chakraborty banerjee ea 3790-2011
TRANSCRIPT
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
1/9
Electrochimica Acta 56 (2011) 37903798
Contents lists available atScienceDirect
Electrochimica Acta
j o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / e l e c t a c t a
Electrochemical impedance spectroscopic investigation of the role of alkalinepre-treatment in corrosion resistance of a silane coating on magnesium alloy,ZE41
P. Chakraborty Banerjee a,b, R.K. Singh Raman a,c,
a Department of Chemical Engineering, Monash University, Clayton, VIC-3800, Australiab CAST Cooperative Research Centre, Hawthorn,VIC-3122, Australiac Department of Mechanical and Aerospace Engineering, Monash University, Clayton, VIC-3800, Australia
a r t i c l e i n f o
Article history:
Received 6 November 2010
Received in revised form 7 February 2011
Accepted 10 February 2011
Available online 17 February 2011
Keywords:
Silane coating
Electrochemical impedance spectroscopy
Magnesium alloys
a b s t r a c t
Theprotective performance of the coatings of bis-1,2-(triethoxysilyl) ethane (BTSE) on ZE41 magnesium
alloywith different surface pre-treatments were evaluated using potentiodynamic polarizationand elec-
trochemicalimpedance spectroscopy(EIS)in 0.1 M sodiumchloride solution. Electricalequivalentcircuits
were developed based upon hypothetical corrosion mechanisms and simulated to correspond to the
experimental data. The morphology and cross section of the alloy subjected to different pre-treatments
and coatings were characterized using scanning electron microscope. A specific alkaline pre-treatment
of the substrate prior to the coating has been found to improve the corrosion resistance of the alloy.
2011 Elsevier Ltd. All rights reserved.
1. Introduction
Magnesium alloys are the lightest metallic material with excel-
lent physical and mechanical properties [1]. High strength to
weight ratio makes them very attractive to the automobile and
aerospace industries. But the use of magnesium alloys is restricted
due to their poorcorrosion resistance. Thesurface filmformed upon
immersion of magnesium in aqueous solution consists of a non-
compact duplex layer comprising of an inner MgO layer next to
the metal and an external porous layer of Mg(OH)2 [2].The pro-
tection offered by this film is highly dependent on the conditions
of exposure[3].Moreover, the presence of several anions such as,
chloride, sulphate and nitrate in the aqueous solution hinder the
formation of the surface film and also disrupts the existing film,
which in turn accelerate the corrosion rate[3].The partially pro-
tective surface film, low standard reduction potential, presence
of certain impurities (viz., Fe, Cu, Ni) and microgalvanic couplingbetween the secondary phases and the -solid solution, as well as
galvanic coupling with other metals accelerate the corrosion prob-
lems of magnesium and its alloys. Thus magnesium alloys undergo
different types of corrosion, such as, general, galvanic, pitting and
granular corrosion[3]. It is believed that desired corrosion resis-
Corresponding author at: Department of Mechanical and Aerospace Engineer-
ing, Monash University, Clayton, VIC-3800, Australia. Tel.: +61 3 9905 3671;
fax: +61 3 9905 1825.
E-mail address:[email protected](R.K. Singh Raman).
tance of magnesium alloys will necessitate application of suitable
surface barrier, such as chemical treatments and/or coatings.
Silanes are emerging as an attractive environmentally friendly
alternative for improving the corrosion resistance of the metal-
lic substrates as well as for enhancing the compatibility of the
metal surface with the paint systems [48]. The coupling abil-
ity of silanes is attributed to their unique chemical structure,
which is given by, R(CH2)nSiX3, where R is any organofunc-
tional group, CH2 is the linker and X is the hydrolysable group.
When a silane is used for modification of a polymericinorganic
interface, the organofunctional group as well as the hydrolysable
groups of silane independently bond with the polymer and inor-
ganic surfaces. Silanes form oxane bonds with the hydroxyl groups
of inorganic substrates as well as can form covalent bonds with
suitable functional groups of different polymers.
