supplementary materials


Acta Cryst. (2009). E65, m547-m548    [ doi:10.1107/S1600536809013828 ]

Bis(2,2'-bipyridine N,N'-dioxide)bis(tricyanomethanido)manganese(II)

J. Luo, F. Yang, L.-J. Qiu, X.-X. Wang and B.-S. Liu

Abstract top

In the title complex, [Mn(C4N3)2(C10H8N2O2)2], the MnII atom lies on an inversion center and is coordinated by two 2,2'-bipyridine N,N'-dioxide (dpdo) molecules and two tricyanomethanide (tcm) ligands to form a distorted octahedral geometry. Weak intermolecular C-H...O or C-H...N hydrogen bonds, involving either the O atom of the dpdo molecule and the pyridyl H atom, or the N atom of the tcm anion and the pyridyl H atom, result in the formation of a three-dimensional network structure.

Comment top

Coordination polymers constructed by tricyanomethanide (tcm) have attracted considerable interest due to their diverse structures and fascinating magnetic properties (Batten & Murray, 2003; Miller & Manson, 2001; Feyerherm et al., 2003). Notably, except a doubly interpenetrated (6,3) sheet was observed in Ag(tcm)2 (Abrahams et al., 2003), most binary tcm complexes display a rutile-like structure (Manson et al., 2000, 1998; Hoshino et al., 1999; Feyerherm et al., 2004). To gain insight into the influence of the coligands on the structures and magnetic properties of tcm complexes, some coligands such as hexamethylenetetramine, 4,4-bipyridyl, 1,2-bi(4-pyridyl)ethane were introduced to the binary tcm systems. Among the CuI or CdII tcm complexes with these coligands, numerous structure types range from doubly interpenetrated (4,4) sheet to three-dimensional rutile networks were observed (Batten et al., 2000, 1998). By contrast, modification of the MnII–tcm binary system with 4,4-bipyridyl as coligands leads to the formation of a one-dimensional chain-like structure (Manson & Schlueter, 2004). On the other hand, 2,2'-dipyridyl N,N'-dioxide (dpdo) is a novel coligand and has two potential oxygen donor atoms. However, no tcm complexes with dpdo as coligand have ever been reported. During our systematic investigation of the nature of dpdo coligand on the structures and properties of tcm complexes, we obtained a new tcm complex with dpdo as coligand, we herein report the synthesis and crystal structure of the new tricyanomethanide complex Mn(dpdo)2(C4N3)2 (I).

The Mn atom which lies on an inversion center displays an octahedral geometry in which the equatorial plane is formed by four O atoms (O1, O2, O1i, O2i) of the dpdo molecules, and the apical sites are occupied by two N atom (N3, N3i) of the tcm ligands (Fig. 1). The Mn—O(dpdo) distances are in the range from 2.1290 (13) Å to 2.1780 (13) Å, these value are comparable to the corresponding distances in manganese–nitroxide complexes (Liu et al., 2001). The Mn—N(tcm) distances are from 2.2336 (17) Å to 2.2337 (17) Å, and the data are similar to the corresponding distances observed in manganese tcm complex (Batten et al., 1999). Each tricyanomethanide moiety is almost planar. Bond distances and bond angles within the anions are in good agreement with those found in other tricyanomethanide complexes (Hoshino et al., 1999; Batten et al., 1999).

Weak intermolecular C—H···O or C—H···N hydrogen bonds involving either the O atom of the dpdo molecule and the pyridyl H atom or the N atom of the tcm anion and the pyridyl H atom, result in the formation of a three-dimensional network structure (Table 1, Fig. 2).

