<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">MSA</journal-id><journal-title-group><journal-title>Materials Sciences and Applications</journal-title></journal-title-group><issn pub-type="epub">2153-117X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msa.2023.1411033</article-id><article-id pub-id-type="publisher-id">MSA-129011</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Corrosion Behaviour of Zr-Ag Alloys for Dental Implant Application
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Francesco</surname><given-names>Rosalbino</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Daniele</surname><given-names>Macciò</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Giorgio</surname><given-names>Scavino</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Dipartimento di Chimica e Chimica Industriale (DCCI), Università Degli Studi di Genova, Genova, Italy</addr-line></aff><aff id="aff1"><addr-line>Dipartimento di Scienza dei Materiali e Ingegneria Chimica (DICHI), Politecnico di Torino, Torino, Italy</addr-line></aff><pub-date pub-type="epub"><day>13</day><month>11</month><year>2023</year></pub-date><volume>14</volume><issue>11</issue><fpage>501</fpage><lpage>514</lpage><history><date date-type="received"><day>18,</day>	<month>July</month>	<year>2023</year></date><date date-type="rev-recd"><day>11,</day>	<month>November</month>	<year>2023</year>	</date><date date-type="accepted"><day>14,</day>	<month>November</month>	<year>2023</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The electrochemical corrosion behaviour of three Zr-Ag alloys (Zr-1Ag, Zr-3Ag and Zr-5Ag) was investigated. Open circuit potential, linear potentiodynamic polarization and electrochemical impedance spectroscopy (EIS) techniques were employed in aerated artificial saliva (pH = 4.0) at 37&amp;deg;C. Silver alloying additions are found to be effective in enhancing the corrosion resistance of zirconium in artificial saliva environment. In fact, Zr-Ag alloys exhibit higher open circuit potentials, larger breakdown potentials and higher impedance values as compared to cp Zr. This behaviour can be ascribed to the formation of a thicker and more stable passive film with increasing compactness, able to provide better protection against the corrosion attack.
 
</p></abstract><kwd-group><kwd>Zr-Ag Alloys</kwd><kwd> Corrosion Resistance</kwd><kwd> Open Circuit Potential</kwd><kwd> Potentiodynamic Polarization Curves</kwd><kwd> Electrochemical Impedance Spectroscopy (EIS)</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Zr is a valve metal characterized by very high stability in several aggressive environments and Zr alloys have been successfully employed in biomedical applications owing to their greater strength, lower cell cytotoxicity, lower magnetic susceptibility than titanium and excellent hemocompatibility [<xref ref-type="bibr" rid="scirp.129011-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref2">2</xref>] . Moreover, in vivo evidences have indicated that zirconium implants exhibit good osteointegration [<xref ref-type="bibr" rid="scirp.129011-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref4">4</xref>] and studies comparing zirconium and titanium implants showed that the degree of bone-implant contact is higher in the case of zirconium [<xref ref-type="bibr" rid="scirp.129011-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref6">6</xref>] . The advantageous Zr behaviour in vitro and in vivo has been ascribed to the presence of a protective surface oxide layer that reduces the corrosion rate, thereby minimizing ion release in bioenvironments and faciliting the osteointegration process [<xref ref-type="bibr" rid="scirp.129011-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref8">8</xref>] . Based on these characteristics, Zr and its alloys have been proposed as candidates for permanent implants [<xref ref-type="bibr" rid="scirp.129011-ref1">1</xref>] .</p><p>The oral cavity represents a very aggressive environment for metallic materials and the corrosion resistance is a fundamental factor in assessing their role as dental implants. In fact, the release of ions deriving from the corrosion of a metal or alloy stimulates the growth of macrophages. Moreover, a rough surface on the corroded metal promotes the adhesion of bacteria and the formation of plaque, which can induce periodontitis and gingivitis [<xref ref-type="bibr" rid="scirp.129011-ref9">9</xref>] . Furthermore, the fatigue failure of dental implants appears to be intimately related to the corrosion of metallic material [<xref ref-type="bibr" rid="scirp.129011-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref11">11</xref>] . Though zirconium exhibits high corrosion resistance in acid or alkali media, it is susceptible to localized corrosion induced by chloride ions [<xref ref-type="bibr" rid="scirp.129011-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref13">13</xref>] . Consequently, it would be of great importance to develop Zr alloys with a higher corrosion resistance in the oral environment since saliva typically presents concentrations of ca. 0.15 mass % Cl<sup>-</sup> [<xref ref-type="bibr" rid="scirp.129011-ref14">14</xref>] .