J. D´ıez et al. / Journal of Organometallic Chemistry 637–639 (2001) 677–682
681
3.1. [Cu(CNR)2(s2-P,P-dppf )][BF4] (R=tBu (1),
2,6-Me2C6H3 (2), Cy (3), Bz (4))
N, 3.21%. Anal. Found: C, 63.99; H, 4.73; N, 2.79.
Calc. for C52H46N2BCuF4P2Fe (2): C, 64.58; H, 4.79;
N, 2.89%. Anal. Found: C, 62.69; H, 5.38; N, 2.98.
Calc. for C48H50N2BCuF4P2Fe (3): C, 62.46; H, 5.46;
N, 3.03%. Anal. Found: C, 63.93; H, 4.51; N, 2.91.
Calc. for C50H40N2BCuF4P2Fe (4): C, 63.95; H, 4.51;
N, 2.98%.
3.1.1. Procedure A
A mixture of the corresponding isocyanide (0.30
mmol), [Cu2(m-Cl)2(k2-P,P-dppf)2] (0.1 g, 0.15 mmol)
and AgBF4 (0.059 g, 0.30 mmol) in CH2Cl2 (20 ml) was
stirred at room temperature (r.t.) for 4 h. The resulting
solution after filtration was concentrated under vac-
uum. The addition of Et2O (20 ml) to the concentrated
solution led to the precipitation of yellow solids, which
were recrystallized from CH2Cl2–Et2O. Yields: 50–
65%. \M (V−1 cm2 mol−1) 1=114, 2=111, 3=120,
and 4=116. Anal. Found: C, 59.06; H, 5.28; N, 3.08.
Calc. for C44H46N2BCuF4P2Fe (1): C, 60.67; H, 5.32;
3.1.2. Procedure B
The corresponding isocyanide (0.625 mmol.) was
added to a solution of [Cu(MeCN)2(k2-P,P-dppf)][BF4]
(0.23 g, 0.25 mmol) in CH2Cl2 (20 ml) and the mixture
was stirred and heated to reflux for 4 h. The addition of
Et2O (20 ml) to the concentrated solution led to the
precipitation of yellow solids, which were washed with
Et2O (3×10 ml) and vacuum-dried. Analytically pure
samples were obtained by recrystallization from
CH2Cl2–Et2O. Yields: 60–75%.
Table 4
Crystal data and structure refinement parameters for [Cu2(m-Cl)2(k2-
P,P-dppf)2]·CH2Cl2 and [Cu(CNtBu)2(k2-P,P-dppf)][BF4]·CH2Cl2
3.2. X-ray crystal structure determination of D·CH2Cl2
and 1·CH2Cl2
[Cu2(m-Cl)2-
(k2-P,P-dppf)2]·
CH2Cl2
[Cu(CNtBu)2-
(k2-P,P-dppf)][BF4]·
CH2Cl2
Diffraction data were recorded at 293(2) K with the
q–2q technique on a Siemens AED diffractometer for
both compounds. The structures were solved by direct
methods (SIR92) [10] and refined by full-matrix least-
squares methods based on F2 using the SHELXL-97 [11]
program. All the non-hydrogen atoms were refined
anisotropically. The chlorine atoms of CH2Cl2 in
D·CH2Cl2 were found disordered as well as the methyl
Empirical formula
Formula weight
C69H58Cl4Cu2Fe2P4 C45H48BCl2CuF4FeN2P2
1391.61
0.71073
Monoclinic
C2/c
955.89
,
Wavelength (A)
0.71073
Monoclinic
P21/n
Crystal system
Space group
Unit cell dimensions
,
a (A)
24.801(5)
13.393(3)
18.751(4)
93.130(10)
6219(2)
4
18.280(6)
15.221(5)
18.498(6)
115.65(2)
4640(3)
4
,
b (A)
t
,
c (A)
i (°)
V (A )
carbon atoms of the Bu groups in 1·CH2Cl2. Crystal
data and some details of the structure determination
are listed in Table 4. All calculations were carried out
on the DIGITAL AlphaStation 255 of the ‘Centro di
Studio per la Strutturistica Diffrattometrica’ del CNR,
Parma.
3
,
Z
Dcalc (Mg m−3
)
1.486
1.368
Absorption coefficient 1.449
(mm−1
F(000)
1.004
)
2840
1968
Crystal size (mm)
q range for data
collection (°)
0.12×0.15×0.25
3.04–28.03
0.16×0.21×0.34
3.32–25.00
4. Supplementary material
Index ranges
−325h532,
−65k517,
−245l523
7721
−215h521,
−185k517,
−135l521
8384
Crystalllographic data for the structural analysis
have been deposited with the Cambridge Crystallo-
graphic Data Centre, CCDC nos. 158660 and 158661
for compounds D·CH2Cl2 and 1·CH2Cl2, respectively.
Copies of this information may be obtained free of
charge from The Director, CCDC, 12 Union Road,
Cambridge CB2 1EZ, UK (Fax: +44-1223-336033;
e-mail: deposit@ccdc.cam.ac.uk or www: http://www.
ccdc.cam.ac.uk).
Reflections
collected/unique
Unique reflections
Data/restraints/
parameters
Final R indices
[I\2|(I)]
7507 [Rint=0.0477] 8127 [Rint=0.0322]
7507/0/417
8127/24/579
R1=0.0403,
wR2=0.0869
R1=0.0928,
wR2=0.1224
R1=0.0696,
wR2=0.1983
R1=0.1030,
wR2=0.2251
1.096
R indices (all data)
Goodness-of-fit on F2 1.087
Largest difference
0.405 and −0.443 1.285 and −0.647
peak and hole
Acknowledgements
−3
,
(e A
)
This work was supported by the Direccio´n General
de Investigacio´n Cient´ıfica y Te´cnica of Spain (DGI-
CYT). Project PB96-0558.
GOF=[ꢀ[w(F2o−F2c)2]/(n−p)]1/2
,
R1=ꢀꢁ ꢁFoꢁ−ꢁFcꢁ ꢁ/ꢀꢁFoꢁ, wR2=
[ꢀ[w(Fo2−Fc2)2]/ꢀ[w(Fo2)2]]1/2, w=1/[|2(F2o)+(aP)2+bP], where P=
[max(F2o,0)+2F2c]/3.