effect of small amount of h2s on the corrosion behavior
TRANSCRIPT
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Accepted Manuscript
Title: Effect of small amount of H2S on the corrosion behaviorof carbon steel in the dynamic supercritical CO2 environments
Author: Liang Wei Xiaolu Pang Kewei Gao
PII: S0010-938X(15)30150-5
DOI: http://dx.doi.org/doi:10.1016/j.corsci.2015.11.009
Reference: CS 6547
To appear in:
Received date: 15-7-2015Revised date: 29-10-2015
Accepted date: 5-11-2015
Please cite this article as: Liang Wei, Xiaolu Pang, Kewei Gao, Effect of small amount
of H2S on the corrosion behavior of carbon steel in the dynamic supercritical CO2
environments, Corrosion Science http://dx.doi.org/10.1016/j.corsci.2015.11.009
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Effect of small amount of H2S on the corrosion behavior of carbon steel in the
dynamic supercritical CO2 environments
Liang Wei, Xiaolu Pang, Kewei Gao*
Department of Materials Physics and Chemistry,University of Science and Technology Beijing,
Beijing 100083, China* Corresponding author: E-mail: [email protected]
Tel: +86 1062334909; Fax: +86 1062334909
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Highlights
(1) Effect of H2S on the corrosion of carbon steel in supercritical CO2 was studied.
(2)
H2S changed the adsorbability of H2O on the steel surface in supercritical CO2
phase.(3) H2S presented more significant effect on the corrosion of steel in the aqueous
phase.
(4) H2S did not change the dominant corrosion type in supercritical CO2 phase.
(5)
H2S changed the dominant corrosion type of carbon steel in aqueous phase.
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Abstract
The effect of small amount of H2S on the corrosion of carbon steel in both dynamic
supercritical CO2 and aqueous phase was investigated. H2S changed the adsorbability
of H2O on the steel surface, causing the adsorption of H2O on the whole steel surface,
which accelerated the general and localized corrosion of carbon steel in supercriticalCO2 phase. The small amount of H2S presented more significant effect in the aqueous
phase - it changed the microstructure and compositions of the corrosion product scale,
ultimately changed the dominated corrosion type of carbon steel from localized to
general corrosion.
Keywords: A. Carbon steel; B. SEM; B. Raman spectroscopy; B. XRD; C. Acid
corrosion
1. Introduction
Carbon capture and storage (CCS) technology is regarded as one of the most
effective methods to significantly reduce CO2 emission and mitigate globing warming.
CCS process generally consists of capturing CO2 from different emission sources (e.g.,
coal-fired power stations, oil refineries), compressing CO2 into supercritical or liquid
states, then transporting and injecting it into storage sites (such as underground
aquifers or depleted oil and gas reservoirs). The transportation and injection of CO2,
which is important in CCS application, is usually accomplished by pipelines made by
carbon steel. For abating climate change, approximately 10 Gt/year of CO2 must be
transported for sequestration underground by 2050, which requires the construction of
3000 twelve-inch or 1000 twenty-inch carbon steel pipelines [1]. With the rapid
growth for energy demand, the exploitation of high pressure gas fields with large
quantities of CO2 (from 25% to 89%) becomes increasingly valuable [30]. However,
the large quantities of CO2 must be separated from the gas, captured and transported
to storage sites, which presents similar challenges as CO2 transportation in CCS
application. Meanwhile, the captured CO2 can also be injected into oil and gas fields
for enhanced oil/gas recovery (EOR/EGR). Generally, water can present in the
processes stated above, which resulted in potential supercritical CO2 (SC CO2)
corrosion risks to the carbon steel pipelines.
In the past few years, the corrosion problems of steels under SC CO2 conditionshave been given increasing attention [2-8]. It is well known that dry SC CO2 is not
corrosive [9]. When the H2O content in SC CO2 phase was less than its solubility limit,
the corrosion rate of carbon steel was very low [8-10]. If the H2O content exceeded its
solubility limit (steels remaining exposed in SC CO2 phase) or carbon steels
completely immersed in SC CO2-saturated water (aqueous phase), the corrosion rate
significantly increased [9, 11]. Notably, the addition of small amounts of SO2 in the
SC CO2/H2O system could noticeably enhance the corrosion rate of carbon steels,
even if the water content in the SC CO2/H2O/impurity system was much lower than its
solubility limit [12]. This suggested that the presence of impurities may drastically
enhance the corrosivity of SC CO2 to steels.
