1520 Inorganic Chemistry, Vol. 35, No. 6, 1996
Avis et al.
Table 1. Crystallographic Data for 1‚Toluene and 3b‚THF
approximately 23% 3a and 77% 2a. Continued stirring of this mixture
in CH2Cl2 with freshly added NaBF4 (ca. 100 mg) gave 77% 3a and
23% 2a and some decomposition after 5 days. Compound 2a was
completely washed out with Et2O (2 × 20 mL), giving a residue
consisting of 3a and some decomposition. Recrystallization out of CH2-
Cl2/Et2O (1:3) at 20 °C gave 155 mg of pure 3a (23%). IR (KBr):
ν(PdN) ) 1247 and 1225 cm-1. Anal. Calcd. for C46H53BN2F4P3-
ClPt: C, 52.91; H, 5.12; N, 2.68; P, 8.90. Found: C, 52.75; H,
5.19; N, 2.75; P, 8.95. FAB mass found: m/z ) 957.3 (M+, calcd for
C46H53N2P3ClPt: 957.4).
1
3b
formula
mw
space group
cryst syst
a, Å
b, Å
c, Å
C40H38N2P2‚0.5C7H8
654.77
P21/c
monoclinic
8.9591(5)
19.1961(12)
21.9740(9)
105.069(4)
3649.1(3)
4
C48H49Cl2N2P3Pt‚C4H8O
1084.94
P21/c
monoclinic
12.4021(7)
16.9705(11)
23.760(2)
109.544(5)
4712.6(6)
â, deg
V, Å3
Z
[PtCl(PEt3){1,1-BIPE-σN,σN′}]+[PtCl3(PEt3)]- (3a′). To a solu-
tion of 106.2 mg (0.17 mmol) of 1 in 15 mL of CH2Cl2 was added
134.0 mg (0.17 mmol) of Pt2Cl4(PEt3)2, and the mixture was stirred
for 18 h. Evaporation of the solvent resulted in a yellow powder, 240
mg (0.35 mmol, 99.9%) of 3a′. IR (Nujol): ν(PdN) ) 1248 and 1219
4
D
calcd, g cm-3
1.192
1.529
F(000)
µ, cm-1
data set
Ra
1388
2192
13.1 (Cu KR)
-11:7, 0:24, -27:27
0.080 [for 5234Fo >
5.0σ(Fo)]
32.6 (Mo KR)
-10:16, 0:22, -30:28
0.057 [for 6850 Fo >
4.0σ(Fo)]
cm-1 FAB mass found: m/z ) 957.3 (M+, calcd for C46H53N2P3-
.
ClPt: 957.4).
[PtCl(PMe2Ph){1,1-BIPE-σN,σN′}]+[Cl]- (3b). To a solution of
179.1 mg (0.29 mmol) of 1 in 10 mL of CH2Cl2 was added 118.9 mg
(0.15 mmol) of Pt2Cl4(PMe2Ph)2, and the mixture was stirred for 1 h
at 20 °C. The product was obtained by evaporation of the solvent,
yielding 294 mg (0.29 mmol, 99%) of 3b. IR (KBr): ν(PdN) )
1251 and 1230 cm-1. FAB mass found: m/z ) 977 (M+, calcd for
C48H49N2P3ClPt: 977.4). Crystals suitable for X-ray crystal structure
determination were obtained by diffusion of pentane into a THF/CH2-
Cl2 solution of 3b at 20 °C at 1 atm for 7 days.
b
Rw
0.109
wR2c
0.1215
1.00
S
1.28
a R ) ∑||Fo| - |Fc||/∑|Fo|. b Rw ) [∑[w(||Fo| - |Fc||)2]/[∑[w(Fo2)]]1/2
.
2
2
c wR2 ) [∑[w(Fo - Fc2)2]/∑[w(Fo )2]]1/2
.
variance), for 404 parameters and 5234 reflections with Fo > 5σ(Fo).
Hydrogen atoms were included in the refinement on calculated positions
(C-H ) 0.98 Å) riding on their carrier atoms. All non-hydrogen atoms
were refined with anisotropic thermal parameters; the hydrogen atoms
were refined with one common isotropic displacement parameter.
Weights were introduced in the final refinement cycles. The unit cell
contains two toluene molecules disordered over the inversion centers.
No discrete atom model could be fitted. The BYPASS procedure13
was used to take this electron density into account. The application of
BYPASS made refinement more stable. The solvent accessible areas
have a total volume of 550 Å3. A total density of 100 electrons was
counted in this area, consistent with two toluene molecules. The final
difference Fourier showed no residual density outside -0.78 and +0.89
e Å-3. Neutral atom scattering factors were taken from Cromer and
Mann,14 with anomalous dispersion corrections taken from Cromer and
Liberman.15
Compound 3b. Yellowish crystals of 3b, 0.3 × 0.3 × 0.05 mm,
were mounted on a Lindemann-glass capillary and placed on an Enraf-
Nonius CAD4-T diffractometer on rotating anode in the cold dinitrogen
stream (150 K). Data were collected in ω/2θ mode, λ(MoKR) )
0.71073 Å (monochromator), with θ in the range 1.5-27.5°. Scan
angle was ∆ω ) 0.66 + 0.35 tan θ°. Unit cell dimensions and standard
deviations were obtained by least-squares fit (SET4)9 of the setting
angles of 25 reflections in the range 11.6° < θ < 14.0°. The unit cell
parameters were checked for the presence of higher lattice symmetry.10
Three standard reflections were monitored periodically (24h2h, 22h4, 15h2h)
and showed approximately 4% variation in intensity during the 44 h
of data collection. The data were scaled accordingly. Intensity data
were corrected for Lorentz, polarization, and absorption effects (an
empirical absorption/extinction correction was applied (DIFABS16
correction range 0.725-1.00)) and averaged into a unique set of
reflections. Total data of 15 022 reflections were collected of which
10 778 were independent (Rint ) 0.0382).
