supplementary materials


Acta Cryst. (2007). E63, m2543    [ doi:10.1107/S1600536807044066 ]

Poly[bis([mu]2-azido-[kappa]2N1:N3)([mu]2-3,5-di-2-pyridyl-1,2,4-triazole-[kappa]4N1,N5:N2,N3)manganese(II)]

S. Hu, S.-H. Zhang and M.-H. Zeng

Abstract top

In the crystal structure of the polymeric title compound, [Mn2(N3)2(C12H8N5)2]n, the MnII atom exists in an octahedral geometry owing to coordination by four N atoms from two 3,5-bis(pyridin-2-yl)-1,2,4-triazolate ligands and by two azide ligands. The heterocyclic ligand binds in a chelating mode. The bidentate bridging mode of both anions leads to a linear ribbon motif.

Comment top

1,2,4-triazole derivatives are a class of azole compounds that can act as either 2,4- or 1,2-bridging nitrogen donor ligands. 3,5-bis(pyridin-2-yl)-1,2,4-triazole can act as tetradentate ligands and are therefore very suitable for studying exchange-coupled pairs of transition-metal ions. (Prins et al., 1995; Chen et al., 2006). However, only small part of mononuclear and dinuclear complexes were characterized by X-ray crystallography. On the other hand, azide was widely used to connect metal ions, and the correlation between the structure and magnetic properties of different coordination modes was observed (Wang et al., 2006). In this paper, solvothermal technique has been successfully applied in the Mn2+/bpt/N3 system to synthesize the title compound.

There are one MnII atom, one bpt ligand and one azide ligand in the asymmetric unit. The MnII atom has an octahedral environment, formed by four N atoms from two different bpt ligand and two N atoms belonging to two azide ligands. The bpt ligand binds to manganese in a cis-bis(chelate) mode, through two pyridine and two triazole nitrogen atoms, linking the MnII atoms into a helical chain that runs along the b axis. Each pair of MnII ions from adjacent chains are additionally bridged by two azide lingds in the EE mode and further linked the [Mn(bpt)]+ chains into a two-dimensional (4,4) net.

Related literature top

For related literature, see: Prins et al. (1995); Chen et al. (2006); Wang et al. (2006).

Experimental top

A mixture of manganese sulfate monohydrate (0.169 g, 1 mmol), sodium azide (0.065 g, 1 mmol) 3,5-bis(pyridin-2-yl)-1,2,4-triazole (0.223 g, 1 mmol) and methanol (10 ml) was heated in a Teflon-lined stainless steel autoclave (25 ml) for 120 h at 393 K, after which the autoclave was cooled to room temperature over a period of 8 h at a rate of 10 K h−1. Pale yellow block single crystals of (I) were collected in about 15% yield. Elemental analysis, calcd (%) for C12H8MnN8: C, 45.16; H, 2.53; N, 35.11; found (%): C, 45.19; H, 2.50; N, 35.07.

Refinement top

All other H atoms were positioned geometrically and refined as riding, with C–H distances of 0.93 Å and Uiso(H) = 1.2 Ueq(C).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL (Bruker, 1997).

