F. El-Taib Heakal*a,
M. A. Deyabb,
M. M. Osmanb,
M. I. Nessimb and
A. E. Elkholyb
aChemistry Department, Faculty of Science, Cairo University, 12613 Giza, Egypt. E-mail: fakihaheakal@yahoo.com; feltaibheakal@gmail.com; Fax: +20 35738425; Tel: +20 1002449048
bDepartment of Analysis and Evaluation, Egyptian Petroleum Research Institute, 11727 Cairo, Egypt
First published on 9th October 2017
Three gemini surfactants were synthesized having the same length of terminal chain but differing in the spacer chain length and they were evaluated as corrosion inhibitors for carbon steel in oilfield water using weight loss, EIS, potentiodynamic polarization and open-circuit potential measurements. These measurements revealed that the synthesized materials have served as effective mixed-type corrosion inhibitors. Their adsorption on a carbon steel surface was well described by means of the Langmuir adsorption isotherm. The activation parameters for the dissolution of carbon steel in solutions of oilfield water in the absence and presence of these inhibitors were calculated. The effect of immersion time on the stability and durability of protective films adsorbed on a carbon steel surface was studied using weight loss method. Ex situ inspection, i.e. post-exposure analysis, for the treated carbon steel surface has been performed using SEM, EDX and FT-IR tools.
Among the methods followed for protecting metals against their corrosion is using corrosion inhibitors. It is the most suitable procedure because of its high efficiency, economic advantages, and wide applicability in various fields.5 A corrosion inhibitor is any material that can reduce the corrosion rate of a metal6 via displacing water molecules from the vicinity of the metallic surface then its molecules can interact with the anodic and/or cathodic sites by adsorption.7 These materials can be classified according to their chemical nature into three genres: (i) inorganic inhibitors, (ii) organic inhibitors, and (iii) mixed-compound inhibitors.8 Nevertheless, most commonly used inhibitors are organic compounds especially those containing hetero atoms (O, N and/or S)9 and/or those containing multiple bonds or aromatic rings (π-systems).10 Inhibition process can be performed by electrons transfer between the inhibitor and the metal surface (vacant d-orbitals) forming coordinate covalent bonds between them.11 Furthermore, adsorption can be due to electrostatic interaction between the metal surface and inhibitor molecules.12 As a result, inhibitor adsorption relies on the surface charge of the metal, i.e., the adsorption of cations is favored if the net charge is negative while adsorption of anions is favored when the case is reversed.11
Surfactants, or surface active agents, are a general class of organic chemical compounds of amphiphilic molecules, each of them contains a hydrophobic (non-polar) tail and a hydrophilic (polar) head.13 Usually, the hydrophilic head (either polar or ionic group) of surfactant molecule attaches to the metal surface and its tail or hydrophobic moiety extends away from the interface towards the solution bulk forming an array of hydrophobic tails which leads to a change in the electrochemical behavior of metal (increasing the corrosion resistance).14 Gemini surfactants are a class of surfactants in which the molecule is composed of two identical molecules of ordinary surfactant linked together via a linkage called spacer (Fig. 1).15 This spacer may be hydrophilic or hydrophobic, short or long and rigid or flexible.16 The current study aims to investigate the corrosion inhibition efficiency of some developed cationic gemini surfactants for C-steel in oilfield water. These surfactants were prepared in the series of α,ω-alkanediyl bis(3-dodecylimidazolium-1-yl)dibromide with the same length of terminal chains but differing in the length of spacer chain (2, 6 and 10 methylene groups).
The test solution used in this study was oilfield water free from oils and greases. It was collected from several Egyptian oilfields. The physical properties and chemical composition of oilfield water are shown in Tables 1 and 2, respectively. The components of this medium are known to be highly corrosive to the oil extraction structures.17,18
Physical property | Value |
---|---|
Total dissolved solids | 111.9255 g l−1 |
Conductivity | 14.61 mohs cm−1 @ 20.1 °C |
Resistivity | 0.0685 ohm m @ 20.1 °C |
Salinity | 109.5072 g l−1 |
pH | 6.85 @ 25 °C |
Density | 1.0842 g ml−1 @ 15.56 °C |
Specific gravity | 1.0853 |
Hardness | 25.0657 g l−1 |
Constituents | Concentration (mg l−1) | Constituents | Concentration (mg l−1) |
---|---|---|---|
Lithium | 0.01 | Fluoride | 0.00 |
Sodium | 30543.00 | Chloride | 66368.00 |
Potassium | 3402.13 | Bromide | 209.45 |
Magnesium | 1197.24 | Nitrate | Nil |
Calcium | 8063.85 | Hydroxide | Nil |
Iron | 38.69 | Carbonate | Nil |
Copper | 0.15 | Bicarbonate | 244.00 |
Strontium | Nil | Sulfate | 1859.00 |
Barium | Nil |
Anions and cations of oilfield water were determined according to ASTM D-4327 and 6919, respectively using ion chromatography. The instrument used was Dionex IC model ICS 1100 equipped with high capacity columns (AS9 and CS12) for anion and cations, respectively. Heavy metals present in oilfield water were determined using Flame Atomic Absorption Spectrophotometer model Zenit 700p according to ASTM D4691. Physical properties of oilfield water including density, specific gravity, pH, etc., were measured according to the following standard procedures:
• TDS was determined according to ASTM D-1888.