On the basis of the number of the hydrolysable groups, silanes
are of two types, viz., monosilane, having three hydrolysablegroups and bis-silane, having six hydrolysable groups. Though
monosilanes have been widely used on different metal substrates,
bis-silanes are reported to provide superior corrosion protection
[9].As bis-silanes can form more silanol groups, in the reticula-
tion stage, these silanol groups can react with each other to form
siloxane bonds, and thus can build robust hydrophobic polysilox-
ane layers (SiOSi linkages), which, in turn, enhances durability
of silane coatings in aqueous media[10].
The interaction of silanes with metal substrates also depends
on the nature of the inorganic surfaces[9].Plueddamann[11]sug-
gested thatoxide surfaces witha higher number densityof hydroxyl
0013-4686/$ see front matter 2011 Elsevier Ltd. All rights reserved.
doi:10.1016/j.electacta.2011.02.050
http://localhost/var/www/apps/conversion/tmp/scratch_5/dx.doi.org/10.1016/j.electacta.2011.02.050http://localhost/var/www/apps/conversion/tmp/scratch_5/dx.doi.org/10.1016/j.electacta.2011.02.050http://www.sciencedirect.com/science/journal/00134686http://www.elsevier.com/locate/electactamailto:[email protected]://localhost/var/www/apps/conversion/tmp/scratch_5/dx.doi.org/10.1016/j.electacta.2011.02.050http://localhost/var/www/apps/conversion/tmp/scratch_5/dx.doi.org/10.1016/j.electacta.2011.02.050mailto:[email protected]://www.elsevier.com/locate/electactahttp://www.sciencedirect.com/science/journal/00134686http://localhost/var/www/apps/conversion/tmp/scratch_5/dx.doi.org/10.1016/j.electacta.2011.02.050 -
7/26/2019 Chakraborty Banerjee EA 3790-2011
2/9
P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798 3791
Table 1
Nominal composition of ZE41.
Elements present in ZE41
Mg Zn Ce La Nd Pr Zr Fe Cu Ni
w t% 94 .4 3.82 0.64 0.27 0.1 4 0.06 0.69 0.002 0.002
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
3/9
3792 P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798
-1.8
-1.7
-1.6
-1.5
-1.4
-1.3
-1.2
-1.1
-2-3-4-5-6-7-8
log (j/A cm-2
)
EvsSCE/V
Tested after keeping in desiccator for 24 h
Tested after polarizing in hydroxide for 600 s
Tested after dipping in hydroxide for 48 h
Untreated ZE41
Fig.1. Potentiodynamic polarization plotsof thealloywith differentpre-treatments
and untreated alloy.
3. Results and discussion
3.1. Alloy with different pre-treatments: electrochemical
characterization
The potentiodynamic polarization plots of the alloy with dif-
ferent pre-treatments and the untreated alloy are shown in Fig. 1.
Bothcathodic andanodiccurrentdensities of all thepre-treatedand
untreated specimens were respectively similar. The similar shapes
of the anodic plots as well as the similar magnitudes infer that
the dissolution rate and the dissolution mechanism are analogous.
However, EIS were conducted to further assess the protection, if
any offered by different pre-treatments. The Nyquist plots (Fig. 2)
of the alloy with different pre-treatments and the untreated alloy
are characterizedby two capacitive semicircles. The highfrequency
semi circles correspond to the charge transfer processes whereas
the medium/low frequency semicircles correspond to the masstransport relaxation (Mg+) in the solid phase, i.e., in an aggregating
layer [17]. The corrosion resistance is determined by the com-
bined diameter of these two semicircles[18].A marginal increase
in the corrosion resistance was observed in case of the pre-dipped
and pre-polarizedspecimens, whereas the specimen withnaturally
developed hydroxide film (upon storing in a desiccator for 24 h)
showeda similar corrosion resistance as that of the untreated alloy
(scatter in the data was 500 cm2).
0
500
1000
1500
2000
2500
3000
300025002000150010005000
Z'/ cm2
Z"/
cm
2
Tested after keeping in desiccator for 24 h
Tested after polarizing in hydroxide for 600 s
Tested after dipping in hydroxide for 48 huntreated ZE41
Fig. 2. Nyquist plots of the alloy with different pre-treatments and untreated alloy.
