Kinetics and mechanisms of the reactions of diaryl- and dialkylgermylenes with alcohols and ethers in solution

Article abstract of DOI:10.1021/om060595s

The reactions of methanol, tert-butanol, and THF with a series of simple germylene derivatives-dimethyl- (GeMe₂), diphenyl- (GePh ₂), and dimesitylgermylene (GeMes₂; Mes = 2,4,6-trimethylphenyl)-have been studied in hexane solution at 25 °C by laser flash photolysis methods. The results are consistent with rapid, reversible reaction to form weakly stabilized Lewis acid-base complexes, which exhibit UV absorption maxima in the range 290-360 nm and decay with mixed order kinetics with concomitant formation of the corresponding digermene, Ge ₂R₄ (R = Me, Ph, or Mes). Absolute rate constants for formation of the complexes could be measured for GePh₂ with all three substrates and for GeMe₂ with THF and were found to vary over the range (4-10) × 10⁹ M^-1 s^-1. Equilibrium constants were measured in all cases; they vary between 1.2 and 15 M ^-1 for GeMes₂, decreasing in the order MeOH > t-BuOH > THF, while those for GeMe₂ and GePh₂ are 2-4 orders of magnitude larger and decrease in the order THF > MeOH > t-BuOH. For a given substrate, the equilibrium constants are consistently larger for GePh ₂ than for GeMe₂, reflecting the greater ability of phenyl compared to methyl substituents to stabilize negative charge at germanium in the zwitterionic complexes. In spite of the differences in the stabilities of the complexes, the rate constant for complexation with THF is almost twice as large for GeMe₂ than for GePh₂. The results indicate that the O - H insertion reaction of germylenes with alcohols proceeds via initial, reversible Lewis acid - base complexation, followed by slow proton transfer from oxygen to germanium, most likely via a catalytic route.

Full text of DOI:10.1021/om060595s

5
424
Organometallics 2006, 25, 5424-5434
Kinetics and Mechanisms of the Reactions of Diaryl- and
Dialkylgermylenes with Alcohols and Ethers in Solution
William J. Leigh,* Farahnaz Lollmahomed, Cameron R. Harrington, and
Jacklyn M. McDonald
Department of Chemistry, McMaster UniVersity, 1280 Main Street West, Hamilton, Ontario,
Canada L8S 4M1
ReceiVed July 3, 2006
The reactions of methanol, tert-butanol, and THF with a series of simple germylene derivativess
dimethyl- (GeMe ), diphenyl- (GePh ), and dimesitylgermylene (GeMes ; Mes ) 2,4,6-trimethylphenyl)s
2 2 2
have been studied in hexane solution at 25 °C by laser flash photolysis methods. The results are consistent
with rapid, reversible reaction to form weakly stabilized Lewis acid-base complexes, which exhibit UV
absorption maxima in the range 290-360 nm and decay with mixed order kinetics with concomitant
formation of the corresponding digermene, Ge
2
R
4
(R ) Me, Ph, or Mes). Absolute rate constants for
with all three substrates and for GeMe with
THF and were found to vary over the range (4-10) × 10 M s . Equilibrium constants were measured
in all cases; they vary between 1.2 and 15 M for GeMes , decreasing in the order MeOH > t-BuOH
THF, while those for GeMe and GePh are 2-4 orders of magnitude larger and decrease in the order
THF > MeOH > t-BuOH. For a given substrate, the equilibrium constants are consistently larger for
GePh than for GeMe , reflecting the greater ability of phenyl compared to methyl substituents to stabilize
negative charge at germanium in the zwitterionic complexes. In spite of the differences in the stabilities
of the complexes, the rate constant for complexation with THF is almost twice as large for GeMe than
for GePh
formation of the complexes could be measured for GePh
2
2
9
-1 -1
-
1
2
>
2
2
2
2
2
2
. The results indicate that the O-H insertion reaction of germylenes with alcohols proceeds
via initial, reversible Lewis acid-base complexation, followed by slow proton transfer from oxygen to
germanium, most likely via a catalytic route.
Introduction
Insertion into the O-H bonds of simple alcohols is one of
is supported by the results of fast kinetic studies of the reactions
1
1,13
14
of the parent species (SiH2
and GeH2 ) with water and
alcohols in the gas phase, but there have not yet been any
detailed mechanistic studies of the reaction in simple aryl- and
alkyl-substituted derivatives by time-resolved kinetic methods
in solution at ambient temperatures.
the best known reactions of silylenes and germylenes and one
of the most commonly employed trapping reactions used to
demonstrate the involvement of these species as reactive
intermediates in the thermal and photochemical reactions of
organosilicon and organogermanium compounds.1 In both
cases, the reactions are thought to be initiated by Lewis acid-
base complexation, followed by proton transfer from oxygen
to silicon or germanium within the first-formed zwitterionic
complex (eq 1). This mechanism has been inferred primarily
on the basis of low-temperature spectroscopic studies, which
have allowed the direct spectroscopic detection of silylene-
-5
6
,7
and germylene-alcohol complexes in matrixes at 77 K, and
the results of theoretical calculations.8 The same mechanism
-12
*
Corresponding author. E-mail: leigh@mcmaster.ca.
The mechanism of silylene O-H insertions was first studied
by Steele and Weber in the early 1980s, who measured primary
kinetic isotope effects in the range 1.8-2.4 for the reactions of
SiMe2 with ethanol and tert-butanol by competitive product
(1) Gaspar, P. P.; West, R. Silylenes. In The chemistry of organic silicon
compounds, Vol. 2; Rappoport, Z., Apeloig, Y., Eds.; John Wiley and
Sons: New York, 1998; pp 2463-2568.
(
(
(
(
(
2) Neumann, W. P. Chem. ReV. 1991, 91, 311.
3) Barrau, J.; Rima, G. Coord. Chem. ReV. 1998, 180, 593.
4) Weidenbruch, M. Eur. J. Inorg. Chem. 1999, 1999, 373.
5) Tokitoh, N.; Okazaki, R. Coord. Chem. ReV. 2000, 210, 251.
6) Gillette, G. R.; Noren, G. H.; West, R. Organometallics 1989, 8,
15
analysis methods. They concluded that the reaction most likely
proceeds via rapid, reversible Lewis acid-base complexation
followed by rate-determining proton transfer (see eq 1), but
could not rule out a concerted insertion mechanism. Later work
by the same group, again based on competition kinetic methods,
4
87.
(
(
(
(
7) Ando, W.; Itoh, H.; Tsumuraya, T. Organometallics 1989, 8, 2759.
8) Su, M.-D.; Chu, S.-Y. J. Phys. Chem. A 1999, 103, 11011.
9) Su, M.-D.; Chu, S.-Y. J. Chin. Chem. Soc. 2000, 47, 135.
10) Heaven, M. W.; Metha, G. F.; Buntine, M. A. J. Phys. Chem. A
(13) Alexander, U. N.; King, K. D.; Lawrance, W. D. J. Phys. Chem. A
2002, 106, 973.
(14) Alexander, U. N.; King, K. D.; Lawrance, W. D. Phys. Chem. Chem.
Phys. 2003, 5, 1557.
2
001, 105, 1185.
11) Becerra, R.; Cannady, J. P.; Walsh, R. J. Phys. Chem. A 2003, 107,
1049.
12) Su, M.-D. Chem. Eur. J. 2004, 10, 6073.
(
1
(
(15) Steele, K. P.; Weber, J. Inorg. Chem. 1981, 20, 1302.
1
0.1021/om060595s CCC: $33.50 © 2006 American Chemical Society
Publication on Web 09/28/2006

Reactions of Diaryl- and Dialkylgermylenes with Alcohols
Organometallics, Vol. 25, No. 22, 2006 5425
revealed a complex dependence of the relative rates of the
reaction on alcohol concentration.16 Shizuka and Das and their
2,4,6-trimethylphenyl), and dimethylgermylene (GeMe2)swith
methanol (MeOH), tert-butanol (t-BuOH), and tetrahydrofuran
(THF) in hexane solution. The germylenes have been generated
and monitored by laser flash photolysis of the corresponding
germacyclopent-3-ene derivatives 1a-c (eq 2), as in our
previous studies of the reactivities of these transient molecules
10
-1 -1
co-workers later reported rate constants of k ≈ 10
M
s
for the reaction of SiMe2 with various aliphatic alcohols in
hydrocarbon solution at ambient temperatures, monitoring the
17-19
decay of the silylene directly by laser flash photolysis.