</p><p>Recently, it has been reported that silver plays an important role in improving the corrosion resistance of titanium alloys in biological environments [<xref ref-type="bibr" rid="scirp.129011-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref18">18</xref>] . The beneficial effect of silver is attributed to its higher standard electrode potential (E<sub>0</sub> = 0.799 V) than titanium (E<sub>0</sub> = −0.98 V), which promotes the formation of stable titanium oxide film. Ag has excellent corrosion resistance in many aqueous solutions, and good in vivo biocompatibility. Some dental amalgams added with Ag have been successfully used as dental materials [<xref ref-type="bibr" rid="scirp.129011-ref19">19</xref>] .</p><p>Aim of the present work is to assess the corrosion behaviour of various Zr-Ag alloys with different compositions during exposure to artificial saliva environment. For the sake of comparison, cp Zr was also investigated in the same experimental conditions. The study was carried out using open circuit potential, linear potentiodynamic polarization and electrochemical impedance spectroscopy techniques in order to assess the potential ranges for the stability of the investigated materials, and to evaluate the resistance of the passive films formed on their surface.</p></sec><sec id="s2"><title>2. Experimental Details</title><p>Zr-Ag alloys (Zr-1Ag, Zr-3Ag, Zr-5Ag, mass %) were prepared starting from zirconium (99.999 mass %) and silver (99.9 mass %). Calculated amounts of the elements were weighed with an accuracy of 0.01 mg and arc-melted on a water-cooled copper plate under argon atmosphere. The samples were re-melted twice for homogenization, and possible mass losses were generally found to be negligible. A scanning electron microscope EVO 40 (Carl Zeiss), equipped with a Pentafet Link (Oxford Instruments) detector for EDXS analysis was used to examine the microstructures and measure alloy composition prior to electrochemical tests.</p><p>The Zr-Ag samples were made into electrodes by inserting insulated copper wires and protecting all sides but one with epoxy resin. Before the electrochemical characterization, all specimens were pre-treated by mechanical polishing of the electrode surface up to a mirror finish. The exposed geometric area was 0.5 cm<sup>2</sup>.</p><p>Electrochemical measurements were performed in Fusayama artificial saliva (0.4 g NaCl, 0.4 g KCl, 0.795 g CaCl<sub>2</sub>, 0.69 g NaH<sub>2</sub>PO<sub>4</sub>, 0.005 g Na<sub>2</sub>S, 1 g urea, and distilled water up to 1000 ml). The pH of the aggressive environment was adjusted to 4.0 by adding lactic acid in order to simulate physiological conditions representative of what a biomedical component would experience [<xref ref-type="bibr" rid="scirp.129011-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref23">23</xref>] . The artificial saliva was naturally aerated and the experiments were conducted without stirring. The temperature was maintained at 37˚C &#177; 1˚C using a thermostatic bath. Electrochemical measurements were performed using a conventional three-electrode glass cell with a large platinum sheet and a saturated calomel electrode (SCE) serving as the counter and the reference electrodes, respectively. The Zr-Ag alloys were studied in as-cast conditions.</p><p>Linear potentiodynamic polarization curves were recorded starting from −1000 mV/SCE and moving in the electropositive direction at a scan rate of 0.5 mV/s, after allowing a steady-state potential to develop. Open circuit potential, E<sub>OC</sub>, was measured with respect to the SCE every minute for a period of 2 h. All stationary measurements were performed using a Solartron 1286 Electrochemical Interface controlled by a personal computer.