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The captured CO2 from various sources (anthropogenic and natural) commonly
contains different impurities. Though the compositions of CO2 streams are rarely
available in the open literature, Table 1 lists a summary of complied data from various
researchers [13-17]. Unfortunately, the content of impurities such as SOx, NOx and O2
was unclear. While to date there are still no recognized specifications of the CO2 quality required for transportation, some tentative CO2 specifications and CO2 quality
tolerances have been suggested in the literature as listed in Table 2 [1]. Combined
with Table 1, 2 and the data summarized by Lee et al. [18], it is worth noting that the
primary impurities, except for H2O, concerned in the CO2 streams were O2, SO2, NO2,
CH4 and H2S. The effects of SO2 and O2 on the corrosion behaviors of carbon steels in
the SC CO2/H2O/impurity system have been investigated in depth by researchers [12,
19-23], nevertheless, studies on the effect of H2S on the corrosion behavior of steels
in the SC CO2/H2O/impurity system was very limited. Most studies for the effect of
H2S on the corrosion of steels in the CO2/ H2S system were at low CO2 partial
pressure conditions or in CO2 environment with high H2S content [24-33].In deep water oil and gas production, there is also small amounts of H2S existing in
the high pressure CO2 stream [34]. When the water content in the SC CO2 system was
far below its solubility limit, corrosion was very slight in SC CO2/H2O/H2S systems
(
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in Fig. 1, the phase of X65 steel mainly consisted of Ferrite (F) and carbide (Fe3C).
The test specimens were machined with dimensions of 10×10×3 mm3. Specimen
surfaces were ground with SiC papers up to 800 grit, cleaned with deionized water,
followed by alcohol, and dried with cold air. Specimens were then weighed on an
electronic balance with a precision of 0.1 mg and stored in a desiccator until use.During exposure experiment, the samples were fixed in a specimen holder made of
polytetrafluoroethene (PTFE) to prevent galvanic effects, and six samples were placed
in the autoclave for every test.
2.2 Exposure experiments
Exposure experiments were conducted in a high temperature and high pressure
autoclave with a 3 L capacity and its schematic diagram is shown in Fig. 2. According
to Hua et al. [5] and Sim et al. [8], there were two main corrosive systems under
supercritical CO2 conditions: the SC CO2-saturated water system (water-rich phase,
i.e. aqueous phase) - samples completely expose in water, and the water-saturated SCCO2 system (SC CO2-rich phase, i.e. SC CO2 phase) - samples expose to the SC CO2
phase. Therefore, the corrosive environments considered in this study included these
two systems.
The corrosion medium was 3.5 wt.% NaCl (the content of Cl- is ~ 21g/L), which
was made from deionized water and analytical reagents. During the exploitation of
high pressure CO2 fields or the injection of CO2, formation water normally presents in
the environments, which mainly consisted of corrosive ions such as Cl-. Researchers
[39-40] have confirmed that the most detrimental chloride content in the corrosion
solution for CO2 corrosion of carbon steel was around 15-25 g/L. As a result, the
chloride content (~21 g/L), was selected in this study to evaluate the corrosion
behavior of carbon steel in the worst corrosion medium.
The NaCl solution was de-aerated by CO2 bubbling in a conical flask for 12 h prior
to the exposure experiments. Then the corrosion medium was introduced into the
autoclave at ambient temperature and pressure and sealed, and continuously bubbled
CO2 to remove the oxygen within the system. Subsequently, pure CO2 or a mixture of
CO2 and H2S with certain ratio was directly injected into the autoclave and adjusted to
the required temperature and pressure. The starting point of each test was taken from
the time once the system reached the required temperature and pressure. The
experimental conditions are listed in Table 3.The solubility of water in CO2 has been investigated by Spycher [41] and Choi [11],
which presented as a function of temperature and pressure. According to Spycher et al.
[41], the solubility limit of water in SC CO2 phase at 10 MPa and 80 °C is around
10,000 ppm. Consequently, to ensure the water-saturated SC CO2 states during the test,
100 ml of solution was introduced to the autoclave. The specimens were all exposed
to the SC CO2 phase and the free aqueous phase was at the bottom of the autoclave, as
shown in Fig. 2. However, during the aqueous phase test, specimens were all
immersed in the 1000 ml of solution.
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2.3 Weight loss tests and microstructure characterization
After the exposure experiments, the six samples were taken out and cleaned by
deionized water and alcohol. Of which, three specimens were pickled in 10%
hydrochloric acid inhibited with 10g/L hexamethylenetetramine to remove thecorrosion product scale and the general corrosion rate was calculated according to the
following equation [42]:
RG =87600 ∆m
Sρt
(1)
where RG is the general corrosion rate, mm/y; Δm is the weight loss, g; S is the
exposed surface area, cm2; ρ is the density of steel, g/cm3; t is the exposure time, h.
Localized corrosion was measured by profilometer. All the scale-removed
samples were analyzed by profile meter and the pit depth analysis was in alignment
with ASTM Standard G46-94 [43]: an average of the 10 deepest pits and themaximum pit depth were used for pit damage. The localized corrosion rate was
calculated by the following equation:
RL=0.365h
t
(2)
where RL is the localized corrosion rate, mm/y; h is the pit depth, μm; t is the
exposure time, d.
The surface and cross-section morphologies of corrosion product scale were
analyzed by Scanning Electron Microscopy (SEM). The chemical composition and
the microstructure of the corrosion product scale were characterized by Energy
Dispersive Spectrometer (EDS), X-ray Diffraction (XRD) and Raman Spectroscopy.
The surface morphology of localized corrosion was also characterized by SEM.
3.
