C.-S. Hwang, P.P. Power / Journal of Organometallic Chemistry 589 (1999) 234–238
235
2. Experimental
posed to a black powder at 150–152°C. 1H-NMR
(THF-d8, 25°C) l 6.59 (t, J=7.2 Hz, p-C6H3); 6.54 (s,
m-Mes); 6.32 (d, J=7.2 Hz, m-C6H3); 3.58 (br, THF-
d8); 2.13 (br, s, o-CH3 (Mes)); 1.74 (br, THF-d8); 1.59
(br, s, p-CH3(Mes)). Small peaks at 3.34 (q) and 1.08 (t)
ppm were assigned to Et2O (solvant) which, upon inte-
gration, afforded an intensity ratio of 0.13:1 with re-
spect to the cation and anion peaks. 13C{1H}-NMR
(THF-d8, 25°C) l 180.89 (br, i-C6H3); 152.09 (i-Mes);
148.93 (o-C6H3); 136.36 (o-Mes); 132.27 (p-Mes);
128.75 (p-C6H3); 127.50 (m-Mes); 121.91 (m-C6H3);
67.41 (quintet, THF-d8); 25.32 (quintet, THF-D8); 21.89
(o-CH3(Mes)); 21.51 (p-CH3(Mes)) very small peaks at
59.21 and 15.65 ppm were assigned to be Et2O (sol-
vent). 7Li-NMR (THF-d8, 25°C: LiCl–D2O was used as
reference) l −0.62 ppm (br, s).
2.1. General procedures
All experiments were performed under a nitrogen
atmosphere either by using modified Schlenk techniques
or in a Vacuum Atmospheres HE43-2 drybox. Solvents
were freshly distilled from a sodium–potassium alloy
and degassed twice prior to use. The 13C-, 1H- and
7Li-NMR spectra were recorded in C6D6 or THF-D8
solutions by using a General Electric QE-300 NMR
spectrometer. The compounds (Et2O)2LiTriph [7] and
(LiC6H3-2,6-Mes2)2 [8] were synthesized by literature
procedures. Silver cyanate was obtained commercially
and used as received.
2.2. [Li(THF)4][Ag(Triph2)]·THF
2.4. X-ray data collection, the solution and refinement
(Et2O)2LiTriph (2.30 g, 5.0 mmol) was dissolved in
Et2O (30 ml) and the solution was added dropwise to a
rapidly stirred suspension of AgOCN (0.37 g, 2.50
mmol) in a 3:1 Et2O–THF mixture (20 ml) and cooled
to ca. −78°C. During the reaction, light was excluded
by wrapping the Schlenk tube with aluminum foil.
After 2 h stirring at ca. −78°C, the mixture was
allowed to warm to ca. 0°C over 3 h. The gray precipi-
tate was then removed by filtration. The resultant pale-
green filtrate was stored in a ca. −20°C freezer for 3
days to afford the product as colorless crystals: yield
of the structures
The crystals were coated with a layer of hydrocarbon
oil upon removal from the Schlenk tube. Suitable crys-
tals were selected, attached to a glass fiber, and immedi-
ately placed in the low-temperature N2 stream [9]. Both
X-ray data sets were collected with Cu–Ka (u=1.54178
,
A) radiation by using a Siemens P4RA diffractometer
equipped with a rotating anode X-ray source, nickel
filter and a locally modified LT apparatus. Calculations
were carried out on a Micro Vax 3200 computer using
1
0.94 g (35%); m.p.: 122–124°C dec. H-NMR (C6D6,
the SHELXTL-PLUS [10] program system. The structures
25°C) l 7.79, (br, s); 7.72 (d, J=6.0 Hz); 7.65 (d,
J=6.0 Hz); 7.56 (br, s); 7.32 (d, J=6.0 Hz); 7.17ꢀ
6.96 (m) [aromatic H’s]; 7.15 (C6D6); 2.99 (br, s, THF);
0.93 (br, s, THF). 13C{1H}-NMR (C6D6, 25°C) l
192.23 (i-C6H2); 153.76 (o-C6H2); 153.04 (p-C6H2);
144.59 (i-(o-Ph)); 143.76 (i-(p-Ph)); 142.85 (o-(p-Ph));
141.52 (p-(p-Ph)); 137.68 (m-(p-Ph)); 129.10 (m-C6H2);
128.00 (t, C6D6); 125.52 (p-(o-Ph)); 125.04 (o-(o-Ph));
121.89 (m-(o-Ph)); 68.18 (THF); 25.24 (THF). 7Li-
NMR (C6D6, 25°C: LiCl in D2O was used as a refer-
ence) l 1.49 ppm (br, s).
were solved by direct methods. The data were subse-
quently refined by full-matrix least-squares procedures.
Hydrogen atoms were included by the use of a riding
,
model with C–H distance of 0.96 A and fixed isotropic
2
,
thermal parameters with UH(iso)=0.06 A . For the
absorption correction, an empirical method, XABS2,
was applied [11]. Although the data for 1 generally
refined satisfactorily, there were residual electron den-
−3
,
sity values of 1.79 and 1.44 e A
that were 1.226 and
,
1.339 A distant from the silver. These probably resulted
from absorption problems associated with use of cop-
per radiation. For 2, the higher than usual R value is
probably due to disorder problems in the Li(THF)4 and
OEt2 (solvent) groups. The atoms in these groups were
located from successive difference maps. But poor con-
vergence during refinement was observed, probably as a
result of their large thermal motion. For several of
these atoms, more reasonable geometries were obtained
from the difference map positions than from those
obtained after anisotropic refinement. Consequently,
the original positions were retained and their isotropic
2.3. [Li(THF)4][Ag(C6H3-2,6-Mes2)2]·1/8 Et2O
(LiC6H3-2,6-Mes2)2 (1.6 g, 5.0 mmol) was dissolved
in Et2O (30 ml) and added dropwise to a stirred suspen-
sion of AgOCN (0.37 g, 2.50 mmol) in a 3:1 Et2O–
THF mixture (20 ml) and cooled to ca. −78°C. Light
was excluded by wrapping the Schlenk with aluminum
foil during the reaction. After 2 h stirring at ca.
−78°C, the mixture was allowed to warm to ca. 0°C,
whereupon the gray residue was filtered off. The yel-
low–green supernatant liquid was placed in a −20°C
freezer for 1 day, which afforded the product 2 as
colorless crystals: yield: 1.97 g (37.9%); m.p.: the white
crystalline became light-brown at 134°C and decom-
thermal parameters were simply fixed at a relatively
2
,
high value of 0.15 A by use of the SHELXTL AFIX
1
feature during the final cycle of the refinement. Both
Li(2) and C(117) were successfully modeled with two
split positions; Li(2A) and Li(2B) (50:50) and C(117)