</p><p>Electrochemical impedance spectroscopy (EIS) measurements were carried out on the specimens subjected to various potential condition while exposed to artificial saliva. An EG&amp;G PAR system Model 2263 driven by a computer was employed for EIS measurements using 10 mV amplitude of sinusoidal voltage over a frequency range extending from 100 kHz to 10 mHz at seven points per decade. First EIS spectra were acquired at the open circuit potential attained by the samples after 2 h exposure to the aggressive environment. Next, the potential was set at +500 mV/SCE for 30 min before recording the EIS spectra of the polarized specimen. Experimental data were stored in the computer and processed according to the EQUIVCRT program (B.A. Boukamp, University of Twente).</p><p>For comparison, electrochemical experiments were also performed on cp Zr supplied by Johnson Matthey, London, UK.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>The open circuit potential, E<sub>OC</sub>, variations vs. exposure time of pure Zr and Zr-Ag alloys in artificial saliva, for a period of 2 h are reported in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The time profiles of E<sub>OC</sub> obtained for the investigated samples are typical of passive metals exposed to aerated solutions. For cp Zr, the initial open circuit potential is −850 mV (SCE), then it gradually changes towards more positive values and after 2 h of exposure a potential of −700 mV (SCE) is reached. The time profiles of E<sub>OC</sub> obtained for the Zr-Ag alloys are quite similar. The initial E<sub>OC</sub> for the Zr-1Ag alloy is −770 mV (SCE), then it progressively increases to nobler potentials reaching after 2 h a steady value of about −625 mV (SCE). For the Zr-3Ag alloy, the initial open circuit potential is −690 mV (SCE), then it gradually</p><p>increases and after 2 h exposure a steady value of nearly −550 mV (SCE), is reached. The initial E<sub>OC</sub> value for the Zr-5Ag alloy is −605 mV (SCE), then it increases progressively and after 2 h of immersion it remains stable at approximately −480 mV (SCE). The observed behaviour indicates that all the Zr-Ag alloys studied as well as cp Zr undergo spontaneous passivation due to the formation of an oxide film passivating the metallic surface, in artificial saliva solution.</p><p>Similar behaviour was found by Zhang et al. [<xref ref-type="bibr" rid="scirp.129011-ref20">20</xref>] , where an initial increase in the E<sub>OC</sub>s during the early minutes followed by stabilization observed on all the specimens (cp Ti and Ti-Ag alloys) suggests that a protective film formed rapidly on the metal surfaces in artificial saliva solutions and remained stable during the entire period of immersion (4.5 &#215; 10<sup>3</sup> s) [<xref ref-type="bibr" rid="scirp.129011-ref24">24</xref>] .</p><p>The initial E<sub>OC</sub> increase observed for both cp Zr and Zr-Ag alloys can be ascribed to the thickening of the oxide film formed at the specimen surface, thereby improving its corrosion protection ability in artificial saliva. The open circuit potential increases until the oxide layer reaches its limiting protective capacity, thus resulting in stabilization of E<sub>OC</sub> [<xref ref-type="bibr" rid="scirp.129011-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref26">26</xref>] .</p><p>As can be seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>, Zr-Ag alloys exhibit higher E<sub>OC</sub> values with respect to cp Zr, suggesting that silver alloying additions enhance the protection characteristics of the oxide layer, thus rendering the Zr alloys less prone to corrosion compared to cp Zr.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the potentiodynamic polarization curves of cp Zr and Zr-Ag alloys recorded in aerated artificial saliva at 37˚C. No active-passive transition is observed on the anodic branch of polarization curves, confirming the passive</p><p>behaviour of specimens in the aggressive environment pointed out from the E<sub>OC</sub> measurements. Both cp Zr and Zr-Ag alloys exhibit a passive potential range, ascribed to the formation and growth of a stable and protective oxide film, followed by a sharp increase in current density indicating breakdown of passivity and rapid growth of pitting.