Results and discussion
3.1 Effect of H2S on the general corrosion rate
Fig. 3 shows the general corrosion rates of X65 carbon steel exposed to both SC
CO2 and aqueous phases with 50 ppm H2S and without H2S at 10 MPa and 80 °C for
10 days. The general corrosion rates exposed to the aqueous phase both with andwithout H2S were much higher than those exposed to the SC CO2 phase, which was in
agreement with the results of Choi et al. [11].
In the SC CO2 phase, the general corrosion rate with 50 ppm H2S was slightly
higher than that without H2S, indicating the presence of H2S enhanced the general
corrosion rate of X65 steel. The effect ratio (φ) of H2S on the corrosion rate of carbon
steel in the SC CO2 environments is defined as follow:
= Rwith- Rwithout Rwith
(3)
where Rwith and Rwithout are respective the corrosion rate of carbon steel in the SC CO2
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environments with and without H2S, mm/y.
According to Eq. (3), the effect ratio of 50 ppm H2S in the SC CO2 phase was
approximate 23.5%. The investigation of Choi et al. [34] indicated that the effect ratio
of 200 ppm H2S on the corrosion rate of carbon steel in the SC CO2 phase was 98%,
much higher than that in this study, which should be ascribed to the lower H2S contentin this study. The general corrosion rate of X65 steel exposed to the aqueous phase
with 50 ppm H2S was approximate two times higher than that without H2S. The effect
ratio of H2S in the aqueous phase was 83%, much higher than that in the SC CO2
phase (23.5%), which indicated that the effect of H2S in the flowing aqueous phase
was more significant than that in the flowing SC CO2 phase.
3.2 Effect of H2S in the SC CO2 phase
The surface morphologies of corrosion scale formed on X65 steel exposed to
water-saturated SC CO2 phase with and without 50 ppm H2S at 80 °C and 10 MPa areshown in Fig. 4. In the SC CO2 phase without H2S, two different characteristics on the
X65 steel surface were observed: as shown in Fig. 4(a), some regions were covered by
dense crystalline product, which was confirmed as FeCO3 by XRD measurements in
Fig. 5; on other regions (approximate 30%-50% of the surface), as shown in Fig. 4(b),
the polishing marks were still visible, only some corrosion product scattered, the
Raman spectra of this product (Fig. 6) demonstrated that it was also FeCO3. However,
as observed in Fig. 4 (c) and (d), the whole surface of X65 steel was covered by
corrosion product scale in the SC CO2 phase with 50 ppm H2S. Further, the corrosion
product scale divided into two layers, XRD spectra in Fig. 5 demonstrated it mainly
consisted of FeCO3 and small amount of iron sulfides.
Comparing the surface morphologies of X65 steel exposed to dynamic SC CO2
with and without H2S, it is obvious that the presence of H2S significantly influenced
the corrosion behavior of X65 steel. The addition of small amount of H2S may
increase the solubility of H2O in the system, subsequently increased the H2O content
condensed on the steel surface and accelerated the corrosion of the steel; or the
presence of H2S influenced the adsorbability of H2O on the X65 steel, which
influenced the corrosion of the steel. Therefore, it is very necessary to determine the
main reason effecting the corrosion of the steel. Given the lack of the H2O solubility
data in CO2/H2S/H2O mixed system under SC CO2 conditions, the solubility of H2Oin pure CO2 phase and pure H2S phase was calculated, respectively. The mutual
solubility of CO2, H2S with H2O could be calculated according to the following
equations [44], which referred to the calculation equations of Spycher et al. [41]:
yH2O
=1- ∑ yiBi
1 A⁄ - ∑ yiBi
(4)
xi= yiBi (5)
where yH2O
is the solubility (mole fraction) of H2O in i (i is CO2 or H2S) and xi is
the solubility (mole fraction) of i in H2O, yi is the mole fraction of i in the gas phase.
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Parameters A and Bi in Equation (4) and (5) are defined as follows:
A = KH2O0
∅ H2OP totexp[(P -P 0)V H2O
RT ] (6)
Bi = ∅ i P totγi
H i
T, 1
exp [- ( P - P 0)V i
RT ] (7)
where K is the true equilibrium constant; ∅ H2O is the fugacity coefficient of H2O; P tot
is the total pressure, bar; P is the partial pressure, bar; P 0 is the reference pressure, 1
bar; V H2O and V i are, respectively, the average partial molar volume of the pure
condensed component H2O and i over the pressure val P 0 to P , cm3/mol. ∅ i is the
fugacity coefficient of i; γi is the activity coefficient in mole fraction scale; H iT, 1
is the Henry’s constant; R is the gas constant; T is the temperature, K.
As calculated by Eqs. (4) – (7), the solubility of H2S in the aqueous phase in this
study is 2.1924 mol/kg, which is much higher than that of CO2 in the aqueous phase(~ 0.7778 mol/kg). However, the solubility of H2O in H2S phase is 10,200 ppm (mole)
at the experimental condition in this study, similar to the solubility of H2O in CO2
phase (10,500 ppm). That is the addition of H2S in the SC CO2/H2S mixed system
barely effected the solubility of H2O. Therefore, the presence of small amount of H2S
in the system changed the adsorbability of H2O on the X65 steel surface, which led to
H2O adsorbing on the whole steels surface. This was one reason that the general
corrosion rate of X65 steel exposed to the SC CO2/H2S mixed system was higher than
that exposed to the pure SC CO2 system.
