130
K. Hiraki et al. / Journal of Organometallic Chemistry 574 (1999) 121–132
Table 4
Crystal data for 7 and 8
3.4. Reaction of 1 with 2-methyl-2-propen-1-ol at high
temperature
7
8
A mixture of 1 (602 mg, 0.63 mmol) and dried
2-methyl-2-propen-1-ol (10 ml) was heated at 80°C for
48 h. The reaction mixture was concentrated under a
reduced pressure and applied to silica-gel column chro-
matography. The first fraction was eluted with hexane–
diethyl ether (1:2) to afford pale yellow solids of
[Ru{CH2ꢀC(CH3)CHꢀO}(CO)(PPh3)2] (7) (312 mg,
68%). Anal. Found: C, 67.66; H, 5.13. Calc. for
C41H36O2P2Ru: C, 68.04; H, 5.01%. M.p. 191–193°C
(dec.). IR (cm−1): w(CꢁO) 1915vs. 1H-NMR (CDCl3): l
1.18 (m, 1H, CHaHb), 1.50 (m, 1H, CHaHb), 1.99 (d,
J=2.9 Hz, 3H, CH3), 5.81 (d, J=4.4 Hz, 1H, CH).
13C{1H}-NMR (CDCl3): l 17.4 (s, CH3), 39.7 (d, J=
31.3 Hz, CH2), 99.6 (s, CCH3), 123.8 (s, CHO), 207.6
(t, J=11.7 Hz, CꢁO). 31P{1H}-NMR (CDCl3): l 31.0
(d, J=2.1 Hz), 40.7 (d, J=2.1 Hz).
Formula
C41H36O2P2Ru
723.75
C22H24ClOP
370.86
Formula weight (M)
Color and habit
Crystal size (mm)
Crystal system
Space group
Pale yellow prism
0.40×0.20×0.50
Monoclinic
Cc (No.9)
19.080(2)
10.396(2)
18.994(2)
10.442(8)
3530.3(8)
4
1.362
1488.00
5.69
0.31, 0.028
1.59
Colorless prism
0.40×0.20×0.50
Monoclinic
P21/c (No.14)
11.564(3)
10.032(7)
17.586(2)
106.61(1)
1954(1)
˚
a (A)
˚
b (A)
˚
c (A)
i (°)
V (A )
3
˚
Z
4
Dcalc (g cm−3
F(000)
)
1.260
784.00
2.84
0.050, 0.036
1.59
v(Mo–Kh) (cm−1
R, Rw
)
Goodness-of-Fit
The second fraction was eluted with chloroform–
methanol (4:1) to give [Ph3PCH2CH(CH3)CH2OH]Cl
(8) (112 mg, 48%). Anal. Found: C, 70.53; H, 6.46.
Calc. for C22H24ClOP: C, 71.25; H, 6.52%. M.p. 233–
235°C. IR (cm−1): w(OH) 3275br, w(P–C) 1462vs,
respectively. Tables of hydrogen atom coordinates, an-
isotropic displacement parameters and complete lists of
bond lengths and angles have been deposited at the
Cambridge Crystallographic Data Centre. The intensity
data were collected at 20°C on a Rigaku AFC7S auto-
matic four-circle diffractometer with graphite-
monochromated Mo–Kh radiation. Cell constants were
obtained from the least-squares refinement of the set-
ting angles of the carefully centered reflections (16
reflections in the range 35.87°52q539.42° for 7, and
25 in the range 22.69°52q 536.04° for 8). Azimuthal
scans of several reflections indicated no need for an
absorption correction. The data were corrected for
Lorentz and polarization effects. During the data col-
lection, the intensities of three representative reflections
were measured after every 150 reflections; no variation
was observed.
1
w(C6H5) 1440s, w(C–OH) 1113s. H-NMR (CDCl3): l
0.52 (d, J=6.6 Hz, 3H, CH3), 2.17 (m, 1H, CH), 2.66
(ddd, J=16.0, 9.5 and 12.0 Hz, 1H, PCHaHb), 3.66 (dt,
J=11.4 and 4.6 Hz, 1H, CHcHdO), 3.59 (dd, J=11.4
and 9.0Hz, 1H, CHcHdO),4.94(t, J=16.0 Hz, 1H,
PCHaHb). 13C{1H}-NMR (CDCl3): l 17.6 (s, CH3),
26.1 (d, J=50.9 Hz, PCH2), 32.0 (s, CH), 66.8 (d,
J=11.8 Hz, CH2O), 119.3 (d, J=86.1 Hz, ipso-Ph),
130.5 (d, J=11.8 Hz, m-Ph), 133.7 (d, J=11.8 Hz,
o-Ph), 135.0 (s, p-Ph). 31P{1H}-NMR (CDCl3): l 21.2
(s).
3.4.1. The NMR analysis of the time-programmed
experiment
A mixture of 1 (308 mg) and dried 2-methyl-2-
propen-1-ol (10 ml) was allowed to react in a Schlenk
tube sealed with a rubber septum. After being kept at
room temperature for 72 h, a small part of the reaction
mixture was sampled through the septum with a sy-
ringe. Before the sample was applied to the NMR
measurement, it was concentrated under a reduced
pressure and successively diluted with CDCl3. The rest
of the reaction mixture was allowed to react for addi-
tional 48 h at 50°C before the second sampling. The
last sample was taken after extra 70 h at 65°C.
As for 7, of the 4406 reflections which were collected,
4277 were unique. The structure was solved by heavy-
atom Patterson methods [28] and expanded using
Fourier techniques [29]. The non-hydrogen atoms were
refined anisotropically; the hydrogen atoms were in-
cluded but not refined. The final cycle of full-matrix
least-squares refinement was based on 3572 observed
reflections {I\3|(I)} and 423 variable parameters; the
function minimized was ꢀ w( ꢁ Fo ꢁ−ꢁFc ꢁ )2, where
w
−1=|2(Fo)+[(0.010/2)Fo]2.
As for 8, of the 4966 reflections which were collected,
4740 were unique. The structure was solved by direct
methods [30] and expanded using Fourier techniques
[29]. Thc non-hydrogen atoms were refined anisotropi-
cally; the hydrogen atom coordinates were refined but
their isotropic thermal parameters were held fixed. The
final cycle of full-matrix least-squares refinement was
based on 1730 observed reflections {I\3|(I)} and 299
3.5. Single crystal X-ray structure analysis
Crystal data and details of the measurement for 7
and 8 are summarized in Table 4. The final atomic
coordinates with the equivalent isotropic thermal
parameters for 7 and 8 are reported in Tables 5 and 6,