</p><p><xref ref-type="table" rid="table1">Table 1</xref> reports the values of the corrosion, E<sub>corr</sub>, and breakdown, E<sub>b</sub>, potentials found for the materials investigated, together with the extent of passive range, ΔE = E<sub>b</sub> − E<sub>corr</sub>, which provides a reliable measure of the breakdown resistance [<xref ref-type="bibr" rid="scirp.129011-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref28">28</xref>] . Based on these data, the corrosion resistance of cp Zr and Zr-Ag alloys in artificial saliva can be assessed. The corrosion potentials determined from the polarization curves are lower than those derived from E<sub>OC</sub> measurements. This is expected since polarization curves start at a cathodic potential of −1000 mV/SCE, therefore the passive film at the surface of samples is partially removed owing to the highly reducing initial potential. As can be seen, addition of increasing silver content leads to a positive shift of the corrosion potential, confirming the previous E<sub>OC</sub> measurements. Moreover, the breakdown potential progressively shifts towards more noble values and the extent of passive range gradually increases. Hence, increasing silver amounts progressively enhance the electrochemical stability of the oxide film, thus reducing the susceptibility to localized corrosion. Since the natural potential of human body ranges from +400 to +500 mV (SCE) [<xref ref-type="bibr" rid="scirp.129011-ref29">29</xref>] , the potential for breakdown of the passive film achieved by all Zr-Ag alloys in artificial saliva can be regarded safe enough for these materials to be proposed for dental implant.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> reports the EIS spectra, in the form of Nyquist diagrams, of cp Zr and Zr-Ag alloys at open circuit potential, after 2 h exposure to aerated artificial</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Corrosion potential, E<sub>corr</sub>, breakdown potential, E<sub>b</sub>, and extent of passive range, ΔE, for cpZr and Zr-Ag alloys determined by analysis of the anodic part of the polarization curves recorded in aerated artificial saliva at 37˚C</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sample</th><th align="center" valign="middle" >E<sub>corr</sub> (mV)</th><th align="center" valign="middle" >E<sub>b</sub> (mV)</th><th align="center" valign="middle" >ΔE = |E<sub>corr</sub> − E<sub>b</sub>| (mV)</th></tr></thead><tr><td align="center" valign="middle" >Zr</td><td align="center" valign="middle" >−700</td><td align="center" valign="middle" >420</td><td align="center" valign="middle" >1120</td></tr><tr><td align="center" valign="middle" >Zr-1Ag</td><td align="center" valign="middle" >−665</td><td align="center" valign="middle" >570</td><td align="center" valign="middle" >1235</td></tr><tr><td align="center" valign="middle" >Zr-3Ag</td><td align="center" valign="middle" >−640</td><td align="center" valign="middle" >700</td><td align="center" valign="middle" >1340</td></tr><tr><td align="center" valign="middle" >Zr-5Ag</td><td align="center" valign="middle" >−610</td><td align="center" valign="middle" >840</td><td align="center" valign="middle" >1450</td></tr></tbody></table></table-wrap><p>saliva at 37˚C. All Nyquist diagrams present depressed and incomplete capacitive semicircles, however cp Zr exhibits lower impedance values as compared with Zr-Ag alloys, the highest values being measured for the Zr-5Ag alloy. These results confirm an increase in corrosion resistance of zirconium related to silver alloying additions, in agreement with the results obtained from open circuit potential and potentiodynamic polarization measurements.</p><p>The zirconium/aggressive environment interface can be described by several equivalent circuit models, depending on the structure of the oxide film. The existence of a compact oxide film is represented by an equivalent circuit with one time constant [<xref ref-type="bibr" rid="scirp.129011-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref31">31</xref>] , whereas for a porous film, a circuit with two time constants is employed [<xref ref-type="bibr" rid="scirp.129011-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref33">33</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref34">34</xref>] .</p><p>Both cp Zr and Zr-Ag alloys characterized by EIS at their open circuit potential can be described by an equivalent circuit model with one time constant, and good agreement between experimental data and fitted data is obtained. The proposed equivalent circuit, shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>, assumes that the corrosion of</p><p>the passive metallic material is hindered by the presence of a surface oxide film that acts as a barrier-type compact layer [<xref ref-type="bibr" rid="scirp.129011-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref31">31</xref>] . The equivalent circuit consists of a series combination of the aggressive environment resistance, R<sub>s</sub>, and a single parallel constant phase element/resistor pair, Q<sub>ox</sub>/R<sub>ox</sub>, describing the properties of the passive film formed on the investigate materials, respectively the capacitance and resistance of the compact oxide layer.