Related literature top

For studies of other coordination polymers constructed with tcm, exhibiting a variety of structures, see: Batten & Murray (2003); Miller & Manson (2001); Feyerherm et al. (2003, 2004); Abrahams et al. (2003); Manson et al. (1998, 2000); Hoshino et al. (1999); Batten et al. (1998, 1999, 2000); Manson & Schlueter (2004). For work on manganese–nitroxide complexes, see: Liu et al. (2001). [Please check rephrasing]

Experimental top

A 5 ml warm ethanol solution of 2,2'-dipyridyl N,N'-dioxide (0.10 mmol, 18.82 mg) and a 2 ml aqueous colorless solution of manganese nitrate (0.10 mmol, 25.10 mg) were mixed and stirred for 5 min, the mixed solution was yellow. To the mixture was added a 3 ml ethanol–water solution (EtOH:H2O = 2:1, v/v) of potassium tricyanomethanide (0.20 mmol, 25.83 mg). After stirred for another 5 min, the yellow solution was filtered and the filtrate was slowly evaporated in air. After two week, yellow block crystals of I were isolated in 34% yield. Anal: Calculated for C28H16MnN10O4: C 55.00%, H 2.64%, N 22.91%. Found C 55.16%, H 2.73%, N 23.03%.

Refinement top

In I the dpdo H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms with C—H distances of 0.93 Å and Uiso = 1.2Ueq(C).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. A view of the mononuclear structure in (I), showing the atom-labeling scheme. Displacement ellipsoids are drawn at the 30% probability level. [Symmetry code: (i) -x + 1, -y + 1, -z + 1.]
[Figure 2] Fig. 2. Partial packing view showing the formation of the C—H···O and C—H···N hydrogen-bond interactions. H atoms not involved in hydrogen bonding have been omitted for clarity. [Symmetry codes: (i) x, -y + 1/2, z + 1/2; (ii) x - 1, y, z.]
Bis(2,2'-bipyridine N,N'-dioxide)bis(tricyanomethanido)manganese(II) top
Crystal data top
[Mn(C4N3)2(C10H8N2O2)2]F(000) = 622
Mr = 611.45Dx = 1.538 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 954 reflections
a = 11.514 (4) Åθ = 3.1–24.8°
b = 16.101 (5) ŵ = 0.56 mm1
c = 7.143 (2) ÅT = 293 K
β = 94.375 (4)°Block, yellow
V = 1320.4 (7) Å30.20 × 0.16 × 0.10 mm
Z = 2
Data collection top
Bruker SMART CCD area-detector
diffractometer
2834 independent reflections
Radiation source: fine-focus sealed tube1969 reflections with I > 2σ(I)
graphiteRint = 0.034
φ and ω scansθmax = 27.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1414
Tmin = 0.893, Tmax = 0.937k = 2020
6266 measured reflectionsl = 58
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)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.071H-atom parameters constrained
S = 0.90 w = 1/[σ2(Fo2) + (0.0269P)2]
where P = (Fo2 + 2Fc2)/3
2834 reflections(Δ/σ)max < 0.001
196 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = 0.34 e Å3
Crystal data top
[Mn(C4N3)2(C10H8N2O2)2]V = 1320.4 (7) Å3
Mr = 611.45Z = 2