Das
3
0-32
and co-workers also examined the complexation of SiMe2 with
tetrahydrofuran (THF) in cyclohexane solution, reporting the
silylene to react with the ether at close to the diffusion limit
with other reagents.
Steady-state photolysis of all three of
these compounds in the presence of 0.2-0.5 M MeOH has
previously been shown to afford the corresponding methox-
1
0
-1 -1
30,32
(
kTHF ) 1.3 × 10
M
s
at 22 °C) to form a transient product
ygermanes cleanly and with high quantum efficiency.
that was assigned to the Me2Si-THF Lewis acid-base complex
on the basis of its UV/vis absorption spectrum (λmax ) 310 nm)
and kinetic behavior.19
Evidence is presented herein for the formation of the corre-
sponding Lewis acid-base complexes as the primary initial
products of the reaction; the UV/vis spectra of the complexes
in dilute hexane solution are reported, along with equilibrium
constants and (in several cases) absolute rate constants for their
formation. Absolute rate constants for reaction of the two
alcohols with tetramethyl- and tetraphenyldigermene (Ge2Me4
Neumann and Satge and their co-workers reported product
studies of the reactions of dimethylgermylene (GeMe2) with
alcohols in solution and concluded that the reaction most likely
proceeds via the reversible formation of a relatively long-lived
germylene-alcohol complex,2
0-22
and Ge Ph ) have also been determined under the same
in agreement with the earlier
2
4
7
conditions.
conclusions of Ando and co-workers. No reliable kinetic data
yet exist on the reactions of transient germylenes with alcohols
in solution; while it has been variously reported that transient
dialkyl and diaryl derivatives react with simple alcohols at rates
that are too slow to be detected on the sub-millisecond time
scale,2
2-29
many of these reports are thought to be based on
30-33
erroneous transient assignments.
One exception is an early
time-resolved spectroscopic study of dimesitylgermylene (GeMes2)
from our own laboratory, in which we reported the species to
exhibit no detectable signs of reactivity toward ethanol in
solution.29 More recent experience with this and other transient
germylenes in solution has shown these species to be quite
reactive toward various other nucleophiles30-32 and has prompted
an examination of their reactivity with simple alcohols and
ethers, including a more detailed re-examination of the reactivity
of GeMes2 with substrates of this type.
Results and Discussion
Laser flash photolysis experiments were carried out on
deoxygenated solutions of 1a-c in hexane, using the pulses
from a KrF excimer laser (248 nm, ca. 25 ns, ca. 100 mJ) for
excitation and a flow system to replenish the sample cell
continuously between laser pulses. As reported previously,3
flash photolysis of these compounds in this solvent affords
promptly formed transient absorptions due to the corresponding
germylene (GeR2; λmax 475-560 nm), which decays with
second-order kinetics concomitantly with the growth of absorp-
tions due to the corresponding digermene (Ge2R4; λmax 370-
0-32
In the present paper, we report the results of a laser flash
photolysis study of the reactions of three transient germylene
derivativessdiphenyl- (GePh2), dimesityl- (GeMes2; Mes )
(
16) Steele, K. P.; Tzeng, D.; Weber, W. P. J. Organomet. Chem. 1982,
31, 291.
17) Shizuka, H.; Tanaka, H.; Tonokura, K.; Murata, K.; Hiratsuka, H.;
Ohshita, J.; Ishikawa, M. Chem. Phys. Lett. 1988, 143, 225.
4
40 nm). The absorption spectrum of GePh2 (λmax ) 500 nm)
2
overlaps significantly with that of Ge2Ph4 (λmax ) 440 nm), so
kinetic analysis of the GePh2 transient decays required correction
of the raw absorbance data by scaled subtraction of the
corresponding growth/decay profile for Ge2Ph4, obtained at 440
(
(
(
18) Levin, G.; Das, P. K.; Lee, C. L. Organometallics 1988, 7, 1231.
19) Levin, G.; Das, P. K.; Bilgrien, C.; Lee, C. L. Organometallics 1989,
8
, 1206.
20) Klein, B.; Neumann, W. P.; Weisbeck, M. P.; Wienken, S. J.
Organomet. Chem. 1993, 446, 149.
21) Neumann, W. P.; Weisbeck, M. P.; Wienken, S. Main Group Met.
Chem. 1994, 17, 151.
22) Barrau, J.; Bouchaut, M.; Lavayssiere, H.; Dousse, G.; Satge, J. J.
Organomet. Chem. 1983, 243, 281.
23) Mochida, K.; Wakasa, M.; Nakadaira, Y.; Sakaguchi, Y.; Hayashi,
H. Organometallics 1988, 7, 1869.
24) Konieczny, S.; Jacobs, S. J.; Braddock Wilking, J. K.; Gaspar, P.
P. J. Organomet. Chem. 1988, 341, C17.
25) Mochida, K.; Yoneda, I.; Wakasa, M. J. Organomet. Chem. 1990,
99, 53.
26) Mochida, K.; Wakasa, M.; Sakaguchi, Y.; Hayashi, H. Bull. Chem.
Soc. Jpn. 1991, 64, 1889.
27) Mochida, K.; Kikkawa, H.; Nakadaira, Y. J. Organomet. Chem.
991, 412, 9.
28) Bobbitt, K. L.; Maloney, V. M.; Gaspar, P. P. Organometallics 1991,
0, 2772.
29) Toltl, N. P.; Leigh, W. J.; Kollegger, G. M.; Stibbs, W. G.; Baines,
K. M. Organometallics 1996, 15, 3732.
30) Leigh, W. J.; Harrington, C. R.; Vargas-Baca, I. J. Am. Chem. Soc.
004, 126, 16105.
3
0,31
(
nm under identical instrumental conditions.
The spectra of
GeMe2 (λmax ≈ 475 nm) and GeMes2 (λmax ≈ 550 nm) are
(
sufficiently well separated from those of the corresponding
3
2,34
digermenes (Ge2Me4, λmax ) 370 nm;
Ge2Mes4, λmax ) 410
(
2
9,30,35
nm
) that their decay kinetics could be evaluated without
(
resorting to such corrections.
Addition of the alcohols or THF to hexane solutions of 1a-c
resulted in quenching of the germylene and digermene signals
in a manner consistent with reVersible reaction of the germylene
with the added substrate, as will be described in detail below.
The specific effects observed varied from system to system
according to the relative magnitudes of the “forward” rate and
equilibrium constants for reaction (kQ and Keq, respectively),
the secondary reactivities of both the primary reaction product
and the corresponding digermene toward further reaction, and
the magnitude of the rate constant for dimerization of the free
germylene. One feature that was common to all systems was
(
(
3
(
(
1
(
1
(
(
2
2
(
(
31) Leigh, W. J.; Harrington, C. R. J. Am. Chem. Soc. 2005, 127, 5084.
32) Leigh, W. J.; Lollmahomed, F.; Harrington, C. R. Organometallics
(34) Mochida, K.; Kayamori, T.; Wakasa, M.; Hayashi, H.; Egorov, M.
P. Organometallics 2000, 19, 3379.
(35) Masamune, S.; Hanzawa, Y.; Williams, D. J. J. Am. Chem. Soc.
1982, 104, 6136.
006, 25, 2055.
33) Harrington, C. R.; Leigh, W. J.; Chan, B. K.; Gaspar, P. P.; Zhou,
D. Can. J. Chem. 2005, 83, 1324.
(

5
426 Organometallics, Vol. 25, No. 22, 2006
Leigh et al.
) ) 1 + K [Q] (5)
the formation of new long-lived transient absorptions in the
90-360 nm range, which increased in intensity with increasing
(∆A
) /(∆A
Ge R ,max 0 Ge R ,max Q
SV
2
4
2 4
2
substrate concentration and could be clearly ascribed to the
primary products of reaction. These species are assigned to the
corresponding Lewis acid-base complexes 2-4 (eq 3) on the
basis of their spectroscopic and kinetic behavior (vide infra).
