supplementary materials


pv2332 scheme

Acta Cryst. (2010). E66, m1478    [ doi:10.1107/S1600536810042558 ]

Poly[hexa-[mu]-acetato-bis(dimethyl sulfoxide)trimanganese(II)]

C.-Q. Wan, N.-Y. Xiao and Z.-J. Wang

Abstract top

In the title complex, [Mn3(CH3CO2)6(C2H6SO)2]n, the MnII ions exhibit similar MnO6 octahedral coordination geometries but with different coordination environments. One type of MnII ion is surrounded by five acetate groups and a terminal dimethyl sulfoxide group, while the other lies on a twofold axis and is coordinated by six O atoms from three symmetry-related acetate ions. The acetate anions exhibit three independent bridging modes, which flexibly bridge the MnII ions along the c-axis direction, forming an infinite chain structure; the chains are further interconnected through weak C-H...O and C-H...S hydrogen-bonding interactions.

Comment top

The coordination chemistry of dimethyl sulfoxid (DMSO) has been widely studied. Herein, we report the preparation and crystal strcuture of a new manganese(II) complex with dimethyl sulfoxide (DMSO). In the title complex, the two independent MnII ions (Mn1 and Mn2) exhibit a similar O6-octahedral coordination geometry with different coordination environments (Fig. 1). The Mn1 ion is surrounded by five acetates and one η1-bonding DMSO, while the Mn2 lies on a two-fold axis and is coordinated by six oxygen atoms of three symmetry related acetate ions. The acetate anions exhibit three independent bridging modes, syn, syn η1:η12-mode (C2-symmetric O3-containing acetate and O5-, O6-containing acetate), the syn, syn, ant η1:η23-mode (O1-, O2-containing acetate) and the syn, ant, syn, ant η2:η23-mode (C2-symmetric O7-containing acetate). The Mn1 and Mn2 ions are flexibly bridged by these anions and assemble into an infinite chain along the c direction (Fig. 2). The parallel arrays interconnect through C—H···O and C—H···S type H-bonding interactions (Table 1). In the termianl dimethyl sulfoxide, the S1O4 of 1.501 (2)Å bond is slightly longer than that of the neat DMSO, which can be ascribed to the reduced bond order as that found in the protonated and η1-coordinated alkyl sulfoxides (Calligaris et al., 2004). The Mn1—O4 bond length of 2.153 (2)Å is comparable to 2.158 (2)Å found in catena-(tetrakis(µ2-thiocyanato-N,S)-bis(dimethyl sulfoxide-O)- manganese(II)-mercury(II) (Wang et al., 2000), in which the dimethyl sulfoxide shows a similar terminal η1-coordinated bonding to the MnII.

Related literature top

For metal complexes of DMSO, see: Calligaris et al. (2004). For the structure of a related complex, see: Wang et al. (2000). Scheme - Mn atoms should not be lablelled Mn2, Mn2

Experimental top

Mn(CH3CO2)2.4H2O (25 mg, 0.1 mmol) was dissolved in 3 ml deionized water with stirring at room temperature. After half an hour, 1 ml dimethyl sulfoxide was added to the solution. The mixed solution was stirred for another half hour, and then filtered. The clear solution obtained was left to stand in the air to let the solvent to evaporate. The colorless crystals were deposited after one week (12.60 mg, yield 56%).

Refinement top

An absolute structure was determined using the Flack (1983) method. The hydrogen atoms were placed in idealized positions and allowed to ride on the parent carbon atoms, with C—H = 0.96 Å and Uiso(H) = 1.5Ueq(C).

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); 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) and PLATON (Spek, 2009).