3.2. Alloy with different pre-treatments: surface characterization
Since the structure of the hydroxide film determines the bond-
ing of silane with the metal as well as the performance of silane
coatings in corrosive media, it became essential to develop a broad
understanding of the hydroxide film formed on the metal surface
upondifferentpre-treatments. SEM of the surface and crosssection
of the alloy after different pre-treatments provided some useful
information.Fig. 3shows a thick (average thickness 20m) and
uniform hydroxide layer on the specimen that was pre-dipped in
hydroxidefor 48h. Thesurfacehydroxide films formedon theother
two specimens (polarized in hydroxide and held in desiccator for
24 h) were too thin to be observed by SEM. Surface topography
of the polarized specimen (Fig. 4(b)) confirmed that the surface
hydroxide layer was indeed very thin, which allowed imaging of
the intermetallics at the grain boundaries of the underlying alloy
microstructure. The topographic features of the specimen that was
held in desiccator for 24 h were similar to those shown inFig. 4(b).
However, the very thick hydroxide layer that developed over the
specimen dipped in hydroxide for 48h (Fig. 3) did not allow obser-
vation of the underlying microstructure (Fig. 4(c)).
3.3. Coated alloy with different pre-treatments: surface
characterization
As shown in Fig. 5, the silane coated specimens with differ-
ent pre-treatments have different surface morphologies. Thickness
of the coatings that are developed upon the silane treatments is
expected to be limited to a fewhundreds of nanometres [19], which
allows the features underneath the coating to be observed. There-
fore, it was possible to observe intermetallic precipitates present at
the surface of the coated specimenswithoutalkaline pre-treatment
(Fig. 5(a)) and, to some degree, even in the case of the alloy with
presumably very thin hydroxide layer as developed upon polariza-
tion (Fig. 5(b)). In this context, it is interesting to observe a few
precipitates on the alloy pre-dipped in hydroxide for 48h and then
BTSE coated (Fig. 5(c)), in spite of the considerably thicker hydrox-
ide layer developed upon this pre-treatment (Figs. 3 and 4(c)).However, a careful observation of the cross section of the spec-
imen pre-dipped in sodium hydroxide (Fig. 3(a)) would suggest
that though the alloy matrix had reacted with sodium hydroxide
to produce a thick hydroxide layer, the intermetallic particles had
not reacted and were embedded into the hydroxide layer. In fact,
some of these particlesextend right up to the surface of the hydrox-
ide layer, which explains the observed particles under the silane
coated specimens(Fig.5(c)).Examinationof thecross section of this
specimen (Fig. 6)confirms the silane coating to be thinner in com-
parison with the thickness of the hydroxide layer and it is barely
distinguishable.
3.4. Polarization and electrochemical impedance spectroscopy
tests: uncoated and different coated specimens
Fig. 7 depicts the potentiodynamic polarization plots for the
uncoated, only hydroxide pre-dipped (without any coating) and
BTSE coated (with and without different alkaline pre-treatments)
specimens. The anodic current densities of the BTSE coated alloy
with prior alkaline pre-treatments (both pre-dipped and pre-
polarized) were higherthan othersup to1.2VSCE, which confirms
that the alkaline pre-treatments and then BTSE coating were effec-
tive in impeding the anodic dissolution reaction for these coated
specimens. Beyond this potential, anodic current densities of all
the specimens were similar, implying that the protective coatings
formed on thealkalinepre-treated andthen BTSEcoated specimens
disintegrate at these high anodic over potentials. The effectiveness
of the combined role of alkaline pre-treatment and BTSE coating is
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
4/9
P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798 3793
Fig. 3. Back scattered electron (BSE) image of the cross section of the alloy pre-dipped in hydroxide.
