3.1. Synthetic routes and structures of the two ligands EOIT and BOIT
The two valuable thiosemicarbazone ligands EOIT and BOIT (compounds 4 & 5, respectively in Scheme 1) were synthesized as sketched in Scheme 1 from the condensation of N-substituted isatin derivatives 2 and 3 with the thiosemicarbazide 1 under the known acidic method in EtOH/HCl under reflux for only 10 min under microwaves irradiations as reported previously [39]. The 1H NMR spectrum for the EOIT in dimethylsulfoxide-d6 is described in Figure 1. This 1H NMR data glistened with the four singlet signals at δ = 4.67 (CH2COOEt), 8.78, 9.13, 12.23 (3NH) ppm, the appearance of the two protons of the amino group (NH2) with two different chemical shift values at δ = 8.78 and 9.13ppm this means that they are magnetically different due to intramolecular-hydrogen bond which restricted or slowed rotation about the N–C bond [40, 41]. In addition, the presence of the two triplet (CH3) and the quartet (CH2) for the ethyl ester protons at δ = 1.2 and 4.15 ppm.
3.2. Comprehensive properties and constitution
All the physical, spectral and analytical data describing the two used ligands, POIT & BOIT and their Co(II) & Cu(II) chelates, POIT-Co, POIT-Cu, BOIT-Co and BOIT-Cu are illustrated in experimental section. Investigation of these results indicated good correlation between the found and calculated percent of carbon, hydrogen, nitrogen and metal content assuring the proposed composition of the metal chelates and also assuring the formation of the complexes in 1:1 (M:L) ration. The molar conductivity of complexes EOIT-Co, EOIT-Cu, BOIT-Co measured from 10-4 M solution of dimethyl formamide were found to lie within 19.5 -26.6 (W−1 cm2 mol−1) range which strongly supported the formation of non-conductance neutral complexes [42, 43]. On the other hand, the quite high value of molar conductance of BOIT-Cu; 85 W−1 cm2 mol−1, strongly recommended formation of 1:1 (cationic:Cl‑) electrolytic complex. The electrolytic or non-electrolytic behaviors of the complexes were qualitatively proved by the precipitation test with aqueous AgNO3 solution where only BOIT-Cu formed the white AgCl precipitate. Thus the formed complexes has been corroborated to have the formulae [Co(EOIT)Cl]•1.5H2O, [Cu(EOIT)Cl], [Co(BOIT)Cl2(H2O)]•5H2O and [Cu(BOIT)Cl]•Cl for EOIT-Co, EOIT-Cu, BOIT-Co and BOIT-Cu, successively. Solubility test of the metal chelates indicated that all the compounds are readily soluble in most polar solvent while hardly soluble or insoluble in alternative non-polar solvents.
3.3. Mass spectroscopy
Information excluded from the mass spectroscopy of the four isolated chelates have been investigated as it provides sufficient evidence to conclude the formula weights of the compounds in addition to their fragments and hence ensures the formation the complexes in the proposed formulae. The mass spectra of complexes EOIT-Co, EOIT-Cu, BOIT-Co and BOIT-Cu are illustrated in Figures 2 and 3. The molecular ion peak appearing in the spectra of complexes EOIT-Co, EOIT-Cu, BOIT-Co and BOIT-Cu at m/z = 399.5, 401, 496.02 and 444 amu have been assigned for [M], [M-3], [M+2] and [M], successively, excluding all the hydration water for EOIT-Co and 3 of the hydration water for BOIT-Co supporting the proposed formulae of the metal complexes. The multi‐peaks and other fragments are formed by cleavage at alternative positions in the complexes molecules..
