supplementary materials


Acta Cryst. (2007). E63, m1433    [ doi:10.1107/S160053680701882X ]

Bis(dimethylammonium) tetrabromidomanganate(II)

T. Morawitz, B. Kern, H.-W. Lerner and M. Bolte

Abstract top

The title compound, (C2H10N)2[MnBr4], consists of discrete dimethylammonium cations and tetrabromidomanganate(II) anions which are held together in the crystal structure by N-H...Br hydrogen bonds.

Comment top

Recently we have found that the manganese complex [Mn(CO)5Br] can easily transformed into Mn(II) and [Mn(CO)5]2 in the presence of strong nucleophiles such as NaSSitBu3 or Na2PSitBu3 (Kückmann, 2007; Lerner et al., 2005). In attempting to synthesize the 1,4-phenylene-brigded Mn(I) scorpionate (I) from the corresponding lithium scorpionate and [Mn(CO)5Br] in the presence of [NMe2H2][Br], we obtained [NMe2H2]2[MnBr4] as a side-product. X-ray quality crystals of [NMe2H2]2[MnBr4] were grown by diffusion of hexane into a solution of [NMe2H2]2[MnBr4] in tetrahydrofuran at ambient temperature.

The title compound, 2(C2H10N)+·MnBr42−, consists of discrete dimethylammonium cations und tetrabromo-manganese anions which are held together in the crystal by N—H···Br hydrogen bonds. The title compound is isostructural with 2(C2H10N)+.HgBr42− (Pabst et al., 1990) 2(C2H10N)+.CdBr42− (Daoud, 1976; Waskowska, 1994), 2(C2H10N)+.HgCl42− (Salah et al., 1982) and 2(C2H10N)+.CoCl42− (Williams et al., 1992).

Related literature top

For related literature, see: Daoud (1976); Kückmann (2007); Lerner et al. (2005); Pabst et al. (1990); Waskowska (1994); Williams et al. (1992); Salah et al. (1982).

Experimental top

By the reaction of the 1,4-phenylene-brigded Li scorpionate (I) (0.59 g, 1.10 mmol) with [Mn(CO)5Br] (0.64 g, 2.31 mmol) and [NMe2H2][Br] (ca 0.2 mmol) in 30 ml THF [NMe2H2]2[MnBr4] was obtained as a side-product. X-ray quality crystals of [NMe2H2]2[MnBr4] were grown by diffusion of hexane into a solution of [NMe2H2]2[MnBr4] in tetrahydrofuran at ambient temperature.

Refinement top

H atoms were refined with fixed individual displacement parameters [Uiso(H) = 1.2 Ueq(C, N)] using a riding model with N—H = 0.92Å or C—H = 0.98 Å.