</p><p>A constant phase element, CPE, was used for fitting the impedance spectra instead of a pure capacitance owing to the non-ideal capacitive response due to the distributed relaxation feature of the oxide film. The impedance of the CPE is given by:</p><p>Z C P E = [ Y 0 ( j ω ) n ] − 1 (1)</p><p>where Y<sub>0</sub> is a constant, j<sup>2</sup> = −1 is the imaginary number, ω is the angular frequency and −1 ≤ n ≤ 1. The value of n seems to be associated with the non-uniform distribution of current as a result of roughness and surface defects [<xref ref-type="bibr" rid="scirp.129011-ref35">35</xref>] .</p><p>Analysis of the EIS spectra in terms of the equivalent circuit shown in <xref ref-type="fig" rid="fig4">Figure 4</xref> allows the parameter Q<sub>ox</sub> and R<sub>ox</sub> to be determined, and their values are reported in <xref ref-type="table" rid="table2">Table 2</xref>. The agreement between experimental and simulated data indicates that the experimental impedance spectra are well fitted to the proposed equivalent circuit. The fitting quality was evaluated by chi-squared (χ<sup>2</sup>) values of about 10<sup>−</sup><sup>4</sup>, with a relative error less than 5%. On the Nyquist plots in <xref ref-type="fig" rid="fig3">Figure 3</xref>, the experimental data are shown as individual points, while the fitted spectra are presented as continuous lines.</p><p>Capacitance values of the passive oxide film can be extracted from the CPE parameter, Q<sub>ox</sub>, using [<xref ref-type="bibr" rid="scirp.129011-ref36">36</xref>] :</p><p>C o x = ( R o x 1 − n Q o x ) 1 / n (2)</p><p>and are given in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>Comparing the capacitances for cp Zr and Zr-Ag alloys samples, it is possible to observe that pure zirconium has the highest capacitance value (about 82 μF cm<sup>−</sup><sup>2</sup>) when compared with that of the Zr-Ag alloys. This indicates a better capacitive effect of the oxide layers formed on Zr-1Ag, Zr-3Ag, Zr-5Ag specimens</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Electrical parameters of the equivalent circuit for cpZr and Zr-Ag alloys in aerated artificial saliva, pH = 4.0, at 37˚C. AC polarization was applied at their corresponding open circuit potential values in the aggressive environment</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sample</th><th align="center" valign="middle" >Q<sub>ox</sub> (10<sup>5</sup> S cm<sup>−2</sup> s<sup>n</sup>)</th><th align="center" valign="middle" >n</th><th align="center" valign="middle" >R<sub>ox</sub> (W cm<sup>2</sup>)</th><th align="center" valign="middle" >C<sub>ox</sub> (F cm<sup>−2</sup>)</th></tr></thead><tr><td align="center" valign="middle" >cpZr</td><td align="center" valign="middle" >1.5<sup> </sup></td><td align="center" valign="middle" >0.87</td><td align="center" valign="middle" >3.45 &#215; 10<sup>5 </sup></td><td align="center" valign="middle" >8.17 &#215; 10<sup>−5 </sup></td></tr><tr><td align="center" valign="middle" >Zr-1Ag</td><td align="center" valign="middle" >1.3</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >4.90 &#215; 10<sup>5 </sup></td><td align="center" valign="middle" >6.53 &#215; 10<sup>−5 </sup></td></tr><tr><td align="center" valign="middle" >Zr-3Ag</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >6.30 &#215; 10<sup>5 </sup></td><td align="center" valign="middle" >4.78 &#215; 10<sup>−5 </sup></td></tr><tr><td align="center" valign="middle" >Zr-5Ag<sub> </sub></td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >7.75 &#215; 10<sup>5</sup></td><td align="center" valign="middle" >2.94 &#215; 10<sup>−5</sup></td></tr></tbody></table></table-wrap><p>and, assuming a similar dielectric constant for such oxides, an increasing film thickness [<xref ref-type="bibr" rid="scirp.129011-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref38">38</xref>] , thereby confirming the previous E<sub>OC</sub> measurements. As can be seen in <xref ref-type="table" rid="table2">Table 2</xref>, both cp Zr and Zr-Ag alloys exhibit high R<sub>ox</sub> values, &gt;10<sup>5</sup> Ω cm<sup>2</sup>, indicating high corrosion resistance of these materials in artificial saliva. The presence of protective passive film provides the high corrosion resistance of specimens in this aggressive environment. However, the resistance of the oxide layer formed on cp Zr is lower than that measured for Zr-Ag alloys, the highest value being observed for the Ti-5Ag alloy. Low capacitances combined with high resistances suggest that the spontaneously formed passive film on Zr-Ag specimens becomes more compact and isolating on increasing the silver content in the alloy, affording better protection of the electrode surface against corrosion in artificial saliva.