pac technique
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Processes ◽  
2020 ◽  
Vol 8 (6) ◽  
pp. 712
Author(s):  
Alexandra Kuriganova ◽  
Daria Chernysheva ◽  
Nikita Faddeev ◽  
Igor Leontyev ◽  
Nina Smirnova ◽  
...  

Pt/C, PtMOn/C (M = Ni, Sn, Ti, and PtX/C (X = Rh, Ir) catalyst systems were prepared by using the pulse alternating current (PAC) technique. Physical and electrochemical parameters of samples were carried out by x-ray powder diffraction (XRD), transmission electron microscopy (TEM), and CO stripping. The catalytic activity of the synthesized samples for the ethanol electrooxidation reaction (EOR) was investigated. The XRD patterns of the samples showed the presence of diffraction peaks characteristic for Pt, NiO, SnO2, TiO2, Rh, and Ir. The TEM images indicate that the Pt, Rh, and PtIr (alloys) particles had a uniform distribution over the carbon surface in the Pt/C, PtRh/C, PtIr/C, and PtMOn/C (M = Ni, Sn, Ti) catalysts. The electrochemically active surface area of catalysts was determined by the CO-stripping method. The addition of a second element to Pt or the use of hybrid supported catalysts can evidently improve the EOR activity. A remarkable positive affecting shift of the onset potential for the EOR was observed as follows: PtSnO2/C > PtTiO2/C ≈ PtIr/C ≈ PtNiO/C > PtRh/C ≈ Pt/C. The addition of SnO2 to Pt/C catalyst led to the decrease of the onset potential and to significantly facilitate the EOR. The long-term cyclic stability of the synthesized catalysts was investigated. Thereby, the PtSnO2/C catalyst prepared by the PAC technique can be considered as a promising anode catalyst for direct ethanol fuel cells.


2013 ◽  
Vol 39 (5) ◽  
pp. 5577-5583 ◽  
Author(s):  
Nicolás M. Rendtorff ◽  
Gustavo Suárez ◽  
Esteban F. Aglietti ◽  
Patricia C. Rivas ◽  
Jorge A. Martinez

2011 ◽  
Vol 25 (3) ◽  
pp. S12
Author(s):  
Rajesh P. Bhavsar ◽  
Peter Juhl-Olsen ◽  
Jacob Raben Greisen ◽  
Erik Sloth ◽  
Carl-Johan Jakobsen
Keyword(s):  

2011 ◽  
Vol 311 ◽  
pp. 105-133 ◽  
Author(s):  
Michael Uhrmacher

The PAC-technique always claims to test the micro-surrounding of the probe atoms. Typically, the samples are macroscopic and more or less homogeneous and there is no debate about the usefulness of the method: substitutional sites, trapped vacancies or phase transitions are easily seen. Even the PAC-“fingerprint” of an amorphous material is known. In case of inhomogeneous samples, perhaps made out of different constituents, the question arises whether the PAC can contribute to the understanding of such materials or not. The article will show the different ways to introduce the probe atoms into the samples and discuss then the influence of these histories on the final site of the probe in the sample. In general, diffusion tends to place the probes into grain boundaries, whereas implantation reaches the bulk. This becomes important for nano-materials with their high fraction of internal surfaces. As a second, important difference for possible experiments the spatial distribution of the probes has to be considered. Implantation leads to a Gaussian shaped depth distribution of the probes. This corresponds – in a certain region – to a 3-dimensional distribution of probes in the sample, used e.g. when doping a semiconductor. In the production of special sensors (which apply e.g. the giant magnetoresistance (GMR) effect) one needs a different package, thin films (1-2 mono-layers). To apply PAC here, the probes have to be introduced during the fabrication of such a sensor. In these cases the probes have to be placed within a plane of nano-scale thickness.


2010 ◽  
Vol 198 (1-3) ◽  
pp. 41-45 ◽  
Author(s):  
F. H. M. Cavalcante ◽  
M. R. Gomes ◽  
A. W. Carbonari ◽  
L. F. D. Pereira ◽  
D. A. Rossetto ◽  
...  

2010 ◽  
pp. 387-391
Author(s):  
F. H. M. Cavalcante ◽  
M. R. Gomes ◽  
A. W. Carbonari ◽  
L. F. D. Pereira ◽  
D. A. Rossetto ◽  
...  

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