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A. Thoume, D. Benmessaoud Left, A. Elmakssoudi et al.
Journal of Molecular Liquids 337 (2021) 116398
C0 ꢂ C
final geometry by means of the Gaussian 09 software suite at the
DFT level in a functional B3LYP implementing a 6-31G (d, p) basis
set [35].
gað%Þ ¼
ꢀ 100
ð3Þ
C0
Here C0 and C refer to the concentration of iron in the absence and
presence respectively of CO and CO-NO2 inhibitors.
The quantum descriptors like LUMO and HOMO energies, gap
energy (
quantum descriptors such as, ‘‘
can be calculated using the Eq. (9), fraction of electrons transferred
from the inhibitor molecule to the metal surface ‘‘ N110” can be
determined using Eq. (10), where the work function presents
the theoretical value of in the plan (1 1 0) of iron (
= 4.82 eV) and the represent the metallic bulk (
= 0 eV) [36], ‘‘
the nucleophilic indexes (Eq. (12)),.
DEgap) (Eq. (7)), electronegativity ‘‘
v” (Eq. (8)), and other
g
” is the global hardness which
2.5. Electrochemical measurements
D
The inhibitory activity of the investigated compound on carbon
steel corroding were examined through Potentiodynamic Polariza-
tion(PDP) and Electrochemical impedance spectroscopy(EIS) in
1 M HCl in absence and presence of CO and CO-NO2 concentrations
going from 4.48 ꢀ 10-4 to 2.24 ꢀ 10ꢂ3 M at various temperatures
293–323 K. A classical cell with a three electrodes configuration
was used in the present study. The working electrode consisted
of carbon steel, whereas a platinum grid and a saturated calomel
electrode (SCE) were employed as a counter and reference elec-
trodes, respectively. Before electrochemical tests, the working elec-
trode was immersed in 1 M HCl solution without and with
different inhibitors concentrations for 40 min at open circuit
potential (OCP). The PDP plots were drawn with a scan rate of
0.5 mV sꢂ1 at the standard potential range found by
adding 200 mV to the OCP. EIS spectra were recorded between
100 kHz and 10 mHz at OCP with an amplitude of 10 mV. Three
replicas of the trials were performed and the average values were
regarded. The inhibitory efficacy was assessed as follows [31,32]:
U
v
U
=
v
(Fe110
)
)
g
g (Fe110
x
” is the electrophilic indexes (Eq. (11)), and ‘‘
e
” is
D
Egap ¼ ELUMO ꢂ EHOMO
ð7Þ
ð8Þ
1
v
¼
¼
ðEHOMO þ ELUMO
Þ
Þ
2
1
2
g
ðEHOMO ꢂ ELUMO
ð9Þ
v
ꢂ vinh
U
2
ꢂ
vinh
ginh
Fe110
ꢀ
ꢁ
D
N110
¼
¼
ð10Þ
2
gFe
þ
ginh
110
v2
i0corr ꢂ icorr
x
¼
ð11Þ
ð12Þ
2g
gPð%Þ ¼
ꢀ 100
ð4Þ
i0corr
1
i0corr and icorr denote the corrosion current densities values in absence
and presence of the inhibitory molecule, respectively.
e
¼
x
Rip ꢂ Rbp
2.7.2. Molecular dynamics (MD) simulations
gEISð%Þ ¼
ꢀ 100
ð5Þ
Rpi
The adsorbed inhibitors CO and CO-NO2 neutral and unnatural
forms on the metal surface was established using the MD simula-
tion using Forcite module implemented in Materials Studio 8.0
software [37,38]. The study of these interactions of the molecules
with the Fe (1 1 0) surfaces was carried out from a simulation
box (22.34* 22.341* 35.13 Å3) with periodic boundary conditions.
The Fe (1 1 0) surface was presented with a six-layer slab model
in each layer representing a (11 ꢀ 11) unit cell. The constructed
simulation box is emptied by 20.13 Å3. This vacuum is occupied
by 500H2O, 5H3O+, 5Cl- and the inhibitory molecule. The tempera-
ture of the simulated system of 293 K was controlled by the Ander-
sen thermostat, NVT ensemble, with a simulation time of 400 ps
and a time step of 1.0 fs, all under the COMPASS force field [39].
where Rbp and Rip are polarization resistances obtained in the blank
and the inhibited solutions, respectively.
The surface coverage, h is expressed as:
gPð%Þ
h ¼
ð6Þ
100
gP is the inhibitory efficiency determined by PDP.
2.6. Scanning electron microscopic measurement (SEM)
Carbon steel surface was examined after 6 h of immersion in
1 M HCl free of an inhibitor, and with the optimum concentration
of CO and CO-NO2. Carbon steel samples were transferred from the
test media, rinsed with water and dried. The morphological aspect
of carbon steel surface was examined by SEM (FEI FEG 450).
3. Results and discussion
3.1. Weight loss measurements and atomic adsorption
Table 2 displays the values of weight loss trials, the calculated
2.7. Computational details
corrosion rates (m), and the inhibition efficacy (gw%) values with-
2.7.1. DFT calculations
out and with diverse concentrations of CO and CO-NO2 in 1 M
HCl at a temperature of 293 K for 6 h. The analysis of Table 2
encloses the subsidence of corrosion rate and increment of the
inhibitory efficiency with increasing CO and CO-NO2 concentra-
Quantum chemical calculations on the DFT approach have been
carried for CO and CO-NO2 neutral and protonated forms to pro-
vide an understanding of the key influence of molecular structures
and electronic characteristics on the inhibitory properties [33].
Moreover, this complementary theoretical part has been carried
out with the attempt to correlate the experimentally computed
corrosion inhibition for the inhibitors with the chemical reactivity
descriptors of the DFT calculations [34]. The lowest energy inhibi-
tor shapes were tested in the DFT calculations conducted under
pressure and in the gaseous phase. Additionally, the molecular
structures of the compounds studied have been optimized to the
tions. Maximal
gW values of 95 and 92% were reached in the pres-
ence of 2.24 ꢀ 10-3 M of CO and CO-NO2, respectively. Through the
increment of the blocked portion of the steel by the synthesized
inhibitors, the interaction between the metallic substrate and the
destructive solution can be prevented [40]. Interestingly, identical
results were found by atomic adsorption technique, where we
observed that the concentration of iron decreases in 1 M HCl by
the addition of CO and CO-NO2, which main role are not only to
3