The relevant kinetic equations used to analyze the germylene
transient absorption data in the presence of a reversibly reacting
substrate Q are given in eqs 6-8, where kdecay is the pseudo-
first-order decay constant for approach to equilibrium with the
primary scavenging product, kQ and k-Q are the forward and
reverse rate constants for reaction, Keq is the equilibrium constant
()kQ/k-Q), ∆A0 and ∆At are the transient absorbance values
immediately and at time ) t after the laser pulse, respectively,
and ∆Ares is the transient absorbance due to free germylene
remaining after equilibrium is achieved and undergoing rela-
tively slow decay due to the dimerization reaction. It should be
noted that these equations describe the kinetics precisely only
in the limit where ∆Ares is nondecaying, which is never strictly
true. Nevertheless, we have shown previously that within certain
limitations analysis of the data in this way provides reasonably
accurate values of kQ and Keq for systems with Keq values in
The general mechanistic scheme employed for analysis of
the germylene transient absorption data is outlined in eq 4. We
begin by noting that in order for kinetic parameters associated
with reversible reaction of the germylene with a given substrate
to be measurable under the conditions of our experiments, one
needs to be above some threshold concentration at which the
rate of approach to equilibrium significantly exceeds that of
dimerization in the earliest stages of both reactions (i.e., at the
end of the laser pulse). Under these conditions the decay of the
3
1
the large or intermediate range.
∆At ) ∆A + (∆A - ∆A ) exp(-kdecayt)
(6)
(7)
(8)
res
0
res
kdecay ) k-Q + k [Q]
Q
∆
A0/∆Ares ) 1 + K [Q]
eq
The simplest situation is obtained when Keq is sufficiently
large that the concentration of free germylene remaining at
equilibrium is too small to be detected at any substrate
concentration, and the germylene absorption decays from its
initial value (∆A0) with clean pseudo-first-order kinetics to an
absorbance level indistinguishable from that before the laser
pulse (i.e., ∆Ares ≈ 0). Only the forward rate constant for
reaction (kQ) can be determined in such cases, but it can
nevertheless be determined with the same degree of precision
as those for irreversible reactions. Behavior of this type is
exhibited by the reaction of GePh2 and GeMe2 with aliphatic
germylene proceeds in two stages: a fast pseudo-first-order
component due to approach to equilibrium with the primary
scavenging product, and a slower second-order component due
to dimerization of residual free germylene at equilibrium with
the scavenging product. This threshold is determined (inter alia)
by the magnitude of the dimerization rate constant, which for
the three germylenes studied in this work varies between kdim
9
-1 -1
30
≈
5 × 10 M
s
for GeMes2 and the diffusion limit in the
10
-1 -1
case of GeMe2 (kdiff ≈ 2.1 × 10
M
s
in hexane at 25
3
0-32
amines.
3
2
°
C). Once this condition is satisfied, then the response that is
The systems studied in the present work were found to fall
actually observed takes on one of three basic forms depending
into either the intermediate-Keq regime (similar to that exhibited
-1
on whether Keq is large (i.e., Keq > ca. 25 000 M ), intermediate
3
1
by the reaction of GePh2 with isoprene ) or the small-Keq
regime, which we have encountered previously in a study of
the complexation of dimethylstannylene (SnMe2) with metha-
-
1
(
1
i.e., ∼1000 < Keq < 25 000 M ), or small (i.e., Keq < ca.
-
1
000 M ), given a “forward” reaction rate constant (kQ) on
9
-1 -1
the order of ca. 10 M
s
or greater and typical initial
3
6
nol. Both kQ and Keq can be estimated with reasonable
precision for systems in the intermediate-Keq regime, even
though the kinetic analysis is necessarily an approximate one.31
On the other hand, for those in the small-Keq regime only Keq
can be determined, because at concentrations high enough to
cause a measurable reduction in the amount of free germylene
remaining at equilibrium, the initial pseudo-first-order decay is
too fast to be resolved from the laser pulse. As a result, the
only effect observed upon addition of substrate is a reduction
in the apparent strength of the germylene signal relative to its
value in the absence of substrate; thus, at each substrate
concentration the measured ∆A0 value is actually that due to
the free germylene at equilibrium with the germylene-substrate
product (i.e., ∆A0 ) ∆Ares). The equilibrium constant is then
obtained from analysis of the initial germylene signal strengths
according to eq 9, where (∆A0)0 and (∆A0)Q are the initial
germylene transient absorbances in the absence and presence
of the substrate.
germylene concentrations of 10-20 µΜ. The prevailing feature
that distinguishes reversible reactions from irreversible ones is
the efficiency relative to dimerization, which can be easily
monitored because the dimerization reaction leads to its own
detectable signal: the transient absorption due to the corre-
sponding digermene. Qualitatively, reversible reactions are
distinguishable by the fact that dimerization remains detectable
even at substrate concentrations where the free germylene can
no longer be detected. Scavenging efficiency can be assessed
semiquantitatively by monitoring the peak intensity of the
digermene signal (∆AGe R ,max) as a function of scavenger
2
4
concentration under conditions of constant laser intensity,
according to eq 5. As we have shown previously,3 reversible
reactions are characterized by KSV values that are significantly
smaller than those for irreversible ones of similar forward rate
constant (kQ). A good deal of caution is required in interpreting
the results of these analyses however, because the magnitude
of KSV is also affected (inversely) by variations in laser intensity
and (directly) by the reactivity of the digermene toward the
1,32
(36) Becerra, R.; Harrington, C. R.; Gaspar, P. P.; Leigh, W. J.; Vargas-
3
1,32
added substrate.
Baca, I.; Walsh, R.; Zhou, D. J. Am. Chem. Soc. 2005, 127, 17469.

Reactions of Diaryl- and Dialkylgermylenes with Alcohols
∆A ) /(∆A ) ) 1 + K [Q]
Organometallics, Vol. 25, No. 22, 2006 5427
(
(9)
increasing THF concentration is due to the presence of reactive
impurities (such as water) in the sample of THF used in our
experiments. While we made every attempt to render it
anhydrous, there is no obvious reaction pathway involving the
ether itself that might otherwise account for the effect.
0
0
0 Q
eq
The kinetic details of the reactions of the three transient
germylenes with the three oxygen-centered nucleophiles studied
in this work varied quite significantly from system to system,
requiring slightly different methods for analysis of the data for
each of the germylenes studied. The data obtained for GePh2
in the presence of both alcohols and THF allowed extraction
of both the rate and equilibrium constants in all three cases,
and thus will be presented first.
Diphenylgermylene. In all three cases, addition of small
amounts of substrate to hexane solutions of 1a resulted in kinetic
behavior consistent with reversible scavenging in the intermedi-
ate-Keq regime; that is, the germylene decays (after scaled
subtraction of the underlying absorption due to Ge2Ph4) took
on a bimodal form at “low” substrate concentrations and could
be analyzed reasonably precisely according to eqs 6-8 within
certain concentration ranges. The response of the digermene
signals to added THF, MeOH, or t-BuOH varied with the
substrate, due to differences in the secondary reactivity of the
digermene toward the added reagent: kMeOH > kt-BuOH . kTHF.
Analysis of the germylene transient absorption data according
to eqs 6-8 (see Figure 1c) afforded values for the forward rate
9
-1 -1
and equilibrium constants of kQ ) (6.3 ( 0.6) × 10 M
s
-
1
and Keq ) 23 000 ( 5000 M . A plot of the relative peak
intensities of the Ge2Ph4 absorptions versus [THF] according
to eq 5 over the 0-0.6 M concentration range afforded KSV )
-1
6
.1 ( 0.4 M , which as mentioned above should be considered
an upper limit of the true value. Nevertheless, the ratio KSV/kQ
e1 ns) that is defined by these data is at least 3 orders of
(
magnitude smaller than those characteristic of formally irrevers-
ible reactions of GePh2 that we have studied previously, as
3
1
expected for a reversible reaction. Within certain limitations,
the KSV/kQ ratio provides a numeric indicator of the efficiency
of a scavenging reaction relative to dimerization, and the values
measured in the present work are the lowest that we have yet
encountered.
