Transfer Dehydrogenation of Cyclooctane
A R T I C L E S
General Procedure for in Situ Generation of COE Complexes
6a-d,f. To a mixture of complex 5a and 1.1 equiv of NaOtBu in a
medium-walled J. Young NMR tube was added ca. 330 mg of COA
containing the appropriate amount of COE in an argon atmosphere
glovebox. The tube was occasionally shaken and treated with ultrasound
until 5a was completely dissolved. After 30-60 min at 23 °C, the
starting complex had disappeared, and the solution was deep red
colored. If no COE was added to the reaction mixture, 1:1 mixtures of
4a/6a were obtained at 23 °C. A similar technique was used to generate
1:1 mixtures of 4b,c,f/6b,c,f. Complexes 6c and 6f were alternatively
generated by reaction of complexes 4c and 4f, respectively, with 2 to
kinetic studies established an inverse first-order dependence of
the catalytic turnover frequency on [TBE] because of the
unfavorable equilibrium between C + TBE and the vinyl
hydride complex, {C6H3-2,6-[CH2P(tBu)2]2}Ir(H)[CHdCHC-
(CH3)3].11a In contrast, the affinity of {4-X-C6H2-2,6-[OP-
(tBu)2]2}Ir (A) for TBE is rather low; TBE is not oxidatively
added but simply π-coordinated to the metal. Such a different
binding mode of TBE, despite the very similar geometric
environment at the Ir centers in A and C, is clearly electronic
in nature considering that A is much more electron-deficient
than C and therefore prefers substrate interactions which do not
increase its oxidation state from Ir(I). Furthermore, the steric
requirements for coordination (instead of oxidative addition)
of TBE or COE at A are rather different, radically disfavoring
TBE coordination. Consequently, TBE is only a weak inhibitor
of the catalytically active fragment A, and high TONs and TOFs
can be achieved even at high [TBE] (∼5.5 M). However, the
much higher affinity of A for COE compared to TBE causes
the catalytic inhibition after ca. 2200 TON for the best
performing fragment Af due to pre-equilibrium formation of
6f.
The second, and truly striking, difference between catalysts
1 and 4 is that 4f hydrogenates TBE or COE at much lower
temperatures (-70 °C) than 1 (55 °C) with comparable rate
constants. Significantly, the rate-determining step for the
hydrogenation of COE, and probably of TBE, by 4f is the
coordination of the olefin to 4f rather than reductive elimination
of neo-hexane, for example, from the intermediate (pincer)Ir-
(H)(neo-hexyl) complex, as was demonstrated by Goldman for
the Kaska/Jensen/Goldman system.11a Once again, the higher
stability of the Ir(III) oxidation state in complexes derived from
{C6H3-2,6-[CH2P(tBu)2]2}Ir (C) might account for this behavior
when compared to a higher stability of Ir(I) oxidation states in
complexes derived from (p-XPCP)Ir (A). Furthermore, the
increased electrophilicity in these bis(phosphinite) complexes
suggests a higher rate of insertion of the olefin dihydride
complex.
1
2.5 equiv of COE in neat COA at 23 °C. H NMR spectra in neat
COA were referenced to the COA signal ()1.57 ppm). NMR data for
6a-d,f are reported in neat COA. The 31P resonances are temperature-
dependent. Samples for 31P {1H}NMR spin saturation transfer experi-
ments were prepared by an identical procedure in the absence of COE.