The cross-section morphologies of corrosion product scale formed on X65 steel
exposed to SC CO2 phase with and without 50 ppm H2S at 80 °C and 10 MPa are
shown in Fig. 7 (a) and (b). There were two layers of corrosion product scale under
both conditions of H2S content. In the SC CO2 phase without H2S, the EDS analysis
of the inner layer formed on X65 steel (Fig. 7 (c)) confirmed that this layer possessed
similar compositions with that of the outer layer. Raman spectra of the inner layer
indicated that it also consisted of FeCO3, as shown in Fig. 8. In the SC CO2 phase
with 50 ppm H2S, EDS result indicated the dense outer layer and relatively loose
inner layer all contained Fe, C and O, while S element existed in the inner layer only,
as shown in Fig. 7 (e). Combined with the XRD spectra (Fig. 5), it can be confirmed
that the outer layer consisted of FeCO3, while the inner layer consisted of FeCO3 andiron sulfides. Notably, the inner layer of corrosion product scale formed in SC CO2
phase without H2S was dense, while the inner layer formed in SC CO2 phase with H2S
was loose, which was in alignment with that observed by Banas et al. [45].
Once the water condenses on the steel surface and forms a thin water film (Eq.
(8)), CO2 can immediately dissolve in this film and produce H2CO3, then H2CO3
dissociates in two steps to produce H+, HCO3- and CO3
2- [46]:
H2Odi ↔ H2Oaq (8)
CO2g + H2Ol ↔ H2CO3(aq) (9)
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H2CO3 ↔ H+ + HCO3- (10)
HCO3- ↔ H++CO32- (11)
During the initial corrosion period of steel in the SC CO2-saturated thin water film,the main cathodic reactions are the direct reduction of H+, the reduction of H2CO3 and
HCO3- [47]:
2H+ + 2e- ↔ H2 (12)
2H2CO3 + 2e- → H2 + 2HCO3- (13)
2HCO3- + 2e- → H2 + 2CO32- (14)
The anodic reaction is the oxidation of Fe:
Fe → Fe2+ + 2e- (15)When the concentrations of Fe2+ and CO3
2- exceed the solubility limit K sp of
FeCO3, FeCO3 will initiate to precipitation:
Fe2+ + CO32- ↔ FeCO3 (16)In the SC CO2 phase, the water film condensed on the steel is normally very thin,
reaction ions such as H+ can easily reach the steel surface, which leads to the fast
dissolution of Fe (Eq. (15)), and a mass of Fe2+ forms quickly and accumulates on the
steel surface. In addition, the effect of dynamic SC CO2 flow on the diffusion of Fe2+
in the thin water film is very limited. As a consequence, a high concentration of Fe2+
is obtained near the steel surface and leads to the nucleation of FeCO3 crystals
dominating, a dense FeCO3 layer thus forms on the steel surface. This scale impedes
the reactants reaching the steel surface and decreases the corrosion rate effectively.
Correspondingly, the concentration of Fe2+ decreases, which results in a low relative
supersaturation of FeCO3 above the previous formed FeCO3 layer, so an outer FeCO3
layer with larger grain size forms, as shown in Fig. 4 (a).
However, if H2S is contained in the SC CO2 phase, it dissolves in the water film
more easily than CO2, and produces H+, HS- and S2- according to the dissociation
reactions of H2S [48]:
H2S ↔ H+ + HS- (17)
HS- ↔ H+ + S2- (18)The dissolution of H2S further increased the concentration of H+ according to Eq.
(17) and (18), promoting the cathodic reaction process (Eq. (12)) and subsequently
increased the corrosion rate of X65 steel. HS - has greater chemical adsorption ability
than HCO3- and OH- on the steel surface [50], it accelerates the reactions of corrosion
and inhibits other corrosive species (such as H2CO3, HCO3-) from reacting with Fe.
Iron sulfides such as mackinawite (FeS1-x) firstly forms on the steel surface according
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to the solid state reactions from (19) to (21) [31]. Compared to the steel matrix, the
iron sulfides had a more positive potential and possessed certain electrical
conductivity, as reported by researcher [49]. The potential difference between the
inner layer and the steel promoted the corrosion of steel. However, as the researcher
confirmed [24], the initial formed iron sulfide layer was loose and had some defects,which resulted in the poor protective ability of the iron sulfide layer. Corrosive ions
could reach the steel surface due to the defects in the iron sulfide layer, thereby more
Fe2+ formed. With corrosion proceeding, once the concentrations of Fe2+ and CO32- in
the iron sulfide layer exceeded the K sp of FeCO3, FeCO3 precipitated in the layer and
a mixed layer (i.e. the inner corrosion product scale presented in Fig. 7 (b)) contained
FeCO3 and iron sulfides formed. Although this inner layer was relatively porous, it
could still retard the movement of corrosive ions and Fe2+ through the film [25],
decreased the dissolution of Fe and hence the concentration of Fe2+ in the solution. On
the other hand, as listed in Table 4, the solubility limits of FeCO3 and FeS under the
conditions of this study could be calculated, which were also listed in Table 4; theconcentrations of CO3
2- and S2- in the solution in this study could be calculated
according to the corresponding literatures [47, 50], and were respective 5.8×10-5
mol/L and 2.71×10-32 mol/L. As calculated above, FeCO3 was relatively easy to
precipitate according to Eq. (16), while FeS barely precipitated according to
precipitation reaction (22). Therefore, an outer layer which only contained FeCO3
formed on the inner layer.