Alternative Method. Stirring a mixture of 90 mg (0.15 mmol) of
1 and 61 mg (0.07 mmol) of Pt2Cl4(PMe2Ph)2 in 10 mL of THF at 70
°C for 4.5 h gave the same product 3b after workup with pentane,
yielding 111 mg (73%).
[PtCl(PMe2Ph){1,1-BIPE-σN,σN′}]+[PtCl3(PMe2Ph)]- (3b′) was
synthesized from 172.4 mg (0.25 mmol) of 1,1-BIPE (1) and 229.4
mg (0.25 mmol) of Pt2Cl4(PMe2Ph)2 (M:L ) 1:1) in 20 mL of CH2-
Cl2. The solution was stirred for 1 h and evaporated to 5 mL. Addition
of 40 mL of pentane resulted in the precipitation of 3b′, which was
washed with pentane (20 mL) and dried in vacuo. Yield: 344 mg
(87%). IR (KBr): ν(PdN) ) 1250 cm-1 (br). Anal. Calcd.for
C56H60N2P4 Cl4Pt2: C, 47.47; H, 4.72; N, 1.98; P, 8.72. Found: C,
47.28; H, 4.33; N, 1.92; P, 8.61.
Variable temperature NMR studies were carried out on solutions
of 0.035 mmol of 3a in 0.5 mL of CDCl3 at 233-330 K or of 0.035
mmol of 3b in 0.4 mL of CD2Cl2 at 233-293 K. Subsequently, 2.8
µL (0.035 mmol) of pyridine was added to the CDCl3 solution of 3a at
330 K, which gave no reaction and no exchange processes occurred.
X-ray Crystal Structure Determinations of 1 and 3b. Crystal
data and experimental procedures on both crystal structures are collected
in Table 1.
Compound 1. Transparent colorless crystals, 0.3 × 0.3 × 0.6 mm,
suitable for X-ray structure determination, were mounted on a Linde-
mann-glass capillary and placed on an Enraf-Nonius CAD4-F diffrac-
tometer at 298 K. Data were collected in ω/2θ mode, λ(Cu KR) )
1.54184 Å (Ni-filtered), with θ in the range 2.1-75.0°. Scan angle
was ∆ω ) 0.55 + 0.14 tan θ°. Unit cell dimensions and standard
deviations were obtained by least-squares fit (SET4)9 of the setting
angles of 25 reflections in the range 18.4° < θ < 23.7°. Reduced-cell
calculations did not indicate higher lattice symmetry.10 Three standard
reflections were monitored periodically (2h14, 1h24h, 2h1h4) and showed
approximately 14% decay during the 91 h of data collection. The data
were scaled accordingly. Intensity data were corrected for Lorentz,
polarization, but not for absorption, and averaged into a unique set of
reflections. Total data of 11 303 reflections were collected of which
7503 were independent (Rint ) 0.0778). The structure was solved by
direct methods (SHELXS86).11 Refinement on F was carried out by
full-matrix least-squares techniques (SHELX76);12 final R value 0.080,
Rw ) 0.109, w ) 1/{σ2(F) + 0.000248F2], S ) 1.28 (based on the
The structure was solved by automatic Patterson methods and
subsequent difference Fourier synthesis (DIRDIF-92).17 Refinement
on F2 was carried out by full-matrix least-squares techniques (SHELXL-
93);18 final R1 value 0.057 for 555 parameters and 6850 reflections
with I > 2.0σ(I), wR2 ) 0.122 for all 10 778 reflections, S ) 0.996
2
and w ) 1/{σ2(Fo) + 0.0514P2] where P ) (Max(Fo ,0) + 2Fc2)/3. All
(13) van der Sluis, P.; Spek, A. L. Acta Crystallogr. 1990, A46, 194.
(14) Cromer, D. T.; Mann, J. B. Acta Crystallogr. 1968, A24, 321.
(15) Cromer, D. T.; Liberman, D. J. Chem. Phys. 1970, 53, 1891.
(16) Walker, N.; Stuart, D. Acta Crystallogr. 1983, A39, 158.
(17) Beurskens, P. T.; Admiraal, G.; Beurskens, G.; Bosman, W. P.; Garc´ıa-
Granda, S.; Gould, R. O.; Smits, J. M. M.; Smykalla, C. The DIRDIF
program system; Technical report of the Crystallography Laboratory;
University of Nijmegen: Nijmegen, The Netherlands, 1992.
(18) Sheldrick, G. M. SHELXL-93 Program for crystal structure refinement.
University of Go¨ttingen, Germany, 1993.
(9) Boer, J. L. de; Duisenberg, A. J. M. Acta Crystallogr. 1984, A40,
C410.
(10) Spek, A. L. J. Appl. Crystallogr. 1988, 21, 578.
(11) Sheldrick, G. M. SHELXS86 Program for crystal structure determi-
nation. University of Go¨ttingen, Germany, 1986.
(12) Sheldrick, G. M. SHELX76 Program for crystal structure determina-
tion. University of Cambridge, Cambridge, 1976.