evidenced from the observation that the anodic current densities
of the BTSE coated specimen (without alkaline pre-treatment) and
the only hydroxide pre-dipped specimen (without BTSE coating)
were similar to that of the uncoated specimen at all anodic over
potentials. Cathodic current densities for all the specimens were
similar. Thecorrosionpotentials(Ecorr) of the BTSE coatedspecimen(without alkaline pre-treatment) and the specimen polarized in
hydroxide andthen BTSE coated are more active than the uncoated
alloy, whereas, Ecorrof the specimen dipped in hydroxide andBTSE
coated is about 90 mV more positive than the untreated alloy. It
may be interesting to note that the Ecorr of the BTSE coated (with
and without alkaline pre-treatment) specimens varied over a wide
range (maximum variation is about 200mV). However, this kind
of difference in Ecorr between different coated magnesium alloys
has been observed in several other studies [10,2026].It is quite
plausible to assume that the nature (uniformity and thickness) ofthe silane films formed after different pre-treatments will be dis-
similar. In the present study, the observed variation in Ecorr(which
is a measure of the corrosion susceptibility[27]) of the different
BTSE coated specimens, may be attributed to the different corro-
Fig. 4. SEM images of the surface morphology of the alloy: (a) untreated, (b) polarized in hydroxide and (c) dipped in hydroxide for 48 h.
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
5/9
3794 P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798
Fig. 5. SEM images of the surface morphology of silane coated alloy: (a) without alkaline pre-treatment, (b) polarized in hydroxide for 600 s and (c) pre-dipped in hydroxide
for 48 h (arrows show the intermetallic particles underneath the coatings).
sion susceptibility, arising due to dissimilar nature of the silanecoatings formed on these specimens.
The Nyquist plots (Fig. 8)of all the specimens show that while
slight improvement in impedance was observed in the case of the
only hydroxide pre-treated and only BTSE coated specimens, the
highest improvement in impedance was observed in case of the
BTSE coated specimens with alkaline pre-treatments. A compar-
ison of the plots would suggest that the total impedances, which
arethe measure of the corrosionresistances, offered by the alkaline
pre-treated specimens to be 56 times superior to that of uncoated
alloy. The total impedance of thespecimenpre-dipped in hydroxide
and then BTSE coated is 6 k, and that of the specimen pre-
polarized in hydroxide and then BTSE coated is 5 k, whereas
the total impedance of the uncoated alloy is in the range of 1 k.
From the polarization and EIS results, it can be concluded thatthe improvement in corrosion resistance was not only due to the
alkaline pre-treatment or BTSE coating alone, but due to the com-
bined effect of both. Electrical equivalent circuits (EEC) can be
employed to obtain a mechanistic insight into the influence of the
different surface pre-treatments on the corrosion behaviour of the
BTSE coated specimens. In the present study, impedances of the
interfaces of substrate/surface hydroxide/NaCl solution and sub-
strate/surface hydroxide/silane film/NaCl solution were analysed
on the basis of identification of appropriate EEC. In corrosion pro-
cesses, each of these interfaces can be represented as a parallel
combination of a capacitance and a resistance. This concept forms
the basis of EECs that have been employed here. EECs were devel-
oped for different interfacial scenarios based upon hypothetical
corrosion mechanisms, and the simulation data were generated for
each EEC. The experimental data sets were compared with the cor-responding simulated data sets, in order to arrive at an appropriate
corrosion mechanism for each scenario. It was possible to calcu-
late interfacial resistances and capacitances that can be related to
the homogeneity of the films andcan describe the corrosion mech-
anisms. The relative magnitudes of these components provide an
estimation of the protection provided by a given coating.
In the present study, complex nonlinear least squares fitting
(CNLS) was used to analyse the impedance data. In this method, all
the data are simultaneously fitted to a givenEEC containing a set of
unknown parameters (for example, circuit elements), which may
enter nonlinearly in the formula for the measured function of fre-
quency and impedance. It also provides uncertainty estimates for
all the estimated parameters in a given EEC. Unlike the other meth-
ods (KronigKramers relations, ordinary nonlinear least squares,etc.[28])it allows to fit a very complicated model with large num-
ber of circuit elements. CNLS procedure implies minimization of
the sum of square functions[28],
S=
k
i=1
{wai[faeifat (;p)]
2+wbi[f
beifbt (;p)]
2} (1)
whereft( ;p) is a function of both the angular frequency () and
a set of EEC parameters p. i = 1,. . ., k represents the data points
associated withi.ft( ;p) can be divided into two parts,fat(;p)
andfbt(;p), (both depend on the same set of parameters).fat(;p)
and fbt(;p) can either represent Zreal and Zimaginary or |Z| and
(phase angle of impedance),respectively.wa
i andwb
i arethe weights
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
6/9
P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798 3795
Fig. 6. SEM images of the cross section of the pre-dipped in hydroxide and then BTSE coated specimen: (a) secondary electron image, (b) back scattered electron image and
(c) secondary electron image (higher magnification).
related to the ith data point. faei
and fbei
are the experimentally
obtained data values. Whenfbt(;p) = 0, CNLS reduces to ordinary
non linear least squares [28]. In the present study, since faei
and
fbei
values do not vary over several orders of magnitude, the fit-
ting procedurewas chosen to be unity weighted (i.e.,wai = wb
i = 1).
