supplementary materials


lh2953 scheme

Acta Cryst. (2009). E65, m1659    [ doi:10.1107/S1600536809049149 ]

Dichlorido(2,9-dimethyl-1,10-phenanthroline)manganese(II) hemihydrate

X. Wang

Abstract top

In the title compound, [MnCl2(C14H12N2)]·0.5H2O, all of the non-H atoms apart from the Cl atom lie on a mirror plane and the methyl H atoms are disordered over two sites of equal occupancy about the mirror plane. The MnII ion is coordinated in a distorted tetrahedral environment by two N atoms of the phenanthroline ligand and two chloride ions. A half-occupancy solvent water molecule lies on a mirror plane and close to an inversion center.

Comment top

1,10-phenanthroline is a good bidentate chelating ligand and here, we present the crystal structure of the title complex based on 2,9-dimethyl-1,10-phenanthroline.

The crystal structure of the title compound is shown in Fig. 1. The coordination environment of the MnII ion is distorted tetrahedral, in which two sites are occupied by the two N atoms of the chelating 2,9-dimethyl-1,10-phenanthroline ligand and the other two from two chloride ions. For Mn—N and Mn—Cl bond lengths in other manganese biphenanthroline complexes, see e.g. McCann, et al. (1998); Pan & Xu (2005); Xu et al. (2009). The location of the water H atoms is such that they are disordered over several sites imposed by the crystal symmetry and hence any potential hydrogen bonding is not discussed.

Related literature top

For related crystal structures, see: McCann et al. (1998); Pan & Xu (2005); Xu et al. (2009).

Experimental top

A mixture of 2,9-dimethyl-1,10-phenanthroline, MnCl2.4H2O (1:2, molar ratio) and water (20 ml) was sealed in a Teflon-lined autoclave (25 ml) and heated 393 K for two days. Upon cooling slowly and opening the bomb, yellow crystals suitable for X-ray diffraction were obtained with a yield about 40% (based on phenanthroline).

Refinement top

All H atoms bonded to C atoms were included using the HFIX commands in SHELXL-97 (Sheldrick, 2008b/i>) with C—H distances of 0.93 and 0.96 Å, and were allowed for as riding atoms with Uiso(H) = 1.2Ueq(C) and 1.5Ueq(Cmethyl). The H atoms of the disordered water molecule were found in a difference Fourier map and were refined as riding with O-H fixed at 0.85 Å and Uiso(H) = 1.2Ueq(O).