Figure 2 illustrates the behavior of the transient absorptions
due to GePh2 and Ge2Ph4 in the presence of MeOH. Bimodal
decay behavior was observed over a considerably broader range
in substrate concentration than what was observed with THF,
consistent with a significantly lower equilibrium constant for
reaction. While the effects of added substrate on the germylene
decay profiles are similar to those observed in the presence of
THF, quenching of digermene formation by the added alcohol
as measured by the reduction in the peak signal intensities due
to Ge2Ph4 in the presence of added alcohol) appears to be much
more efficient than is the case with THF; a value of KSV ) 660
60 M was obtained from a plot of the relative Ge2Ph4 signal
The scaling factor used for correction of the raw transient
absorption data for GePh2 (vide supra) was determined from
data recorded at 440 and 500 nm in hexane solution containing
1
1
mM THF, which reduces the lifetime of the germylene to ca.
45 ns but has minimal effects on the strength of the Ge2Ph4
signal or its growth/decay characteristics. The appropriate
scaling factor was then determined from the relative intensities
of the transient absorption versus time profiles for Ge2Ph4 at
(
4
40 and 500 nm; the procedure afforded a value for the scaling
factor of 0.15, which is simply the relative extinction coefficients
of the absorption due to the digermene at 500 and 440 nm.
Details of the experiment are shown in the Supporting Informa-
tion.
Representative growth/decay profiles for GePh2 and Ge2Ph4
in the presence of THF are shown in Figure 1. Residual
absorptions could be detected in the corrected GePh2 decays at
substrate concentrations up to 0.8 mM, above which they could
no longer be distinguished from the pre-pulse absorbance level
-1
(
intensities versus [MeOH] according to eq 5 (see Supporting
Information). The greater apparent efficiency is due to secondary
reaction of the digermene with MeOH, which leads to enhance-
ments in the decay rate of the digermene signals with increasing
substrate concentration and thus enhances the effect of the added
substrate on the peak signal intensities. The decaying portions
of the digermene growth/decay profiles (see Figure 2b) followed
clean pseudo-first-order kinetics in the presence of 1-5 mM
MeOH, and a plot of the decay constants (kdecay) versus [MeOH]
(Figure 1a). Rate constants for decay of the fast initial
component were measurable over the 0.2-2.2 mM range in THF
concentration. Figure 1b shows growth/decay profiles for Ge2-
Ph4, recorded under the same conditions as the germylene
decays, which illustrates that the presence of THF has minimal
effects on the yield of the digermene within this concentration
range. This suggests that there are two mechanisms for formation
of Ge2Ph4 under these conditions, one involving dimerization
of free GePh2 and one involving reaction of free GePh2 with
the primary scavenging product. In fact, the peak intensity of
the Ge2Ph4 signal increased somewhat in the presence of very
small amounts (0.05-0.2 mM) of THF, which can be attributed
to a significant lengthening of the decay time of the signal in
the presence of the ether. This effect is consistent with
suppression of one of the possible decay channels for the
digermene, most likely that involving reaction with free GePh2;
we presented kinetic evidence in an earlier paper that the decay
of Ge2Ph4 in the absence of reactive scavengers proceeds via
competing dimerization (on the long time scale) and reaction
7
according to eq 10 afforded a value of k ) (1.9 ( 0.4) × 10
Q
-
1
-1
M
s
for the absolute rate constant for quenching of the
digermene by the alcohol. Analysis of the germylene decays
according to eqs 6-8 over the 0.3-1.7 mM [MeOH] range
9
-1 -1
afforded values of k ) (6.1 ( 1.1) × 10 M
Q
s
and Keq )
-
1
3300 ( 800 M (see Figure 2c).
kdecay ) k + k [Q]
(10)
0
Q
With both THF and MeOH the effects described above were
accompanied by the formation of new transient absorptions
centered at 350-355 nm, which intensified with increasing
concentration of added substrate. Figure 3 shows transient
absorption spectra recorded in the presence of 2.1 mM THF
(a) and 5 mM MeOH (b), where the lifetime of the free
germylene was less than ca. 60 ns. Three spectra are shown in
each case, one recorded within 50 ns after the laser pulse (the
regions below 350-380 nm are obscured due to sample
fluorescence), one recorded ca. 100 ns after the pulse, and
another recorded ca. 3.5 µs later. In both cases, it is clear that
within 100 ns after excitation the characteristic spectrum of
GePh2 (λmax ) 500 nm) is replaced by that of a second species
(λmax ) 350-355 nm), whose subsequent decay is accompanied
30,31
with free GePh2 (on the short time scale).
The signal due to
the digermene decreased in intensity as the THF concentration
was increased further, but its formation could nevertheless still
be detected in the presence of THF in concentrations in excess
of 0.6 M (see Supporting Information). Presumably, the reduc-
tion in the apparent yield and lifetime of the digermene with

5428 Organometallics, Vol. 25, No. 22, 2006
Leigh et al.
Figure 1. (a) Corrected decay profiles for GePh
contributions due to competing absorption by Ge
2
in deoxygenated hexane solution containing 0-0.4 mM THF, after subtraction of the
4
2
Ph
on the same time scale (data of (b), × 0.15). The solid lines are the best fits of the
data to second- (0 mM) or first-order (0.2, 0.4 mM) kinetics. (b) Growth/decay profiles for Ge
Plots of kdecay (O) and ∆A /∆Ares (0) vs [THF] for GePh
2 4
Ph in the presence of 0-0.4 mM THF. (c)
0
2
.
Figure 2. (a) Corrected decay profiles for GePh
contributions due to competing absorption by Ge
or first-order (0.6, 1.7 mM) decay kinetics. (b) Growth/decay profiles due to Ge
O) and ∆A /∆Ares (0) vs [MeOH] for GePh
2
in deoxygenated hexane solution containing 0-1.7 mM MeOH, after subtraction of the
Ph on the same time scale. The solid lines are the best fits of the data to second- (0 mM)
Ph in the presence of 0-1.7 mM MeOH. (c) Plots of kdecay
2
4
2
4
(
0
2
.
Figure 3. (a) Transient absorption spectra from laser flash photolysis of GePh
6-48 ns ([), 112-144 ns (O), and 3.36-3.47 µs (0) after the laser pulse; the inset shows transient decay profiles recorded at monitoring
wavelengths of 360, 440, and 500 nm. (b) Transient absorption spectra in hexane solution containing 5.0 mM MeOH, recorded 32-48 ns
[), 90-116 ns (O), and 3.3-3.5 µs (0) after the laser pulse; the inset shows a representative transient decay trace recorded at 350 nm.
2
precursor 1a in hexane containing 2.1 mM THF, recorded
1
(
by the formation of Ge2Ph4 (λmax ) 440 nm) on roughly the
same time scale. The second-formed species are assigned to
the Lewis acid-base complexes 2c and 2a, respectively (eq 3).
The absorption maxima of these species in dilute hexane solution
at ambient temperatures lie ca. 25 nm to the red of the values
reported by Ando and co-workers for the complexes of GePh2
with 2-methyltetrahydrofuran and ethanol in a hydrocarbon glass
at 77 K.7
Inspection of the signals due to 2a on shorter time scales
revealed them to grow in over the first 30-60 ns after the laser
pulse at low (e5 mM) MeOH concentrations; they were
unresolvable from the laser pulse at higher concentrations where
the germylene’s decay was also too rapid to be detected. Pseudo-
first-order rate constants for the growth of the species were
estimated from growth/decay profiles recorded over the 0.6-5
mM range in MeOH concentration, and a plot of kgrowth versus
[MeOH] analogous to eq 10 was linear (see Supporting
9
Information). The slope of the plot, kQ ) (3.7 ( 0.3) × 10
-
1
-1
M
s , is in reasonable agreement with the value of kQ
estimated above from the analysis of the corrected germylene
decays at 500 nm. The species decays with clean second-order
kinetics under these conditions (see inset; Figure 3b), with the
concomitant growth of the characteristic absorptions due to Ge2-
Ph4.