Monoclinic, P21/cMo Kα radiation
a = 11.514 (4) ŵ = 0.56 mm1
b = 16.101 (5) ÅT = 293 K
c = 7.143 (2) Å0.20 × 0.16 × 0.10 mm
β = 94.375 (4)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
2834 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1969 reflections with I > 2σ(I)
Tmin = 0.893, Tmax = 0.937Rint = 0.034
6266 measured reflectionsθmax = 27.0°
Refinement top
R[F2 > 2σ(F2)] = 0.034H-atom parameters constrained
wR(F2) = 0.071Δρmax = 0.28 e Å3
S = 0.90Δρmin = 0.34 e Å3
2834 reflectionsAbsolute structure: ?
196 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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 > 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
Mn10.50000.50000.50000.02993 (12)
N10.64563 (12)0.36945 (9)0.7192 (2)0.0332 (4)
N20.41397 (12)0.43113 (9)0.8531 (2)0.0295 (3)
N30.67180 (13)0.55973 (10)0.5796 (2)0.0455 (4)
N41.03850 (17)0.50470 (13)0.7829 (3)0.0790 (7)
N50.96600 (16)0.72092 (13)0.4362 (3)0.0662 (6)
O10.57417 (10)0.37808 (7)0.56602 (18)0.0372 (3)
O20.46743 (10)0.49721 (7)0.78936 (16)0.0324 (3)
C10.76219 (16)0.36510 (12)0.7024 (3)0.0438 (5)
H10.79090.37270.58540.053*
C20.83767 (17)0.34971 (12)0.8549 (4)0.0508 (6)
H20.91720.34640.84120.061*
C30.79652 (17)0.33917 (12)1.0283 (3)0.0476 (5)
H30.84730.32801.13270.057*
C40.67888 (16)0.34541 (11)1.0448 (3)0.0413 (5)
H40.64990.33881.16190.050*
C50.60310 (15)0.36128 (10)0.8902 (3)0.0326 (4)
C60.47602 (15)0.36233 (11)0.9049 (3)0.0306 (4)
C70.42058 (17)0.29644 (12)0.9818 (3)0.0407 (5)
H70.46290.24931.01910.049*
C80.30314 (17)0.29968 (13)1.0040 (3)0.0456 (5)
H80.26590.25551.05800.055*
C90.24191 (16)0.36896 (12)0.9453 (3)0.0416 (5)
H90.16210.37160.95660.050*
C100.29796 (15)0.43425 (12)0.8701 (3)0.0356 (5)
H100.25600.48120.83040.043*
C110.88681 (16)0.59756 (12)0.6110 (3)0.0400 (5)
C120.76883 (17)0.57701 (12)0.5935 (3)0.0375 (5)
C130.96832 (18)0.54529 (14)0.7082 (3)0.0510 (6)
C140.92869 (16)0.66597 (14)0.5135 (3)0.0457 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.0255 (2)0.0319 (2)0.0322 (2)0.00346 (17)0.00101 (17)0.00237 (19)
N10.0290 (8)0.0270 (8)0.0434 (10)0.0017 (7)0.0015 (8)0.0001 (7)
N20.0299 (8)0.0302 (9)0.0283 (8)0.0011 (7)0.0022 (7)0.0002 (7)
N30.0343 (9)0.0523 (11)0.0488 (11)0.0114 (8)0.0041 (8)0.0086 (9)
N40.0531 (12)0.0831 (16)0.0977 (18)0.0124 (12)0.0146 (12)0.0026 (14)
N50.0501 (12)0.0682 (14)0.0823 (16)0.0136 (10)0.0188 (11)0.0018 (12)
O10.0382 (7)0.0355 (7)0.0373 (8)0.0019 (6)0.0017 (6)0.0017 (6)
O20.0357 (7)0.0273 (7)0.0346 (7)0.0034 (6)0.0051 (6)0.0036 (6)
C10.0307 (11)0.0434 (12)0.0586 (14)0.0050 (9)0.0128 (11)0.0003 (11)
C20.0276 (10)0.0438 (13)0.0807 (18)0.0037 (9)0.0020 (12)0.0016 (12)
C30.0373 (12)0.0405 (12)0.0627 (15)0.0046 (9)0.0111 (11)0.0025 (11)
C40.0406 (12)0.0356 (11)0.0469 (13)0.0032 (9)0.0019 (10)0.0042 (10)
C50.0317 (10)0.0250 (10)0.0410 (12)0.0016 (8)0.0020 (9)0.0013 (9)
