Electrochimica Acta 47 (2001) 395 – 403
www.elsevier.com/locate/electacta
Determination of the morphology factor of oxide layers
L.M. Da Silva
a
, L.A. De Faria
b
, J.F.C. Boodts
a,b,
*
,1
a
Departamento de Quı ´mica, FFCLRP/USP, A. Bandeirantes, 3900, 14040 -901 Ribeira ˜o Preto, SP, Brazil
b
Instituto de Quı ´mica, UFU, Campus Santa Mo ˆnica, A. Joa ˜o Naes de A
´
ila, 2160, 38400 -902 Uberla ˆndia, MG, Brazil
Received 17 January 2001; received in revised form 29 May 2001
Abstract
From the linear dependencies of the voltammetric capacitive current, i
c
, with the potential sweep rates, , observed in the low
and high domains, it is possible to determine the inner and outer differential capacities of oxide coatings. The morphological
factor, , defined as the ratio of the inner and total differential capacities (C
d,i
/C
d
) shows a linear relationship with the radius/ionic
charge ratio of the anion of the supporting electrolyte. The dependence of the capacitive voltammetric charge, q
c
, on was
interpreted on the basis of a purely capacitive model for the oxide/solution interface. © 2001 Elsevier Science Ltd. All rights
reserved.
Keywords: Oxide films; Differential capacity; Morphology factor; Capacity charge; Ionic radius
1. Introduction
A revision of the different methods proposed to
determine the real surface area of solid electrodes was
published by Trasatti and Petrii [1]. The voltammetric
methods are of particular interest since they permit the
‘in situ’ monitoring of the surface of oxide electrodes
[2–13].
The procedure based on the voltammetric hydrogen
adsorption/desorption peaks, to determine the real area
of metal electrodes is well established [14]. However,
the surface charging of oxide electrodes, particularly
conductive metallic oxides, is much more complex also
depending on the pH of the supporting electrolyte and
the acid/base surface properties of the oxide through a
proton injection/ejection process involving the solid-
state surface redox transitions, SSSRT (the surface
behaves as a ‘protonic condenser’) [1,6,12,15]. The fun-
damental problem of charging of electrode films was
extensively treated by Conway [16].
A procedure was proposed [7,8,12] to determine the
‘porosity’ of oxide layers from the dependence of the
voltammetric charge, q * (obtained by integration of the
voltammetric profiles recorded covering a potential in-
terval which includes the SSSRT) on the potential
sweep rate, . The procedure assumes that the q * versus
behaviour is related to the existence of less accessible
surface areas (loose grain boundaries, pores, cracks,
etc.) which become progressively excluded from the
electrochemical response as increases. Trasatti et al.
[7,8,13] emphasised that the determination of the
‘porosity’ based on the q * versus dependence can be
affected by spurious factors such as: irreversibility of
the SSSRT and uncompensated ohmic drop. Both fac-
tors can lead to distorted voltammetric charge data.
The distortion is more drastic at lower q *-values [8].
An alternative to the above-mentioned procedure is
based on the linear dependence of the capacitive cur-
rent on (i
c
), normally observed for porous/rugged
electrode films. Frequently, the linear relationship is
only observed over a short range; deviation from
linearity already starting at rather low sweep rates,
typically around 200 mV s
-1
[11]. The linear behaviour
can be used to determine the differential capacity, C
d
,
of the solid/solution interface recording CVs at several
s covering a small capacitive potential range (typically
100–200 mV). C
d
is then obtained from the slope of the
i
c
versus graphs, i
c
normally being measured in the
middle of the CV [1,3,9,11].
The description of the real surface area of an oxide
electrode by a roughness factor, defined as C
d
/C
reference,
suffers from the drawback that the value of a reference
* Corresponding author. Fax: +55-1663-38151.
E-mail address: jfcboodts@ufu.br (J.F.C. Boodts).
1
ISE member.
0013-4686/01/$ - see front matter © 2001 Elsevier Science Ltd. All rights reserved.
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