3.4. FTIR spectra assignments
Comparison of the IR spectrum of each of EOIT and BOIT with that of their metal chelates is beneficial method to assign the binding function groups of the ligand to the cobalt or copper centers in the metal complexes and hence can help in structure identification of the metal complexes. From the spectrum of EOIT and BOIT, the bands obvious at 3377, 3238, 1743, 1697, 1557 & 1288 cm-1 for EOIT and at 3456, 3257, 1681, 1588 & 1275 cm-1 for BOIT. These bands, respectively, has been attributed to the stretching vibrations of NH(asy), NH(sym), C=O, C=N, and C=S [33]. All these bands underwent a position movement in complexes spectra owing to different reasons which helped in structure identification through assignment of binding modes. Firstly, the symmetric and asymmetric stretching vibrations of NH of amino group appearing in the ranges 3441-3380 cm-1 and 3257-3220 cm-1, undergoing a shift in their position whenever compared with the same bands in the ligand’s spectra. Such shift is mostly due to the participation of the group in hydrogen bond with the nearest electronegative atoms which coincided with the generation of alternative medium to weak intensity bands inside the range 2831-2710 cm−1 [43]. On the other hand, the significant shift recorded in the position of C=O, C=N and CS (C=S or C-S) peaks in the spectra of complexes upon comparison with their place in the ligand spectra has been explained by the coordination of the ligand to the Co or Cu centers as OSN tridentate monobasic thiol (i.e. EOIT-Co) or neutral thione ( i.e. EOIT-Cu, BOIT-Co and EOIT-Cu) modes of chelation [21,44]. Further support of the coordination of the carbonyl oxygen and azomethine nitrogen to the metal center is the appearance of two bands in the spectra of metal chelates within the ranges 574-510 cm−1 and 470-424 cm−1 with no corresponding bands in the spectra of free ligands. Such bands correspond to the stretching vibrations of M-O and M-N bonds, respectively [43].
3.4. Thermogravimetric analysis
Thermal responses of the metal chelates have been evaluated through TG analysis (thermogravimetric analysis). The TG thermograms of the four compounds are illustrated in Figure 4. From these thermograms it is obvious that the metal complexes decomposed within either two steps (EOIT-Cu), three steps (BOIT-Cu), four steps (EOIT-Co) or within five stages (BOIT-Co). The two steps thermogram of EOIT-Cu showed the first step of degradation within the temperature range 25-238 °C with weight loss of 33.67% (calcd 33.78%) which assigned to the loss of 1/2Cl2 and the organic fragment C4H7NO2. The rest of organic moiety completely lost giving Cu metal as residual product. For BOIT-Cu, the decomposition of the complex that occurred within three stages started at room temperature where the first step extended to 198 °C corresponding to loss of 8.36% (calcd 7.96%) of the total weight which corresponded to the forfeiture 1/2Cl2 of coordinated chloride. The following step which occurred within v198-262 °C range assigned to the loss of 11.93% (calcd 11.67) of the total weight and within this stage, the counter chloride anion get lost in addition to NH2 group. The last and third step appeared in the range 262-566 °C and appointed to the forfeiture of the rest of organic ligand with mass loss of 62.11% (calcd 62.57%) leaving CuO as residual product.
Thermal decomposition of the EOIT-Co and BOIT-Co occur according to the following Schemes (see Supplemental Files)
3.6. Electronic spectra and magnetic moments
UV-Vis spectra is regarded as one of the most helpful tools to assign the geometrical architectures around the metal centers and also to assure the binding modes of the ligands to the central metal ion. The UV-Vis of the two ligands EOIT & BOIT and their Co(II) & Cu(II) chelates, EOIT-Co, EOIT-Cu, BOIT-Co and BOIT-Cu were measured from DMSO solutions. Investigation of the spectra of the ligands indicated that spectral bands apparent at 265 & 370 nm and at 264 & 375 nm in the spectrum of EOIT & BOIT, respectively, are assignable to π→π* and n→π* transitions, respectively [43, 45]. Such transitions underwent a movement in their place in the spectra of metal chelates (Table 1) assuring the attachment of the azomethine nitrogen to the metal centers.
Addition to the to π→π* and n→π* transition bands appearing in the spectra of all complexes, the spectrum of the Co(II) complex EOIT-Co showed the medium to low intensity bands in the visible region at 528 & 736 nm, for EOIT-Co which are credited to 4A2→4T1 (υ2) and 4A2→4T1(P) (υ3) transitions, respectively, assuring four coordinate tetrahedral stereochemistry around Co(II) ions [46]. For the six coordinated Co(II) chelate and BOIT-Co, The spectrum exhibited low intensity bands at 588 nm assigned to 4T1g(F)→4A2g(F). The shoulder band appearing at 483 nm that can be assigned to 4T1g(F)→4T1g(p). Such transitions are characteristic for octahedral Co(II) chelates [47]. The values of the µeff was measured to be 4.25 and 4.63 B.M. for EOIT-Co and BOIT-Co, successively, which are close to reported values for high spin tetrahedral [48] and octahedral [1] Co(II) complexes.
The spectra of Cu(II) complexes; EOIT-Cu and BOIT-Cu complexes also allowed broad with low intensity bands at the low energy region which centered at 737 and 676 cm-1, respectively corresponding to 2B1g→2A1g transitions special for square planar divalent copper chelates [46]. The two complexes afforded µeff values of 1.82 and 1.88 B.M. for EOIT-Cu and BOIT-Cu, respectively, which supports the results of electronic spectra.