Fe+ HS- → FeSHads
- (19)
FeSHads- → FeSHads+ + 2e- (20)
FeSHads+ → FeS1-x+xHS
-+ (1-x)H+ (21)
Fe2+ + S2- → FeS (22)It is worth noting that, as show in Fig. 7 (a) and (b), localized corrosion was
observed on the steel exposed to SC CO2 phase both with and without H2S, the effect
of H2S on the localized corrosion of steel would be depth discussed in the later
section.
3.3 Effect of H2S in the aqueous phase
The surface morphologies of corrosion product scales formed on X65 steel
immersed in SC CO2-saturated NaCl solution at 80 °C and 10 MPa with and without
H2S are shown in Fig. 9. In the aqueous phase without H2S (Fig. 9(a)), a relatively
dense FeCO3 scale with some pores was observed. However, when 50 ppm H2S
presented, a loose corrosion product scale, covered by some granular corrosion
products, was observed on the X65 steel surface, as shown in Fig. 9(b). Similar scale
structure was reported by Valdes et al. [53]. XRD results in Fig. 10 indicated that this
corrosion product scale formed in the aqueous phase with H2S also consisted of
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FeCO3 and iron sulfides, the same as the microstructure of scale formed in the SC
CO2 phase with H2S.
Fig. 11 presents the cross-section morphologies of corrosion product scales on X65
steel. In the aqueous phase without H2S, localized corrosion pits were clearly
observed, shown in Fig. 11(a). The corrosion product scale was comprised of twolayers (Fig. 11(b)): the outer layer consisted of FeCO3 crystal grains; the inner layer
consisted of dark grey corrosion products and granular substances with a light contrast,
which was similar to the steel matrix. Localized Raman spectroscopy analysis at the
dark grey corrosion product locations (Fig. 12) confirmed that it was FeCO3. EDS
result of the granular substance showed that it only contained Fe and C, and the
corresponding atomic ratio was near 3:1, which indicated that these granular
substances were Fe3C. Therefore, the inner layer scale consisted of FeCO3 and Fe3C,
this was in agreement with the results of Gao [42].
FeCO3 and Fe3C are the typical compositions of corrosion product scale of carbon
steel during CO2 corrosion process [31, 42], while Fe3C is not the corrosion product but the remainder of carbon steel after the selective dissolution of ferrite. As shown in
Fig. 1, the microstructure of X65 steel consists of ferrite and Fe3C. Fe3C has a positive
potential comparing with ferrite, which leads to the formation of a galvanic cell
between ferrite and Fe3C in the steel. Therefore, ferrite, as an anodic phase, dissolves
preferentially; Fe3C, as a cathodic phase, accumulates on the surface during initial
corrosion process [54]. This remaining Fe3C is a metallic conductor with low
hydrogen overvoltage and accelerates the corrosion of carbon steel. The initial formed
porous Fe3C layer influences the concentration gradient of the solution in it, leading
the local increase of pH and the concentration gradient of Fe2+, allowing the formation
of FeCO3 in the Fe3C layer. Meanwhile, Fe3C can act as the nucleation points of
FeCO3 crystal precipitation [55]. FeCO3 precipitated around Fe3C and first formed the
inner layer scale, which protected the steel and decreased the corrosion rate. This
protective inner layer scale hindered the diffusion of Fe2+ from the scale/matrix
interface to the scale/solution interface effectively and decreased the concentration of
Fe2+ above the inner layer scale. The flowing liquid promoted the diffusion of Fe2+
and further decreased the concentration of Fe2+ above the inner layer scale. Therefore,
the relative supersaturation of FeCO3 in the solution near the inner layer was low, the
growth of FeCO3 crystals was thus dominating and a relatively porous outer FeCO3
layer formed above the inner layer, as shown in Fig. 11 (a) and (b).As observed in Fig. 11 (c) and (d), the corrosion product scale formed in the
aqueous phase with H2S also consisted of two layers: the porous outer layer consisted
of FeCO3 crystals; the loose inner layer mainly contained FeCO3 and iron sulfide
(mackinawite), which was confirmed by the EDS and XRD results. Meanwhile, the
gaps between the inner layer scale and the steel surface were obviously visible,
indicating the adhesion stress of the inner layer to the steel matrix was poor, so the
inner scale easily spalled by the wall shear stress in the dynamic aqueous phase. The
distance between the original steel surface and the scale/matrix interface was much
larger than the thickness of the corrosion product scale, which demonstrated that the
scale spalled seriously in the dynamic aqueous phase dissolved H2S.
