3.3.1 OCP
The evolution of the Open circuit potential value, EOCP, with time for Al immersed in the 20% ethanol – 80% gasoline blend solution, without and with A. muricata extract is shown in Fig. 4. In the absence of the inhibitor, the EOCP value decreases from − 0.35 V to -0.43 V over 1800 s. The shift toward a slightly more negative EOCP value may be related to the reaction of Al and ethanol. According to Song et al., in the absence of water, ethanol causes the corrosion of Al through an alkoxidation reaction [36] where oxygen will react with ethanol to form acetic acid and water plus according to [37]:
$${C_2}{H_5}OH+{O_2} \to C{H_3}COOH+{H_2}O$$
6
Because the ethanol-gasoline blend has a high resistivity, acetic acid will corrode Al not in an electrochemical way, but in a chemical way that produces hydrogen gas and aluminum acetate:
$$Al+C{H_3}COOH \to Al{\left( {C{H_3}COO} \right)_3}+{H_2}$$
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Corrosion process will be enhanced by water and will produce protective layers of corrosion products, such as bayerite (Al(OH)3) or boehmite (AlOOH). The addition of the inhibitor causes a decrease in the EOCP value in the presence of 5 ppm, moving towards more active values from − 0.46 V to -0.48 V, indicating a greater susceptibility to corrosion, which can be attributed to a limited adsorption of the inhibitor. However, at concentrations of 10 ppm an increase in the EOCP value is observed compared to the concentration of 5 ppm. At concentrations of 20 ppm and 25 ppm, a slight variation in the EOCP values is evident, ranging between − 0.26 V to -0.32 V with a stable behavior. At a concentration of 50 ppm, the noblest potential is observed from − 0.28 V to 0.03 V with a trend towards more positive values as the immersion time passes. This shift of the EOCP value into the noble direction is due to the formation of a protective layer of corrosion products onto Al due to the adsorption of A. muricata extract which suggests a greater protection provided by the inhibitor due to its ability to adsorb on the Al surface.
3.3.2 LPR experiments
The linear polarization resistance (LPR) technique was used to determine the polarization resistance (Rp). The value of Rp can be used to calculate the corrosion current, which is inversely proportional to Rp, according to the Stern-Geary Eq. (8):
$${i_{corr}}=\frac{B}{{{R_p}}}$$
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Where B is a constant which depends upon the anodic and cathodic Tafel slopes, βa and βc respectively, according to following expression [38]:
$$B=\frac{{{\beta _a}{\beta _c}}}{{2.303({\beta _a}+{\beta _b})}}$$
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In the present study, the variation of Rp with time at different concentrations of the A. muricata extract over the Al exposed to the 20% ethanol-80% gasoline blend solution was evaluated as shown in Fig. 5. This figure shows that the Rp values of Al without corrosion inhibitor fluctuate between 1.2 x107 and 2.3 x108 ohm cm2 over time, indicating the formation and desorption of an aluminum oxide layer, Al2O3, on the surface of the material. When adding the A. muricata extract to concentrations higher than 5 ppm, an increase in the Rp values is observed due to the formation of a protective layer of corrosion products onto the metal surface, although some fluctuations ranging between 1.6 x107 and 9.5 x108 ohm cm2 can be observed. These fluctuations are to the adsorption/desorption processes of the corrosion products layer from the Al surface. It is evident that the highest Rp value during the first weeks of exposure is obtained with an inhibitor concentration between 25 and 50 ppm; however, as exposure time continues, towards the end of the test, the highest Rp values are obtained with an inhibitor concentration of 25 ppm due to the inhibitor degradation and desorption from the Al surface. It is evident that A. muricata extract provides protection to Al during the whole time of exposure and continues to demonstrate its effectiveness after 90 days. These results demonstrate the adsorption capacity of the molecules present in the A. muricata extract.
3.3.3 Electrochemical Impedance Spectroscopy (EIS)
To have an insight on the corrosion mechanism for Al in the ethanol-gasoline blend solution in the absence and in the presence of different concentrations of the A. muricata extract, EIS diagrams in both the Nyquist and Bode representations, obtained after 7 and 91 immersion, are represented in Fig. 6 and Fig. 7 respectively. The Nyquist diagram after 7 days of immersion is shown in Fig. 6a, where it can be observed the presence of a single depressed, capacitive semicircle at high and low frequencies, indicating that the corrosion process is controlled by charge transfer. The addition of the inhibitor at all concentrations does not modify the shape of the spectra, indicating that the corrosion mechanism remains unaltered by the addition of the inhibitor, and is controlled by the transfer of electrons through the double electrochemical layer. The diameter of the semicircle increased in the presence of the inhibitor, reaching its maximum value when 50 ppm of A. muricata extract was added. This indicates the formation of a protective layer formed by the adsorption of the inhibitor on the metal surface, which increases the corrosion resistance of Al in the ethanol-gasoline blend solution.
