A R T I C L E S
Zhu et al.
including those on the pincer ligand, were assigned a double-ú quality
21G basis set.36
resting states (e.g., (pincer)IrH2) are also thermodynamically
favored by the substitutions; this factor should inhibit catalytic
activity. A comparison of relative stabilization of resting states
vs stabilization of TSs by the different ligands is probably not
meaningful. Such differences in relatiVe stabilization are
calculated to be very small (ca. several tenths of a kilocalorie
per mole) and probably too small to be meaningful. Extrapolat-
ing these difference to the alkanes, acceptors, and phosphi-
noalkyl groups (t-butyl or i-propyl) used experimentally, seems
particularly unreasonable. It is especially important to note in
this context that completely nonanalogous resting states might
be operative in different systems. Only a very detailed compara-
tive kinetic study (including the determination of resting states)
will allow the key differences to be elucidated.
Resistance to the formation of catalytically inactive species
(either reversible deactivation or decomposition) may be as
important as the relative kinetics of various steps within the
catalytic cycle. It seems likely that potential inactive species
would typically have an 18e configuration. Both POCOP and
MeO-PCP ligands are calculated to disfavor all reactions that
yield 18e species which we have studied, including the addition
of either H2 or CO to (pincer)IrH2 and the addition of H2 to
(pincer)Ir(CO).
Finally, we note that the calculations, in combination with
the experimental observations, offer indications that the kinetics
of C-H addition are favored by both O f C(aryl) π-donation
to the aryl ring and by σ-withdrawal from the phosphorus atoms.
In reference to POCOP, it is noteworthy that the oxygen atoms
presumably afford both these effects. The effect of σ-withdrawal
from the phosphorus atoms, if indeed it favors the TS for C-H
addition and elimination while disfavoring resting states such
as C-H addition products and dihydrides, is of particular interest
with respect to the design of future pincer catalysts.
Reactant, transition state, and product geometries were fully
optimized using gradient methods with the ECP/basis set combination
described above. The exact nature of a particular stationary point on
the potential energy surface was ascertained via standard vibrational
frequency/normal-mode analysis. Additional single-point calculations
used a more extended basis set for Ir in which the default LANL2DZ
functions for the Ir(6p) orbital were replaced by the functions
reoptimized by Couty and Hall,37 and sets of diffuse d functions
(exponent ) 0.07) and f functions (exponent ) 0.938) were added as
well. All computed energy values discussed in the text or presented in
the tables are based on data from the extended basis set calculations.
The parent (POCOP)Ir complex optimizes to a structure of C2V
symmetry as do the simple dihydride and carbonyl complexes. The
(p-MeO-POCOP)Ir complexes tend to possess Cs symmetry. The
complexes containing PCP pincer ligands optimize so that the aryl group
is canted away from alignment with the P-Ir-P axis to give structures
of C2 molecular symmetry for the parent, the carbonyl, and the dihydride
complexes; most substituted (PCP)Ir complexes possess no symmetry
(C1). On all pincer ligands, methyl groups were attached to the
phosphorus atoms. This represents a compromise between the use of
hydrogen atoms and the alkyl groups (i-Pr or t-Bu) that are typically
employed in experimental systems. Methyl groups capture most of the
electronic effects of the larger alkyl groups, but do not fully represent
the steric bulk exerted by those systems. However, steric effects are
not expected to play a role in the comparisons of reactions considered
here.
Electronic population analysis was carried out with the NBO module
incorporated into Gaussian98.38 Higher symmetry (Cs, C2V) was imposed
on the (PCP)Ir complexes to more clearly illustrate the σ- vs π-effects.
The energetic cost of regularizing the structures of these molecules
was in all cases less than 1.5 kcal/mol, and a comparison of net atomic
charges on corresponding symmetric (constrained) and asymmetric
(relaxed) structures showed a maximum difference of 0.01e.