The circuit description code (CDC) used by Boukamp [29], has been
followed in the present study.
For the uncoated alloy, a simple EEC was used to simulate
the data corresponding to a hypothetical corrosion mechanism,
where electrical double layerand naturallyformed surface hydrox-
ide film behave as a set of capacitance and resistance in parallel
(as shown inFig. 9).Theoretical simulation was conducted usinga Rs(Cf[Rf(CdlRc)]) electrical equivalent circuit (Fig. 9), where the
solution resistance is represented byRs. The surface film, which is
represented by a parallel combination of a capacitance (Cf) and the
surface film resistance (Rf), is in parallel with the electrical dou-
ble layer (represented by the parallel combination of the electrical
double layer capacitance (Cdl) and charge transfer resistance (Rc)).
A comparison with the simulated results based upon other EECs
suggested that Rs(Cf[Rf(CdlRc)]) was the closest fit to the experi-
mental impedance data for the uncoated alloy with a relatively low
chi square value (2103) as well as a low error (4%)in impedance
measurement. The calculated parameters for the proposed EEC are
shown inTable 2.
The simulated results and the observed Bode impedance plots
forthe uncoated ZE41 alloy areshown in Fig. 10. Errorplots(Fig. 11)
for the uncoated alloy show that the maximum error in simulated
data is less than 7% for both |Z| and angle. Though the coated spec-
imens were found to conform to a different EEC, the trend of error
plots for all of them was similar to that shown inFig. 11.
-1.7
-1.6
-1.5
-1.4
-1.3
-1.2
-1.1
-2-3-4-5-6-7-8
log (j/A cm-2
)
E
vsSCE
/V
Uncoated
BTSE coated (without alkaline pre-treatment)
Dipped in hydroxide and BTSE coated
Polarized in hydroxide and BTSE coated
Only hydroxide pre-treated (dipped)
Fig.7. Potentiodynamic polarizationplots ofBTSE coated (withandwithoutalkaline
pre-treatment), hydroxide pre-treated (without any coating) and uncoated ZE41
alloy.
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
7/9
3796 P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798
0
1000
2000
3000
4000
5000
6000
6000500040003000200010000
Z'/ cm2
Z"/
cm
2
BTSE coated (without alkaline pre-treatment)
Polarised in hydroxide and BTSE coated
Dipped in hydroxide and BTSE coated
Uncoated
Only hydroxide pre-treated (dipped)
Fig. 8. Nyquist plots of the BTSE coated (with and without alkaline pre-treatment),
hydroxide pre-treated (without any coating) and uncoated ZE41 alloy.
RcCdl
Rf
Rs
Cf
Electrical
double layer
Surface film
Metal
Fig. 9. The electrical equivalent circuit fitted to the experimentally obtained
impedance data of the uncoated alloy.
Table 2
Calculated parameters for the components in Rs(Cf[Rf(CdlRc)]).
Parameters Estimated values Rel. std. error/%
Rs/ cm2 157 1
Cf/Fcm2 1.1105 5
Rf/ cm2 364 17
Cdl/Fcm2 1.3105 18
Rc/cm2 523 11
Fig. 10. Bode plots for measured and calculated values of uncoated ZE41 alloy.
Fig. 11. Error plots for measured and calculated values of uncoated ZE41 alloy.
Several EECs were employed to fit the experimental impedance
data for the BTSE coated specimens with different pre-treatments.