Figures top
[Figure 1] Fig. 1. A view of the title complex with the atom-numbering scheme; hydrogen atoms are omitted for clarity. Displacement ellipsoids are drawn at 30% probability level. Symmetry codes: i x, y, z-1; ii -x+2,y,-z; iii -x + 2, y, -z +1.
[Figure 2] Fig. 2. Infinite chain of the MnII ions bridged by acetate anions along the c direction in a unit cell. Symmetry code: i -x + 2, y, -z.
Poly[hexa-µ-acetato-bis(dimethyl sulfoxide)trimanganese(II)] top
Crystal data top
[Mn3(C2H3O2)6(C2H6OS)2]Z = 2
Mr = 675.34F(000) = 690
Monoclinic, C2Dx = 1.622 Mg m3
Hall symbol: C 2yMo Kα radiation, λ = 0.71073 Å
a = 12.8475 (16) Åθ = 2.4–25.1°
b = 12.5439 (16) ŵ = 1.56 mm1
c = 8.6095 (11) ÅT = 293 K
β = 94.906 (2)°Block, colorless
V = 1382.4 (3) Å30.41 × 0.36 × 0.29 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1953 independent reflections
Radiation source: fine-focus sealed tube1919 reflections with I > 2σ(I)
graphiteRint = 0.020
ω scansθmax = 25.1°, θmin = 2.4°
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
h = 1515
Tmin = 0.883, Tmax = 1.000k = 1214
3821 measured reflectionsl = 109
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)] = 0.021H-atom parameters constrained
wR(F2) = 0.056 w = 1/[σ2(Fo2) + (0.033P)2 + 0.3155P] P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
1953 reflectionsΔρmax = 0.39 e Å3
161 parametersΔρmin = 0.16 e Å3
1 restraintAbsolute structure: Flack (1983), 653 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.034 (17)
Crystal data top
[Mn3(C2H3O2)6(C2H6OS)2]V = 1382.4 (3) Å3
Mr = 675.34Z = 2
Monoclinic, C2Mo Kα radiation
a = 12.8475 (16) ŵ = 1.56 mm1
b = 12.5439 (16) ÅT = 293 K
c = 8.6095 (11) Å0.41 × 0.36 × 0.29 mm
β = 94.906 (2)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
1953 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
1919 reflections with I > 2σ(I)
Tmin = 0.883, Tmax = 1.000Rint = 0.020
3821 measured reflectionsθmax = 25.1°
Refinement top
R[F2 > 2σ(F2)] = 0.021H-atom parameters constrained
wR(F2) = 0.056Δρmax = 0.39 e Å3
S = 1.05Δρmin = 0.16 e Å3
1953 reflectionsAbsolute structure: Flack (1983), 653 Friedel pairs
161 parametersFlack parameter: 0.034 (17)
1 restraint
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 > 2sigma(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. An absolute structure was established with the Flack parameter of 0.034 (17).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Mn10.91731 (2)0.56819 (3)0.13931 (4)0.02995 (11)