Experimental Section
Computational Methods
General Experimental. (tBuPCP)IrH4 and (MeO-tBuPCP)IrH4
3a
5
All calculations used DFT methodology29 as implemented in the
Gaussian98 series of computer programs.30 We have made use of the
three-parameter exchange functional of Becke31 and the correlation
functional of Lee, Yang, and Parr (B3LYP).32 The Hay-Wadt
relativistic, small core ECP, and corresponding basis sets (split valence
double-ú) were used for the Ir atom (LANL2DZ model);33 all-electron,
full double-ú plus polarization function basis sets were applied to the
elements C, O, and P (Dunning-Huzinaga D95(d)).34 Hydrogen atoms
in H2 or in a hydrocarbon, which formally become hydrides in the
product complexes, were described by the triple-ú plus polarization
311G** basis set;35 other hydrogen atoms in alkyl or aryl groups,
were prepared as described previously. All manipulations were
conducted under an argon atmosphere (note: dinitrogen will poison
all catalysts in this work24) either in a glovebox or using standard
Schlenk techniques. All solvents (COA, n-octane, n-hexane) were
distilled under vacuum from Na/K alloy. NBE was purified by vacuum
sublimation. Catalytic reactions were monitored using a Varian 3400
gas chromatograph with a 60 m × 0.32 mm SUPELCO SPB-5 capillary
column. Calibration curves were prepared using authentic samples.
GC-MS was performed using a Hewlett-Packard 5980 Series II gas
chromatograph with an HP5971 mass spectrometer. All NMR spectra
were recorded with Varian Mercury and Inova spectrometers operating
at 300 or 400 MHz, respectively.
(29) Parr, R. G.; Yang, W. Density-Functional Theory of Atoms and Molecules;
Oxford University Press: Oxford, 1989.
Transfer Dehydrogenation. Alkane transfer dehydrogenation ex-
periments were typically conducted as follows. A 5-mL reactor vessel
was fitted with a Kontes high-vacuum stopcock, which allows freeze-
pump-thaw cycling and addition of argon, and an Ace Glass
“Adjustable Electrode Ace-Thred Adapter”, which allows removal of
0.5-µL samples. In the argon-atmosphere glovebox, 0.5 mL of alkane
solution (15 mM catalyst, and acceptor) was charged into the reactor.
The charged apparatus was removed from the glovebox, and additional
argon was added on a vacuum line to give a total pressure of 800 Torr.
The reactor was put into a GC oven at the desired temperature. Samples
were periodically taken by microliter syringe for GC analysis. After
(30) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M.
A.; Cheeseman, J. R.; Zakrzewski, V. G.; Montgomery, J. A., Jr.; Stratmann,
R. E.; Burant, J. C.; Dapprich, S.; Millam, J. M.; Daniels, A. D.; Kudin,
K. N.; Strain, M. C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi, M.; Cammi,
R.; Mennucci, B.; Pomelli, C.; Adamo, C.; Clifford, S.; Ochterski, J.;
Petersson, G. A.; Ayala, P. Y.; Cui, Q.; Morokuma, K.; Malick, D. K.;
Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.; Ortiz,
J. V.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.; Komaromi, I.;
Gomperts, R.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham, M. A.; Peng,
C. Y.; Nanayakkara, A.; Gonzalez, C.; Challacombe, M.; Gill, P. M. W.;
Johnson, B. G.; Chen, W.; Wong, M. W.; Andres, J. L.; Head-Gordon,
M.; Replogle, E. S.; Pople, J. A. Gaussian 98, revision A.9; Gaussian,
Inc.: Pittsburgh, PA, 1998.
(31) Becke, A. D. J. Chem. Phys. 1993, 98, 5648-5652.
(32) Lee, C.; Yang, W.; Parr, R. G. Phys. ReV. B 1988, 37, 785.
(33) Hay, P. J.; Wadt, W. R. J. Chem. Phys. 1985, 82, 299.
(34) Dunning, T. H.; Hay, P. J. In Modern Theoretical Chemistry; Schaefer, H.
F., Ed.; Plenum: New York, 1976; pp 1-28.
(36) Binkley, J. S.; Pople, J. A.; Hehre, W. J. J. Am. Chem. Soc. 1980, 102,
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(37) Couty, M.; Hall, M. B. J. Comput. Chem. 1996, 17, 1359.
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