P.K. Paul et al. / Journal of Molecular Liquids 314 (2020) 113513
3
of loss in weight of MSTC which were immersed in a corrosive medium
3. Result and discussion
with and without corrosion inhibitor for a period of 6 h. Measurement of
weight was taken from Mettler Toledo analytical weighing balance sta-
ble up to four decimal points. For this experiment, each finely polished
MSTC of dimension 3 × 4 × 0.5 cm was cleaned, dried and accurately
weighted and then dipped in the prepared test medium of concentra-
tion 0–300 ppm. After 6 h all the samples were carefully removed
from the test medium, washed, dried and again weighted. Since this
method is manually handled, so for the better observation this process
was repeated three times and the average of the findings was reported.
For determining the effect of corrosion at higher temperatures, thermo-
stat was used and correspondingly, the experiment was repeated for
higher temperature (303−333K) studies.
3.1. Gravimetric measurement
Corrosion parameters after the gravimetric measurements were
computed and listed in Table 1. On configuring the results, it was ob-
served that these corrosion parameters: corrosion rate (C
erage (θ) and inhibition efficiency (% η ) were dependent on the
amount of inhibitors added to the corrosive medium and temperature.
Observations were made for different concentrations where 10 ppm is
the lowest concentration and 300 ppm is the highest concentration (op-
timized concentration), beyond this range no considerable change was
observed. The results were computed with the help of given equations:
R
), surface cov-
g
4
CR ¼ 8:76 ꢀ 10 ðWI−W F Þ=Saρt
ð1Þ
ð2Þ
2
.3.3. Electrochemical measurement (EM)
The three-electrode system in a three-necked flat-bottomed flask
.
i
C
R
θ ¼ 1−
connected to the CHI-760D electrochemical analyzer set up was used
for polarization and electrochemical impedance studies. The outcomes
of the experiments were resolved by using CHI-760D electrochemical
software. The prepared MS electrode is used as a working electrode,
platinum electrode as auxiliary electrode and saturated calomel elec-
trode as reference electrode. This setup was kept on rest for 30 min
for ensuring the stabilization of open circuit potential (OCP) and after
the stabilization, the different electrochemical techniques were per-
formed. The obtained constant value of OCP is used as initial potential
value for running AC impedance technique keeping the higher and
lower frequency range as 100 kHz and 1 Hz, respectively, with 5 mV am-
plitude. After the completion of the AC impedance technique, the pa-
rameters were set for the polarization study. Polarization study was
performed in potential range of −250 to −250 mV with respect to
b
R
C
%η ¼ θ ꢀ 100
ð3Þ
g
where W and W is the weight (in mg) of the sample before and after
I
F
immersion in the corrosive test solution, t is the time of immersion in h,
S and ρ are the exposed surface area and density of MSTC respectively.
a
i
b
R
C
R
and C are the corrosion rates with and without inhibitors
respectively.
The inhibition efficiency consequently increases with inhibitor con-
centration and is ascribed as the mechanism of inhibition acquired by
inhibitors through forming an adsorbed thin layer on the exposed sur-
face of MS [23].The inhibition efficiency of AMPC and ACPC at
300 ppm concentration and 303 K temperature was found as 98.26
and 96.21%, respectively. The efficiency of these inhibitors (AMPC and
ACPC) are better than most of the reported similar types of inhibitors
−1
open circuit potential with a scan rate of 1 mVs
.
[
6,14–19,24,25]. The quantitative comparison of inhibition efficiency
2
.3.4. Surface characterization (FE-SEM, AFM & XPS)
of some reported similar type of inhibitors and our inhibitors (AMPC
and ACPC) are given in Table 2. From Table 2, it is clear that AMPC and
ACPC are better corrosion inhibitor as compared to the most of the al-
ready reported inhibitors.
The impact of temperature was also investigated to understand the
corrosion behavior on elevated temperatures and the experimental out-
comes were compared with the results found at room temperature. The
condition of metal surface in the corrosive medium at elevated temper-
atures becomes more adverse due to an increase in the metal dissolu-
tion process and shows better efficiency at room temperature
compared to other temperatures. For the better visual understanding,
Surface characterization was made using FESEM (Field Emission-
Scanning Electron Microscopy), AFM (Atomic Force Microscopy) and
XPS (X-ray Photoelectron Spectroscopy) analysis to understand the cor-
rosion damage and protection behavior of introduced corrosion inhibi-
tors into the corrosive medium. For the FESEM analysis, the
instrument with model Hitachi S-3400N was used. AFM analysis was
done by contact mode using an instrument from Bruker Corporation,
Berkovich type. Surface characterization by XPS analysis was done by
a PHI 5000 Versaprobe-II focus spectrometer from the facility provided
by IIT Kharagpur which uses Al Kα X-ray of 1486.6 eV monochromatic
radiation source [22].
g
the variation of inhibition efficiency (% η ) with concentration and tem-
perature is represented in Fig. S1 (Supporting information). The find-
ings in the corrosion rate with temperature might be connected to the
molecular rearrangement or fragmentation and disturbance on the
adsorbed layer of inhibitors on the surface [26].
Kinetic and thermodynamic parameters were extracted from the
slope and intercept of Arrhenius and Transition state plots represented
as Figs, S2 & S3 (Supporting information), respectively, and obtained pa-
rameters are portrayed in Table 3. The basic relation of temperature
with corrosion rate is mathematically represented by Arrhenius and
Transition state equations
2
.3.5. Computational studies
Computational methods were applied for both inhibitors to get more
structural and orbital energy related information. The quantum chemi-
cal calculations and energy optimization were observed with Gaussian
0
9 software program using the DFT method with B3LYP, 6–31 G (d,
p) basis set. The calculations of Fukui functions were carried out at
B3LYP /6–31 G (d, p) level. Monte Carlo simulation, was simulated for
getting the adsorption energy and to showing the interaction of the in-
hibitors with the steel surface, the adsorption locator module was ap-
plied based on the Metropolis Monte Carlo approach. The calculation
was performed using the COMPASS (Condensed-phase Optimized Mo-
lecular Potentials for Atomistic Simulation Studies) force field. The ad-
sorption of the inhibitors AMPC and ACPC was simulated on the Fe
lnCR ¼ ½lnA−ðEa=RTÞꢁ
ð4Þ
ð5Þ
ꢂ
ꢂ
R
C =T ¼ RT=Nh½ expðΔS =RÞ expðΔH =RTÞꢁ
(
110) crystal plane. The process involved cleaving from bcc Fe crystal,
followed by enlargement to a (10 × 10) supercell and, thereafter, build-
ing of a 30 Å thick vacuum slab on the Fe (110). For the simulating an-
nealing process, the maximum and minimum temperature was set at
where C
R
is the rate of corrosion, A is the preexponential factor, E
a
is the
energy of activation, R is the universal gas constant, T is the absolute
∗
temperature, h is the Planck's constant, ΔS is the deviation in entropy
5
00 K and 298 K respectively. The adsorption energy for the most stable
and ΔH ∗ represents the enthalpy change.
corrosion inhibitors–Fe (110) configuration was calculated by consider-
These mathematical expressions provide the activation energy (E
a
),
ing 50 molecules of water in order to account for the solvent effects.
some alteration in entropy and enthalpy during the corrosion process