 (8)0.0285 (9)0.0011 (8)
C20.0372 (11)0.0487 (12)0.0398 (10)0.0025 (9)0.0271 (9)0.0038 (9)
C30.0354 (10)0.0545 (12)0.0380 (10)0.0069 (9)0.0271 (9)0.0022 (9)
C40.0367 (10)0.0359 (10)0.0339 (9)0.0072 (8)0.0222 (8)0.0005 (8)
C50.0268 (9)0.0287 (9)0.0235 (7)0.0027 (7)0.0139 (7)0.0004 (7)
C60.0274 (9)0.0247 (8)0.0237 (7)0.0027 (7)0.0133 (7)0.0007 (6)
C70.0360 (10)0.0268 (9)0.0351 (9)0.0042 (8)0.0193 (8)0.0030 (7)
C80.0426 (16)0.0201 (12)0.0409 (14)0.0000.0210 (13)0.000
Geometric parameters (Å, °) top
Br1—Zn12.4179 (2)C2—H20.9300
Zn1—N12.106 (2)C3—C41.388 (3)
Zn1—N2i2.1861 (14)C3—H30.9300
Zn1—N22.1861 (14)C4—C51.389 (2)
Zn1—Br1i2.4179 (2)C4—H40.9300
N1—C6i1.3441 (19)C5—C61.485 (2)
N1—C61.3441 (19)C6—C71.388 (3)
N2—C11.336 (2)C7—C81.385 (2)
N2—C51.348 (2)C7—H70.9300
C1—C21.385 (3)C8—C7i1.385 (2)
C1—H10.9300C8—H80.9300
C2—C31.374 (3)
N1—Zn1—N2i74.75 (4)C3—C2—H2120.5
N1—Zn1—N274.75 (4)C1—C2—H2120.5
N2i—Zn1—N2149.49 (8)C2—C3—C4119.27 (17)
N1—Zn1—Br1121.815 (7)C2—C3—H3120.4
N2i—Zn1—Br198.34 (4)C4—C3—H3120.4
N2—Zn1—Br197.60 (4)C3—C4—C5118.78 (18)
N1—Zn1—Br1i121.815 (7)C3—C4—H4120.6
N2i—Zn1—Br1i97.60 (4)C5—C4—H4120.6
N2—Zn1—Br1i98.34 (4)N2—C5—C4121.69 (16)
Br1—Zn1—Br1i116.370 (14)N2—C5—C6114.99 (14)
C6i—N1—C6120.6 (2)C4—C5—C6123.32 (16)
C6i—N1—Zn1119.68 (10)N1—C6—C7121.01 (16)
C6—N1—Zn1119.68 (10)N1—C6—C5114.25 (15)
C1—N2—C5118.88 (15)C7—C6—C5124.74 (15)
C1—N2—Zn1124.80 (12)C8—C7—C6118.57 (17)
C5—N2—Zn1116.32 (11)C8—C7—H7120.7
N2—C1—C2122.43 (18)C6—C7—H7120.7
N2—C1—H1118.8C7i—C8—C7120.2 (2)
C2—C1—H1118.8C7i—C8—H8119.9
C3—C2—C1118.93 (18)C7—C8—H8119.9
N2i—Zn1—N1—C6i0.68 (9)C1—C2—C3—C40.6 (3)
N2—Zn1—N1—C6i179.32 (9)C2—C3—C4—C51.3 (3)
Br1—Zn1—N1—C6i91.12 (8)C1—N2—C5—C40.1 (2)
Br1i—Zn1—N1—C6i88.88 (8)Zn1—N2—C5—C4179.88 (12)
N2i—Zn1—N1—C6179.32 (9)C1—N2—C5—C6179.87 (15)
N2—Zn1—N1—C60.68 (9)Zn1—N2—C5—C60.19 (18)
Br1—Zn1—N1—C688.88 (8)C3—C4—C5—N20.9 (3)
Br1i—Zn1—N1—C691.12 (8)C3—C4—C5—C6179.12 (16)
N1—Zn1—N2—C1179.71 (15)C6i—N1—C6—C70.96 (12)
N2i—Zn1—N2—C1179.71 (15)Zn1—N1—C6—C7179.04 (12)
Br1—Zn1—N2—C159.30 (14)C6i—N1—C6—C5179.02 (15)
Br1i—Zn1—N2—C158.90 (14)Zn1—N1—C6—C50.98 (15)
N1—Zn1—N2—C50.23 (11)N2—C5—C6—N10.74 (19)
N2i—Zn1—N2—C50.23 (11)C4—C5—C6—N1179.33 (14)
Br1—Zn1—N2—C5120.76 (11)N2—C5—C6—C7179.29 (16)
Br1i—Zn1—N2—C5121.05 (11)C4—C5—C6—C70.6 (3)
C5—N2—C1—C20.8 (3)N1—C6—C7—C81.9 (2)
Zn1—N2—C1—C2179.16 (14)C5—C6—C7—C8178.10 (13)
N2—C1—C2—C30.4 (3)C6—C7—C8—C7i0.91 (11)
Symmetry codes: (i) −x+1, y, −z+1/2.
Acknowledgements top

The authors are grateful to the Henan Administration of Science and Technology for financial support (grant No. 092300410031).

references
References top

Alizadeh, R., Heidari, A., Ahmadi, R. & Amani, V. (2009). Acta Cryst. E65, m483–m484.

Bai, F. Q., Zhou, X., Xia, B. H., Liu, T., Zhang, J. P. & Zhang, H. X. (2009). J. Organomet. Chem. 694, 1848–1860.

Bruker (2005). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.

Huang, W., You, W., Wang, L. & Yao, C. (2009). Inorg. Chim. Acta, 362, 2127–2135.

Ma, Z., Xing, Y. P., Yang, M., Hua, M., Liu, B. Q., da Silva, M. F. C. G. & Pombeiro, A. J. L. (2009). Inorg. Chim. Acta, 362, 2921–2926.

Mahmoudi, A., Khalaj, M., Gao, S., Ng, S. W. & Mohammadgholiha, M. (2009). Acta Cryst. E65, m555.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.