• Conductivity and resistivity was determined on site using digital conductivity meter WTW 330I according to ASTM D-1125.
• Density and specific gravity was determined according to ASTM D-1429.
• pH value was determined according to ASTM D-1293 using digital pH meter model Mettler Toledo-Seven Go.
• Alkaline species (CO32−, OH−, and HCO3−) were measured according to ASTM D-3875 calculations was done using Alkalinity calculator ver. 2.10 (USGS).
The corrosion inhibitors used in this study are some cationic gemini surfactants differing in the length of spacer chain (2, 6 and 10 methylene groups). For simplicity, they are abbreviated according to their spacer length as GS2, GS6 and GS10, respectively. The chemicals from which these gemini surfactants are prepared have been purchased from Alfa Aesar Co. These chemicals are namely, 1H-imidazole (99%), 1-bromododecane (98%), 1,2-dibromoethane (99%), 1,6-dibromohexane (97%), 1,10-dibromo decane (97%), acetonitrile (HPLC grade) and KOH (pellets).
(1) |
(2) |
In case of the electrochemical impedance spectroscopy, the corrosion inhibition efficiency (Ei%) for all inhibitors was calculated from the value of the total resistance (Rt) of the metal surface (Rt = Rf + Rct = R1 + R2) obtained from EIS measurements, according to the following equation:20,21
(3) |
The potentiodynamic polarization measurements were carried out at a scan rate of 5 mV s−1 starting from −1 to −0.4 V (vs. SCE). The inhibition efficiency (Ep%) was determined using corrosion current density according to eqn (4):20,22
(4) |
• Aliphatic C–H stretching bands appear at 2923–2854 cm−1.
• Aromatic C–H stretching bands appear at 3099 cm−1.
• N–H stretching bands (broad) appear at 3407 cm−1. This could be attributed to the presence of the carbene proton in the form of NH+ (Scheme S1†).
• CC stretching bands appear at 2028 cm−1.
• C–C stretching bands appear at 1563 cm−1.
Fig. S3† demonstrates the H1-NMR spectrum of the intermediate compound. From the data listed in Table S2,† we can observe the following:
• The proton (a) has a high chemical shift which could be attributed to the presence of the carbene proton.
• The same protons (b) [with the value of 7.436 ppm], possesses the carbene type.
• The aromatic proton (c) has the value (6.969 ppm), whereas the aromatic protons (d) have the chemical shifts of 6.843 ppm. Both of the two types showed doublet spin multiplicity.
• Protons of the type (e), attached directly to nitrogen atom, have the value of 4.274.
• In the case of protons (f), the chemical shift appears at 3.864 ppm.
• The δ value of (g) protons is 1.703 ppm.
• In case of four protons (h), δ value is 1.187 ppm.
• The highly shielded protons of the monomer have the value of 0.812 ppm.
Fig. S5 through Fig. S7† display the FT-IR spectra of GS2, GS6 and GS10. The FT-IR absorption bands of the prepared gemini surfactants are listed in Table S1† and can be discussed as following:
• N–H stretching bands (broad) appear at: 3417 cm−1; GS2, 3416 cm−1; GS6 and 3419 cm−1; GS10 due to the presence of the carbene proton in the form of NH+ (Scheme 2).
• Aromatic C–H stretching bands appear at: 3039 cm−1 (GS2), 3073 cm−1 (GS6) and 3070 cm−1 (GS10).
• Aliphatic C–H stretching bands appear at: 2922–2852 cm−1 (GS2), 2924–2854 cm−1 (GS6) and 2923–2853 cm−1 (GS10).
• CC stretching bands appear at: 2042 cm−1 (GS2), 2062 cm−1 (GS6) and 2055 cm−1 (GS10).
• C–C stretching bands appear at: 1563 cm−1 (GS2), 1625 cm−1 (GS6) and 1623 cm−1 (GS10).
• C–Br (ionic bond) bands appear at: 635.7 cm−1 (GS2), 634.9 cm−1 (GS6) and 634.8 cm−1 (GS10).
Fig. S8 through Fig. S10† demonstrates the H1-NMR spectrum of GS2, GS6 and GS10. The chemical shifts of H1-NMR spectra for different types of protons in the three gemini surfactants (Fig. S11†) are listed in Table S3† and we can observe the following:
• The proton (a), [compounds GS2, GS6 and GS10], has high chemical shift (10.168, 10.177 and 10.323 ppm, respectively). This could be attributed also to the presence of the carbene proton in the form of NH+.
