A R T I C L E S
Franz et al.
1
Electronic Structure Calculations. Geometry optimizations
were carried out using the B3LYP32 density functional with the
LANL2DZ ECP basis set which includes the D9533 basis set
on first row elements and the Los Alamos ECP plus D95 basis
set for second row and higher elements,34 using the Gaussian
9835 or NWChem 4.536 programs. Single-point calculations were
carried out with the LANL2DZ geometries of the Mo species
and organosulfur species using three basis sets, (1) the LANL2DZ
ECP basis set augmented with diffuse and polarization functions,
LANL2DZdp,37 (2) a basis set (denoted ELANL2DZ) consisting
of the LANL2DZ ECP basis set for Mo enhanced with the
6-311++G(2d,2p) basis set for H, C, and S, and (3) ECEP-
121G, corresponding to the CEP-121G ECP38 basis set for Mo
and the 6-311++G(2d,2p)39 basis set for C, H, and S. For
examination of S-S bonding in structures 6, geometries were
optimized at B3LYP/LANL2DZ ECP (Mo) and 6-31G* (CHS)
with single-point energies calculated at B3LYP/LANL2DZ ECP
(Mo) and 6-311++G(2d,2p) (CHS). Analytical gradient cal-
culations were employed to confirm ground states and to correct
electronic energies to ambient temperature enthalpy values. Total
enthalpy corrections to the electronic energy at 298 K were
computed according to eq 30:40
cm-1 were replaced by /2RT. The electronic energy for the
hydrogen atom was taken as -0.5 hartree. The present approach
resembles the methodology of DiLabio et al.42 with exception
of the use of UB3LYP treatment of open shell systems.
Electronic energies and total thermal corrections are presented
in Table 3, and calculated bond dissociation energies are
presented in Table 4. Cartesian coordinates for B3LYP/
LANL2DZ geometries are available in the Supporting Informa-
tion.
Experimental Section
Reagents. [CpMo(µ-S)(µ-SH)]2 was synthesized using a literature
procedure.8 Phenylbenzyl ketone (PBK) and dibenzyl ketone (DBK)
were purchased from Aldrich and recrystallized from methanol or
purified by radial chromatography on silica gel using methylene
chloride/hexane eluent. Benzene was purchased from Aldrich and triply
fractionally distilled to reduce trace toluene to ∼10-7 M. 1-Octanethiol
was purchased from Aldrich and distilled. Cyclohexane, tert-butylben-
zene, and dichloromethane were purchased from Aldrich and used
without further purification.
Rate Constants for Reaction of Benzyl Radical with [CpMo(µ-
S)(µ-SH)]2, 1-Octanethiol, and 2-Mercaptonaphthalene. Pyrex reac-
tion tubes (5 mm) containing 200 µL of solution (0.02 M DBK or
0.02 M PBK, 10-4 M [CpMo(µ-S)(µ-SH)]2 (or 0.01 M CH3(CH2)7SH,
or 2 × 10-3 M 2-mercaptonaphthalene), and 10-3 M tert-butylbenzene
in benzene) were freeze-thaw degassed 3 times and flame sealed with
an approximate headspace of 600 ( 50 µL. The tubes were placed
inside a thermostated oven equipped with a quartz window and allowed
to achieve temperature equilibrium for 1 min. The sample was
photolyzed with a water-filtered 1-kW high-pressure xenon arc lamp
for controlled periods of time (0.50-20.00 ( 0.005 s) using a Uniblitz
model 225L0AOT522952 computer-controlled electronic shutter. Re-
agent concentrations were corrected for solvent vapor pressure and
density.43 Rate constants for hydrogen abstraction were calculated using
eq 10c at 0.5-8.0 s photolysis times, using the measured product
concentrations, the calculated average molybdenum-thiol donor con-
centration, and the benzyl self-radical termination rate, 2kt, calculated
from the expression ln(2kt/M-1 s-1) ) 27.23-2952.5/RT. This expres-
sion was calculated using the von Smoluchowski equation, eq 33, using
the Spernol-Wirtz modification of the Debye-Einstein equation, eq
34, where f in eq 34 is the SW microfriction factor.44
H298° ) 3/2RT + nRT +
k,b
R
(Θ (1/ + 1/(eΘ /T - 1))) + RT (30)
∑
k,a 2
k
Θk,x ) (c1)hc/kbλk
x ) a, c1 ) 0.9806
x ) b, c1 ) 0.9989
n ) 1, linear
n ) 3/2, nonlinear
Equation 30 includes a translational, a rotational, an internal
(ZPE and vibrational), and a PV term. Each vibration, λk, was
scaled by 0.9806 for the ZPE term (x ) a) and by 0.9989 for
the vibrational term (x ) b).41 Each vibration was examined to
identify group rotations, and scaled internal rotations under 260
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2kt ) (8π/1000)σFDAB
DAB ) kT/6πrAηf
N
(33)
(34)
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2497.6/RT, and in toluene, ln(2kt/M-1 s-1) ) 27.05-2797.4/RT. For
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