Capillaries containing a toluene-d8 solution of the p-HPCP ligand of
complex 4c {)C6H4-1,3-[OP(tBu)2]2} were used as internal integration
standards and gave identical results when compared to the software
calibration routine provided by the Bruker XWinNMR package. T1
relaxation times for the 31P NMR resonances were determined by the
inversion recovery method. The relaxation delay was uniformly set to
15 s (>5 × T1) for each SST experiment. Five independent SST
experiments at 80 °C were conducted with 64 transients each, to obtain
accurate rate data for the equilibrium of Scheme 2. Irradiation of the
31P{1H} NMR resonance of complexes 4 or 6 with dB ) 120 gave no
changes of the integrals of 4 and 6. Irradiation of the 31P{1H} NMR
resonance of complexes 4 with dB ) 35 gave complete saturation of
complex 4 and signal depletion of the respective complex 6. Irradiation
of the 31P{1H} NMR resonance of complexes 6 with dB ) 35 gave
complete saturation of complex 6 and signal depletion of the respective
complex 4. Finally, irradiation in the middle of both resonances with
dB ) 35 gave no signal depletion of 4 or 6. The T1 relaxation times,
in combination with the degree of signal depletion (and the thermo-
dynamic ratio of 4/6 as a crosscheck), allowed for a quantitative analysis
of the rates of the separated forward and back reactions of the
equilibrium 6 + COA h 4 + 2COE. Rates Robs1 for the half reaction
6 + COA f 4 + 2COE were obtained by the algorithm Robs1 ) T1(6)-1
× [(1/I(6)) - 1] after irradiation of the 31P NMR signal of 4, where
I(6) is the relative integral of 6 obtained by complete versus no
saturation of 4. Rates Robs-1 for the back reaction were obtained by the
respective algorithm Robs-1 ) T1(4)-1 × [(1/I(4)) - 1] after irradiation
of the 31P NMR signal of 6, where I(4) is the relative integral of 4
obtained by complete versus no saturation of 6.
Experimental Section
General Considerations. All manipulations were carried out using
standard Schlenk, high vacuum, and glovebox techniques. Argon was
purified by passage through columns of BASF R3-11 (Chemalog) and
4 Å molecular sieves. Toluene-d8, benzene-d6, and methylcyclohexane-
d14 were degassed, vacuum-transferred, and stored over mol sieves in
an argon atmosphere glovebox. COA was stirred with concentrated
H2SO4 for several hours until it was olefin- and arene-free (GC and
NMR analysis), and then it was distilled under vacuum and stored in
an argon atmosphere glovebox. Cyclooctene was degassed and distilled
under vacuum and stored in an argon atmosphere glovebox prior to
use. TBE as received from Aldrich was degassed, vacuum-transferred,
and stored in an argon atmosphere glovebox. Complexes 4 and 5 were
synthesized by known procedures,12,13 and complex 4f-d38 (deuterated
in all tert-butyl and hydridic positions) was obtained by heating a
benzene-d6 solution of 4f for 12 h to 150 °C followed by high vacuum
sublimation of the frozen solvent at 0 °C.23 NMR spectra were recorded
on a Bruker DRX 400 MHz instrument and are referenced either to
residual protio solvent or to TMS as internal standard. Samples in neat
protio solvent were shimmed by optimizing the intensity of the FID
and referenced to the solvent chemical shift in CDCl3. 31P chemical
shifts are referenced to an external H3PO4 standard.
1
6a: H NMR (400.1 MHz, 80 °C, neat COA): δ 6.11 (s, 2 H, 3-
and 5-H), 4.18 [m br, 2 H, Ir(COE)], 3.67 (s, 3 H, OCH3), remaining
signals not observed because of COA. 31P{1H} NMR (162 MHz, 80
°C, neat COA): δ 171.4. 6b: 1H NMR (400.1 MHz, 80 °C, neat
COA): δ 6.33 (s, 2 H, 3- and 5-H), 4.22 [m br, 2 H, Ir(COE)],
remaining signals not observed because of COA. 31P{1H} NMR (162
1
MHz, 80 °C, neat COA): δ 171.2. 6c: H NMR (400.1 MHz, 80 °C,
2
neat COA): δ 6.78 (t br, 1 H, 4-H), 6.47 (d, JH-H ) 8.0 Hz, 2 H, 3-
and 5-H), 4.28 [m br, 2 H, Ir(COE)], remaining signals not observed
because of COA. 31P{1H} NMR (162 MHz, 80 °C, neat COA): δ 170.5.
6d: 1H NMR (400.1 MHz, 80 °C, neat COA): δ 6.2 (d, 2JF-H ) 10.3
Hz, 2 H, 3- and 5-H), 4.25 [m br, 2 H, Ir(COE)], remaining signals
not observed because of COA. 31P{1H} NMR (162 MHz, 80 °C, neat
COA): δ 174.5. 6f: 1H NMR (400.1 MHz, 80 °C, neat COA): δ 7.79
(s, 2 H, 2′- and 6′-H), 7.52 (s, 1 H, 4′-H), 6.59 (s, 2 H, 3- and 5-H),
(23) In analogy to complex 1, complexes 4 exchange their protio or deuterio
label in the hydridic positions with the tert-butyl groups. See also ref 11k.
9
J. AM. CHEM. SOC. VOL. 126, NO. 30, 2004 9337