• The same protons (b) [with the values of 8.409, 9.375 and 9.274 ppm], possess the carbene type.
• The aromatic protons (c) have the values (7.376, 7.453 and 7.421 ppm), whereas the aromatic protons (d) have the chemical shifts of 7.270, 7.272 and 7.271 ppm. Both of the two types showed doublet spin multiplicity.
• Protons of the type (e), attached directly to N+, have the values of 4.534, 4.308 and 4.335 ppm respectively. The spin multiplicity of (e) proton is triplet.
• In case of compound GS2, the four protons (f) possess (δ) value of 4.202 ppm (triplet). Whereas the four (f) protons of compounds GS6 and GS10 have the values of 4.248 and 3.370 ppm with triplet spin multiplicity and the four (f*) protons possess (δ) values of 4.283 and 3.393 ppm respectively with multiplet spin multiplicity.
• The (δ) value of the four multiplet (g) protons in (GS2) is 4.094 ppm. In the case of GS6 and GS10, the eight (multiplet g) protons are approximately equal and possess 3.462 and 2.568 ppm respectively.
• In case of four protons (h) of GS2 and GS6, δ values are 1.881 and 1.854 ppm respectively with multiplet spin multiplicity. While in GS10, the twelve protons possess 1.844 ppm with multiplet multiplicity.
• The 32 protons (i) for GS2, GS6 and GS10 have the values of 1.273, 1.383 and 1.235 ppm respectively, with multiplet multiplicity.
• The highly shielded six protons of GS2, GS6 and GS10, have the values of 0.838, 0.811 and 0.842 ppm respectively with triplet spin multiplicity.
Table S4† illustrates the results of elemental analysis where the observed results are in good agreement with the calculated ones. The thermal stability of the three prepared gemini surfactants was assessed using thermogravimetric analysis (TGA). Fig. S12† shows that the three surfactants are stable up to 250 °C and completely lose their weights at 340 °C. Both GS6 and GS10 have comparable thermal stability but the gemini surfactant of shortest spacer (GS2) has showed a slight increase in the degradation temperature in comparison to both GS6 and GS10.
Inhibitor | Concentration (ppm) | Weight loss rate × 103 (mg cm−2 h−1) | Ew% |
---|---|---|---|
Blank | — | 5.30 | — |
GS2 | 50 | 4.16 | 21.49 |
100 | 1.98 | 62.69 | |
150 | 1.83 | 65.47 | |
200 | 1.72 | 67.64 | |
300 | 1.75 | 67.04 | |
400 | 1.75 | 67.05 | |
GS6 | 50 | 4.79 | 17.89 |
100 | 3.46 | 34.76 | |
150 | 3.29 | 37.93 | |
200 | 3.12 | 41.13 | |
300 | 2.65 | 62.30 | |
400 | 3.02 | 43.05 | |
GS10 | 50 | 2.04 | 61.53 |
100 | 0.85 | 83.98 | |
150 | 0.78 | 85.21 | |
200 | 0.85 | 83.96 | |
300 | 0.98 | 81.52 | |
400 | 1.27 | 76.01 |
Fig. 2 EIS spectra for C-steel in oilfield water as a function of GS2 concentration at 293 K in the Bode format (a) and Nyquist format (b). |
In an attempt to analyze the experimental impedance data, the equivalent circuit depicted in Fig. 330 was found to give a satisfactory fitting result with a maximum average error 0.3%. In this electrical model, two constant phase elements (Q1 and Q2) are used instead of the two real capacitances to give the best fitting. For a rough or porous surface, non-homogeneity can cause the double layer capacitance to appear as a constant phase element.31 This model consists of two-time constants ((Q1R1W) and (Q2R2)) parallel to each other and all in series to the solution resistance (Rs). The first time constant (Q1R1W) expresses the behavior at LF region and is attributed to the adsorbed film while the other one (Q2R2) is related to the HF region and describes the behavior of the double layer at the base of pores or defects in the film. The constant phase element has a non-integer parameter called the phase shift (n) which is used to compensate the system heterogeneity. So, the phase shift (n) can be described as a degree of surface roughness or non-homogeneity.32