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Similar to the effect of H2S on the corrosion of carbon steel exposed to SC CO2
phase, according to Eq. (17), H2S dissolved in the solution and formed HS-, which
could adsorb on the steel surface and temporarily block the action of CO2, therefore,
FeS preferentially formed on the steel surface [49]. Reactive ions such as H+, HCO3-
and CO32-
could penetrate through the porous iron sulfide layer and continuouslycorroded the steel, meanwhile iron sulfide could also promote the dissolution of steel
due to its potential being more positive than the steel matrix. As a consequence, large
amounts of Fe2+ was produced and diffused through the layer to the bulk solution.
Fe2+ combined with CO32- in the iron sulfide layer and formed FeCO3, leading to
tension in the layer and resulted in the formation of cracks. On the other hand, in the
initial CO2 corrosion period, the corrosion rate was much higher than the formation
rate of the layer, which resulted in the poor adhesion stress of scale to steel matrix
[56]. Therefore, the defective FeCO3/FeS mixed layer easily spalled in the dynamic
aqueous phase.
It is worth noting that Fe3C could remain on the steel surface due to the selectivedissolution of ferrite. When no H2S presented in the solution, FeCO3 could nucleate
and grow quickly around Fe3C and formed a FeCO3 scale, which presented good
adhesion stress to the steel and anchored Fe3C on the steel surface [42]. However,
when H2S dissolved in the solution, the preferentially adsorbed HS- resulted in the
formation of porous and loose iron sulfide layer, and impeded the formation of FeCO3.
As a result, the remained Fe3C was easily scoured off in the dynamic aqueous phase.
Moreover, the porous and cracked iron sulfide layer, which may contain some Fe3C,
also easily spalled off on account of the poor adhesion stress of the scale to steel
matrix. Therefore, almost no Fe3C existed in the corrosion product scale on X65 steel
immersed in the dynamic aqueous phase dissolved H2S.
As mentioned before, when small amount of H2S presented in the system, the iron
sulfide formed mainly via the solid state reactions (19) to (21) rather than the
precipitation reaction (22). So an outer layer only containing FeCO3 formed above the
inner FeCO3 and iron sulfides mixed layer in SC CO2 phase with H2S. However, in
the aqueous phase dissolved H2S, the effect of flow velocity on the diffusion of Fe2+
was much more significant than that in the SC CO2 phase, and a much lower
concentration of Fe2+ was expected to obtain near the inner iron sulfide layer. As a
result, the growth of FeCO3 was dominated and some FeCO3 crystals with large grain
size precipitated above the inner layer. However, the diffusion of Fe2+ in the thinwater film in the dynamic SC CO2 phase was restricted due to the small volume of
water film, the higher Fe2+ concentration was expected to obtain, which accelerated
the formation of a relative compact FeCO3 layer with small grain size. The grain size
of FeCO3 crystals formed in the aqueous phase with and without H2S was
approximately 50 μm, one order of magnitude larger than that formed in the SC CO2
phase (approximate 5 μm), as shown in Fig. 4 and 9.
3.4 Effect of H2S on localized corrosion
Fig. 13 and 14 show the surface morphologies of X65 steel exposed to different
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systems after scale removal and the corresponding surface topographies measured by
profile meter, respectively. It can be observed that the surface morphologies after
scale removal seemed to correspond with the surface characteristics of corrosion
product scales.
In the SC CO2 phase without H2S, as shown in Fig. 13 (a), some localized corrosion pits were observed on the steel surface, and on other regions the polishing marks were
still visible. The surface topography of X65 steel in Fig. 14 (a) also shows that partial
surface area was smooth and not corroded. This implied that the corrosion of X65
steel exposed to SC CO2 phase without H2S was very localized. However, large
amounts of localized corrosion pits appeared on the whole steel surface in the SC CO 2
phase containing H2S, as shown in Fig. 13 (b). A much rougher steel surface was
observed on X65 steel (Fig. 14 (b)), which indicated that the whole surface of X65
steel suffered different degrees of corrosion. The maximum depth of localized
corrosion pits on X65 steel exposed to SC CO2 phase with H2S (20.4 µm) was
approximate two times larger than that without H2S (10.6 µm), suggesting thatlocalized corrosion was more serious when H2S existed in the SC CO2 system. The
calculated localized corrosion rates are presented in Fig. 15, the localized corrosion
rate of X65 steel exposed to SC CO2 phase with H2S was also approximate two times
higher than that without H2S. In pure SC CO2 phase, H2O only condensed on the local
surface of the steel [5, 10], this was the reason resulting in localized corrosion. In SC
CO2 phase, flow velocity barely effects the formation of corrosion product scale, so
the difference of localized corrosion in SC CO2 phase between with and without H2S
obviously ascribed to the addition of H2S. As confirmed above, when H2S existed in
the SC CO2 phase, H2O could condense on the whole steel surface and formed a water
film. HS- preferentially adsorbed on the steel surface and led to the formation of
porous iron sulfide layer. The corrosive ions such as HCO3- and HS- could penetrate
this layer through the defects in the layer and resulted in localized corrosion. On the
other hand, HS- enriched at the steel surface above which the corrosion scale was
defective, and resulted in the accumulation of the iron sulfides at these areas. The
accumulated iron sulfides on these areas could couple with the steel and promote
further dissolution of steel, ultimately aggravating localized corrosion.
