metal-organic compounds
Table 1
Selected bond lengths (A).
monoclinic (space group P21/c). Its structure has been deter-
mined at room temperature (Huang et al., 1987), at 173 K
(Bolte et al., 2002) and at 150 K (Parsons et al., 2004).
Ê
Mg1ÐO31
Mg1ÐO41
Mg1ÐO21
Mg1ÐO11
Mg1ÐBr1
Mg1ÐBr2
2.099 (8)
Mg2ÐO51
Mg2ÐO71
Mg2ÐO81
Mg2ÐO61
Mg2ÐBr4
Mg2ÐBr3
2.087 (9)
2.096 (8)
2.128 (8)
2.138 (8)
2.562 (4)
2.605 (4)
2.105 (9)
2.105 (8)
2.106 (8)
2.569 (3)
2.592 (3)
Table 2
Coordinates of the Mg atoms in the unit cell of (I).
Atom
x
y
z
Mg1
Mg2
Mg1i
Mg2i
0.5332 (4)
0.5228 (4)
0.4668 (4)
0.4772 (4)
0.2517 (2)
0.2559 (2)
0.7483 (2)
0.7441 (2)
0.2364 (2)
0.7201 (2)
0.7636 (2)
0.2799 (2)
Symmetry code: (i) 1 x; 1 y; 1 z.
The frames collected during data collection did not show split
re¯ections and there was no warning sign that the structure deter-
mination would be problematic. The cell parameters of (I) indicate a
Ê
Ê
Ê
monoclinic C-centred cell (a = 23.945 A, b = 20.271 A, c = 8.662 A, ꢀ =
3
ꢀ
ꢀ
ꢀ
Ê
90.05 , ꢁ = 96.35 , ꢂ = 89.97 and V = 4178.64 A ) and the Rint value
for the monoclinic crystal system is 0.096 (compared with 0.080 for
the triclinic crystal system). However, there are no systematic
extinctions and the structure cannot be solved in any of the mono-
clinic space groups. Thus, the structure was solved in the triclinic
space group P1 by locating the heaviest atoms in a Patterson map and
using successive Fourier syntheses to ®nd the remaining atoms. After
encountering severe problems during structure solution, anisotropic
re®nement remained stalled at R1 = 0.278 and wR2 = 0.685, with
several atoms going nonpositive de®nite. It was therefore assumed
that the crystal was twinned. The warning signs for twinning are,
®rstly, that E2 1 is just 0.768, which is a little bit too small for a
centrosymmetric structure and, secondly, that Rint for the higher-
symmetry Laue group is only slightly higher than for the lower-
symmetry Laue group. Nevertheless, the twin law is not a symmetry
operation of the higher-symmetry Laue group, but a twofold rotation
axis along the face diagonal of the bc plane interchanging b and c,
which are almost equal in length, i.e. (100/001/010). Applying this
twin law ultimately provided success and R1 dropped below 0.1. All H
atoms could now be located by difference Fourier synthesis. They
were re®ned using a riding model with ®xed individual displacement
Figure 3
Packing diagram of the tetragonal polymorph of dibromidotetrakis(tetra-
hydrofuran)magnesium, (Ia), viewed in the ab plane. C and H atoms have
been omitted for clarity. Key: Mg atoms are shaded, Br atoms are dotted
and O atoms are cross-hatched.
Experimental
A solution of Me3SnCl (26.08 g, 130.9 mmol) and 1,2-dibromo-
benzene (7.8 ml, 64 mmol) in tetrahydrofuran (THF) (100 ml) was
added dropwise to a mixture of magnesium (7.45 g 306 mmol) and
CH3MgCl (0.6 mmol) in THF (100 ml). The reaction mixture was
heated under re¯ux for 90 min. After cooling to ambient tempera-
ture, colourless crystals of Mg(THF)4Br2 suitable for X-ray crystal-
lographic analysis were obtained (yield 23%).
Crystal data
[MgBr2(C4H8O)4]
Mr = 472.55
Triclinic, P1
a = 8.6620 (9) A
b = 15.6820 (12) A
Ê
c = 15.6910 (13) A
ꢀ = 80.501 (9)ꢀ
ꢁ = 85.131 (11)ꢀ
ꢂ = 85.190 (11)ꢀ
3
Ê
V = 2089.3 (3) A
Z = 4
Ê
Mo Kꢀ radiation
Ê
parameters [Uiso(H) = 1.2Ueq(C)] and with CÐH = 0.99 A. Finally,
1
Ê
ꢃ = 3.93 mm
T = 173 (2) K
the ratio of the twin components re®ned to 0.534 (3):0.466 (3).
Data collection: X-AREA (Stoe & Cie, 2001); cell re®nement:
X-AREA; data reduction: X-AREA; program(s) used to solve
structure: SHELXS97 (Sheldrick, 1997); program(s) used to re®ne
structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in
SHELXTL-Plus (Sheldrick, 1991); software used to prepare material
for publication: SHELXL97.
0.27 Â 0.26 Â 0.24 mm
Data collection
Stoe IPDSII two-circle
diffractometer
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing,
1995)
22055 measured re¯ections
7347 independent re¯ections
4969 re¯ections with I > 2ꢄ(I)
Rint = 0.080
Tmin = 0.342, Tmax = 0.420
(expected range = 0.318±0.390)
Supplementary data for this paper are available from the IUCr electronic
archives (Reference: SK3104). Services for accessing these data are
described at the back of the journal.
Re®nement
R[F2 > 2ꢄ(F2)] = 0.087
wR(F2) = 0.232
S = 1.44
416 parameters
H-atom parameters constrained
References
3
Ê
Áꢅmax = 0.97 e A
3
Ê
1.11 e A
7347 re¯ections
Áꢅmin
=
Allen, F. H. (2002). Acta Cryst. B58, 380±388.
ꢁ
Acta Cryst. (2007). C63, m174±m176
Lorbach et al. [MgBr2(C4H8O)4] m175