Fig. 4 The X-ray structure of the metallamacrocycle [12Cu2(CF3SO3)2]2+
obtained between 1 and Cu(CF3SO3)2. Then triflate anions are disordered.
H atoms, anions and solvent molecules are omitted for clarity.
Fig. 2 The X-ray structure of the metalloamacrocycle [12Cu2Cl2]2+ obtained
between 1 and CuCl2. H atoms, anions and solvent molecules are omitted
for clarity.
coordination networks with tubular topology.5,7,8 In relation to
this, it may be of interest that, since the two anions occupying
the summit of the square pyramid on each Cu centre are oriented
in a divergent fashion, by interconnecting the metalloacyclo-
phanes new types of coordination polymers may be obtained
using bridging bidentate anionic ligands such as azido or
isocyanato anions.
In conclusion, the synthesis of paramagnetic binuclear copper
metallacyclophanes has been achieved and their solid state
structural elucidation revealed that the Cu(II) cation adopts a
slightly distorted square pyramidal geometry with the axial
position occupied either by chloride or triflate anion. The
formation of extended metallacyclophanes using ligand 2 is
being currently pursued. Furthermore, the interconnection of
the obtained metallamacrocyles leading to paramagnetic coor-
dination networks through the substitution of monodentate
coordinated anions by bidentate anions is currently under
investigation.
anions. Owing to the parallel orientation of the two phenyl
rings, the binuclear metallamacrocycle is of the cyclophane type
with an internal cavity of 4.29 3 7.42 Å (Scheme 1). The
coordination sphere around the pentacoordinated Cu(II) cations
is composed of four nitrogen atoms belonging to two ligands 1
and one chloride anion with a slightly distorted square
pyramidal geometry. The two poles of the ligand 1, composed
each of two pyrazolyl moieties (dNN = 1.37 Å, dC(Ph)N = 1.42
Å; NNCC dihedral angle of 57.8°) and occupying the square
base in the coordination sphere around the metal, act as
bidentate units and form two seven membered metallarings of
type 4A (Scheme 1) with Cu–N distances of ca. 2.01 Å and
NCuN angles of 86.9–91.4° (Scheme 1). The axial position is
occupied by a Cl anion with Cu–Cl distance of 2.44 Å. The two
positive charges on the [12Cu2Cl2]2+ complex are neutralised by
a [CuCl4]22 anion with dCuCl = 2.283 Å and ClCuCl angle of
90° (Fig. 3).
The [12Cu2(CF3SO3)2(CF3SO3)2] complex was obtained as a
blue-violet crystalline solid upon reaction of
1 and
Notes and references
Cu(CF3SO3)2 in CHCl3–MeOH. The latter complex was also
structurally characterised by X-ray diffraction (Fig. 4).† The
solid contains the complex unit [12Cu2(CF3SO3)2(CF3SO3)2]
and two CH2Cl2 solvent molecules with no specific interactions
with the complex. The triflate anions are disordered. The
cationic part of the complex of type 4A (Scheme 1) shows
almost identical structural features as the above chloride
complex (Scheme 1). Again a metallamacrocycle (internal
cavity of 4.16 Å 3 7.29 Å) composed of two ligands 1, two
Cu(II) cations and two triflate anions is observed. The
coordination sphere around the pentacoordinated Cu(II) cations
is, as in the chloride case, comprised of four nitrogen atoms
belonging to two ligands 1 and one triflate anion (dNN = 1.38
Å dC(Ph)N = 1.42 Å; NNCC dihedral angles of 259.6 and 58.9°,
Cu–N distances of ca. 1.99 Å and NCuN angles of 87.4–92.6°.
Interestingly, the axial position is occupied by a triflate anion
with Cu–O distance of 2.20 Å. The two positive charges on the
[12Cu2(CF3SO3)2]2+ complex are neutralised by two external
triflate anions (Fig. 4).
† Crystal data: (colourless, 294 K), C18H14N8, M = 342.37, triclinic, a =
6.384(1), b = 7.007(1), c = 9.941(1) Å, a = b = 76.00, g = 80.00, U =
416.5(2) Å3, Z = 1, space group P1, Dc = 1.36 g cm23, m = 0.089 mm21
,
¯
1508 data with I > 3s(I), R = 0.040, Rw = 0.0649. [(12Cu2Cl2(CuCl4))],
(green, 294 K), 2(CuClC18H14N8)·CuCl4·2CHCl3·2MeOH, M = 1390.91,
orthorhombic, a = 10.0302(5), b = 11.3568(6), c = 23.5388(7) Å, U =
2681.3(4) Å3, Z = 2, Immm, Dc = 1.72 g cm23, m = 1.830 mm21, 1486
data with I > 3s(I), R = 0.042, Rw = 0.052. [12Cu2(CF3SO3)2(CF3SO3)2],
(blue-violet, 173 K), C38H28Cu2F6N16O6S2·2CF3SO3·2CH2Cl2
M =
1577.95, orthorhombic, a = 19.7081(7), b = 17.9293(6), c = 17.1966(6)
Å, U = 6076.5(6) Å3, Z = 4, space group Cmca Dc = 1.72 g cm23, m =
1.121 mm21, 2127 data with I > 3s(I), R = 0.077, Rw = 0.096. Data for
all 3 structures have been obtained on a Nonius Kappa CCD (Mo-Ka)
diffractometer Structural determinations were performed using the Nonius
OpenMolenN package.9 CCDC 182/1781. See http://www.rsc.org/supp-
data/cc/b0/b006665f/ for crystallographic data in .cif format.
1 R. W. Saalfrank, A. Stark, K. Peters and H.-G. von Schnering, Angew.
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Atwood, J. E. D. Davies, D. D. MacNicol and F. Vo¨gtle, Vol. 9 (ed. J. P.
Sauvage and M. W. Hosseini, Elsevier, 1996, p. 253).
We have previously reported examples of metallatubulanes
based on interconnection of metallamacrocyles into infinite 1-D
3 J. K. M. Sanders, in Comprehensive Supramolecular Chemistry, ed. J. L.
Atwood, J. E. D. Davies, D. D. MacNicol and F. Vo¨gtle, Vol. 9 (ed. J. P.
Sauvage and M. W. Hosseini), Elsevier, 1996, p. 131; P. J. Stang and B.
Olenyuk, Acc. Chem. Res., 1997, 30, 502; C. M. Drain and J.-M. Lehn,
J. Chem. Soc., Chem. Commun., 1994, 2313; T. Beissel, R. E. Powers and
K. N. Raymond, Angew. Chem., Int. Ed. Engl., 1996, 35, 1084.
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Inorg. Chem., 1999, 1981.
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Jpn., 1990, 63, 80; V. K. Yamamoto, Bull. Chem. Soc. Jpn., 1954, 27,
501.
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Fischer, Chem. Commun., 1998, 2545.
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9 OpenMolenN, Interactive Structure Solution, Nonius B. V., Delft, The
Netherlands, 1997.
Fig. 3 The packing of the dicationic metallamacrocycle [12Cu2Cl2] and
CuCl4 anions. H atoms and solvent molecules are not presented for
clarity.
22
2086
Chem. Commun., 2000, 2085–2086