Exactly analogous behavior was observed in the presence of
t-BuOH (see Supporting Information), and analysis of the data
9
-1 -1
as above led to values of kQ ) (4.8 ( 1.6) × 10 M s , Keq
-
1
-1
) 800 ( 400 M , and KSV ) 163 ( 16 M , while analysis
of the digermene decays in the presence of 4-20 mM t-BuOH
6
-1 -1
afforded a value of kQ ) (2.1 ( 0.5) × 10 M s . The

Reactions of Diaryl- and Dialkylgermylenes with Alcohols
Organometallics, Vol. 25, No. 22, 2006 5429
spectrum of the Ph2Ge-t-BuOH complex (2b) exhibited λmax
)
340 nm in hexane containing 5 mM t-BuOH; the species
again decayed with kinetics similar to those of the growth of
the digermene absorption. It should be noted that the plot of
the ∆A0/∆Ares data predicts an intercept significantly greater
than unity. This is most likely due to overestimation of the
absorbance ratios at the lower concentrations, where it is more
difficult to distinguish the fast initial decay from the slower
residual one than at higher substrate concentrations, where the
initial decay is faster and the residual decay is slower. A value
In addition, the peak intensities of the digermene signals
increased quite significantly upon addition of small concentra-
tions of the three substrates (due to a lengthening of the decay
time of the signal) and then decreased in the expected fashion
as the concentration was increased further. As we indicated
above, the increases in digermene signal strength at low substrate
concentrations are consistent with suppression of one of the
possible decay channels for the digermene, most likely that
involving reaction with free GeMes2. Considerably higher
concentrations of added substrate were required in order to elicit
these effects compared to those required in the experiments with
GePh2. Nevertheless, the observed reductions in the strength
of the germylene and digermene signals were clearly coupled
to the formation of new transient absorptions assignable to the
Mes2Ge-substrate complexes, the spectra of which are in
reasonably good agreement with those reported by Ando et al.
for the complexes of GeMes2 with 2-methyltetrahydrofuran and
-
1
of Keq ) 1000 ( 250 M was obtained when the analysis was
restricted to the two highest concentration data points and the
unity intercept predicted by eq 6.
The data indicate there to be only slight variation in the
forward rate constant for complexation of GePh2 with the
O-donors studied in this work, with those for complexation with
THF and MeOH being slightly higher than that for t-BuOH.
The complexation reaction is very fast, proceeding within a
factor of 4 of the diffusion limit in hexane solution in all three
cases. The main variable is the equilibrium constant, which
decreases in the order KTHF ≈ 8KMeOH ≈ 25Kt-BuOH and thus
appears to reflect both electronic and steric effects of substitution
in the substrate on the thermodynamic stabilities of the
complexes. The greater stability of the THF complex compared
to those with the alcohols can be attributed to a greater degree
of electronic stabilization of positive charge at oxygen and is
in keeping with the higher gas-phase proton affinity of THF
compared to MeOH and t-BuOH.37 A similar analysis would
predict that t-BuOH should form a stronger complex than
MeOH, so the fact that it does not most likely reflects steric
destabilization in the complex involving the bulkier alcohol.
The fact that the Ph2Ge-ROH complexes decay with clean
second-order kinetics indicates that digermene formation is the
main mode of decay of these species under the conditions of
our experiments; further reaction of the complex to yield the
net insertion product proceeds much more slowly than dissocia-
tion to and subsequent formation of the digermene from the
free germylene. As we concluded in the case of THF, our data
indicate that the digermene is formed via two competing routes,
one involving dimerization of free GePh2 and one involving
reaction of free GePh2 with the Ph2Ge-ROH complex (see eq
7
ethanol in hydrocarbon matrixes at 77 K. The results are
broadly consistent with scavenging in the small-Keq regime as
discussed above, and so the transient absorption data for GeMes2
were analyzed according to the model defined by eq 9.
Figure 4 illustrates the effects of added MeOH on the transient
absorptions due to GeMes2 and Ge2Mes4, showing (in Figure
4a) the steady reduction in signal strength for the GeMes2
absorption with increasing [MeOH] and the corresponding
changes in the strength of the digermene absorption (in Figure
4b), starting with an initial increase at low concentration
followed by a steady decrease as the concentration is increased
to higher levels. Figure 4c shows the plot of the relative initial
strengths of the GeMes2 signals versus [MeOH] according to
eq 9. Of particular interest is the fact that the latter plot exhibits
positive curvature, indicating a mixed order dependence of the
intensity ratios on alcohol concentration. One possible inter-
pretation of such a result is that GeMes2 forms higher order
complexes with MeOH in addition to that with the 1:1
stoichiometry. The interpretation is complicated somewhat by
the fact that in hexane solution the monomeric form of methanol
exists in mobile equilibrium with the hydrogen-bonded dimer
and higher oligomers; the equilibrium constants are such that
the concentration of the monomeric form decreases from ca.
90% of the nominal bulk concentration at 0.01 M MeOH to ca.
1
1); once formed, Ge2Ph4 undergoes secondary reaction with
31
ROH to afford the 1,2-addition product. In the case of THF,
a third possible pathway involving dimerization of the complex
can be ruled out on the basis of the fact that formation of the
digermene is eventually suppressed as the substrate concentra-
tion is increased to high levels. It is more difficult to address
this possibility in the cases of the alcohols, because our ability
to detect the digermene at high substrate concentrations is
reduced owing to its secondary reaction with the alcohols. The
present data do not provide any information on the mechanism
for the formation of the final (alkoxygermane) product, except
that the germylene-alcohol complex is a crucial intermediate
in the overall process and that its transformation to alkoxyger-
mane via proton transfer is much slower than digermene
formation under the conditions of our experiments.
3
8
50% at 0.1 M at 20 °C. Nevertheless, this demands that if
GeMes2 formed only a 1:1 complex with MeOH, then the plot
of Figure 4c should exhibit negative rather than positive
curvature. In any event, a quadratic fit of the data of Figure 4c
-
1
defines a limiting slope of Keq ) 15 ( 6 M as [MeOH] f 0,
as an estimate of the equilibrium constant for formation of the
putative 1:1 complex with MeOH. The plot of the relative
digermene peak signal intensities versus [MeOH] is similarly
curved (see Supporting Information) and is characterized by a
Dimesitylgermylene. Very different behavior was observed
in flash photolysis experiments with the GeMes2 precursor (1b),
the main feature being that addition of the alcohols or THF
resulted only in successive reductions in the peak signal
intensities due to the germylene with increasing substrate
concentration and had no discernible effect on its decay kinetics.
-
1
limiting slope of KSV ) 3 ( 2 M as [MeOH] f 0.
Similar effects were observed in flash photolysis experiments
with 1b in the presence of THF and t-BuOH, although
considerably higher concentrations of added substrate were
required before changes in the signal characteristics could be
(
37) Anslyn, E. V.; Dougherty, D. A. Modern Physical Organic
Chemistry; University Science Books: New York, 2005; pp 259-296.
(38) Landeck, H.; Wolff, H.; Goetz, R. J. Phys. Chem. 1977, 81, 718.

5430 Organometallics, Vol. 25, No. 22, 2006
Leigh et al.
Figure 4. Growth/decay profiles for (a) GeMes
wavelengths of 550 and 410 nm, respectively; (c) plots of (∆A
2
and (b) Ge
2
Mes
4
in hexane containing 0-0.09 M MeOH, determined at monitoring
0 Q
0
)
0
/(∆A ) for the germylene (O) signals vs [MeOH].
Figure 5. Transient absorption spectra recorded in hexane containing (a) 0.25 M t-BuOH, 0.16-0.48 µs (O) and 35.7-36.0 µs (0) after
the laser pulse, and (b) 2.55 M t-BuOH, 0.13-0.26 µs (O) and 35.6-35.9 µs (0) after the laser pulse. The insets show decay/growth
2
profiles recorded at monitoring wavelengths of 280, 410, and 550 nm. The spectrum of GeMes in deoxygenated hexane (- - -), scaled to
match the intensities of the 550 nm absorption band under the two sets of conditions, is also shown.
observed. Plots of the relative initial intensities of the GeMes2
absorptions versus substrate concentration (eq 9) were linear
in both cases and afforded values of Keq ) 1.1 ( 0.2 and 3.7
0.25 M; Figure 5a) the 330 nm absorption might appear to be
due to GeMes2 alone, the spectra at higher concentrations (e.g.,
2.5 M; Figure 5b) clearly show that another species is present,
which exhibits absorption bands centered at λmax ) 290 and
330 nm.
-1
(
0.2 M for THF and t-BuOH, respectively. Complete details
of the data obtained for the Mes2Ge-THF and Mes2Ge-BuOH
systems are provided in the Supporting Information. Interest-
ingly, the KSV values for all three Mes2Ge-substrate systems
are remarkably close to the corresponding Keq values. We
interpret this as indicating that the additional pathway for
formation of the digermene that was proposed in the cases of
the GePh2 systems, involving reaction of the free germylene
with the germylene-substrate complex, is much slower relative
to that involving dimerization of the free germylene than is the
case with the less hindered GePh2.
