In
this work, the impact of structure and composition on the dealloying
of bulk and nanoscale alloys Cu
x
Au(1–x) have been discussed. In comparison
with the dealloying of AgAu alloys, the CuAu system
exhibits dealloying curves with more features associated generally
with multistage dealloying. It has been shown for the first time that
three stages exist during dealloying process of bulk Cu
x
Au(1–x) (x = 0.7 and 0.8) alloys. The dealloying critical potential, E
c, has been associated with the starting point
of stage II in which the anodic current slowly increases. Analysis
of data from this work along with results of others suggests a monotonic
potential dependence of E
c upon the composition
of bulk Cu
x
Au(1–x) alloys in the range of x from 0.70 to 0.95.
The dealloying behavior of Cu0.75Au0.25 (Cu3Au) intermetallic (length ∼19 nm, width ∼10
nm) and random alloy (length ∼23 nm, width ∼9 nm) nanorods
have also been discussed. Very close values of E
c have been determined for both types of nanorods with the
random alloy dealloying at slightly more negative potentials (c.a.
15–20 mV) than the intermetallic. In addition, both Cu3Au nanorods feature close to 200 mV lower E
c than bulk alloys with identical composition. Formic
acid oxidation tests reveal that the catalysts generated by platinization
of as-synthesized and dealloyed nanorods exhibit very good activity
with peak current densities in the range of 3.5 to 5.5 mA.cm–2. Both catalysts withstand testing of more than 1500 cycles. Overall,
the results of this study demonstrate unique aspects of Cu
x
Au(1–x) dealloying
and ascertain the feasibility of nanosized frameworks (dealloyed structures
or nanoparticles) as catalyst supports in fuel cell applications.