Mn21.00000.43103 (4)0.50000.03045 (14)
S10.70961 (5)0.67013 (7)0.27681 (10)0.0504 (2)
O10.91650 (12)0.53278 (16)0.88461 (19)0.0352 (4)
O20.87911 (14)0.44946 (19)0.6590 (2)0.0447 (5)
O30.94917 (16)0.73193 (16)0.0982 (2)0.0446 (5)
O40.75455 (15)0.6046 (2)0.1528 (2)0.0526 (6)
O50.87347 (19)0.4057 (2)0.1696 (3)0.0641 (6)
O60.89783 (16)0.3166 (2)0.3901 (2)0.0517 (5)
O71.05675 (14)0.59438 (15)0.60213 (19)0.0379 (4)
C10.85462 (19)0.4827 (2)0.7865 (3)0.0318 (5)
C20.7442 (2)0.4630 (3)0.8279 (4)0.0454 (7)
H2A0.73550.49280.92870.068*
H2B0.73120.38770.82990.068*
H2C0.69580.49610.75150.068*
C31.00000.7770 (3)0.00000.0376 (8)
C41.00000.8965 (4)0.00000.0634 (14)
H4A1.04250.92200.07860.095*0.50
H4B1.02770.92200.10030.095*0.50
H4C0.92980.92200.02170.095*0.50
C50.7587 (3)0.2664 (4)0.2103 (5)0.0792 (13)
H5A0.72910.28980.10990.119*
H5B0.70690.27120.28410.119*
H5C0.78140.19370.20330.119*
C60.8501 (2)0.3355 (2)0.2627 (3)0.0386 (6)
C70.6698 (3)0.5766 (5)0.4144 (5)0.0873 (14)
H7A0.73030.54830.47360.131*
H7B0.63200.51970.36070.131*
H7C0.62570.61130.48340.131*
C80.5846 (3)0.7060 (4)0.1907 (5)0.0799 (13)
H8A0.59180.75980.11300.120*
H8B0.54320.73330.26940.120*
H8C0.55110.64440.14290.120*
C91.00000.7628 (4)0.50000.0727 (16)
H9A0.95310.78830.41540.109*0.50
H9B1.06930.78830.48780.109*0.50
H9C0.97760.78830.59690.109*0.50
C101.00000.6450 (4)0.50000.0383 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.02796 (17)0.0394 (2)0.02291 (18)0.00325 (16)0.00453 (12)0.00263 (16)
Mn20.0318 (3)0.0360 (3)0.0238 (3)0.0000.00371 (19)0.000
S10.0378 (4)0.0585 (5)0.0547 (5)0.0060 (3)0.0025 (3)0.0202 (4)
O10.0278 (8)0.0502 (11)0.0278 (9)0.0062 (8)0.0037 (7)0.0038 (8)
O20.0401 (9)0.0648 (14)0.0305 (9)0.0086 (9)0.0107 (8)0.0127 (9)
O30.0549 (11)0.0398 (11)0.0407 (11)0.0029 (9)0.0141 (9)0.0029 (8)
O40.0341 (10)0.0810 (17)0.0428 (11)0.0108 (9)0.0043 (8)0.0150 (11)
O50.0691 (15)0.0525 (15)0.0704 (16)0.0129 (12)0.0037 (12)0.0102 (12)
O60.0554 (11)0.0611 (14)0.0382 (11)0.0123 (10)0.0010 (9)0.0110 (10)
O70.0454 (9)0.0452 (12)0.0229 (8)0.0039 (8)0.0019 (7)0.0009 (8)
C10.0285 (12)0.0419 (14)0.0248 (12)0.0027 (10)0.0020 (10)0.0013 (11)
C20.0345 (13)0.065 (2)0.0369 (15)0.0113 (13)0.0062 (11)0.0079 (13)
C30.0337 (17)0.039 (2)0.040 (2)0.0000.0017 (15)0.000