In the aqueous phase, the localized corrosion of X65 steel without H2S was clearly
more serious than that with H2S, as observed in Fig. 13 (c) and (d). The surface
topographies shown in Fig. 14 (c) and (d) also demonstrated that X65 steel sufferedmore serious localized corrosion when no H2S existed. The maximum depth of
localized corrosion pits without H2S (316 µm) was nearly 4 times larger than that with
H2S (81 µm). Fig. 15 shows that the localized corrosion rate in the aqueous phase
without H2S was much higher. This was contrary to the phenomenon observed in the
SC CO2 phase. The wall shear stress was weak in the SC CO2 phase and had
essentially no effect on the formation of corrosion product scale, though it was strong
in the aqueous phase where it had a significant effect on the formation of corrosion
product scale. In a dynamic aqueous phase, without H2S, the wall shear stress could
cause cracking or spalling of a relatively compact scale due to defects inside the scale
or at the scale/matrix interface, as described in Fig. 16 (a) and (b). The lower pH and
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local flow intensity resulted in the localized dissolution and further destruction of the
scale, as a result, aggressive ions could reach the fresh steel surface and localized
corrosion occurred. The aggressive solution was also capable of reaching the steel
surface through cracks and induced localized corrosion, as presented in Fig. 16 (c). In
addition, the acceleration of the localized anodic reaction rate produced more Fe
2+
, promoting the precipitation of FeCO3 in the destructive scale area, as shown in Fig. 16
(d). When trace H2S dissolved in the aqueous phase, a defective iron sulfide scale
preferentially formed on the steel surface due to the preferential adsorption of HS- on
the steel surface (Fig. 17 (a)). This scale had poor protectiveness and corrosive ions
still easily reached the steel surface through this scale and accelerated the dissolution
of Fe. The dissolved Fe2+ combined with CO32- in the iron sulfide layer and resulted in
the formation of a cracked FeCO3/FeS mixed layer, as shown in Fig. 17 (b). The
mixed layer presented poor adhesion stress to the steel surface and easily spalled
under the action of the wall shear stress, resulted in serious general corrosion, as
presented in Fig. 17 (c). The corrosive ions could penetrate through this cracked andspalled scale and accelerated the general corrosion of the whole steel surface, thereby
localized corrosion was slight on X65 steel.
4. Conclusions
1 In the SC CO2 phase, the presence of small amount of H2S slightly enhanced the
general and localized corrosion rates of X65 steel. In the aqueous phase, the small
amount of H2S greatly increased the general corrosion rate of X65 steel, while
significantly decreased the localized corrosion rate.
2 The effect of H2S on the corrosion behavior of X65 steel in the dynamic aqueous
phase was much larger than that in the flowing SC CO2 phase. H2S did not change the
dominated corrosion type in the SC CO2 phase, localized corrosion was still the main
corrosion type. However, in the aqueous phase, H2S changed the dominated corrosion
type of X65 steel from localized corrosion to general corrosion.
3 In the SC CO2 phase without H2S, the local condensation of H2O on the steel
surface resulted in localized corrosion of the steel. However, the addition of small
amount of H2S in the SC CO2 phase changed the adsorbability of H2O on the steel
surface, resulting in the corrosion of the whole steel surface; the defects of the
siderite/iron sulfide mixed scale and the local enrichment of iron sulfides acceleratedin the localized corrosion of the steel.
4 In the dynamic aqueous phase without H2S, a dense FeCO3 scale with some defects
formed on the steel, which cracked and spalled easily from the location of defects and
led to severe localized corrosion. However, when small amount of H2S dissolved in
the dynamic aqueous phase, a porous and cracked siderite/iron sulfide mixed scale
formed on the steel surface. This layer had poor adhesion stress to steel matrix and
easily spalled completely from the steel surface, led to severe general corrosion.
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Acknowledgement
This research was supported by the Natural Science Foundation of Beijing (major
project) (No. 2131004) and the National Natural Science Foundation of China (No.
51271024).
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Figure captions
Fig. 1. Optical micrograph of X65 steel.
Fig. 2. Schematic diagram of autoclave and the location of sample in the autoclave.
Fig. 3. General corrosion rates of X65 steel exposed to both SC CO2 and aqueous
phases with 50 ppm and without H2S at 10 MPa and 80 °C for 10d.
Fig. 4. Surface morphologies of corrosion product scale on X65 steel exposed to SC
CO2 phase at 10 MPa and 80 °C without H2S (a, b) and with 50 ppm H2S (c, d).
Fig. 5. XRD spectra of corrosion product scale formed on X65 steel exposed to SC
CO2 phase with 50 ppm and without H2S.
Fig. 6. Raman spectra of the corrosion products on X65 steel in Fig. 3 (b) in SC CO2
phase without H2S at 10 MPa and 80 °C.