On the other hand, bode plots in the modulus-frequency mode (Fig. 6b), shows that the impedance modulus values increased with the addition of the inhibitor, reaching values between 107 and 108 ohm cm2, but there is a decrease in the concentration of 25 ppm, the protective layer formed on the metal surface may be desorbed in this case. In the bode phase angle diagram (Fig. 6b), broader peaks can be observed at low frequencies with the addition of the inhibitor at all concentrations, where the phase angle remained constant over a wide interval of frequencies, which implies the presence of at least two time constants and at the frequency intermediate, the phase angle is close to 90º, which represents the capacitive behavior of the Al surface. According to the literature, a phase angle of 90º corresponds to an ideal capacitive behavior indicating a metal covered by a very protective corrosion products layer [39].
After 91 days of immersion, Nyquist diagrams (Fig. 7a), a single capacitive semicircle can be observed at all frequency values without and with the A. muricata extract, indicating that the corrosion mechanism is still controlled by charge transfer. With the addition of the inhibitor, the diameter of the semicircle increased at all concentrations, which means that the dissolution of Al in the ethanol-gasoline blend solution decreased considerably. This is attributed to the adsorption of the A. muricata extract molecules on the metal surface.
The bode plots (Fig. 7b) show higher impedance modulus values than those obtained after an exposure time of 7 days at all inhibitor concentrations, this indicates an improvement in protection over time that may be due to the continuous formation of a protective layer on the metal surface that acts as a barrier that reduces the transport of corrosive species to the Al surface. The phase angle (Fig. 7b) remains almost constant over a wide intervals of frequency values, with values close to -90, which is characteristic of the capacitive response of a compact protective film.
The data obtained by EIS were simulated using an equivalent electrical circuit model, as shown in Fig. 8. In this figure, Rs represents the solution resistance, Rct is the charge transfer resistance, CPEdl is a phase element constant that replaces the electrochemical double layer capacitance (Cdl), due to surface roughness, non-uniform distribution of current during the corrosion process and inhomogeneous distribution of reaction rates on the electrode surface [40]. Rf and CPEF are the resistance and constant phase element related to the capacitance of the corrosion products film formed on the Al surface, respectively. The electrochemical impedance of the constant phase element follows Eq. (6):
$${Z_{CPE}}=\frac{1}{{Q{{\left( {J\omega } \right)}^n}}}$$
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where Q is a constant associated with the double layer capacitance, j=√-1 is the imaginary unit, ω is the angular frequency and n represents the empirical exponent with values between − 1 and 1. The value of n is related to the electrode surface heterogeneity in relation to the electrochemical response of the EIS measurement. A value of n = 1 corresponds to an ideal capacitor behavior, n = 0 to an ideal resistance and n=-1 to an ideal inductance [41, 42].
Electrochemical parameters obtained by simulating the EIS data are shown in Tables 2 and 3. The efficiency of A. muricata extract (I.E.%) according to the EIS parameters can be evaluated by Eq. (7):
$$I.E.(\% )=\frac{{{R_{ct}} - R_{{ct}}^{ \circ }}}{{{R_{ct}}}} \times 100$$
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where Rct and Rºct represent the charge transfer resistance in the presence and absence of the A. muricata extract. Results given in Tables 2 and 3 show high values of Rs that can be attributed to a higher percentage of gasoline in the blend, resulting in an increase in the solution resistivity. The presence of A. muricata extract reduces the CPEdl value due to the replacement of water molecules by the adsorbed organic molecules of the A. muricata extract at the metal-solution interface, which leads to an increase in the thickness of the electrochemical double layer because the inhibitor molecules size is higher than that for water, since, according to the following expression, the double electrochemical layer capacitance is given by:
$${C_{dl}}=\left( {\frac{{\varepsilon {\varepsilon _0}}}{\lambda }} \right)A$$
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where ε0 is the free space permittivity, ε the dielectric constant of that space, λ the thickness of the double layer, and A the electrode surface area. An increase in the thickness of the double layer leads to a decrease in the Cdl value [43]. On the other hand, the reduction in the CPEf value is due to an increase in the film resistance value, Rf, when the inhibitor is added since these parameters are inversely proportional.
Generally speaking, the Rct values were higher than those for Rf, and this is due to the low dissolution rate of Al in this environment, which implies a low diffusion of Al3+ ions through the double electrochemical layer. The values for Rct and Rf increase from values of 107 to 108 ohm cm2 in the presence of the A. muricata extract, indicating the adsorption of organic molecules to the Al surface. In addition, Rf and Rct increase after 91 days of immersion in the ethanol-gasoline blend solution (Table 4). This suggests the formation of a more resistant protective layer on the surface of the metal that decreases the corrosion rate of Al. The values of ndl and nf are close to 1, which indicates a low heterogeneity on the surface of Al due to a low metal corrosion rate and a behavior capacitive. The inhibitory efficiency reaches a value of 94% at concentrations of 20 ppm and 25 ppm after 91 days of immersion. These concentrations agree with the results of greater efficiency obtained in the gravimetric measurement of weight loss.