-1
From the value of Keq that characterizes this system (∼4 M )
and eq 8, the free germylene and 3b are predicted to be present
in roughly equal amounts in the presence of 0.25 M t-BuOH,
and in a ratio of ca. 1:10 in the presence of 2.5 M of the alcohol.
The insets in Figure 5a,b demonstrate that the complex
(monitored at 280 nm) decays on a similar time scale as the
decay of free GeMes2 and the growth of the signal due to Ge2-
Mes4 under both sets of conditions, consistent with the free
germylene and 3b existing in mobile equilibrium and being
consumed together as dimerization proceeds. Analogous be-
havior was observed for hexane solutions of 1b containing 0.1
M MeOH and 1-3 M THF, data for which are included in the
Supporting Information. In these two cases, spectral subtraction
was required in order to extract the spectra of the corresponding
complexes, because the long-wavelength bands are somewhat
broader and more diffuse than is the case for the Mes2Ge-t-
BuOH complex. Nevertheless, the spectra obtained appear to
be in good agreement with those reported by Ando and co-
workers for the complexes of GeMes2 with 2-methyltetrahy-
Discrete absorptions assignable to the corresponding Lewis
acid-base complexes (3a-c) were more difficult to detect for
GeMes2 in dilute hexane solution than was the case with GePh2.
This was found to be due to significant overlap between the
S0fS2 transition of free GeMes2 (λmax ) 325 nm)3 and the
S0fS1 transitions of the complexes, which are expected to fall
in the 330-360 nm range on the basis of the spectra reported
by Ando and co-workers for GeMes2 in neat 2-methyltetrahy-
drofuran and alcohol matrixes at 77 K7 and the results
presented above for GePh2. Nevertheless, transient spectra
recorded in the presence of relatively high concentrations of
MeOH and t-BuOH showed clear evidence of the presence of
the respective complexes. For example, Figures 5a and 5b show
transient spectra recorded at similar time delays after the laser
pulse for hexane solutions of 1b containing 0.25 and 2.5 M
t-BuOH, along with the spectrum of GeMes2 in hexane without
added alcohol. While at low concentrations of t-BuOH (e.g.,
0
,39
7
drofuran and ethanol at 77 K.
While the forward rate constants for complexation (kQ) could
not be determined in these cases, we can estimate that minimum
8
-1 -1
values on the order of 10 M
s
would be required to produce
the behavior that was actually observed, given equilibrium
-
1
constants in the range 1-10 M and the maximum time
resolution of our system. The true values could very well be
9
-1 -1
closer to 10 M s , on the basis of the values of kQ ()(4-6)
(
39) Ando, W.; Itoh, H.; Tsumuraya, T.; Yoshida, H. Organometallics
9
-1 -1
1
988, 7, 1880.
× 10 M s ) determined above for GePh2 and the fact that

Reactions of Diaryl- and Dialkylgermylenes with Alcohols
Organometallics, Vol. 25, No. 22, 2006 5431
GeMes2 reacts with other nucleophiles (i.e., n-butyl amine and
acetic acid) with rate constants roughly half those exhibited by
GePh2.30 On the other hand, the present data indicate the
equilibrium constants for reaction of GeMes2 with the three
substrates to be as much as 4 orders of magnitude lower than
the corresponding values for GePh2. The trends in Keq as a
function of substrate also differ for the two germylenes, with
the value for THF complexation being smallest in the case of
GeMes2 and largest in the case of GePh2. This can be attributed
to a greater sensitivity of the THF complexes to steric
destabilization compared to those with the alcohols, to such an
extent that it overrides the greater degree of electronic stabiliza-
tion of positive charge at oxygen that the second alkyl
substituent in the ether would normally afford.
In contrast to one of the conclusions of our own earlier study
Figure 6. Transient absorption spectra of a solution of 1c in hexane
containing 15.4 mM THF, recorded 28-190 ns (O) and 8.58-
29,40
of GeMes2 in hydrocarbon solution,
the results reported here
2
8.69 µs (0) after the laser pulse. The spectrum of GeMe in hexane
for GeMes2 clearly indicate that the species reacts quite rapidly
with aliphatic alcohols in solution, albeit reversibly and with
such unfavorable equilibrium constants that the reaction pro-
duces no discernible effect on the decay kinetics of the
germylene under the typical conditions of laser flash photolysis
experiments; the signal simply grows weaker as the substrate
concentration is increased until it can no longer be detected at
all.
solution (- - -) is included for comparison, while the inset shows
transient growth/decay profiles recorded at 300 nm (bold) and 370
nm (regular).
for purposes of comparison. The early spectrum shows evidence
of new, broad absorptions centered at λmax ) 310 nm, which
decay over the first few microseconds after excitation with the
concomitant growth of the spectrum of Ge2Me4 (λmax ) 370
nm). The spectrum is assigned to the Me2Ge-THF Lewis acid-
base complex (4c). The inset in the figure shows transient signals
recorded at 300 and 370 nm, illustrating the decay of the 310
nm species and the concomitant growth of the signal due to
Ge2Me4. Interestingly, the peak intensity of the Ge2Me4 absorp-
tion increased more or less continuously over the 0.2-45 mM
concentration range in added THF, in contrast to the behavior
observed with the arylated systems. This may be partly due to
better control of reactive impurities (such as water) in the sample
of THF used for the experiments with the dialkylgermylene, as
this is the behavior that would actually be expected for a
substrate that cannot react productively with either the germylene
or its dimer. The other contributing factor is the laser intensity,
which was significantly higher in this experiment than in most
of the others. Saturation of the solution with air had no
discernible effect on the transient decays throughout the
monitoring range studied, nor on the transient spectra of Figure
Dimethylgermylene. The reactivity of GeMe2 toward the
three substrates proved to be much more difficult to quantify
than was the case with the diarylgermylenes, because the
dialkylgermylene is a significantly weaker absorber than the
aryl derivatives (hence producing weaker transient signals),
dimerization is significantly faster, and the equilibrium constants
proved to be significantly smaller than those of GePh2. Kinetic
behavior similar to that presented above for GePh2 was clearly
evident in the data recorded for the Me2Ge-THF system; the
free germylene decayed with bimodal kinetics at low THF
concentrations (0.2-1.1 mM) and could not be detected at all
at concentrations in excess of 2.5 mM, with little accompanying
effect on the peak intensities of the digermene absorptions other
than a slight increase in intensity and a lengthening of the decay
time. There was also a systematic drop in the initial signal
intensity of the germylene absorption with increasing substrate
concentration, which is due to problems of inadequate time
resolution; this presented particular difficulties in the determi-
nation of the equilibrium constant. A plot of the kdecay values
obtained from analysis of the raw germylene decay profiles over
the 0.1-1.1 mM range afforded an estimate of kQ ) (10.5 (
6
.
The effects of added MeOH and t-BuOH on the transient
absorptions due to GeMe2 proved to be rather more similar to
what was observed with GeMes than with GePh ; complete
9
-1 -1
2
.2) × 10 M
s
for the forward rate constant. Analysis of
2
2
details are provided in the Supporting Information. With MeOH
as substrate, the germylene decays appeared to take on a bimodal
form over the 1-4.2 mM concentration range, but the slower
of the two decay components remained sufficiently fast that
the ∆A0/∆Ares versus [THF] data according to eq 8 afforded a
-
1
value of Keq ) 4400 ( 900 M when the ∆A0 values at each
concentration were taken directly from the least-squares analyses
of the decay profiles; this analysis afforded an intercept of ca.
-
1
the approximate treatment used for estimation of kQ and Keq
4
, however. A value of Keq ) 9800 ( 3800 M was obtained
for the GeMe2-THF and GePh2-substrate systems could not
when the analysis was restricted to the three highest concentra-
tion data points and the unity intercept was included, and
employing the ∆A0 value obtained in the absence of added
scavenger as a constant at all concentrations. We believe the
higher value of Keq to be the more realistic estimate. Examples
of decay/growth profiles and the resulting data plots are shown
in the Supporting Information.