</p><p>EIS measurements were also carried out on the specimens polarized at +500 mV/SCE and the corresponding Nyquist plots are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>. By considering the impedance values two different behaviours can be distinguished: 1) Zr-Ag alloys exhibit higher impedances under anodic polarization than at the open circuit potential; and 2) cp Zr displays the opposite trend. The enhanced impedance showed by Zr-Ag alloys is indicative of additional growth of the passive film favoured by anodic oxidation. In this case, the impedance spectra can be satisfactorily fitted with the equivalent circuit reported in <xref ref-type="fig" rid="fig6">Figure 6</xref>, which is widely used to represent a bilayer structure of the anodic oxide films grown on valve metals such as Zr [<xref ref-type="bibr" rid="scirp.129011-ref39">39</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref40">40</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref41">41</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref42">42</xref>] . The model assumes that the duplex structure consists of a barrier-type compact inner layer and a porous outer layer. The equivalent circuit includes the solution resistance, R<sub>s</sub>, in series with two parallel constant phase element/resistor pairs, Q<sub>p</sub>/R<sub>p</sub> and Q<sub>b</sub>/R<sub>b</sub>, where R<sub>p</sub> corresponds to the resistance of the porous layer, R<sub>b</sub> to the resistance of the barrier layer, Q<sub>p</sub> to the capacitance of the porous layer and Q<sub>b</sub> to the capacitance of the barrier layer. A constant phase element, Q, representing a shift from the ideal capacitor was employed instead of the capacitance itself. A very good correlation between the fitted and the experimental data is also obtained for the polarized specimens. The values of fitted parameters are reported in <xref ref-type="table" rid="table3">Table 3</xref>. It can be seen that the values of R<sub>b</sub> are significantly higher than those determined for R<sub>p</sub>, indicating that the protection provided by the passive oxide film is predominantly due to the compact inner layer.</p><p>On the contrary, cp zirconium exhibits smaller resistances, over one order of magnitude, as compared to Zr-Ag alloys when anodically polarized, indicating a thinning of the oxide film or even losses of the film continuity attributable to localized corrosion phenomena. This means that the oxide film spontaneously formed at the surface of this sample at E<sub>oc</sub> during exposure to artificial saliva becomes instable during application of +500 mV (SCE). Accordingly, the underlying metal is directly exposed to the aggressive environment and corrodes in artificial saliva. In this case, a good agreement between fitted and experimental data is attained with the electrical model reported in <xref ref-type="fig" rid="fig7">Figure 7</xref>, which is typical for a corroding metal. The parameters R<sub>ct</sub> and Q<sub>dl</sub> account for the properties of the reactions at the passive film/artificial saliva interface and their values are displayed in <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>The observed behaviour suggests that the passive layers formed at the surface of Zr-Ag alloys more efficiently resist the onset of localized corrosion, in agreement with the results obtained from potentiodynamic polarization measurements.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Electrical parameters of the equivalent circuits for cpZr and Zr-Ag alloys after polarization at +500 mV (SCE) in aerated artificial saliva, pH = 4.0, at 37˚C</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sample</th><th align="center" valign="middle" >Q<sub>p</sub> (10<sup>5</sup> S cm<sup>−2</sup> s<sup>−n</sup>)</th><th align="center" valign="middle" >n<sub>p</sub><sub> </sub></th><th align="center" valign="middle" >R<sub>p</sub> (W cm<sup>2</sup>)</th><th align="center" valign="middle" >Q<sub>b</sub> (10<sup>5</sup> S cm<sup>−2</sup> s<sup>−n</sup>)</th><th align="center" valign="middle" >n<sub>b</sub><sub> </sub></th><th align="center" valign="middle" >R<sub>b</sub> (W cm<sup>2</sup>)</th><th align="center" valign="middle" >Q<sub>dl</sub> (10<sup>5</sup> S cm<sup>−2 </sup>s<sup>−n</sup>)</th><th align="center" valign="middle" >n<sub> </sub></th><th align="center" valign="middle" >R<sub>ct</sub> (W cm<sup>2</sup>)</th></tr></thead><tr><td align="center" valign="middle" >cpZr</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >2.8</td><td