Investigating the simulated data listed in Table 4 illustrates the following important points:
Inhibitor | C (ppm) | W (Ω cm2 s−0.5) | R1 (Ω cm2) | Q1 (μF cm−2) | n1 | R2 (Ω cm2) | Q2 (μF cm−2) | n2 | Rs (Ω cm2) | Ei% |
---|---|---|---|---|---|---|---|---|---|---|
Blank | — | 66.23 | 491.34 | 100.21 | 0.47 | 10.10 | 68.11 | 0.82 | 1.13 | — |
GS2 | 50 | 24.74 | 1010.04 | 136.81 | 0.537 | 14.25 | 62.21 | 0.836 | 1.2 | 51.05 |
100 | 7.5 | 1056.21 | 252.32 | 0.585 | 12.41 | 71.44 | 0.815 | 1.29 | 53.08 | |
150 | 7.21 | 1181.33 | 306.00 | 0.609 | 12.52 | 72.32 | 0.819 | 1.11 | 58.00 | |
200 | 11.39 | 1726.53 | 314.21 | 0.601 | 11.39 | 69.02 | 0.819 | 1.20 | 71.15 | |
300 | 30.75 | 1574.06 | 280.67 | 0.591 | 11.63 | 71.33 | 0.806 | 1.33 | 68.38 | |
400 | 35.23 | 1529.88 | 255.05 | 0.611 | 11.75 | 70.25 | 0.814 | 1.32 | 67.47 | |
GS6 | 50 | 150.08 | 654.08 | 62.67 | 0.42 | 17.12 | 51.75 | 0.804 | 1.29 | 25.29 |
100 | 27.87 | 802.85 | 104.14 | 0.484 | 13.47 | 47.65 | 0.753 | 1.35 | 38.57 | |
150 | 128.14 | 993.23 | 118.91 | 0.498 | 13.86 | 50.98 | 0.777 | 1.57 | 50.21 | |
200 | 1.85 | 1362.3 | 215.16 | 0.556 | 21.79 | 57.26 | 0.725 | 1.59 | 63.77 | |
300 | 740.15 | 1393.65 | 132.04 | 0.501 | 15.04 | 45.65 | 0.749 | 1.16 | 64.40 | |
400 | 2.62 | 1206.98 | 182.46 | 0.534 | 19.31 | 55.96 | 0.746 | 1.61 | 59.11 | |
GS10 | 50 | 7.46 | 1093.55 | 207.47 | 0.6 | 14.09 | 58.42 | 0.79 | 1.27 | 54.73 |
100 | 10.66 | 1471.74 | 177.05 | 0.61 | 19.93 | 54.81 | 0.79 | 1.28 | 66.38 | |
150 | 75.13 | 1951.4 | 131.65 | 0.58 | 22.54 | 51.79 | 0.79 | 1.36 | 74.60 | |
200 | 74.53 | 1749.33 | 129.4 | 0.58 | 20.09 | 52.35 | 0.82 | 1.37 | 71.66 | |
300 | 9.1 | 1633.34 | 161.19 | 0.62 | 25.95 | 48.25 | 0.8 | 1.33 | 69.78 | |
400 | 48.22 | 1507.94 | 121.37 | 0.57 | 22.65 | 49.26 | 0.82 | 1.15 | 67.24 |
(a) The solution resistance (Rs) is low and nearly remains constant either in the absence or presence of inhibitors (ranges between 1.11 and 1.61 Ω cm2) due to good conductivity of all tested solutions.33
(b) The resistance (R1) denoting to the resistance of the adsorbed film resistance (Rf) is generally with much higher values than those for R2 representing the charge transfer resistance (Rct). R2 possesses a value of 10.01 Ω cm2 (in blank oilfield water) and slightly increases up to a maximum value of 14.25 Ω cm2 in presence of GS2, 21.79 Ω cm2 in presence of GS6 and 25.95 Ω cm2 in presence of GS10. So, the change in R2 is not significant.
(c) Upon increasing the concentration of any gemini surfactant, a continuous significant increase in R1 value is observed. In the blank solution, R1 = 491.34 Ω cm2 but R1 increases to 1726.53 Ω cm2 (for oilfield water inhibited by 200 ppm GS2), 1393.65 Ω cm2 (for solution inhibited by 300 ppm GS6) and 1951.40 Ω cm2 (for solution inhibited by 150 ppm GS10). Above these concentrations, R1 suffers a small decrease in its value.