Computing details top

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 1991); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. Perspective view of the title compound, with the atom numbering scheme; displacement ellipsoids are at the 50% probability level; H atoms are drawn as small spheres of arbitrary radii.
Bis(dimethylammonium) tetrabromidoomanganese(II) top
Crystal data top
(C2H8N)2[MnBr4]F(000) = 876
Mr = 466.77Dx = 2.137 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 10816 reflections
a = 8.1854 (7) Åθ = 3.5–25.4°
b = 11.7492 (9) ŵ = 11.89 mm1
c = 15.1444 (11) ÅT = 173 K
β = 95.087 (6)°Block, yellow
V = 1450.7 (2) Å30.22 × 0.21 × 0.18 mm
Z = 4
Data collection top
Stoe IPDSII two-circle
diffractometer
2693 independent reflections
Radiation source: fine-focus sealed tube2105 reflections with I > 2σ(I)
graphiteRint = 0.079
ω scansθmax = 25.6°, θmin = 3.4°
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing, 1995)
h = 99
Tmin = 0.090, Tmax = 0.114k = 1414
12230 measured reflectionsl = 1816
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)] = 0.050H-atom parameters constrained
wR(F2) = 0.113 w = 1/[σ2(Fo2) + (0.0617P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
2693 reflectionsΔρmax = 1.57 e Å3
101 parametersΔρmin = 0.85 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0058 (5)
Crystal data top
(C2H8N)2[MnBr4]V = 1450.7 (2) Å3
Mr = 466.77Z = 4
Monoclinic, P21/nMo Kα radiation
a = 8.1854 (7) ŵ = 11.89 mm1
b = 11.7492 (9) ÅT = 173 K
c = 15.1444 (11) Å0.22 × 0.21 × 0.18 mm
β = 95.087 (6)°
Data collection top
Stoe IPDSII two-circle
diffractometer
2693 independent reflections
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing, 1995)
2105 reflections with I > 2σ(I)
Tmin = 0.090, Tmax = 0.114Rint = 0.079
12230 measured reflectionsθmax = 25.6°
Refinement top
R[F2 > 2σ(F2)] = 0.050H-atom parameters constrained
wR(F2) = 0.113Δρmax = 1.57 e Å3
S = 1.06Δρmin = 0.85 e Å3
2693 reflectionsAbsolute structure: ?
101 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
Mn10.28760 (13)0.70597 (8)0.54751 (8)0.0256 (3)
Br10.53567 (9)0.78194 (6)0.63851 (6)0.0345 (2)
Br20.28514 (9)0.49320 (6)0.55910 (6)0.0334 (2)
Br30.03107 (10)0.79225 (7)0.59464 (6)0.0391 (2)
Br40.32489 (10)0.76510 (6)0.38986 (5)0.0325 (2)
N10.6983 (9)0.5194 (5)0.6703 (5)0.0348 (15)
H1A0.66400.47050.62500.042*
H1B0.66350.59130.65360.042*
C10.6192 (11)0.4864 (7)0.7498 (6)0.0393 (19)
H1C0.49980.48860.73690.059*
H1D0.65180.53950.79810.059*
H1E0.65330.40910.76750.059*
C20.8784 (10)0.5188 (8)0.6814 (7)0.046 (2)
H2C0.92150.54130.62570.068*
H2D0.91730.44210.69780.068*
H2E0.91680.57250.72830.068*
N20.2655 (9)0.1858 (5)0.5713 (5)0.0383 (16)
H2A0.36600.22050.56980.046*
H2B0.19670.21530.52570.046*
C30.2002 (14)0.2138 (8)0.6547 (8)0.055 (3)
H3A0.19020.29660.65990.082*
H3B0.27440.18490.70400.082*
H3C0.09190.17870.65660.082*
C40.2855 (13)0.0612 (8)0.5559 (9)0.061 (3)
H4A0.32930.04930.49840.092*
H4B0.17870.02350.55600.092*
H4C0.36150.02920.60300.092*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.0270 (6)0.0230 (5)0.0264 (6)0.0006 (4)0.0006 (4)0.0000 (4)