Computing details top

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT-Plus (Bruker, 2001); data reduction: SAINT-Plus (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008b); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008b); molecular graphics: SHELXTL (Sheldrick, 2008b); software used to prepare material for publication: SHELXTL (Sheldrick, 2008b).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. The disordered water molecule and all the H-atoms are omitted for clarity.
Dichlorido(2,9-dimethyl-1,10-phenanthroline)manganese(II) hemihydrate top
Crystal data top
[MnCl2(C14H12N2)]·0.5H2OF(000) = 696
Mr = 343.10Dx = 1.411 Mg m3
Monoclinic, C2/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yCell parameters from 1089 reflections
a = 18.763 (4) Åθ = 2.9–26.8°
b = 7.7343 (15) ŵ = 1.14 mm1
c = 11.362 (2) ÅT = 293 K
β = 101.532 (3)°Block, yellow
V = 1615.5 (5) Å30.31 × 0.23 × 0.19 mm
Z = 4
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1511 independent reflections
Radiation source: fine-focus sealed tube1199 reflections with I > 2σ(I)
graphiteRint = 0.020
φ and ω scansθmax = 25.0°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2008a)
h = 2222
Tmin = 0.719, Tmax = 0.813k = 89
4794 measured reflectionsl = 1313
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)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.134 w = 1/[σ2(Fo2) + (0.1015P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.001
1511 reflectionsΔρmax = 0.59 e Å3
120 parametersΔρmin = 0.31 e Å3
0 restraints
Crystal data top
[MnCl2(C14H12N2)]·0.5H2OV = 1615.5 (5) Å3
Mr = 343.10Z = 4
Monoclinic, C2/mMo Kα radiation
a = 18.763 (4) ŵ = 1.14 mm1
b = 7.7343 (15) ÅT = 293 K
c = 11.362 (2) Å0.31 × 0.23 × 0.19 mm
β = 101.532 (3)°
Data collection top
Bruker APEXII CCD area-detector
diffractometer
1511 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2008a)
1199 reflections with I > 2σ(I)
Tmin = 0.719, Tmax = 0.813Rint = 0.020
4794 measured reflectionsθmax = 25.0°
Refinement top
R[F2 > 2σ(F2)] = 0.044?
wR(F2) = 0.134Δρmax = 0.59 e Å3
S = 1.01Δρmin = 0.31 e Å3
1511 reflectionsAbsolute structure: ?
120 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*/UeqOcc. (<1)
Mn10.35177 (3)0.00000.27709 (5)0.0558 (3)
Cl10.40493 (4)0.25282 (10)0.24304 (8)0.0815 (3)
O10.5351 (5)1.00000.0528 (9)0.155 (4)0.50
H2A0.52570.94260.11280.186*0.25
H1A0.57450.95580.03990.186*0.25
N10.30817 (15)0.00000.4374 (3)0.0555 (8)
N20.24030 (17)0.00000.2034 (3)0.0601 (8)
C10.3433 (2)0.00000.5521 (4)0.0625 (10)
C20.3066 (2)0.00000.6486 (4)0.0715 (12)
H20.33290.00000.72720.086*
C30.2337 (2)0.00000.6273 (4)0.0715 (12)
H30.20890.00000.69050.086*
C40.1951 (2)0.00000.5056 (3)0.0604 (10)
C50.1191 (2)0.00000.4745 (4)0.0781 (13)
H50.09190.00000.53460.094*
C60.0848 (2)0.00000.3584 (4)0.0768 (13)
H60.03420.00000.33990.092*
C70.1240 (2)0.00000.2635 (4)0.0655 (11)
C80.0910 (3)0.00000.1374 (4)0.0840 (15)
H80.04060.00000.11360.101*
C90.1330 (3)0.00000.0535 (4)0.0875 (15)
H90.11130.00000.02760.105*
C100.2073 (3)0.00000.0872 (4)0.0703 (11)
C110.1985 (2)0.00000.2896 (3)0.0562 (9)
C120.2350 (2)0.00000.4153 (3)0.0532 (9)
C130.4239 (2)0.00000.5734 (4)0.0819 (14)
H13A0.43970.07240.51500.123*0.50
H13B0.44310.04340.65250.123*0.50
H13C0.44100.11580.56660.123*0.50
C140.2542 (3)0.00000.0069 (4)0.0933 (17)
H14A0.27130.11520.01630.140*0.50
