D.F. Mullica et al. / Inorganica Chimica Acta 285 (1999) 318±321
319
Table 1
removal of the check re¯ections, the averaging of duplicate
and equivalent data was carried out (Rint 0.052). The
remaining intensity data were corrected for Lorentz, polar-
ization and X-ray absorption effects [6] (max., min., trans-
mission factors 0.9908, and 0.5461). Systematic absences
of 0k0 where k 2n 1 and h0l where l 2n 1 were
consistent with space group P21/c. A zero moment test (NZ-
test) [7] on the observed data set indicated that it was
centrosymmetric in nature.
Experimental and statistical summary of compound 2
Molecular formula
Formula weight
Crystal system
Space group
C49H45BF4N2OP2Ru
927.7
monoclinic
P21/c (No. 14, C25h
15.395(3)
18.156(4)
17.352(3)
110.53(3)
4542.0(15)
4
)
Ê
a (A)
Ê
b (A)
Ê
c (A)
ꢄ (8)
V (A )
Ê 3
The phase problem was resolved by using the Siemens
SHELXTL PLUS (PC version) [8] which located the heavy atom
(Ru). A series of difference Fourier maps located the atomic
positions of the phosphorous, nitrogen, carbon, and oxygen
atoms. These positions were re®ned isotropically for several
full-matrix least-squares cycles before attempting to locate
the BF4 anion, which was subsequently located by electron
density mapping. Hydrogen atoms at calculated positions
Z
3
Dcalc. (Mg m
Dmeas. (Mg m
)
1.357
3
)
1.351(3)
0.459
1
)
ꢅ (Mo Ka) (mm
F(000) (e )
2ꢂ Range (8)
Á! (8) (!±2ꢂ)
Rint
1904
3.0±40.0
1.15 0.34 tan ꢂ
0.052
R (Rw, Rall
)
0.070 (0.091, 0.094)
Ê
(C±H, 0.96 A) on the phenyl rings and the 4-picoline groups
Unique reflections
3131
1.3(9)
560
Extinction correction (e 2)(Â 10
No. variable parameters
Goodness-of-fit
)
4
were allowed to ride on their respective bonding atoms with
3
Ê 2
®xed isotropic thermal parameters, Uiso 80 Â 10 A .
1.24
Ê
The hydride was also positioned at a distance of 1.78 A (Ru±
3
Ê 2
H, Uiso 80 Â 10 A ). Several cycles varying the aniso-
C49H45BF4N2OP2RuÁC4H8O (2ÁTHF): C, 63.67; H, 5.34; N,
tropic thermal parameters of all non-hydrogen atoms
and applying a secondary correction to the data yielded
®nal residual index values, R ÆÁF=ÆFo and Rw
2.80. Found: C, 63.88; H, 5.61; N, 2.78%. IR (mineral oil):
ꢀ
max (cm 1) (CO) 1 1938 (1934 [2]); 2 1933; 3 1954
2
(1950 [2]). NMR (CD2Cl2): 1 ꢁH 6.6±7.8 [40H, m, py/
PPh3] and 13.0 [1H, t, JPH 19.8, RuH] ( 12.1, JPH 19.5
[2]); ꢁP 49.8 [s, PPh3]; 2 ꢁH 6.4±7.6 [38H, m, 4-Mepy/
PPh3], 2.2 [3H, s, Me], 2.1 [3H, s, Me] and 13.0 [1H, t, JPH
20.0, RuH]; ꢁP 49.5 [s, PPh3]; 3 ꢁH 6.4±8.6 [38H, m, bpy/
PPh3] and 11.3 [1H, t, JPH 19.6, RuH] ( 11.4, JPH 19.2
[2]); ꢁP 48.5 [s, PPh3]. Single crystals for X-ray analysis
were prepared by layering diethyl ether over a solution of 2
in CH2Cl2.
ÆwÁF=ÆwÁFo where ÁF jjFo Fcjj and w ꢃ
(Fo ), see Table 1. A ®nal difference Fourier map revealed
3
a maximum peak of 1.07 e A in the vicinity of the Ru
Ê
atom which is quite normal in compounds containing heavy
metals. Elsewhere, the map was virtually featureless dis-
playing only a random ¯uctuating background. Atomic
scattering factors and associated anomalous dispersion cor-
rections were obtained from the usual source [9].
3. Results and discussion
2.3. Crystallographic study of 2
3.1. Synthesis and spectroscopy of
[RuH(CO)(PPh3)2L2][BF4]
Conoscopic examination of 2 using crystal rotation
between two crossed polarizers on a Zeiss Photomicroscope
(II) provided evidence that the system was biaxial (aniso-
tropic in nature, birefringent) and optically homogeneous.
Data were collected from a clear colorless parallelepiped-
shaped crystal (0.36 mm  0.08 mm  0.49 mm). An
Enraf-Nonius CAD4-F automated diffractometer equipped
with graphite-monochromated Mo Ka radiation was em-
ployed, see Table 1 for crystal data and solution details. A
least-squares re®nement of 25 well centered high angle
(30.0 ꢀ 2ꢂ ꢀ 50.08) re¯ections yielded ®nal lattice para-
meters. Crystal stability and hardware reliability were ver-
i®ed by monitoring three standard re¯ections as a function
It has been shown previously that OsH2(CO)(PPh3)3 can
be converted to [OsH(CO)(PPh3)2py2] and related com-
plexes by oxidation, hydride abstraction, and protonation,
all performed in CH2Cl2 in the presence of an excess of a
pyridine type ligand [1]. The second pyridine apparently
substitutes for one PPh3 after the ®rst pyridine replaces a
hydride in the oxidation, hydride abstraction, or protonation
step. It was subsequently found that the ruthenium analog,
RuH2(CO)(PPh3)3, reacts similarly with hydride abstractors
in CH2Cl2 in the presence of pyridine type ligands. Upon
further investigation THF proved to be a more convenient
solvent for the reaction since the product, [RuH-
(CO)(PPh3)2L2][BF4], spontaneously precipitates from this
solvent. Tropylium tetra¯uoroborate, [C7H7][BF4], was
more reactive than triphenylcarbenium and so was used
as the hydride abstractor in the present study. As formed, the
Ru±pyridine complexes contain a small amount of an
1
of time (every h). An intensity loss of 0.04% h (1.8%,
total decay) was observed which required a linear decay
correction to the data set (maximum correction of 1.00933,
average 1.00451) using the program DECAY [6]. A total of
4410 intensity measurements were collected of which 4222
were independent and 3131 ®tted F > 6.0ꢃ(F). After the