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such as the Claisen rearrangement to give products 3a,b, the
Pd-catalyzed Suzuki coupling to give product 3c, and
a cyclization coupling to give product 3d, in one-pot after
the hydrochlorination step without need of isolation, to give
products otherwise tedious to obtain by multistep synthetic
routes.[26] These results illustrate the practicality of activating
HCl on Au surfaces.
Experimental mechanistic studies were performed in
order to assess that the selective hydrochlorination of alkynes
on Au NPs comes and is controlled by HCl activation. First,
cyclic and horizontal touch voltammetry measurements[27]
confirm that the transfer of electron density from Au NPs to
HCl also occurs in the presence of the alkyne (Supporting
Information, Figures S4, S10). Second, the hydrochlorination
of 1a follows a first-order reaction rate for HCl and also Au
catalyst (Supporting Information, Figure S11). Third, the
hydrochlorination rate increases linearly with the number of
Au0 atoms on the NP, since Au0 is more prone to give
electrons (Supporting Information, Figure S12). For this
À
study, three samples of Au CeO2 with variable amounts of
Au0 according to X-ray photoelectron spectroscopy (XPS)
and in situ CO probe IR spectroscopy (Supporting Informa-
tion, Figure S13) were prepared, since the metallic-to-cationic
À
À
Au ratio can be much easily varied on Au CeO2 than in Au
TiO2.[28] A possible participation of TiO2 in the hydrochlori-
nation of alkynes was also discarded, since the kinetic profile
of the reaction under UV/Vis light (Hg lamp) is very similar
to the thermal reaction (Supporting Information, Figure S14).
And fourth, an inverse kinetic isotopic effect KIEH = 0.71(1)
was found for the hydrochlorination of phenylacetylene (PA)
Figure 2. Optimized geometries of the structures involved in the
hydrochlorination of phenylacetylene (PA) over an Au38 nanoparticle
and calculated energy profiles for PA (black line), methylacetylene
(MA; blue line), and dimethylacetylene (DMA; purple line) hydro-
chlorination yielding the Markovnikov product. Attempts to obtain the
anti-Markovnikov product for PA are depicted in red. Distances are
given in ꢄ. Optimized geometries of all structures plotted in the
energy profile are given in the Supporting Information, Figures S16–
S18.
À
with DCl catalyzed by Au TiO2, which strongly supports the
idea that the H atom is bound to a heavy atom, Au0 in this
case, during the reaction, in accordance to the location of the
s*H-Cl LUMO of HCl on the H atom.[3,10]
Density functional theory (DFT) calculations, shown in
À
Figure 2, support the Au···H Cl electron transfer, since all the
optimized geometries for HCl adsorbed on Au38 NPs show the
H atom pointing to the Au surface, with the Cl atom far from
cally competitive (solid red line in Figure 2). However, no
transition states could be found for the subsequent attack of
Cl to either M5 or M10, suggesting that these highly stable
intermediates should accumulate on the gold NPs, in agree-
ment with the spectroscopic observation of aromatic poly-
alkenes strongly adsorbed on the catalyst surface after
reaction. On the other hand, initial addition of Cl to the
terminal C atom yielding M7 is energetically disfavored
(dotted red line in Figure 2), in agreement with the high
regioselectivity experimentally observed. Similar structures
and energy profiles were obtained for methylacetylene (MA)
and dimethylacetylene (DMA) hydrochlorination (Support-
ing Information, Figures S17, S18). Experimentally, neither
alkenes (hydrogenation product) nor polychlorinated com-
pounds (from Cl2) are found during reaction, and the lack of
reactivity of styrene as a substrate discards the formation and
polymerization of simple alkenes from alkynes. These results
support that the regio- and stereoselective hydrochlorination
event occurs very rapidly on the Au NP surface, without any
spillover of the dissociated atoms of the HCl molecule.
Taking into account the experimental and theoretical
evidence shown above, a plausible mechanism for the hydro-
À
the metal, and the H Cl bond weakens and increases its
length from 1.285 ꢀ in the isolated molecule up to 1.344 ꢀ
when adsorbed on Au (Supporting Information, Figure S15).
À
À
Once the Au···H Cl interaction occurs, dissociation of H Cl
is an exothermic process by 8–10 kcalmolÀ1, with activation
energy barriers of 5–7 kcalmolÀ1 depending on the presence
or not of co-adsorbed alkyne (Figure 2; Supporting Informa-
tion, Figure S15). The experimental values found for DH##
and Ea, obtained by an Eyring plot, are 8.6(8) and 10.0-
(5) kcalmolÀ1, respectively, which approach reasonably well
the values given by calculations.
After HCl dissociation yielding structure M2, the Cl atom
attacks the internal position of the alkyne via transition state
TS23, forming the intermediate system M3 with an activation
energy of 12.5 kcalmolÀ1. Then, addition of the hydride
occurs stereoselectively via transition state TS34 to give the
adsorbed Markovnikov product M4 with an activation barrier
of 20.2 kcalmolÀ1. Initial H addition to form intermediate
species M5 involves a higher activation barrier (dotted black
line in Figure 2), while initial H addition to the terminal C
atom yielding a stable M10 intermediate species is energeti-
Angew. Chem. Int. Ed. 2017, 56, 1 – 6
ꢀ 2017 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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