Transient absorption spectra recorded in the presence of 15
mM THF, where the lifetime and concentration of residual free
GeMe2 were too small for its signal to be detected, are shown
in Figure 6, along with a spectrum of GeMe2 in pure hexane
be applied. A fast component could not be discerned at all in
transient decays recorded in the presence of higher concentra-
tions of added alcohol; all that was observed was the ca. 2 µs
decay due to residual dimerization, with an apparent initial
intensity that decreased between 5 and ca. 10 mM MeOH until
it could no longer be detected. An estimate of Keq was thus
obtained from the initial absorbance values of the slow decay
component, which were estimated by eyeball extrapolation of
data recorded in the presence of 3-6 mM MeOH and plotted
according to eq 9 (using the value of (∆A0)0 from the decay
recorded in the absence of MeOH). The analysis afforded an
-
1
estimate of Keq ) 900 ( 60 M for the equilibrium constant.
(40) The cause of the error is unknown. W.J.L. apologizes for the
-
1
misdirection, particularly to his co-authors on ref 29.
A value of KSV ) 105 ( 16 M was obtained from a plot of

5
432 Organometallics, Vol. 25, No. 22, 2006
Leigh et al.
Table 1. Absolute Rate and Equilibrium Constants for
Reaction of Transient Germylenes with Alcohols and THF in
Deoxygenated Hexane Solution at 25 °C and UV/Vis
the peak signal intensity ratios for Ge2Me4 over the 0-6 mM
concentration range in this experiment; again, the intensity of
the digermene signal increased slightly at the lower end of the
concentration range and then decreased in the expected fashion
as the concentration was increased further.
Absorption Maxima of the Resulting Germylene-Substrate
a
Complexes (2-4; see eq 3) in Dilute Hexane Solution
germylene
GePh2
THF
kQ/10 M-1s-1 6.3 ( 0.6
MeOH
t-BuOH
Transient absorption spectra recorded in hexane containing
4 mM MeOH at lower laser intensities showed a single
9
6.1 ( 1.1
4.8 ( 1.6
5
-
1
Keq/M
23 000 ( 5000 3300 ( 800 1000 ( 250
transient species, which absorbs with λmax ≈ 295 nm and decays
with complex kinetics over a time scale of several tens of
microseconds (see Supporting Information). It should be noted
that the species exhibits completely different temporal behavior
from the long-lived absorption at ca. 290 nm that is present in
the transient spectra of 1c in pure hexane solution;32 the latter
is thought to be due to GeMe2 oligomerization products and is
in any event not associated with free GeMe2. It is thus clear
that the 295 nm species is due to the presence of the alcohol,
and it is thus assigned to the Me2Ge-MeOH complex (4a).
With higher excitation laser intensities, formation of the
digermene remained readily detectable in the presence of up to
-
1
KSV/M
6.1 ( 0.4
355
b
1.2 ( 0.2
1.9 ( 0.6
285, ∼360
660 ( 60
350
163 ( 16
340
2
λmax /nm
GeMes2 k /10 M s-1
9
-1
b
b
Q
-
1
c
Keq/M
15 ( 6
3.7 ( 0.2
1.6 ( 0.2
-
1
3 ( 2c
KSV/M
3
λmax /nm
285, ∼330 290, ∼330
kQ/10 M s-1 10.5 ( 2.2
9
-1
GeMe2
b
b
-1
Keq/M
9800 ( 3800
d
900 ( 60
105 ( 16
∼295
335 ( 50
82 ( 25
300
-
1
KSV/M
4
λmax /nm
310
a Errors are reported as twice the standard deviation obtained from linear
least-squares analysis of transient absorption data according to eqs 6-9;
the spectra of the complexes were recorded in dilute hexane solution
containing 0.01-2.5 M of the added substrate (see text), depending on the
4
5 mM MeOH, and its signals decayed with reasonably clean
b
c
d
system. Could not be determined. Limiting slope as [MeOH] f 0. Not
pseudo-first-order kinetics over the 10-45 mM range in added
alcohol. A plot of the rate constants for decay of the digermene
according to eq 10 was linear (see Supporting Information) and
determined.
with lowest energy absorption maxima in the 340-355 nm range
for GePh , ca. 325-360 nm for GeMes , and 295-310 nm for
6
-1 -1
afforded a value of kQ ) (2.7 ( 0.8) × 10 M
s
for the
2
2
GeMe2 in dilute hexane solution. There are generally only slight
differences in the absorption maxima of the complexes of a
given germylene with the three O-donors studied in this work,
and the absorption maxima of the complexes with GePh2 and
GeMes2 are similar to those reported previously in hydrocarbon
rate constant for reaction of Ge2Me4 with MeOH. We consider
the value to be in satisfactory agreement with the data reported
by Mochida and co-workers for the reaction of Ge2Me4 with
ethanol in cyclohexane, which were recorded over a much
broader range in alcohol concentrations and exhibited a non-
linear dependence of the digermene decay rate constant on
alcohol concentration.34
7
matrixes at 77 K. The spectrum of the Me2Ge-THF complex
is quite similar to that reported for the Me Si-THF complex
2
under similar experimental conditions, as is the absolute rate
The results obtained upon addition of t-BuOH were similar
to those obtained with MeOH, except no hint of bimodal decay
kinetics could be discerned in the germylene decays at any
19
constant for its formation as well. The main difference between
the silicon and germanium systems lies in the relative thermo-
dynamic stabilities of the resulting complexes. The silylene
complex enjoys much greater thermodynamic stability than the
corresponding germylene complex; in contrast, the activation
barriers for formation of the silylene and germylene complexes
are evidently quite similar and also quite small.
concentration within the range in which they could be detected.
A value of Keq ) 335 ( 50 M-1 was obtained for the
equilibrium constant from analysis of the germylene absorption
intensities over the 1-6 mM range in added alcohol, while KSV
)
intensities in the 0-4 mM concentration range. A transient
spectrum recorded in the presence of 8 mM t-BuOH again
showed enhanced prompt absorptions in the 290-350 nm range,
which decayed with the concomitant growth of the absorptions
-
1
82 ( 5 M was estimated from the digermene signal
Correlations have been noted previously between the positions
of the absorption maxima of the complexes of silylenes and
germylenes with various Lewis bases and the “strength” of the
6
,7
complex. This may be valid for the complexes of a variety
of substrates with a single metallylene, but the equilibrium
constants and spectral data presented in this work make it clear
that it is not valid for complexes of different germylenes with
the same Lewis base. The difference between the energies of
the lowest energy electronic transitions of the free and com-
t
due to Ge2Me4 and are thus assigned to the Me2Ge- BuOH
complex (4b). Representative data are shown in the Supporting
Information. Addition of the alcohol also caused reductions in
the lifetime of Ge2Me4, and a plot of kdecay versus [t-BuOH]
over the 0.01-0.1 M range in added alcohol was linear,
5
-1 -1
plexed germylene is significantly larger for GeMe2 than GePh2
affording a value of kQ ) (5 ( 1) × 10 M
s
for the absolute
in every case, in spite of the fact that the equilibrium constants
are uniformly larger for the diarylgermylene. Similarly, GeMes2
rate constant for reaction of Ge2Me4 with t-BuOH. The value
is again in satisfactory agreement with that reported for the same
34
and GePh exhibit spectral shifts of similar magnitudes upon
reaction in cyclohexane solution by Mochida and co-workers.
2
complexation, in spite of the fact that the latter forms consider-
ably stronger complexes with each of the three O-donors.
Interestingly, our results suggest that GeMes2 forms 1:2 and
perhaps even higher order complexes with methanol, in prefer-
ence to the 1:1 complexes that the data indicate to be formed
with the more reactive germylenes GePh and GeMe .
Overview and Conclusions
The rate and equilibrium constants determined in this work
for the reactions of GePh2, GeMes2, and GeMe2 with THF,
MeOH, and t-BuOH in dilute hexane solution are summarized
in Table 1, along with the absorption maxima of the germylene-
substrate complexes. The trends in the data can be summarized
as follows.