H14B0.22600.03950.08200.140*0.50
H14C0.29500.07560.01810.140*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.0481 (4)0.0703 (5)0.0501 (4)0.0000.0127 (3)0.000
Cl10.0781 (6)0.0818 (7)0.0876 (6)0.0094 (4)0.0235 (4)0.0054 (4)
O10.108 (7)0.226 (12)0.134 (9)0.0000.031 (6)0.000
N10.0413 (15)0.074 (2)0.0503 (17)0.0000.0063 (13)0.000
N20.0572 (17)0.073 (2)0.0483 (17)0.0000.0069 (14)0.000
C10.056 (2)0.076 (3)0.053 (2)0.0000.0032 (17)0.000
C20.061 (2)0.100 (4)0.049 (2)0.0000.0002 (18)0.000
C30.064 (2)0.101 (4)0.050 (2)0.0000.0127 (19)0.000
C40.053 (2)0.077 (3)0.052 (2)0.0000.0100 (17)0.000
C50.055 (2)0.112 (4)0.071 (3)0.0000.020 (2)0.000
C60.045 (2)0.110 (4)0.073 (3)0.0000.006 (2)0.000
C70.047 (2)0.080 (3)0.064 (3)0.0000.0017 (18)0.000
C80.062 (3)0.111 (4)0.070 (3)0.0000.008 (2)0.000
C90.078 (3)0.120 (4)0.056 (3)0.0000.010 (2)0.000
C100.078 (3)0.076 (3)0.054 (2)0.0000.006 (2)0.000
C110.051 (2)0.070 (3)0.0456 (19)0.0000.0040 (16)0.000
C120.053 (2)0.054 (2)0.052 (2)0.0000.0073 (16)0.000
C130.049 (2)0.127 (4)0.064 (3)0.0000.000 (2)0.000
C140.095 (3)0.133 (5)0.052 (2)0.0000.014 (2)0.000
Geometric parameters (Å, °) top
Mn1—N22.092 (3)C5—C61.347 (6)
Mn1—N12.140 (3)C5—H50.9300
Mn1—Cl12.2633 (9)C6—C71.421 (6)
Mn1—Cl1i2.2633 (9)C6—H60.9300
O1—O1ii1.59 (2)C7—C111.371 (5)
O1—H2A0.8610C7—C81.443 (6)
O1—H1A0.8530C8—C91.353 (7)
N1—C11.338 (5)C8—H80.9300
N1—C121.345 (5)C9—C101.370 (7)
N2—C101.342 (5)C9—H90.9300
N2—C111.371 (5)C10—C141.514 (7)
C1—C21.407 (6)C11—C121.454 (5)
C1—C131.482 (6)C13—H13A0.9600
C2—C31.341 (6)C13—H13B0.9600
C2—H20.9300C13—H13C0.9600
C3—C41.428 (6)C14—H14A0.9600
C3—H30.9300C14—H14B0.9600
C4—C121.387 (5)C14—H14C0.9600
C4—C51.399 (6)
N2—Mn1—N179.57 (12)C7—C6—H6119.2
N2—Mn1—Cl1111.79 (4)C11—C7—C6119.7 (4)
N1—Mn1—Cl1113.70 (4)C11—C7—C8115.5 (4)
N2—Mn1—Cl1i111.79 (4)C6—C7—C8124.8 (4)
N1—Mn1—Cl1i113.70 (4)C9—C8—C7120.4 (4)
Cl1—Mn1—Cl1i119.53 (5)C9—C8—H8119.8
O1ii—O1—H2A109.0C7—C8—H8119.8
O1ii—O1—H1A119.0C8—C9—C10120.4 (4)
H2A—O1—H1A104.5C8—C9—H9119.8
C1—N1—C12117.9 (3)C10—C9—H9119.8
C1—N1—Mn1129.1 (3)N2—C10—C9121.2 (4)
C12—N1—Mn1113.0 (2)N2—C10—C14118.4 (4)
C10—N2—C11119.1 (3)C9—C10—C14120.3 (4)
C10—N2—Mn1128.4 (3)C7—C11—N2123.3 (3)
C11—N2—Mn1112.5 (2)C7—C11—C12118.2 (3)
N1—C1—C2122.5 (3)N2—C11—C12118.5 (3)
N1—C1—C13116.6 (4)N1—C12—C4123.0 (3)
C2—C1—C13121.0 (4)N1—C12—C11116.5 (3)
C3—C2—C1120.0 (4)C4—C12—C11120.5 (3)
C3—C2—H2120.0C1—C13—H13A109.5
C1—C2—H2120.0C1—C13—H13B109.5
C2—C3—C4118.5 (4)H13A—C13—H13B109.5
C2—C3—H3120.8C1—C13—H13C109.5
C4—C3—H3120.8H13A—C13—H13C109.5
C12—C4—C5119.2 (4)H13B—C13—H13C109.5
C12—C4—C3118.2 (4)C10—C14—H14A109.5
C5—C4—C3122.6 (4)C10—C14—H14B109.5
C6—C5—C4120.7 (4)H14A—C14—H14B109.5
C6—C5—H5119.7C10—C14—H14C109.5
C4—C5—H5119.7H14A—C14—H14C109.5
C5—C6—C7121.7 (4)H14B—C14—H14C109.5
C5—C6—H6119.2
Symmetry codes: (i) x, −y, z; (ii) −x+1, −y+2, −z.
references
References top

Bruker (2001). SAINT-Plus. Bruker AXS Inc., Madison, Wisconsin, USA.

Bruker (2004). APEX2. Bruker AXS Inc., Madison, Wisconsin, USA.

McCann, S., McCann, M., Casey, M. T., Jackman, M., Devereux, M. & Mckee, V. (1998). Inorg. Chim. Acta, 279, 24–29.

Pan, T.-T. & Xu, D.-J. (2005). Acta Cryst. E61, m740–m742.

Sheldrick, G. M. (2008a). SADABS. University of Göttingen, Germany.

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

Xu, M.-L., Sun, S.-B., Li, X.-Y. & Che, G.-B. (2009). Acta Cryst. E65, m136.