C40.061 (3)0.041 (2)0.092 (4)0.0000.031 (3)0.000
C50.078 (2)0.087 (3)0.068 (2)0.039 (2)0.020 (2)0.009 (2)
C60.0384 (13)0.0347 (14)0.0433 (15)0.0019 (11)0.0079 (11)0.0041 (12)
C70.076 (2)0.134 (4)0.054 (2)0.005 (3)0.0194 (18)0.000 (3)
C80.0454 (17)0.081 (3)0.110 (3)0.0282 (19)0.0133 (19)0.029 (3)
C90.120 (5)0.046 (3)0.051 (3)0.0000.000 (3)0.000
C100.047 (2)0.043 (2)0.0272 (19)0.0000.0116 (17)0.000
Geometric parameters (Å, °) top
Mn1—O32.130 (2)C1—C21.513 (4)
Mn1—O52.136 (2)C2—H2A0.9600
Mn1—O42.1533 (19)C2—H2B0.9600
Mn1—O1i2.2076 (15)C2—H2C0.9600
Mn1—O1ii2.2365 (17)C3—O3iv1.247 (3)
Mn1—O7i2.2467 (17)C3—C41.498 (6)
Mn2—O62.113 (2)C4—H4A0.9600
Mn2—O6i2.113 (2)C4—H4B0.9600
Mn2—O22.1690 (18)C4—H4C0.9600
Mn2—O2i2.1690 (18)C5—C61.499 (5)
Mn2—O72.3224 (19)C5—H5A0.9600
Mn2—O7i2.3224 (19)C5—H5B0.9600
S1—O41.501 (2)C5—H5C0.9600
S1—C81.768 (3)C7—H7A0.9600
S1—C71.773 (5)C7—H7B0.9600
O1—C11.275 (3)C7—H7C0.9600
O1—Mn1i2.2076 (15)C8—H8A0.9600
O1—Mn1iii2.2365 (17)C8—H8B0.9600
O2—C11.239 (3)C8—H8C0.9600
O3—C31.247 (3)C9—C101.477 (7)
O5—C61.245 (4)C9—H9A0.9600
O6—C61.233 (4)C9—H9B0.9600
O7—C101.264 (3)C9—H9C0.9600
O7—Mn1i2.2467 (17)C10—O7i1.264 (3)
O3—Mn1—O5175.34 (9)O1—C1—C2117.9 (2)
O3—Mn1—O490.32 (9)C1—C2—H2A109.5
O5—Mn1—O485.91 (10)C1—C2—H2B109.5
O3—Mn1—O1i88.70 (8)H2A—C2—H2B109.5
O5—Mn1—O1i94.97 (9)C1—C2—H2C109.5
O4—Mn1—O1i177.66 (7)H2A—C2—H2C109.5
O3—Mn1—O1ii90.78 (7)H2B—C2—H2C109.5
O5—Mn1—O1ii87.19 (9)O3iv—C3—O3126.1 (4)
O4—Mn1—O1ii99.89 (7)O3iv—C3—C4116.97 (19)
O1i—Mn1—O1ii78.00 (7)O3—C3—C4116.97 (19)
O3—Mn1—O7i90.53 (7)C3—C4—H4A109.5
O5—Mn1—O7i92.12 (9)C3—C4—H4B109.5
O4—Mn1—O7i88.74 (7)H4A—C4—H4B109.5
O1i—Mn1—O7i93.39 (6)C3—C4—H4C109.5
O1ii—Mn1—O7i171.26 (6)H4A—C4—H4C109.5
O6—Mn2—O6i94.44 (13)H4B—C4—H4C109.5
O6—Mn2—O284.50 (8)C6—C5—H5A109.5
O6i—Mn2—O2103.92 (8)C6—C5—H5B109.5
O6—Mn2—O2i103.92 (8)H5A—C5—H5B109.5
O6i—Mn2—O2i84.50 (8)C6—C5—H5C109.5
O2—Mn2—O2i167.76 (13)H5A—C5—H5C109.5
O6—Mn2—O7158.69 (8)H5B—C5—H5C109.5
O6i—Mn2—O7105.48 (8)O6—C6—O5125.5 (3)
O2—Mn2—O783.42 (7)O6—C6—C5118.3 (3)
O2i—Mn2—O785.78 (8)O5—C6—C5116.2 (3)
O6—Mn2—O7i105.48 (8)S1—C7—H7A109.5
O6i—Mn2—O7i158.69 (8)S1—C7—H7B109.5
O2—Mn2—O7i85.78 (8)H7A—C7—H7B109.5
O2i—Mn2—O7i83.42 (7)S1—C7—H7C109.5
O7—Mn2—O7i56.16 (9)H7A—C7—H7C109.5
O4—S1—C8103.40 (16)H7B—C7—H7C109.5
O4—S1—C7105.3 (2)S1—C8—H8A109.5
C8—S1—C798.3 (2)S1—C8—H8B109.5
C1—O1—Mn1i126.19 (15)H8A—C8—H8B109.5