However the lowest chi square values and the minimum over-
all errors in impedance measurements were obtained with
Rs(Qsi[Rsi(CfdlRc)]) (Fig. 12).In this EEC, the solution resistance is
represented by Rs. The silane film is characterized by a constant
phase element (CPE) (Qsi) and pore resistance (Rsi). Other stud-ies [4,7,20,30,31]suggest that it is typical to represent the silane
film using a CPE, instead of a pure capacitor. The other time con-
stant (represented by the parallel combination of a capacitance
Cfdl and a resistance Rc) that is present in the EEC is assumed to
describe the combined responses of the electrical double layer and
the hydroxide film. This aspect will be explained in more details in
thefollowing sections.The calculated andthe measured Bode plots
for the specimens with different coatings are shown inFig. 13.
Table 3presents the calculated values of the different parame-
ters associatedwith the proposed EEC for differentspecimens. Both
Rsi and Rc for the specimen dipped in hydroxide and then BTSE
coated is higher than others. Also, the total impedance, which is a
measure of the corrosion resistance[18],has the highest value for
thepre-dipped specimen.Although Qsi forall specimens aresimilar,Cfdl of different specimens varies over several orders of magnitude.
Also,Cfdl determined for different coated specimens are different
from the typical electrical double layer capacitance for metal elec-
trodes, whichin general ranges inF/cm2 [32]. Thus it is suggested
that the time constant, consisting ofCfdland Rc did not arise due to
the sole response of the electrical double layer, but it did due to a
combined response of the surface hydroxide film and the electrical
double layer. TheCfdl of the BTSE coated specimen pre-dipped in
Rc
Rs
RsiQsi
CfdlElectricaldouble layer
Silane film
Metal
Fig. 12. The electrical equivalent circuit fitted to the experimentally obtained
impedance data of the different BTSE coated specimens.
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
8/9
P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798 3797
Fig. 13. Bode plots for measured and calculated values of the different coated specimens: (a) only BTSE coated, (b) pre-dipped in hydroxide and then BTSE coated and (c)
pre-polarized in hydroxide and then BTSE coated.
hydroxide was 34 orders of magnitude lower than the other two
specimens (Table 3).Since capacitance is directly proportional to
the area of the capacitor, the relatively lower capacitance indicates
a comparativelylowerexposureof themetal/hydroxide interface tothe electrolyte. This can be attributed to the fact that after immer-
sion of the specimen in 3 M sodium hydroxide (pH 12) for 48 h, a
considerably thicker and less defective surface hydroxide film was
developedon this specimen (Fig.3), which enhancedthe cross link-
age of silane with surface hydroxide during coating process, and
thus presumably produced a uniform and less defective coating.
Improvement in the corrosion resistance of the BTSE coated
specimensas a resultof the alkali pre-treatments is understandable
if one considers the Pourbaix diagram for magnesium [33],shown
in Fig. 14. In aqueous environment,magnesium formsa surface film
of magnesiumhydroxide. The protection offered by Mg(OH)2 filmis
highlydependent on the pH andpresence of differentanions in the
solution [34]. From the Pourbaixdiagram,it is evident thata passive
Mg(OH)2 film will form at pH >11. The nature and protectivenessof this hydroxide layer is reported to be profoundly influenced by
the alloying constituents of different magnesium alloys [3436].
For example, in the case of MgAl alloys, the major alloying ele-
ment, Al plays an important role in the surface film formation [35].
Therefore, it maybe importantto consider the role of Zn, the major
alloying element in ZE41 alloy. The surface film formed on a Zn
electrode is stablein an aqueous solution at pH 8.212.1 [37]. Thus,
on immersion in the alkaline solution (3M NaOH) with pH 12 for48h, a thick and uniform hydroxide film was formed on ZE41 alloy
(Fig. 3).The protective performance of any silane coating primar-
ily depends on the successful cross linkage between the silane film
and the metal hydroxide. Plueddamann[11],Franquet et al.[12]
and van Ooij et al.[9]have earlier suggested that the alkaline pre-
treatment facilitates silane deposition, which is consistent withthe
observation of the present study. Formation of a uniform hydrox-
ide film after alkaline pre-treatments indeed aids formation of a
protective coating on the metal surface (as is evidenced from the
electrochemical results).