(d) Comparing the values of the heterogeneity parameter (n) indicates that n1 < n2. The value of n1 (relating to the adsorbed film) increases from 0.47 in the blank solution and reaches maximum values of 0.61, 0.56 and 0.62 in presence of GS2, GS6 and GS10, respectively. On the other hand, the values of n2 (relating to the double layer at the metal/native film interface) nearly remains constant in all cases. These indications suggest that the C-steel surface contains voids and pores and the presence of gemini surfactants leads to reduction in surface roughness due to the adsorption of their molecules on adsorption sites of the C-steel surface.31
Inhibitor | Conc. (ppm) | Icorr (μA cm−2) | Ecorr (V) | βa (V dec.−1) | βc (V dec.−1) | Ep% |
---|---|---|---|---|---|---|
Blank | — | 95.37 | −0.825 | 0.185 | −0.107 | — |
GS2 | 50 | 52.42 | −0.836 | 0.175 | −0.123 | 45.03 |
100 | 45.39 | −0.831 | 0.145 | −0.112 | 52.41 | |
150 | 37.28 | −0.844 | 0.127 | −0.098 | 60.91 | |
200 | 28.67 | −0.847 | 0.090 | −0.084 | 69.93 | |
300 | 31.34 | −0.842 | 0.107 | −0.091 | 67.14 | |
400 | 32.20 | −0.828 | 0.134 | −0.101 | 66.24 | |
GS6 | 50 | 67.93 | −0.861 | 0.195 | −0.113 | 28.77 |
100 | 56.64 | −0.872 | 0.175 | −0.099 | 40.61 | |
150 | 43.12 | −0.878 | 0.140 | −0.086 | 54.79 | |
200 | 35.98 | −0.880 | 0.126 | −0.077 | 62.28 | |
300 | 35.31 | −0.890 | 0.108 | −0.070 | 62.98 | |
400 | 36.58 | −0.887 | 0.047 | −0.039 | 61.65 | |
GS10 | 50 | 34.27 | −0.823 | 0.161 | −0.122 | 64.06 |
100 | 26.22 | −0.823 | 0.164 | −0.123 | 72.51 | |
150 | 18.36 | −0.821 | 0.118 | −0.105 | 80.75 | |
200 | 23.26 | −0.815 | 0.147 | −0.125 | 75.61 | |
300 | 24.34 | −0.822 | 0.169 | −0.128 | 74.47 | |
400 | 28.88 | −0.817 | 0.176 | −0.134 | 69.71 |
Fig. 4 Polarization curves for carbon steel in oilfield water as a function of GS2 concentration at 293 K. |
(1) Icorr values decrease with the increase in concentrations of gemini surfactants till their critical values (200 ppm for GS2, 300 ppm for GS6 and 150 ppm for GS10). After that, Icorr re-increases again because the surface becomes slightly bare and vulnerable to corrosion attack.
(2) For GS2, the maximum displacement in Ecorr is about −22 mV relative to Ecorr recorded in the blank solution. For GS6, the maximum Ecorr displacement is about −65 mV, while GS10 shows a maximum displacement in Ecorr of about +10 mV. By convention, if the magnitude of Ecorr displacement in the presence of inhibitor is >± 85 mV with respect to Ecorr in blank solution, the inhibitor is classified as cathodic or anodic-type inhibitor according to the direction of the potential shift either to the more negative or to the more positive direction, respectively. If the displacement in Ecorr is <85 mV, the inhibitor can be classified as a mixed-type inhibitor.20 So, GS2 and GS6 are mixed-type inhibitors with major cathodic effectiveness, while GS10 is a mixed type inhibitor but with a predominant anodic effect.
(3) Both anodic and cathodic Tafel slopes (βa and βc) are changed significantly for all gemini surfactants which confirms that these inhibitors affect mechanisms of both cathodic and anodic reactions (they belong to mixed-type inhibitors),35 where the displacement in the values of Tafel slopes is attributed to a change in reaction mechanism.20
The inhibition efficiency values increase as a function of concentration of gemini surfactants till certain values. Above these critical concentrations, the inhibition efficiency values start to decrease again with increasing concentration. There are two suggestions for explaining this behavior:
1 Mu et al.36 have studied the inhibitive effect of sodium dodecyl sulfonate (SDS) on mild steel in 2 M HCl and found that the maximum inhibition efficiency was obtained at 150 ppm and the inhibition efficiency decreases when surfactant concentration increases above this value. They explained this behavior in a manner that at the high concentration range, SDS adsorbed on the steel surface may form hemi-micelles through the interaction between their hydrophobic groups and these hemi-micelles are similar in structure to the normal micelles. According to this attitude, high concentrations of gemini surfactants lead to aggregation of their molecules which may lead to the desorption of some initially adsorbed ones.
2 Jiang et al.37 have proposed another mechanism for the decrease in the inhibition efficiency values above an optimum or a critical concentration based on the adsorption mode of surfactant molecules on steel surface as follows (Fig. 5):
(a) Below or at the optimum concentration surfactant molecules adsorb on steel surface in a parallel position (with respect to C-steel surface). As the surfactant concentration increases, more surfactant molecules adsorb on the steel surface leading to covering more active sides on the steel surface. When concentration reaching the optimum value, steel surface becomes covered with surfactant molecules to its maximum extent (Fig. 5(b)).
(b) Above the optimum concentration, the number of surfactant molecules becomes so much that electrostatic interactions between them force the initially adsorbed molecules (in their parallel position) to change their mode of adsorption to allow more number of molecules to adsorb on the metal surface. So, gemini surfactant molecules adsorb on the surface in a perpendicular position (with respect to C-steel surface) to permit steel surface to be attached to more and more surfactant molecules. Accordingly, the surface area occupied by surfactant molecules, despite their huge number, becomes lower than before. So, corrosive species have the chance again to attack the steel surface and hence the corrosion rate increases again (Fig. 5(c)).