align="center" valign="middle" >0.85</td><td align="center" valign="middle" >2.1 &#215; 10<sup>4 </sup></td></tr><tr><td align="center" valign="middle" >Zr-1Ag</td><td align="center" valign="middle" >2.6</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >1.9 &#215; 10<sup>3 </sup></td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >6.0 &#215; 10<sup>5 </sup></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Zr-3Ag</td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >2.7 &#215; 10<sup>3</sup></td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >0.91</td><td align="center" valign="middle" >7.6 &#215; 10<sup>5 </sup></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Zr-5Ag<sub> </sub></td><td align="center" valign="middle" >2.4</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >3.5 &#215; 10<sup>3</sup></td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >9.5 &#215; 10<sup>5 </sup></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>The electrochemical results obtained in this study showed that silver is very effective in enhancing the corrosion resistance of zirconium, as evidenced by the increase in open circuit potential, breakdown potential and impedance values. Such increase in corrosion resistance is expected because Ag is a nobler element than Zr. Previous studies have shown that silver alloying additions improve the corrosion resistance of Ti by promoting spontaneous passivation in chloride-containing environments owing to enhanced cathodic reaction [<xref ref-type="bibr" rid="scirp.129011-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.129011-ref43">43</xref>] . The presence of silver at the solution/metal or solution/oxide/metal interface affects the kinetics of cathodic reaction on Zr by the following mechanisms: (a) increasing the exchange current density, i<sub>0</sub>, and/or (b) reducing the cathodic Tafel slope, b<sub>c</sub>. Therefore, the open circuit potential shifts to more noble values and the formed oxide film tends to thicken [<xref ref-type="bibr" rid="scirp.129011-ref44">44</xref>] . On the other hand, because of the higher electromotive force of silver compared to zirconium, Ag atoms may accumulate at the surface of Zr-Ag alloys during the initial stage of corrosion due to the preferential dissolution of Zr, thus promoting the formation of a more stable and compact passive film. As a result, the oxide film grown at the surface of Zr-Ag alloys exhibits improved barrier properties thereby exerting an effective inhibiting action towards the corrosion process.</p></sec><sec id="s4"><title>4. Conclusions</title><p>The corrosion behaviour of three Zr-Ag alloys has been assessed in artificial saliva (pH = 4.0) in order to investigate their potential use as materials for dental applications. The development of passivity for all the investigated materials is deduced from both open circuit potential measurements and potentiodynamic polarization curves, and the corrosion resistance of Zr-Ag alloys results from the development of a passive film at their surface.</p><p>Silver alloying additions reduce the susceptibility of zirconium towards localized corrosion, as evidenced by the shift of breakdown potential to more positive values. All Zr-Ag alloys exhibit pitting potentials higher than the potential values that may occur in the human body [<xref ref-type="bibr" rid="scirp.129011-ref29">29</xref>] . The potential for breakdown of the passive film achieved by all the investigated alloys can be regarded safe enough for these materials to be proposed for dental implant.</p><p>EIS measurements performed at the open circuit potential indicate that the oxide films formed at the surface of Zr-Ag alloys show better barrier properties compared to pure Zr. Such passive layers significantly inhibit the penetration of chloride ions, thus reducing the electrode corrosion rate. Moreover, impedance data obtained at potentials reported to be achieved in the human body for Ti implants highlight a thickening of these passive layers without the onset of localized corrosion phenomena, unlike what occurs on cp Zr where a thinning of the passive film or even losses of the film continuity due to localized corrosion reactions is observed.</p><p>Silver alloying additions not only promote the development of a thicker and more stable passive oxide film, but also increase its compactness, which contributes significantly to improve the corrosion resistance of Zr-Ag alloys.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Rosalbino, F., Macci&#242;, D. and Scavino, G. 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