Chemistry Reference
In-Depth Information
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Figure 8.3
Schematic representation of the chlorination of RuO
2
(110). The oxygen
atoms are indicated as green balls and the Ru atoms as blue (bulk-
coordinated) and red (under-coordinated) balls. Ball-and-stick model of
bulk truncated RuO
2
(110) (left) revealing under-coordinated surface
atoms: bridging O atoms (O
br
) and one-fold coordinatively unsaturated
Ru sites (Ru 1f-cus: red balls). Upon HCl exposure at higher temperatures
the stoichiometric surface transforms into a chlorinated surface (right)
where the bridging O
br
atoms are partly replaced by bridging chlorine
(Cl
br
) atoms (shown in gray color).
7,101,102
Reprinted with permission from ref. 102. Copyright
r
2010 American
Chemical Society.
layer of RuO
2
(110). A deeper reduction/chlorination of RuO
2
(110) has not
been observed under ultra-high vacuum (UHV)-typical conditions
7
nor at
higher pressures in the mbar range.
99,100
The maximum surface chlorination
of RuO
2
attained has been estimated to be 70-80%.
101
Surface chlorination of RuO
2
(110) proceeds via a multi-step process. The
adsorption energy of molecular HCl on RuO
2
(110) is only 40-60 kJ mol
1
.
Therefore, above T
ΒΌ
200 K HCl can only be stabilized on the catalyst's
surface by dissociative adsorption in that the Cl binds to 1f-cus Ru forming
Cl
ot
and hydrogen is transferred to under-coordinated bridging O atoms
forming bridging (O
br
H) hydroxyl groups. The dissociative adsorption of HCl
takes place on RuO
2
(110) without activation barrier and is exothermic by
130 kJ mol
1
. Via a second hydrogen transfer by dissociative HCl adsorption
O
br
H is transformed to bridging water. Finally, bridging water is replaced
(either concerted or sequentially) by chlorine, a process which is activated by
140 kJ mol
1
as determined by DFT calculations.
101,102
In situ surface X-ray diffraction (SXRD)
100
revealed that chlorinated
RuO
2
(110) and RuO
2
(100) model catalysts are long-term stable under
reaction conditions where the gas feed p(HCl):p(O
2
) was varied from 1 : 4 to
4 : 1 for pressures in the mbar range and temperatures as high as 850 K. Even
pure HCl exposure in the mbar range is not able to chemically reduce RuO
2
below 600 K, since the bridging oxygen positions are mainly populated by
chlorine, and on-top adsorbed chlorine blocks part of the under coordinated
Ru sites. Without the presence of under-coordinated surface oxygen further
HCl uptake is suppressed due to missing partners for the H-transfer.
Therefore, the RuO
2
(110) surface is resistant against pure HCl exposure in
the mbar range as long as the temperature is below 600 K. Above 650 K
chemical reduction of RuO
2
(110) to metallic Ru sets in. Substitution of a
bridging oxygen atom by a bridging chlorine (Cl
br
) is associated with a
.
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