Inh(sol) + xH2O(ads) → Inh(ads) + xH2O(sol) | (5) |
The mechanism of corrosion inhibition can be thus explained on the basis of adsorption principle41 and the nature of the interaction between the inhibitor and C-steel surface can be understood using an adsorption isotherm.42 Assuming that the gemini surfactants reduce the rate of corrosion process mainly through the increase in the degree of C-steel surface coverage (θ) by surfactant molecules, the inhibition efficiency can be considered as a function of θ, i.e. θ = 10−2 × E%.22 Frumkin, Freundlich, Temkin, Flory–Huggins and Langmuir adsorption isotherms have been attempted for fitting the adsorption of molecules of GS2, GS6 and GS10 on C-steel surface in oilfield water. It was found that the Langmuir model have showed the best fitting where it had the highest values of regression factor, r2. Langmuir isotherm is represented with a relation between and C according to eqn (6):40,43
(6) |
ΔGads = −RTln(106Kads) | (7) |
Fig. 6 Langmuir adsorption plots for carbon steel in oilfield water inhibited by gemini surfactants based on data from weight loss (a), EIS (b) and polarization (c). |
Inhibitor | Technique | r2 | Kads (ppm−1) | ΔG (kJ mol−1) |
---|---|---|---|---|
GS2 | Weight loss | 0.9995 | 0.107 | −28.20 |
EIS | 0.9806 | 0.022 | −24.39 | |
Tafel polarization | 0.9882 | 0.020 | −24.17 | |
GS6 | Weight loss | 0.9271 | 0.005 | −20.58 |
EIS | 0.9591 | 0.007 | −21.50 | |
Tafel polarization | 0.9793 | 0.009 | −22.14 | |
GS10 | Weight loss | 0.9877 | 0.267 | −30.44 |
EIS | 0.9930 | 0.079 | −27.47 | |
Tafel polarization | 0.9947 | 0.195 | −29.67 |
Fig. 8 Polarization curves for carbon steel in oilfield water free (a) and containing 300 ppm GS2 (b) at different temperatures. |
Inhibitor | Temperature (K) | Icorr (μA cm−2) | Ecorr (V) | βa (V dec.−1) | βc (V dec.−1) | Ep% |
---|---|---|---|---|---|---|
Blank | 283 | 63.58 | −0.793 | 0.239 | −0.132 | — |
293 | 95.37 | −0.824 | 0.185 | −0.107 | — | |
303 | 101.05 | −0.825 | 0.135 | −0.121 | — | |
313 | 114.70 | −0.827 | 0.057 | −0.569 | — | |
GS2 | 283 | 20.00 | −0.813 | 0.158 | −0.139 | 68.54 |
293 | 31.34 | −0.842 | 0.129 | −0.099 | 67.14 | |
303 | 38.78 | −0.831 | 0.128 | −0.096 | 61.62 | |
313 | 51.09 | −0.847 | 0.171 | −0.112 | 54.20 | |
GS6 | 283 | 23.51 | −0.811 | 0.139 | −0.109 | 63.02 |
293 | 35.31 | −0.890 | 0.108 | −0.070 | 62.98 | |
303 | 42.11 | −0.848 | 0.153 | −0.102 | 58.33 | |
313 | 49.12 | −0.815 | 0.079 | −0.082 | 57.17 | |
GS10 | 283 | 14.71 | −0.809 | 0.131 | −0.117 | 76.87 |
293 | 24.34 | −0.822 | 0.169 | −0.128 | 74.47 | |
303 | 34.27 | −0.806 | 0.174 | −0.134 | 66.09 | |
313 | 40.24 | −0.802 | 0.169 | −0.141 | 64.91 |
Thermodynamic activation parameters have an important role in understanding the inhibitive mechanism of organic additives.22 The apparent activation energy associated with C-steel corrosion in free and inhibited solutions of oilfield water was determined using Arrhenius plot (Fig. 9(a)) according to the following equation:24
Icorr = Ae(−Ea/RT) | (8) |
Fig. 9 Arrhenius plot (a) and transition state plot (b) for carbon steel in oilfield water in absence and presence of GS2, GS6 and GS10. |
Inhibitor | Ea (kJ mol−1) | r2 | ΔH* (kJ mol−1) | ΔS* (J mol−1 K−1) | r2 |
---|---|---|---|---|---|
Blank | 13.59 | 0.8731 | 11.12 | −170.01 | 0.8198 |
GS2 | 22.37 | 0.9813 | 19.89 | −148.93 | 0.9760 |
GS6 | 17.70 | 0.9529 | 15.22 | −163.94 | 0.9363 |
GS10 | 24.92 | 0.9626 | 22.44 | −142.29 | 0.9753 |
Analysis of the dependence of inhibition efficiency on temperature as well as the comparison of corrosion activation energies in the absence and presence of an inhibitor give useful information about the mechanism of inhibitor adsorption. Upon elevating the ambient temperature a simultaneous decrease in the inhibition efficiency together with a concurrent increase in corrosion activation energy (Ea) in presence of inhibitor compared to its absence confirms the formation of an adsorption film of physical nature (electrostatic). On the other hand, the increase in inhibition efficiency with raising temperature accompanied with a decrease in activation energy in the presence of inhibitor suggests a chemisorption mechanism.48 Physical adsorption arises by electrostatic interaction, while chemical adsorption occurs through a bond formation by sharing an electron.49 So, these gemini surfactants adsorb mainly via physical adsorption on C-steel surface.