Table 2
Electrochemical parameters used to simulate EIS data for Al exposed to the 20% ethanol-80% gasoline blend solution with different concentrations of A. muricata extract after 7 days of immersion.
Cinh (ppm) | Rs (ohm cm2) | CPEdl (F/cm2) | ndl | Rf (ohm cm2) | CPEf (F/cm2) | nf | Rct (ohm cm2) | I.E. (%) |
0 | 479 | 2.99 x 10− 9 | 1.0 | 9.81 x 106 | 1.06 x 10− 8 | 0.9 | 3.13 x 107 | --- |
5 | 422 | 2.48 x 10− 9 | 1.0 | 2.28 x 107 | 2.28 x 10− 7 | 0.9 | 1.04 x 108 | 70 |
10 | 489 | 2.84 x 10− 9 | 1.0 | 5.06 x 107 | 5.10 x 10− 8 | 0.9 | 4.84 x 107 | 35 |
20 | 133 | 2.74 x 10− 9 | 1.0 | 4.25 x 107 | 1.36 x 10− 9 | 0.9 | 7.65 x 107 | 60 |
25 | 591 | 4.24 x 10− 9 | 1.0 | 5.94 x 106 | 3.41 x 10− 8 | 0.8 | 2.09 x 107 | -50 |
50 | 480 | 2.54 x 10− 9 | 1.0 | 3.27 x 107 | 1.17 x 10− 9 | 0.9 | 2.07 x 108 | 85 |
Table 3
Electrochemical parameters used to simulate EIS data for Al exposed to the 20% ethanol-80% gasoline blend solution with different concentrations of A. muricata extract after 91 days of immersion.
Cinh (ppm) | Rs (ohm cm2) | CPEdl (F/cm2) | ndl | Rf (ohm cm2) | CPEf (F/cm2) | nf | Rct (ohm cm2) | I.E. (%) |
0 | 359 | 3.73 x 10− 9 | 1.0 | 7.84 x 107 | 1.22 x 10− 8 | 0.9 | 1.25 x 108 | --- |
5 | 405 | 3.61 x 10− 9 | 1.0 | 1.35 x 108 | 1.39 x 10− 8 | 0.9 | 4.52 x 108 | 38 |
10 | 401 | 3.13 x 10− 9 | 1.0 | 3.03 x 108 | 5.08 x 10− 9 | 0.9 | 1.75 x 109 | 93 |
20 | 461 | 3.43 x 10− 9 | 1.0 | 1.39 x 109 | 1.71 x 10− 9 | 1.0 | 2.15 x 109 | 94 |
25 | 330 | 3.65 x 10− 9 | 1.0 | 1.16 x 109 | 2.68 x 10− 8 | 0.9 | 1.93 x 109 | 94 |
50 | 334 | 3.07 x 10− 9 | 1.0 | 3.47 x 108 | 1.21 x 10− 9 | 0.9 | 1.23 x 109 | 90 |
3.3.4 Electrochemical noise (EN)
The time noise series in current and potential obtained for Al after an immersion time of 91 days in the ethanol-gasoline blend solution and in the absence and presence of different concentrations of A. muricata extract are shown in Fig. 9.
In the absence of the inhibitor (Fig. 9a), low-frequency current transients in the order of 10− 8 mA/cm2 are observed, which are characterized by a rapid increase in current followed by a slow drop in current. These types of transients indicate the formation of a localized type of corrosion such a pitting, due to the breakdown of a passive layer formed on the metal surface when an increase in current occurs and a slow repassivation when the current decreases [44]. In the time series of electrochemical noise in potential, low-intensity transients are observed with a tendency towards more noble potentials that can be attributed to the ability of Al to form a passive layer of aluminum oxide on its surface.
With the addition of the A. muricata extract (Figs. 9b-9f), the current density decreases in the order of up to 10− 9, that is, the A. muricata extract adsorbs to the Al surface, forming a layer of corrosion products much more resistant to be broken down, and thus, reducing the susceptibility to pitting corrosion. In the time series but in the potential, a trend towards more noble potentials is observed at all concentrations of the inhibitor, which indicates a lower susceptibility of aluminum to corrode in the 20% ethanol-80% gasoline blend solution in the presence of the inhibitor.
The noise resistance (Rn) was calculated by the ratio of the standard deviation in potential, σE, and the standard deviation in the noise in current, σI, (Eq. 9) [45].
$${R_n}=\frac{{{\sigma _E}}}{{{\sigma _I}}}$$
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Figure 10 shows the results obtained for the noise resistance of Al in relation to the concentration of the A. Muricata extract during 91 days of immersion in the ethanol-gasoline blend solution. The Rn values increased in the presence of the inhibitor in the order of 108 ohm cm2, which are in agreement with the values obtained for Rp and Rct obtained in the linear polarization resistance and electrochemical impedance spectroscopy techniques, respectively, which is very encouraging.