Br10.0352 (4)0.0282 (4)0.0379 (5)0.0011 (3)0.0093 (3)0.0036 (3)
Br20.0396 (4)0.0233 (3)0.0368 (4)0.0012 (3)0.0013 (3)0.0034 (3)
Br30.0315 (4)0.0391 (4)0.0475 (5)0.0064 (3)0.0072 (3)0.0062 (4)
Br40.0392 (4)0.0292 (4)0.0283 (4)0.0015 (3)0.0014 (3)0.0054 (3)
N10.051 (4)0.026 (3)0.028 (4)0.006 (3)0.001 (3)0.005 (3)
C10.047 (5)0.037 (4)0.034 (5)0.004 (3)0.001 (4)0.004 (3)
C20.035 (4)0.052 (5)0.050 (6)0.006 (4)0.008 (4)0.004 (4)
N20.038 (4)0.030 (3)0.045 (5)0.006 (3)0.001 (3)0.006 (3)
C30.062 (6)0.049 (5)0.056 (7)0.004 (4)0.017 (5)0.010 (5)
C40.062 (6)0.033 (4)0.089 (9)0.004 (4)0.010 (6)0.011 (5)
Geometric parameters (Å, °) top
Mn1—Br32.4924 (13)C2—H2D0.9800
Mn1—Br22.5062 (12)C2—H2E0.9800
Mn1—Br12.5145 (13)N2—C31.453 (13)
Mn1—Br42.5309 (14)N2—C41.493 (11)
N1—C21.469 (11)N2—H2A0.9200
N1—C11.469 (11)N2—H2B0.9200
N1—H1A0.9200C3—H3A0.9800
N1—H1B0.9200C3—H3B0.9800
C1—H1C0.9800C3—H3C0.9800
C1—H1D0.9800C4—H4A0.9800
C1—H1E0.9800C4—H4B0.9800
C2—H2C0.9800C4—H4C0.9800
Br3—Mn1—Br2111.93 (5)N1—C2—H2E109.5
Br3—Mn1—Br1111.01 (5)H2C—C2—H2E109.5
Br2—Mn1—Br1109.08 (5)H2D—C2—H2E109.5
Br3—Mn1—Br4109.49 (5)C3—N2—C4114.3 (8)
Br2—Mn1—Br4110.02 (5)C3—N2—H2A108.7
Br1—Mn1—Br4105.10 (5)C4—N2—H2A108.7
C2—N1—C1114.5 (7)C3—N2—H2B108.7
C2—N1—H1A108.6C4—N2—H2B108.7
C1—N1—H1A108.6H2A—N2—H2B107.6
C2—N1—H1B108.6N2—C3—H3A109.5
C1—N1—H1B108.6N2—C3—H3B109.5
H1A—N1—H1B107.6H3A—C3—H3B109.5
N1—C1—H1C109.5N2—C3—H3C109.5
N1—C1—H1D109.5H3A—C3—H3C109.5
H1C—C1—H1D109.5H3B—C3—H3C109.5
N1—C1—H1E109.5N2—C4—H4A109.5
H1C—C1—H1E109.5N2—C4—H4B109.5
H1D—C1—H1E109.5H4A—C4—H4B109.5
N1—C2—H2C109.5N2—C4—H4C109.5
N1—C2—H2D109.5H4A—C4—H4C109.5
H2C—C2—H2D109.5H4B—C4—H4C109.5
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···Br10.922.473.377 (6)167
N1—H1A···Br2i0.922.893.492 (7)125
N1—H1A···Br4i0.922.783.466 (6)132
N2—H2A···Br4i0.922.563.401 (7)153
N2—H2B···Br3ii0.922.493.346 (7)155
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x, −y+1, −z+1.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1B···Br10.922.473.377 (6)167
N1—H1A···Br2i0.922.893.492 (7)125
N1—H1A···Br4i0.922.783.466 (6)132
N2—H2A···Br4i0.922.563.401 (7)153
N2—H2B···Br3ii0.922.493.346 (7)155
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x, −y+1, −z+1.
references
References top

Blessing, R. H. (1995). Acta Cryst. A51, 33–38.

Daoud, A. (1976). Bull. Soc. Chim. Fr. pp. 1418–1418.

Kückmann, T. (2007). PhD Thesis, Universität Frankfurt.

Lerner, H.-W., Margraf, G., Bats, J. W. & Wagner, M. (2005). Chem. Commun. pp. 4545–4547.

Pabst, I., Bats, J. W. & Fuess, H. (1990). Acta Cryst. B46, 503–508.

Salah, A. B., Bats, J. W., Fuess, H. & Daoud, A. (1982). Inorg. Chim. Acta, 63, 169–175.

Sheldrick, G. M. (1991). SHELXTL-Plus. Release 4.1. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.

Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen Germany.

Spek, A. L. (2003). J. Appl. Cryst. 36, 7–13.

Stoe & Cie (2001). X-AREA. Stoe & Cie, Darmstadt, Germany.

Waskowska, A. (1994). Z. Kristallogr. 209, 752–754.

Williams, I. D., Brown, P. W. & Taylor, N. J. (1992). Acta Cryst. C48, 263–266.