Thermodynamic parameters of activation, enthalpy change (ΔH*) and entropy change (ΔS*), were calculated from eqn (9) using plot (Fig. 9(b)) where its slope equals and its intercept represents where h is Planck's constant (6.626 × 10−34 J s), NA is Avogadro's number (6.022 × 1023 mol−1), R is the general gas constant (8.314 J K−1 mol−1).24
(9) |
The ΔH* values of activation for the dissolution reaction of C-steel surface in oilfield water in the presence of GS2, GS6 and GS10 are high (19.89, 15.22 and 22.44 kJ mol−1, respectively) in comparison to that in absence of inhibitors (11.12 kJ mol−1). The positive signs of ΔH* reflect the endothermic nature of C-steel dissolution activated process which suggests the slow dissolution of C-steel surface in presence of inhibitors.38 Large and negative values of ΔS* show that the activated complex in the rate determining step represents an association rather than a dissociation step, meaning that a decrease in disordering or randomness takes place on going from reactants to the activated complex (molecules are in higher ordered state in the activated complex than in the initial state).22 Comparing the entropy of activation in both inhibited and uninhibited oilfield water reveals that the values of ΔS* are less negative in solutions containing GS2, GS6 and GS10 (−148.93, −163.94 and −142.29 J mol−1 K−1, respectively) than for uninhibited solution (−170.01 J mol−1 K−1). The thermodynamic values obtained for ΔS* are the algebraic sum of the adsorption of inhibitor molecules (solute) and desorption of water molecules (solvent). Hence, the increase in entropy of activation in presence of gemini surfactants is attributed to the increase in the solvent (H2O) entropy as a result of H2O molecules desorbed from C-steel surface.38
Fig. 11 Variation of the capacitance as a function of potential applied on carbon steel in oilfield water in the absence and presence of gemini surfactants at 293 K. |
Inhibitor | Ess vs. SCE (mV) | pzc vs. SCE (mV) |
---|---|---|
Blank | −656 | −737 |
GS2 | −670 | −760 |
GS6 | −656 | −738 |
GS10 | −645 | −739 |
Since the C-steel is positively charged either in inhibited or uninhibited oilfield water, the inhibitor molecules can be adsorbed on the metal/solution interface by one or more of the following ways 38: (i) donor–acceptor interactions between the π-electrons of aromatic imidazolium ring and vacant d-orbitals of iron surface atoms. (ii) Unshared electron pairs of tertiary imidazolium N atoms and vacant d-orbitals of iron surface atoms. (iii) Interaction of d-electrons of iron surface atoms and the positive charge delocalized over the imidazolium ring. Gemini surfactants may also adsorb on positively charged C-steel surface in a manner that anions (e.g. Cl−, Br− and HCO3−) adsorb directly on C-steel surface then molecules of cationic gemini surfactants adsorb on the anionic layer.35
According to Heakal and Elkholy,15 research works that have studied the effect of spacer revealed two contradictory opinions: (i) the inhibition efficiency decreases with increasing the length of spacer chain. This behavior has been explained such that the increase in the number of methylene units in the spacer chain leads to an increase in the molecule flexibility. This hinders the adsorption of the gemini surfactant on metal surface and thus the inhibition efficiency decreases. (ii) The inhibition efficiency increases as the length of spacer chain is increased. This can be explained assuming that lengthening the spacer chain increases the degree of surface coverage and also the average area occupied by each adsorbed molecule. Hence, the inhibition efficiency increases. Both phenomena have been observed in our study for the three gemini surfactants having the same terminal chain length (dodecyl group) and differing in the spacer length (2, 6 and 10 methylene groups). Data obtained from electrochemical and chemical measurements confirm that GS10 > GS2 > GS6 in inhibition efficiency as well as their critical concentrations follows the trend: GS10 < GS2 < GS6, i.e. 150 ppm, 200 ppm and 300 ppm, respectively. In other words, GS10 demonstrates higher efficiency at lower concentration than GS2 which, in turn, shows also higher efficiency at lower concentration than GS6. This behavior can be elucidated as follows (Fig. 12):
(1) For the gemini surfactant of shortest spacer (GS2), the very short spacer allows the terminal chains to be very close to each other. So, there is a degree of attraction forces between adjacent chains in the same molecule and between neighboring molecules by hydrophobic interaction.51 This leads to the presence of arrays of stacked molecules which represent a barrier against corrosive molecules to penetrate to C-steel surface (Fig. 12(a)).