Figures top
[Figure 1] Fig. 1. The asymmetric unit of (I), showing displacement ellipsoids drawn at the 30% probability level for non-H atoms. Hydrogen atoms have been omitted. Symmetry codes: (i) −x, y − 1/2, −z; (ii) 1 − x, y-1/2,-z.
[Figure 2] Fig. 2. 3-D Packing diagram of title complex; Hydrogen atoms have been omitted.
Poly[bis(µ2-azido-κ2N1:N3)(µ2-3,5-di-2-pyridyl- 1,2,4-triazole-κ4N1,N5:N2,N3)manganese(II)] top
Crystal data top
[Mn2(N3)2(C12H8N5)2]F000 = 322
Mr = 638.38Dx = 1.660 Mg m3
Monoclinic, P21Mo Kα radiation
λ = 0.71073 Å
a = 8.6965 (9) ÅCell parameters from 2337 reflections
b = 6.5597 (7) Åθ = 1.8–27.0º
c = 11.8601 (13) ŵ = 1.04 mm1
β = 109.245 (2)ºT = 293 (2) K
V = 638.77 (12) Å3Block, pale yellow
Z = 10.31 × 0.26 × 0.22 mm
Data collection top
Bruker APEX area-detector
diffractometer
2337 independent reflections
Radiation source: fine-focus sealed tube2207 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.019
T = 293(2) Kθmax = 27.0º
φ and ω scansθmin = 1.8º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 8→11
Tmin = 0.732, Tmax = 0.796k = 6→8
3598 measured reflectionsl = 15→11
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.035  w = 1/[σ2(Fo2) + (0.0334P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.076(Δ/σ)max = 0.001
S = 1.05Δρmax = 0.40 e Å3
2337 reflectionsΔρmin = 0.23 e Å3
190 parametersExtinction correction: none
1 restraintAbsolute structure: Flack (1983), with 825 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.02 (2)
Secondary atom site location: difference Fourier map
Crystal data top
[Mn2(N3)2(C12H8N5)2]V = 638.77 (12) Å3
Mr = 638.38Z = 1
Monoclinic, P21Mo Kα
a = 8.6965 (9) ŵ = 1.04 mm1
b = 6.5597 (7) ÅT = 293 (2) K
c = 11.8601 (13) Å0.31 × 0.26 × 0.22 mm
β = 109.245 (2)º
Data collection top
Bruker APEX area-detector
diffractometer
2337 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2207 reflections with I > 2σ(I)
Tmin = 0.732, Tmax = 0.796Rint = 0.019
3598 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.035H-atom parameters constrained
wR(F2) = 0.076Δρmax = 0.40 e Å3
S = 1.05Δρmin = 0.23 e Å3
2337 reflectionsAbsolute structure: Flack (1983), with 825 Friedel pairs
190 parametersFlack parameter: 0.02 (2)
1 restraint
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
Mn10.20518 (4)0.28461 (8)0.01852 (3)0.02671 (12)
C10.2386 (4)0.0499 (5)0.1771 (3)0.0378 (8)
H1A0.28450.13570.11230.045*
C20.2498 (4)0.1043 (6)0.2863 (3)0.0432 (9)
H2A0.30230.22400.29480.052*
C30.1817 (4)0.0222 (6)0.3828 (3)0.0433 (9)
H3A0.18960.00900.45720.052*
C40.1025 (4)0.1938 (6)0.3673 (3)0.0398 (8)
H4A0.05450.28000.43160.048*
C50.0938 (3)0.2397 (5)0.2553 (3)0.0301 (8)
C60.0090 (3)0.4189 (5)0.2304 (2)0.0279 (6)
C70.1260 (4)0.6830 (5)0.2408 (3)0.0271 (6)
C80.2227 (4)0.8677 (5)0.2788 (3)0.0298 (7)
C90.2739 (4)0.9397 (6)0.3957 (3)0.0412 (8)
H9A0.25080.86740.45560.049*
C100.3587 (5)1.1186 (6)0.4209 (3)0.0492 (10)
H10A0.39431.16890.49850.059*
C110.3914 (4)1.2242 (6)0.3312 (3)0.0475 (9)
H11A0.44691.34770.34630.057*
C120.3394 (4)1.1413 (6)0.2185 (3)0.0418 (8)
H12A0.36271.21120.15790.050*
N10.0114 (3)0.4542 (4)0.1192 (2)0.0277 (6)
N20.0767 (3)0.6266 (4)0.1258 (2)0.0272 (6)
N30.0742 (3)0.5565 (4)0.3107 (2)0.0311 (6)
N40.1652 (3)0.1196 (4)0.1599 (2)0.0305 (6)
N50.2582 (3)0.9683 (4)0.1913 (2)0.0315 (6)
N60.3757 (3)0.4973 (5)0.0301 (3)0.0504 (8)
N70.4788 (3)0.5367 (4)0.0680 (2)0.0302 (6)
N80.5818 (3)0.5817 (5)0.1066 (3)0.0400 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.0275 (2)0.0289 (2)0.0258 (2)0.0011 (2)0.01163 (15)0.0022 (2)