Among the specimens that were alkaline pre-treated before
BTSE coating, the specimens pre-dipped in hydroxide and then
coated with BTSE showed a superior corrosion resistance to those
subjected to polarization in hydroxide and then coating (as evi-denced from the Nyquist plots (Fig. 8)). This behaviour may be
attributed to the characteristics of the hydroxide films developed
during thetwo pre-treatments. Also,Figs.3and4show formationof
a thicker and relatively uniform hydroxide film upon prior dipping
Table 3
Calculated parameters of the proposed EEC for the coated specimens.
Specification Rsi/cm2 Rc/ cm
2 Qsi/Fcm2 n Cfdl/Fcm
2 Chi squared
value
Total
error/%
V alue Er ro r/ % Value Er ro r/ % Value E rr or /% Value E rr or /% Value Er ro r/ %
Only BTSE coated 3167 1 899 12 1.1105 3 0.9 1 2.1103 12 8.3104 3
Pre-polarized in NaOH + BTSE coated 4620 2 352 11 1.1105 2 0.9 1 7.5104 6 7.5104 3
Pre-dipped in NaOH + BTSE coated 4881 24 997 6 1.3105 8 0.7 2 9.7107 18 2.8103 5
-
7/26/2019 Chakraborty Banerjee EA 3790-2011
9/9
3798 P. Chakraborty Banerjee, R.K. Singh Raman / Electrochimica Acta 56 (2011) 37903798
Fig. 14. Pourbaix diagram[33].
in hydroxide for 48 h. A cursory comparison may not provide any
convincing reason for the priordipping(as opposed to polarization)
to produce a thicker and less defective hydroxide film. However,
the thermodynamic and kinetic factors seem to provide a convinc-
ing explanation. As the Pourbaix diagram (Fig. 14)would suggest,
little thermodynamic preference for the two scenarios since mag-
nesium will form a stable hydroxide film at every potential when
immersed in an aqueous solution of pH 12. Thus, the film deposi-
tion kinetics would be the only governing factor for the properties
of the hydroxide layer. The long dipping time (48 h) in hydroxide
solution, allowed development of a relatively uniform and thicker
film (Figs. 3 and 4) under close to equilibrium condition. On the
other hand, the effective exposure time of the specimen subjected
to prior polarization was only 600 s and the deposition occurred
in a relatively forced condition, compromising the quality of the
hydroxide film.
4. Conclusions
Influence of alkali surface pre-treatment of BTSE coated ZE41
has been analysed using potentiodynamic polarization and elec-
trochemical impedance spectroscopy. A comparative study of the
corrosion resistance offered by BTSE coated (with and without
alkali pre-treatment) and uncoated ZE41 suggests that alkaline
pre-treatment prior to BTSE coating provides superior corrosion
resistance. However, the nature of the alkaline pre-treatments
influences the corrosion resistance of the coated alloy. This
improvement in corrosion resistance was superior in the case
of a pre-treatment that results in the formation of a thick and
uniform hydroxide film on the surface, which facilitates forma-
tion of a protective silane film on the substrate. The EIS results
are in good agreement with the potentiodynamic polarization
results.
Acknowledgements
Authors would like to acknowledge DSTOfor their financialsup-
port for investigation of silane coating for ZE41 alloy. The kind
assistance of Abhishek Saxena is also gratefully acknowledged.
References
[1] G. Abbas, Z. Liu, P. Skeldon, Appl. Surf. Sci. 247 (2005) 347.
[2] M.Liu,S. Zanna,H.Ardelean, I.Frateur, P.Schmutz, G.Song,A.Atrens,P. Marcus,Corros. Sci. 51 (2009) 1115.
[3] G.L. Markar, J. Kruger, Int. Mater. Rev. 38 (1993) 138.[4] M.F. Montemor, M.G.S. Ferreira, Electrochim. Acta 52 (2007) 7486.[5] A.M. Beccaria, L. Chiaruttini, Corros. Sci. 41 (1999) 885.[6] H. Wang, R. Akid, Corros. Sci. 49 (2007) 4491.[7] L.M. Palomino, P.H. Suegama, I.V. Aoki, M.F. Montemor, H.G. De Melo, Corros.