Table 1: Electronic absorption results and µeff values of the Co(II) and Cu(II) under interest
Complex
|
Wavelength
(cm-1)
|
Assignment
|
Geometry
|
µeff
(B.M.)
|
EOIT
|
265
370
|
π -π*
n-π*
|
-
|
-
|
EOIT-Co
|
273
374
528
736
|
π -π*
n-π*
4A2→4T1 (υ2)
4A2→4T1(P) (υ3)
|
tetrahedral
|
4.25
|
EOIT-Cu
|
251
375
737
|
π -π*
n-π*
2B1g→2A1g
|
square planar
|
1.82
|
BOIT
|
264
375
|
π -π*
n-π*
|
-
|
-
|
BOIT-Co
|
269
359
483
588
|
π -π*
n-π*
4T1g(F)→4T1g(p)
4T1g(F)→4A2g(F)
|
octahedral
|
4.63
|
BOIT-Cu
|
252
377
676
|
π -π*
n-π*
2B1g→2A1g
|
square planar
|
1.88
|
3.7. X-ray diffraction analysis
We recorded the XRD patterns for the four N-substituted-isatin-thiosemicarbazone complexes EOIT-CoCl2, BOIT-CoCl2, EOIT-CuCl2 and BOIT-CuCl2 to investigate their crystal structures and their size. The first look to the for charts of the XRD of the tested complexes indicated that the two complexes CoCl2 are amorphous and on the opposite side the two Cu-complexes reflected the excellent nano-size of the solid samples. From the calculation the size of the investigated tow crystalline Cu-complexes from Figure 5 using FWHM method and Deby–Scherrer and Bragg equations [49]. The size of the particles was found in the nanometer range: for complex EOIT-CuCl2 its size equal 22.15 nm and BOIT-CuCl2 its size equal 26.60 nm.
According to all the previous measurements, the structures and geometry of the metal complexes can be formulated as depicted in Scheme 2
3.8. Assessment of the corrosion rate of Sabic iron and the inhibition efficacy of the interested
compounds
3.8.1. PDP measurements
PDP measurements of Sabic steel in 1.0 M HCl solution without and with various concentrations (100-400 ppm) of the tested compounds were performed at 298 K and the PDP curves of the complex EOIT-Co (as a representative example) are shown in Figure 6. The corrosion parameters, viz. corrosion potential (Ecorr), anodic and cathodic Tafel slopes (βa, βc), corrosion current density (icorr), %IE and θ of the organic ligands were determined and located in Table 1. From Figure 6 and the determined corrosion parameters listed in Table 1, it can be realized that adding the examined compounds to the corrosive solution (blank, 1.0 M HCl) shifted both anodic and cathodic branches of the polarization curves of the corrosive medium to less current densities indicating delay of both anodic and cathodic reactions and thus inhibition of Sabic iron corrosion. The movement of the Ecorr value of Sabic iron in the blank solution to positive directions by the addition of the investigated compounds indicates that these compounds perform as mixed-type inhibitors with a major anodic one [50]. The values of βa and βc did not show obvious change in blank solution and when adding the complexes indicating that the adsorbed compounds’ molecules did not alter the anodic metal dissolution or cathodic hydrogen evolution. In addition, the value of icorr of Sabic iron in the blank solution was found to decrease with raising the compounds concentration, which indicates inhibition effects. The acquired results supported that, under similar experimental conditions, the inhibition efficiencies of the investigated inhibitors were set to slightly increase according to the order: EOIT-Cu > BOIT-Cu > EOIT-Co > BOIT-Co.
Table 2. Corrosion parameters obtained from the polarization curves in the corrosion of Sabic iron in 1.0 M HCl solution without and with various concentrations of the investigated compounds at 298 K.
Inh.
|
Inhibitor Conc. (mg/l)
|
-Ecorr
(mV(SCE))
|
βa
(mV/dec.)
|
-βc
(mV/dec.)