C10.0392 (18)0.0314 (19)0.0395 (18)0.0030 (16)0.0084 (15)0.0001 (15)
C20.0461 (19)0.035 (2)0.048 (2)0.0058 (17)0.0147 (16)0.0104 (17)
C30.053 (2)0.048 (2)0.0321 (18)0.0030 (18)0.0171 (16)0.0110 (16)
C40.0419 (18)0.046 (2)0.0304 (17)0.0092 (16)0.0112 (15)0.0016 (15)
C50.0306 (14)0.032 (2)0.0277 (14)0.0035 (13)0.0100 (12)0.0002 (12)
C60.0285 (15)0.0312 (18)0.0261 (15)0.0018 (13)0.0119 (12)0.0001 (13)
C70.0259 (14)0.0311 (17)0.0256 (15)0.0003 (13)0.0104 (12)0.0005 (12)
C80.0281 (15)0.0306 (16)0.0317 (16)0.0023 (13)0.0113 (13)0.0007 (13)
C90.049 (2)0.042 (2)0.0333 (17)0.0043 (18)0.0149 (15)0.0046 (16)
C100.055 (2)0.049 (2)0.040 (2)0.008 (2)0.0101 (18)0.0164 (17)
C110.050 (2)0.033 (2)0.057 (2)0.0087 (16)0.0147 (18)0.0102 (16)
C120.0446 (19)0.034 (2)0.048 (2)0.0056 (16)0.0171 (17)0.0014 (16)
N10.0283 (13)0.0302 (15)0.0286 (13)0.0021 (11)0.0148 (10)0.0009 (11)
N20.0248 (12)0.0300 (15)0.0282 (13)0.0021 (11)0.0106 (10)0.0027 (11)
N30.0363 (14)0.0314 (15)0.0275 (13)0.0038 (12)0.0133 (11)0.0021 (11)
N40.0329 (13)0.0275 (15)0.0305 (14)0.0015 (12)0.0098 (11)0.0016 (11)
N50.0350 (14)0.0289 (15)0.0326 (14)0.0023 (12)0.0140 (12)0.0003 (12)
N60.0377 (16)0.050 (2)0.068 (2)0.0082 (15)0.0233 (15)0.0086 (17)
N70.0313 (13)0.0225 (13)0.0353 (14)0.0001 (11)0.0089 (12)0.0024 (11)
N80.0380 (15)0.0431 (19)0.0441 (17)0.0086 (13)0.0207 (13)0.0045 (14)
Geometric parameters (Å, °) top
Mn1—N2i2.208 (2)C7—N21.340 (4)
Mn1—N12.221 (2)C7—N31.351 (4)
Mn1—N8ii2.240 (3)C7—C81.459 (4)
Mn1—N62.245 (3)C8—N51.348 (4)
Mn1—N5i2.289 (3)C8—C91.392 (4)
Mn1—N42.299 (3)C9—C101.365 (5)
C1—N41.331 (4)C9—H9A0.9300
C1—C21.377 (5)C10—C111.375 (5)
C1—H1A0.9300C10—H10A0.9300
C2—C31.380 (5)C11—C121.374 (5)
C2—H2A0.9300C11—H11A0.9300
C3—C41.363 (5)C12—N51.319 (4)
C3—H3A0.9300C12—H12A0.9300
C4—C51.389 (4)N1—N21.354 (3)
C4—H4A0.9300N2—Mn1iii2.208 (2)
C5—N41.351 (4)N5—Mn1iii2.289 (3)
C5—C61.468 (4)N6—N71.157 (4)
C6—N11.333 (4)N7—N81.170 (4)
C6—N31.339 (4)N8—Mn1iv2.240 (3)
N2i—Mn1—N1104.67 (9)N2—C7—C8120.1 (3)
N2i—Mn1—N8ii87.13 (10)N3—C7—C8126.5 (3)
N1—Mn1—N8ii162.01 (9)N5—C8—C9121.5 (3)
N2i—Mn1—N6160.37 (11)N5—C8—C7115.1 (3)
N1—Mn1—N684.57 (10)C9—C8—C7123.5 (3)
N8ii—Mn1—N688.54 (11)C10—C9—C8118.8 (3)
N2i—Mn1—N5i73.88 (9)C10—C9—H9A120.6
N1—Mn1—N5i105.95 (9)C8—C9—H9A120.6
N8ii—Mn1—N5i90.21 (10)C9—C10—C11119.9 (3)
N6—Mn1—N5i87.01 (11)C9—C10—H10A120.1
N2i—Mn1—N4110.94 (9)C11—C10—H10A120.1
N1—Mn1—N473.20 (9)C12—C11—C10117.9 (3)
N8ii—Mn1—N490.03 (10)C12—C11—H11A121.1
N6—Mn1—N488.19 (11)C10—C11—H11A121.1
N5i—Mn1—N4175.18 (10)N5—C12—C11123.8 (3)
N4—C1—C2123.2 (3)N5—C12—H12A118.1
N4—C1—H1A118.4C11—C12—H12A118.1
C2—C1—H1A118.4C6—N1—N2105.3 (2)
C1—C2—C3118.7 (3)C6—N1—Mn1113.65 (19)
C1—C2—H2A120.7N2—N1—Mn1137.63 (19)
C3—C2—H2A120.7C7—N2—N1105.9 (2)
C4—C3—C2118.9 (3)C7—N2—Mn1iii113.8 (2)
C4—C3—H3A120.6N1—N2—Mn1iii137.99 (19)
C2—C3—H3A120.6C6—N3—C7100.9 (2)
C3—C4—C5119.8 (3)C1—N4—C5118.0 (3)
C3—C4—H4A120.1C1—N4—Mn1126.9 (2)
C5—C4—H4A120.1C5—N4—Mn1112.7 (2)
N4—C5—C4121.4 (3)C12—N5—C8118.2 (3)
N4—C5—C6114.9 (3)C12—N5—Mn1iii127.3 (2)
C4—C5—C6123.7 (3)C8—N5—Mn1iii113.7 (2)
N1—C6—N3114.5 (3)N7—N6—Mn1154.2 (3)
N1—C6—C5119.6 (3)N6—N7—N8178.3 (4)
N3—C6—C5125.9 (2)N7—N8—Mn1iv126.1 (2)
N2—C7—N3113.3 (3)
Symmetry codes: (i) −x, y−1/2, −z; (ii) −x+1, y−1/2, −z; (iii) −x, y+1/2, −z; (iv) −x+1, y+1/2, −z.
Acknowledgements top

The authors acknowledge financial support by the Natural Science Foundation of China (grant No. 20561001) and the Patent Special Foundation of the Ministry of Education of Guangxi Province (grant No. 2006–26).

references
References top

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