C60.0296 (9)0.0294 (10)0.0324 (11)0.0008 (8)0.0002 (8)0.0029 (8)
C70.0409 (11)0.0327 (11)0.0481 (13)0.0008 (9)0.0019 (10)0.0098 (10)
C80.0415 (12)0.0456 (13)0.0502 (13)0.0103 (10)0.0081 (11)0.0087 (11)
C90.0291 (10)0.0533 (13)0.0430 (12)0.0048 (10)0.0074 (9)0.0001 (11)
C100.0288 (10)0.0435 (12)0.0346 (11)0.0061 (9)0.0018 (9)0.0014 (9)
C110.0265 (10)0.0460 (12)0.0473 (13)0.0047 (9)0.0019 (9)0.0035 (10)
C120.0376 (11)0.0382 (12)0.0360 (12)0.0024 (9)0.0011 (9)0.0021 (9)
C130.0349 (12)0.0564 (14)0.0612 (16)0.0020 (11)0.0008 (11)0.0109 (12)
C140.0249 (10)0.0566 (15)0.0558 (15)0.0023 (10)0.0056 (10)0.0099 (12)
Geometric parameters (Å, °) top
Mn1—O22.1291 (13)C2—H20.9300
Mn1—O2i2.1291 (13)C3—C41.372 (3)
Mn1—O1i2.1780 (13)C3—H30.9300
Mn1—O12.1780 (13)C4—C51.378 (3)
Mn1—N3i2.2337 (17)C4—H40.9300
Mn1—N32.2337 (17)C5—C61.475 (2)
N1—O11.3252 (19)C6—C71.374 (2)
N1—C51.356 (2)C7—C81.374 (3)
N1—C11.358 (2)C7—H70.9300
N2—O21.3269 (16)C8—C91.368 (3)
N2—C101.351 (2)C8—H80.9300
N2—C61.354 (2)C9—C101.365 (2)
N3—C121.148 (2)C9—H90.9300
N4—C131.140 (3)C10—H100.9300
N5—C141.144 (2)C11—C121.394 (2)
C1—C21.363 (3)C11—C131.404 (3)
C1—H10.9300C11—C141.408 (3)
C2—C31.370 (3)
O2—Mn1—O2i180.0C2—C3—C4118.7 (2)
O2—Mn1—O1i97.70 (4)C2—C3—H3120.6
O2i—Mn1—O1i82.30 (4)C4—C3—H3120.6
O2—Mn1—O182.30 (4)C3—C4—C5120.9 (2)
O2i—Mn1—O197.70 (4)C3—C4—H4119.6
O1i—Mn1—O1180.0C5—C4—H4119.6
O2—Mn1—N3i91.14 (5)N1—C5—C4119.32 (16)
O2i—Mn1—N3i88.86 (5)N1—C5—C6119.42 (17)
O1i—Mn1—N3i90.45 (6)C4—C5—C6121.05 (18)
O1—Mn1—N3i89.55 (6)N2—C6—C7119.30 (16)
O2—Mn1—N388.86 (5)N2—C6—C5119.70 (15)
O2i—Mn1—N391.14 (5)C7—C6—C5120.87 (17)
O1i—Mn1—N389.55 (6)C6—C7—C8120.52 (18)
O1—Mn1—N390.45 (6)C6—C7—H7119.7
N3i—Mn1—N3180.00 (8)C8—C7—H7119.7
O1—N1—C5120.64 (14)C9—C8—C7118.95 (18)
O1—N1—C1119.20 (17)C9—C8—H8120.5
C5—N1—C1120.09 (17)C7—C8—H8120.5
O2—N2—C10119.25 (14)C10—C9—C8120.03 (18)
O2—N2—C6120.05 (14)C10—C9—H9120.0
C10—N2—C6120.68 (15)C8—C9—H9120.0
C12—N3—Mn1164.42 (17)N2—C10—C9120.47 (18)
N1—O1—Mn1118.80 (10)N2—C10—H10119.8
N2—O2—Mn1118.06 (10)C9—C10—H10119.8
N1—C1—C2120.8 (2)C12—C11—C13120.78 (19)
N1—C1—H1119.6C12—C11—C14120.63 (18)
C2—C1—H1119.6C13—C11—C14118.19 (17)
C1—C2—C3120.09 (19)N3—C12—C11179.7 (2)
C1—C2—H2120.0N4—C13—C11176.8 (2)
C3—C2—H2120.0N5—C14—C11178.0 (2)
Symmetry codes: (i) −x+1, −y+1, −z+1.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C7—H7···O1ii0.932.433.350 (2)171
C10—H10···N4iii0.932.533.212 (3)130
Symmetry codes: (ii) x, −y+1/2, z+1/2; (iii) x−1, y, z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C7—H7···O1i0.932.433.350 (2)171
C10—H10···N4ii0.932.533.212 (3)130
Symmetry codes: (i) x, −y+1/2, z+1/2; (ii) x−1, y, z.
Acknowledgements top

This project was supported by the National Natural Science Foundation of China (grant No. 20571086).

references
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