Sci. 51 (2009) 1238.[8] R. Supplit, T. Koch, U. Schubert, Corros. Sci. 49 (2007) 3015.[9] W.J. vanOoij,D. Zhu, M. Stacy,A. Seth,T. Mugada, J. Gandhi, P.Puomi, Tsinghua
Sci. Technol. 10 (2005) 639.[10] F. Zucchi, V. Grassi, A. Frignani, G. Trabanelli, Corros. Sci. 46 (2004) 2853.[11] E.P. Plueddamann, Silane Coupling Agents, Plenum Press, New York, 1991.[12] A. Franquet, H. Terryn, J. Vereecken, Surf. Interface Anal. 36 (2004) 681.[13] M. Teo, J. Kim, P.C. Wong, K.C. Wong, K.A.R.Mitchell, Appl. Surf. Sci. 252 (2005)
1293.[14] D. Susac, X. Sun, K.A.R. Mitchell, Appl. Surf. Sci. 207 (2003) 40.[15] J. Kim, P.C. Wong, K.C. Wong, R.N.S. Sodhi, K.A.R. Mitchell, Appl. Surf. Sci. 253
(2007) 3133.[16] A.M. Cabral, R.G. Duarte, M.F. Montemor, M.G.S. Ferreira, Prog. Org. Coat. 54
(2005) 322.[17] G. Baril, N. Pbre, Corros. Sci. 43 (2001) 471.[18] F. Zucchi, V. Grassi, A. Frignani,C. Monticelli,G. Trabanelli,J. Appl.Electrochem.
36 (2006) 195.[19] A. Franquet, J. De Laet, T. Schram, H. Terryn, V. Subramanian, W.J. van Ooij, J.
Vereecken, Thin Solid Films 384 (2001) 37.[20] M.F. Montemor, R. Pinto, M.G.S. Ferreira, Electrochim. Acta 54 (2009) 5179.[21] J. Liang, P.B. Srinivasan, C. Blawert, W. Dietzel, Corros. Sci. 51 (2009) 2483.[22] H.H. Elsentriecy, K. Azumi, H. Konno, Surf. Coat. Technol. 202 (2007) 532.[23] M. Zhao, S. Wu, P. An, J. Luo, Mater. Chem. Phys. 103 (2007) 475.[24] G.H. Lv, H. Chen, L. Li, E.W. Niu, H. Pang, B. Zou, S.Z. Yang, Curr. Appl. Phys. 9
(2009) 126.[25] A.N. Khramov, V.N. Balbyshev, L.S. Kasten, R.A. Mantz, Thin Solid Films 514
(2006) 174.[26] M.B. Kannan, D. Gomes, W. Dietzel, V. Abetz, Surf. Coat. Technol. 202 (2008)
4598.[27] R.K.S. Raman, S. Murray, M. Brandt, Surf. Eng. 23 (2007) 107.
[28] J.R. Macdonald,Impedance spectroscopy theory, experiment, and applications,in: E. Barsoukov, J.R. Macdonald (Eds.), Data Analysis, John Wiley & Sons, Inc.,Hoboken, NJ, 2005.
[29] B.A. Boukamp, Solid State Ionics 169 (2004) 65.[30] X. Zhong,Q. Li,J. Hu,S. Zhang,B. Chen, S.Xu, F. Luo, Electrochim.Acta 55 (2010)
2424.[31] L.E.M. Palomino, P.H. Suegama, I.V. Aoki, Z. Pszti, H.G. de Melo, Electrochim.
Acta 52 (2007) 7496.[32] B. Conway, Impedance spectroscopy theory, experiment, and applications, in:
E. Barsoukov, J.R. Macdonald (Eds.), Impedance Behavior of ElectrochemicalSupercapacitors and Porous Electrodes, John Wiley & Sons Inc., Hoboken, New
Jersey, 2005.[33] M. Pourbaix, Atlasof Electrochemical Equilibria in Aqueous Solutions, National
Association of Corrosion Engineers, Houston, TX, 1974.[34] G.L. Song, A. Atrens, Adv. Eng. Mater. 1 (1999) 11.[35] G.L. Makar, J. Kruger, J. Electrochem. Soc. 137 (1990) 414.[36] G. Song, A. Atrens, W. Xianliang, B. Zhang, Corros. Sci. 40 (1998) 1769.[37] B. Beverskog, I. Puigdomenech, Corros. Sci. 39 (1997) 107.