(2) On the other hand, GS6 has a longer spacer and its terminal chains are far away from each other so there are weak hydrophobic interactions between the terminal chains. In addition, a specific region on C-steel surface can be covered by a number of GS6 less than GS2. In this case there may be voids or weak regions through which corrosive species can attack C-steel surface (Fig. 12(b)).
Unlike GS2 and GS6 whom molecules are predicted to adsorb on C-steel via vertical orientation, GS10 molecules are expected to adsorb on C-steel surface via lateral interactions due to the absence of hydrophobic interactions between terminal chains. So, both terminal chains in GS10 molecule can extend over C-steel surface instead of being extended in the solution (Fig. 12(c)). Moreover, this mode of interaction allows more GS10 molecules to overlay on each other forming multilayers. So, GS10 forms a tough barrier against corrosive species.
A conclusion can be gained from these observations that very short and very long spacer-gemini surfactants are more efficient than those of intermediate spacers. This assumption compromises between the previously mentioned contradictory phenomena concerning the effect of spacer length on the corrosion inhibition efficiency.
Molecule | EHOMO (eV) | ELUMO (eV) | ΔE | I (eV) | A (eV) | χ (eV) | η (eV) | μ (Debye) |
---|---|---|---|---|---|---|---|---|
GS2 | −8.357 | −1.071 | 7.286 | 8.357 | 1.071 | 4.714 | 3.643 | 5.946 |
GS6 | −8.134 | −0.721 | 7.413 | 8.134 | 0.721 | 4.428 | 3.707 | 14.596 |
GS10 | −8.234 | −1.453 | 6.781 | 8.234 | 1.453 | 4.844 | 3.391 | 30.551 |
If Fe and an inhibitor molecule are brought together, electrons will flow from the less electronegative entity to the more electronegative one until the values of the chemical potential become equal. The parameters, electronegativity (χ) and global hardness (η), were calculated for the prepared gemini surfactants. These parameters are related to the electron affinity (A) and ionization potential (I), where: and I and A are related, in turn, to EHOMO and ELUMO as: I = −EHOMO and A = −ELUMO.55 Table 10 indicates that GS10 < GS2 < GS6 in the ELUMO whereas the trend is reversed in the case of the electronegativity of these compounds (χ). Thus, the more electronegative the molecule, the better its interaction with Fe surface. These observations indicate that these compounds may act as potential inhibitors for Fe corrosion via electron transfer from the metal surface to inhibitor where the transferred electrons are hosted in the antibonding molecular orbitals (LUMOs)56 and the measured inhibition efficiency follows the order GS10 > GS2 > GS6.
Fig. 16 SEM micrographs and EDX images for: (a) abraded C-steel surface, (b) surface of C-steel immersed in a solution of oilfield water. |
Assignment59,60 | N–H | Aromatic C–H | Aliphatic C–H | Combination N–H | Aromatic CC or CN | C–Br or γ-Fe2O3 | ||
---|---|---|---|---|---|---|---|---|
Absorption bands (cm−1) | GS2 | Before | 3417 | 3039 | 2922–2852 | 2042 | 1563 | 636 |
After | 3305 | — | 2923–2872 | — | 1628 | 560 | ||
GS6 | Before | 3416 | 3073 | 2924–2854 | 2062 | 1625 | 635 | |
After | 3404 | — | 2924–2854 | — | 1619 | 590 | ||
GS10 | Before | 3419 | 3070 | 2923–2853 | 2055 | 1623 | 635 | |
After | 3383 | — | 2923–2853 | — | 1606 | 600 |
(1) Weight loss method, polarization and EIS measurements have showed that the synthesized gemini surfactants (GS2, GS6 and GS10) are good inhibitors for the corrosion of C-steel in oilfield water and the inhibition efficiency increases with the inhibitor concentration up to a critical value above which the inhibition efficiency starts to decrease.
(2) The maximum inhibition efficiency values obtained from weight loss method for GS2, GS6 and GS10 are 67.64% at 200 ppm, 62.30% at 300 ppm and 85.21% at 150 ppm, respectively.
(3) EIS spectra of C-steel in oilfield water in absence and presence of any of the tested inhibitors show a two-time constant behavior and displays the features of Warburg impedance.
(4) The synthesized gemini compounds act as mixed-type corrosion inhibitors, retarding both anodic metal dissolution and cathodic reactions.
(5) The decrease in corrosion rate of C-steel as a function of each inhibitor concentration (till its critical value) indicates that its molecules adsorb on C-steel surface.
(6) Adsorption of molecules of each gemini surfactant is described according to Langmuir isotherm. Both physisorption and chemisorption processes are present but the former is predominant.
(7) Thermodynamic parameters calculated from polarization measurements indicate that the presence of these inhibitors increases the activation energy and these compounds are spontaneously adsorbed on C-steel surface mainly via physisorption mechanism.
(8) Surface analyses (SEM, EDX and FT-IR) confirm the adsorption of these inhibitors on C-steel surface.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra07176k |
This journal is © The Royal Society of Chemistry 2017 |