C1—O1—Mn1iii134.27 (15)S1—C8—H8C109.5
Mn1i—O1—Mn1iii97.36 (6)H8A—C8—H8C109.5
C1—O2—Mn2147.63 (17)H8B—C8—H8C109.5
C3—O3—Mn1132.0 (2)C10—C9—H9A109.5
S1—O4—Mn1126.07 (12)C10—C9—H9B109.5
C6—O5—Mn1146.5 (2)H9A—C9—H9B109.5
C6—O6—Mn2120.7 (2)C10—C9—H9C109.5
C10—O7—Mn1i142.22 (15)H9A—C9—H9C109.5
C10—O7—Mn292.1 (2)H9B—C9—H9C109.5
Mn1i—O7—Mn2105.15 (7)O7i—C10—O7119.7 (4)
O2—C1—O1124.1 (2)O7i—C10—C9120.16 (19)
O2—C1—C2117.9 (2)O7—C10—C9120.16 (19)
O6—Mn2—O2—C1163.4 (4)O6—Mn2—O7—C1033.4 (2)
O6i—Mn2—O2—C170.2 (4)O6i—Mn2—O7—C10168.01 (9)
O2i—Mn2—O2—C162.4 (4)O2—Mn2—O7—C1089.32 (10)
O7—Mn2—O2—C134.2 (4)O2i—Mn2—O7—C1084.91 (9)
O7i—Mn2—O2—C190.5 (4)O7i—Mn2—O7—C100.0
O5—Mn1—O3—C396.9 (11)O6—Mn2—O7—Mn1i112.59 (19)
O4—Mn1—O3—C3132.66 (18)O6i—Mn2—O7—Mn1i45.97 (9)
O1i—Mn1—O3—C345.22 (18)O2—Mn2—O7—Mn1i56.70 (8)
O1ii—Mn1—O3—C332.76 (18)O2i—Mn2—O7—Mn1i129.08 (8)
O7i—Mn1—O3—C3138.60 (19)O7i—Mn2—O7—Mn1i146.02 (13)
C8—S1—O4—Mn1161.6 (2)Mn2—O2—C1—O12.3 (6)
C7—S1—O4—Mn195.7 (2)Mn2—O2—C1—C2177.9 (3)
O3—Mn1—O4—S166.55 (18)Mn1i—O1—C1—O22.6 (4)
O5—Mn1—O4—S1116.18 (19)Mn1iii—O1—C1—O2161.7 (2)
O1i—Mn1—O4—S1132 (2)Mn1i—O1—C1—C2177.7 (2)
O1ii—Mn1—O4—S1157.39 (17)Mn1iii—O1—C1—C218.5 (4)
O7i—Mn1—O4—S123.97 (18)Mn1—O3—C3—O3iv3.74 (11)
O3—Mn1—O5—C6114.0 (11)Mn1—O3—C3—C4176.26 (11)
O4—Mn1—O5—C678.1 (4)Mn2—O6—C6—O518.9 (4)
O1i—Mn1—O5—C6104.1 (4)Mn2—O6—C6—C5163.8 (3)
O1ii—Mn1—O5—C6178.2 (4)Mn1—O5—C6—O646.7 (6)
O7i—Mn1—O5—C610.5 (4)Mn1—O5—C6—C5135.9 (4)
O6i—Mn2—O6—C6148.6 (2)Mn1i—O7—C10—O7i118.3 (3)
O2—Mn2—O6—C6107.8 (2)Mn2—O7—C10—O7i0.0
O2i—Mn2—O6—C663.2 (2)Mn1i—O7—C10—C961.7 (3)
O7—Mn2—O6—C652.1 (3)Mn2—O7—C10—C9180.0
O7i—Mn2—O6—C623.7 (2)
Symmetry codes: (i) −x+2, y, −z+1; (ii) x, y, z−1; (iii) x, y, z+1; (iv) −x+2, y, −z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C8—H8B···O6v0.962.453.367 (4)160
C2—H2B···S1vi0.962.993.841 (4)147
Symmetry codes: (v) x−1/2, y+1/2, z; (vi) −x+3/2, y−1/2, −z+1.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C8—H8B···O6i0.962.453.367 (4)160
C2—H2B···S1ii0.962.993.841 (4)147
Symmetry codes: (i) x−1/2, y+1/2, z; (ii) −x+3/2, y−1/2, −z+1.
Acknowledgements top

The authors are grateful for financial support from the Project for Academic Human Resources Development in Institutions of Higher Learning Under the Jurisdiction of Beijing Municipality (PHR20100718).

references
References top

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