|
icorr
(µA/cm2)
|
% IE
|
θ
|
|
0
|
-469
|
123
|
118
|
365
|
--
|
--
|
EOIT-Co
|
100
|
453
|
129
|
117
|
175
|
52
|
0.52
|
200
|
462
|
125
|
121
|
113
|
69
|
0.69
|
300
|
449
|
131
|
123
|
77
|
79
|
0.79
|
400
|
447
|
126
|
119
|
62
|
83
|
0.83
|
BOIT-Co
|
100
|
465
|
119
|
113
|
186
|
49
|
0.49
|
200
|
460
|
124
|
121
|
124
|
66
|
0.66
|
300
|
463
|
127
|
115
|
91
|
75
|
0.75
|
400
|
449
|
124
|
109
|
69
|
81
|
0.81
|
EOIT-Cu
|
100
|
457
|
127
|
116
|
175
|
52
|
0.52
|
200
|
458
|
121
|
111
|
95
|
74
|
0.74
|
300
|
448
|
125
|
114
|
63
|
83
|
0.83
|
400
|
451
|
129
|
118
|
47
|
87
|
0.87
|
BOIT-Cu
|
100
|
466
|
132
|
122
|
168
|
54
|
0.54
|
200
|
453
|
127
|
117
|
106
|
71
|
0.71
|
300
|
455
|
118
|
120
|
66
|
82
|
0.82
|
400
|
446
|
123
|
116
|
61
|
83
|
0.83
|
3.8.2. EIS measurements
Corrosion of Sabic iron was studied in 1.0 M HCl solution in the lack and existence of alternative concentrations of the examined compounds at 298 K after immersion of the iron samples in the corrosive medium for around 30 min. by EIS technique. The obtained Nyquist and Bode plots of the complex EOIT-Cu (as a representative example) are shown in Figure 7 (a, b). It was observed from the Nyquist (a) and Bode plots (b) that the resulted impedance spectra comprised of only depressed capacitive loops in addition to one-time constants, correspondingly, suggesting that adsorption of the tested compounds happens through covering the surface and the corrosion is managed by the process of charge transfer [51]. The acquired communal profile of the plots was similar in both lake and existence of the compounds at the alternative concentrations employed revealing that there was no alter in Sabic iron corrosion mechanism [52]. It was realized from the Nyquist plots that the size of the capacitive semicircle increased by addition of the examined compounds revealing a reduce in the corrosion rate and an increase in the %IEs and the later were increased as the concentrations of the examined compounds increased [53]. Additionally, the Bode phase plots, Figure 7(b), showed that the phase angle was increased with increasing the compounds’ concentrations. This indicated that the metal surface was considerably changed to smooth because of formation of a protecting layer of inhibitors’ molecules on the Sabic iron surface resulting in a decrease in the corrosion rate [54].
Analysis of the impedance spectra were done through illustrating the model of the equivalent circuit shown in Figure 8. Impedance parameters values such as solution resistance (Rs), charge transfer resistance (Rct), constant phase element (CPE), % IE and θ were evaluated from the impedance spectra and were tabulated in Table 3. From these results it is obvious that the addition of the examined compounds to the blank solution leads to increasing the value of Rct of the corrosive medium and this behavior was set to significantly increased with increasing inhibitors’ concentrations. This was associated with a reduce in CPE value as a result of a reduce in the dielectric constant and/or an increase in the double-layer thickness. This indicated adsorption of the investigatd compounds’ molecules on the iron/solution interface [55] resulting in the safeguard of the Sabic iron surface from the attack of the corrosive medium. With increasing the concentration of the examined complexes, the inhibition efficiencies were set to increase confirming that these compounds are regarded as efficient inhibitors for the corrosion of Sabic iron in 1.0 M HCl solution. Variation of inhibition efficiencies with the concentrations of the investigated compounds was illustrated in Figure 9.
Table 3. Values of the impedance parameters of the corrosion of Sabic steel in 1.0 M HCl solution without and with various concentrations of the investigated synthesized complexes at 298 K.