The data indicate that reaction of all three germylenes with
the three substrates proceeds rapidly and reversibly to generate
the corresponding germylene-O-donor Lewis acid-base com-
plexes, which are readily detectable as discrete transient species
2
2
Absolute rate constants have been determined for complex-
ation of GePh with all three substrates and of GeMe with THF,
2
2
9
-1 -1
and vary over the narrow range (4-10) × 10 M s ; the
rate constants are within a factor of 5 of the diffusion limit in
hexane at 25 °C. Even though absolute rate constants could not
be determined for any of the three reactions of GeMes2 or for
those of GeMe2 with the two alcohols, it is clear that they must

Reactions of Diaryl- and Dialkylgermylenes with Alcohols
Organometallics, Vol. 25, No. 22, 2006 5433
be of similar magnitudes to those that could actually be
measured. This inference can be made on the basis of the fact
that the reactions of GeMe2 with a wide variety of other
substrates proceed consistently a factor of ca. 2 faster than the
corresponding reactions of GePh2;3 the rate constants for
complexation with THF follow the same trend. There are fewer
data available on which to base similar comparisons between
GeMes2 and GePh2, but those that do exist show that GeMes2
is generally only 2-3 times less reactive than GePh2 under
comparable conditions. In any event, the behavior observed for
GeMes2 in the present work requires forward rate constants for
Table 2. Absolute Rate Constants for Reaction of MeOH
2 4 2 4
and t-BuOH with Ge Me and Ge Ph in Hexane Solution at
2
5 °Ca
6
-1
kt-BuOH/10 M s-1
6
-1
digermene
kMeOH/10 M s-1
2
Ge Me4
Ge2Ph4
2
2.7 ( 0.8
19 ( 4
0.52 ( 0.15
2.1 ( 0.5
a
Errors reported as (2σ.
The absolute rate constants for reaction of Ge2Ph4 and Ge2-
Me4 with MeOH and t-BuOH under the conditions of our
experiments are summarized in Table 2. The reaction of both
digermenes with MeOH has been shown to yield the formal
8
-1 -1
complexation of at least 10 M s .
3
0,34
1
,2-addition products 5 (eq 12),
and it is reasonable to
For GePh2 and GeMe2, the stabilities of the germylene-O-
donor complexes vary in the order THF > MeOH > t-BuOH.
The variation reflects the higher Lewis basicity of the ether
compared to those of the alcohols, which presumably results
from a greater ability to stabilize positive charge on oxygen in
the ether complex through electronic effects. In contrast, THF
forms the least stable complex of the three with GeMes2,
presumably reflecting a greater sensitivity to steric effects on
the stability of the ether complexes compared to those with the
alcohols. GePh2 generally forms slightly more stable complexes
than GeMe2, in keeping with the greater stabilization of negative
charge at germanium that is afforded by phenyl compared to
alkyl substituents.
presume that the reactions with t-BuOH proceed analogously.
The reactivities of the two digermenes with MeOH follow the
same trend as that reported previously for reaction with amines
3
1,32
and opposite that for addition of acetic acid.
rates for both amine and alcohol addition thus correlate with
The relative
32
the relative LUMO energies of the two digermenes, consistent
with either a concerted mechanism or a two-step one involving
initial nucleophilic attack at germanium. The rate constants for
MeOH addition are greater than those for t-BuOH addition in
both cases and by similar amounts. Unlike the germylenes from
which they are formed, none of the digermenes studied in this
work show evidence in their UV/vis absorption spectra of
significant complexation with THF.
The data verify inferences made previously on the basis of
7
low-temperature spectroscopic results, that the O-H insertion
reaction of germylenes with alcohols proceeds via a stepwise
mechanism involving the initial formation of the corresponding
Lewis acid-base complex. It is clear that the second step, proton
transfer from oxygen to germanium, constitutes the rate-
determining step in the overall reaction pathway. The results
are consistent with recent theoretical calculations for the (gas-
phase) reaction of GeMe2 with water, which indicate an overall
activation barrier on the order of 15 kcal mol , with formation
of the initial complex proceeding exothermically by a similar
amount.9
Future work will explore the reactivity of transient ger-
mylene-O-donor complexes in the neat liquids, further ad-
dressing the mechanism of the O-H insertion reaction of
germylenes with alcohols and exploring other facets of ger-
mylene reactivity in complexing solvents.
-1
The mechanism for the proton migration/transfer process that
takes the initially formed complex to the final product cannot
be addressed on the basis of the results reported here, but it is
nonetheless possible to define some limits. For forward rate and
Experimental Section
The germacyclopentenes 1a-c were synthesized and purified
30,32
as described previously.
Hexanes (EMD Omnisolv) for laser
9
-1 -1
equilibrium constants for complexation of ca. 4 × 10 M
s
flash photolysis experiments was dried by refluxing for several days
under argon over sodium/potassium amalgam followed by distil-
lation, or by passing the solvent through activated alumina (250
mesh; Sigma-Aldrich) under nitrogen using a Solvtek solvent
purification system. Methanol and tert-butanol were both spectro-
photometric grade and used as received from Sigma-Aldrich
Chemical Co. Tetrahydrofuran (Caledon Reagent) was also dried
by passage through activated neutral alumina (250 mesh; Aldrich)
under nitrogen.
-
1
and ca. 2000 M , respectively, the unimolecular rate constant
for dissociation of the complex can be calculated to be on the
6
-1
order of 2 × 10 s . The rate constant for unimolecular proton
migration within the complex must clearly be at least 2 orders
of magnitude slower than this, to account for the fact that the
germylene-alcohol complexes are observed at all in our
experiments. It seems most likely that the dominant mechanism
for the second step in solution involves catalytic proton transfer,
in which a second molecule of alcohol serves as the catalyst.
This possibility, as well as the potential for catalysis by stronger
acids and bases, will be addressed in a future paper. In dilute
solution under the conditions of high-intensity laser excitation,
the dominant fate of germylene-alcohol complexes is the
formation of the corresponding digermene, which our data for
GeMe2 and GePh2 indicate proceeds via two competing mech-
anisms: dimerization of residual free germylene in equilibrium
with the complex and reaction of the complex with the free
germylene. Digermene formation is eliminated when the initial
concentration of the germylene is reduced or in the presence of
high concentrations of alcohol, which indicates that it does not
proceed via a pathway involving dimerization of the ger-
mylene-alcohol complex.
Laser flash photolysis experiments employed the pulses from a
Lambda Physik Compex 120 excimer laser, filled with F /Kr/Ne
2
(
248 nm; ∼25 ns; 100 ( 5 mJ) mixtures, and a Luzchem Research
mLFP-111 laser flash photolysis system, modified as described
previously.30 Solutions were prepared at concentrations such that
the absorbance at the excitation wavelength was between ca. 0.7
and 0.9 and were pumped continuously through a vacuum oven-
dried thermostated 7 × 7 mm Suprasil flow cell connected to a
calibrated 100 mL reservoir, fitted with a glass frit to allow bubbling
of argon gas through the solution for at least 30 min prior to and
then throughout the duration of each experiment, using a Masterflex
7
7390 peristaltic pump fitted with Teflon tubing (Cole-Parmer
Instrument Co.). The glassware, sample cell, and transfer lines were
dried in a vacuum oven at 65-85 °C before use. Solution
temperatures were measured with a Teflon-coated copper/constantan

5434 Organometallics, Vol. 25, No. 22, 2006
Leigh et al.
thermocouple inserted into the thermostated sample compartment
in close proximity to the sample cell. Reagents were added directly
to the reservoir by microliter syringe as aliquots of standard
solutions. Transient decay and growth rate constants were calculated
by nonlinear least-squares analysis of the absorbance-time profiles
using the Prism 3.0 software package (GraphPad Software, Inc.)
and the appropriate user-defined fitting equations, after importing
the raw data from the Luzchem mLFP software. Rate constants
were calculated by linear least-squares analysis of decay rate-
concentration data (generally 4-7 points) that spanned as large a
range in transient decay rate as possible. Errors are quoted as twice
the standard deviation obtained from the least-squares analyses.
Acknowledgment. We thank the Natural Sciences and
Engineering Research Council of Canada for financial support,
Teck-Cominco Metals Ltd. for a generous gift of germanium
tetrachloride, and Mr. Paul Billone for technical assistance.
Supporting Information Available: Representative transient
decay and growth/decay profiles, time-resolved UV/vis absorption
spectra, and details of kinetic analyses for each of the nine systems
studied in this work. This material is available free of charge via
the Internet at http://pubs.acs.org.
OM060595S