Inhibitor
|
Inhibitor Conc.(mg/l)
|
Rs
(ohm cm2)
|
Rct
(ohm cm2)
|
CPE
(µF/cm2)
|
% IE
|
θ
|
|
0
|
1.23
|
71
|
224
|
--
|
--
|
EOIT-Co
|
100
|
2.24
|
127
|
122
|
44
|
0.44
|
200
|
3.07
|
207
|
77
|
66
|
0.66
|
300
|
2.18
|
321
|
62
|
78
|
0.78
|
400
|
3.74
|
423
|
59
|
83
|
0.83
|
BOIT-Co
|
100
|
2.31
|
119
|
133
|
40
|
0.40
|
200
|
1.91
|
187
|
95
|
62
|
0.62
|
300
|
2.07
|
298
|
76
|
76
|
0.76
|
400
|
1.82
|
384
|
59
|
82
|
0.82
|
EOIT-Cu
|
100
|
1.05
|
131
|
122
|
46
|
0.46
|
200
|
0.96
|
244
|
73
|
71
|
0.71
|
300
|
3.20
|
368
|
54
|
81
|
0.81
|
400
|
2.33
|
497
|
46
|
85
|
0.85
|
BOIT-Cu
|
100
|
0.95
|
142
|
112
|
50
|
0.50
|
200
|
3.40
|
211
|
84
|
66
|
0.66
|
300
|
2.51
|
316
|
63
|
78
|
0.78
|
400
|
1.71
|
458
|
48
|
84
|
0.84
|
3.8.3. ML measurements
Mass loss (ML) recording of Sabic iron in 1.0 M HCl solution were carried out at specified time intervals in the absence and presence of certain concentrations of the tested compounds at 298 K. Figure 10 shows only the mass-loss versus immersion time plots of the complex BOIT-Co. The same plots were acquired for other investigated compounds but not shown here. Values of the corrosion rates (CR), θ and %IE of the examined compounds are also inserted in Table 4. The data listed in Table 4 indicated that the values of CR were decreased while the inhibition efficiencies were enhanced with raising the inhibitors’ concentrations which attributed to augmenting adsorption coverage of the inhibitor molecules on the steel surface with rising concentration leading to decrease of the corrosion rates of Sabic iron. Therefore, the examined compounds are regarded as effective inhibitors for Sabic iron corrosion in 1.0 M HCl solution. In consistence with both PDP and EIS techniques, at similar inhibitors concentration, the % IEs are slightly increased in the order: EOIT-Cu > BOIT-Cu > EOIT-Co > BOIT-Co. A comparison of the change of the % IEs of the examined compounds with their concentrations at 298 K, obtained from all used techniques, PDP, EIS and ML, is shown in Figure 11 indicating that the results concluded from all employed techniques are in a good consistent with each other’s.
Table 4. Values of CR (mpy) of Sabic iron, % IE and θ of various concentrations of the investigated compounds in 1.0 M HCl solution at 298 K.
Inhibitor
|
Inhibitor
Conc. (mg/l)
|
CR
|
% IE
|
θ
|
|
0
|
166
|
--
|
--
|
EOIT-Co
|
100
|
80
|
52
|
0.52
|
200
|
48
|
71
|
0.71
|
300
|
33
|
80
|
0.80
|
400
|
28
|
83
|
0.83
|
BOIT-Co
|
100
|
81
|
52
|
0.52
|
200
|
53
|
68
|
0.68
|
300
|
40
|
76
|
0.76
|
400
|
35
|
79
|
0.79
|
EOIT-Cu
|
100
|
75
|
55
|
0.55
|
200
|
46
|
72
|
0.72
|
300
|
29
|
83
|
0.83
|
400
|
25
|
85
|
0.85
|
BOIT-Cu
|
100
|
75
|
55
|
0.55
|
200
|
51
|
69
|
0.69
|
300
|
30
|
83
|
0.83
|
400
|
23
|
86
|
0.86
|
3.8.4. Adsorption isotherms
The obtained inhibition efficiencies of the tested compounds were interpreted based on their adsorption on the metal surface. Some adsorption isotherms such as Langmuir, Frumkin, Freundlich, Temkin, etc. have been widely studied to investigate the kind of adsorption of the tested inhibitor molecules on the metallic surfaces and hence the mechanism of corrosion inhibition. In our investigation, Langmuir adsorption isotherm, the relation between the fractional surface coverage ([Inh.]/θ) of the examined compounds versus their concentrations [Inh.], according to the following equation [56],
where Kads is the absorptive equilibrium constant, was fitted and is illustrated in Figure 12. This indicates that the inhibitors adsorption on the surface of Sabic iron was correlated to the Langmuir adsorption isotherm.
3.8.5. Surface morphology
SEM images of Sabic iron specimens in a free 1.0 M HCl (corrosive medium) and with addition of 200 mg/l of the investigated compounds are shown in Figure 13(a–f). Figure 13 (a) and (b) show a polished Sabic iron surface before and after 24 hours immersion in the corrosive medium, successively. Figure 13(b) shows a strong destruction of the surface of iron specimen due to its exposure to the corrosive medium. Figure 13(c) to (f) shows SEM images after addition of a 200 mg/l of the investigated compounds: EOIT-Co, BOIT-Co, EOIT-Cu and BOIT-Cu, correspondingly, to the corrosive medium. It can be detect that, the surface of Sabic iron specimens were considerably covered with the investigated compounds on the most surface areas which was attributed to strong adsorption of the compounds’ molecules on the iron surface, leading to protecting the iron surfaces from the medium, and hence display an efficient corrosion inhibition.