Fig. 7. Cross-section morphologies (a, b) and the corresponding EDS spectra (c, d and
e) of corrosion product scale on X65 steel exposed to SC CO2 phase without (a) and
with 50 ppm H2S (b): (c) is the EDS spectra of outer layer scale in (a); (d) is the EDS
spectra of outer layer scale in (b); (e) is the XRD spectra of inner layer scale in (b).
Fig. 8. Raman spectra of the inner layer scale on X65 steel formed in SC CO2 phase
without H2S at 10 MPa and 80 °C.
Fig. 9. Surface morphologies of corrosion product scale on X65 steel exposed to SC
CO2-saturated NaCl solution at 10 MPa and 80 °C without (a) and with 50 ppm H2S
(b).
Fig. 10. XRD spectra of corrosion product scale formed on X65 steel immersed in SC
CO2-saturated NaCl solution with 50 ppm H2S at 10 MPa and 80 °C.
Fig. 11. Cross-section morphologies of corrosion product scale on X65 steel
immersed in SC CO2-saturated NaCl solution without (a, b) and with 50 ppm H2S (c,
d) at 10 MPa and 80 °C.
Fig. 12. Raman spectra of the inner layer scale on X65 steel formed in SC
CO2-saturated NaCl solution without H2S at 10 MPa and 80 °C.
Fig. 13. Surface morphologies of the corroded X65 steel exposed to different systems
at 10 MPa and 80 °C after the removal of corrosion products: (a) in SC CO2 phase
without H2S; (b) in SC CO2 phase with 50ppm H2S; (c) in aqueous phase without H2S;
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(d) in aqueous phase with 50 ppm H2S.
Fig. 14. The depth of localized corrosion pits on X65 steel measured by profile meter
exposed to different systems at 10 MPa and 80 °C after the removal of corrosion
products.
Fig. 15. Localized corrosion rates of X65 steel exposed to both SC CO2 and aqueous
phases with 50 ppm and without H2S at 10 MPa and 80 °C for 10d.
Fig. 16. Schematic of the crack and spallation of corrosion product scale in the
dynamic aqueous phase without H2S at 10 MPa and 80 °C.
Fig. 17. Schematic of the crack and spallation of corrosion product scale in the
dynamic aqueous phase containing H2S at 10 MPa and 80 °C.
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Fig. 1. Optical micrograph of X65 steel.
Ferrite
Cementite
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Fig. 2. Schematic diagram of autoclave and the location of sample in the autoclave.
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Fig. 4. Surface morphologies of corrosion product scale on X65 steel exposed to SC
CO2 phase at 10 MPa and 80 °C without H2S (a, b) and with 50 ppm H2S (c, d).
(a)
(c)
(b)
(d)
Polishing marks
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Fig. 5. XRD spectra of corrosion product scale formed on X65 steel exposed to SC
CO2 phase with 50 ppm and without H2S.
0
4000
8000
12000
20 40 60 80 100
0
2000
4000
6000
Intensity,CPS
50 ppm H2SFeCO
3
FeFe
1+xS
Fe1-x
S
2, deg
no H2S
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Fig. 6. Raman spectra of the corrosion products on X65 steel in Fig. 3 (b) in SC CO2
phase without H2S at 10 MPa and 80 °C.
200 400 600 800 1000 1200 1400
50
100
150
200
Intensity,a.u.
Wavenumbers shift, cm-1
282
1084
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Fig. 7. Cross-section morphologies (a, b) and the corresponding EDS spectra (c, d and
e) of corrosion product scale on X65 steel exposed to SC CO2 phase without (a) and
with 50 ppm H2S (b): (c) EDS spectra of inner layer scale in (a); (d) EDS spectra of
outer layer scale in (b); (e) EDS spectra of inner layer scale in (b).
2 4 6 8 10 12 14 16 18 200.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
cps/e
C
O
Fe
Fe
MnMnNa
2 4 6 8 10 12 14 16 18 200.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
2.2
cps/e
C
O
Fe
Fe
MnMn S
2 4 6 8 10 12 14 16 18 200.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
2.2
cps/e
C
O
Fe
Fe
(a) (b)
(c) (e)(d)
Epoxy Epoxy
Matrix Matrix
Outer layer
Inner layer
Outer layer
Inner layer
Scale Scale
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200 400 600 800 1000 1200 14000
200
400
600
800
1000
731
1024
282Intensity,a.u.
Wavenumbers shift, cm-1
182
Fig. 8. Raman spectra of the inner layer scale on X65 steel formed in SC CO2 phasewithout H2S at 10 MPa and 80 °C.
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Fig. 9. Surface morphologies of corrosion product scale on X65 steel immersed in SC
CO2-saturated NaCl solution at 10 MPa and 80 °C without (a) and with 50 ppm H2S
(b).
(a) (b)
Pores
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Fig. 10. XRD spectra of corrosion product scale formed on X65 steel immersed in SC
CO2-saturated NaCl solution with 50 ppm H2S at 10 MPa and 80 °C.
20 40 60 80 1000
4000
8000
12000
Intensity,CPS
2,deg
FeCO3
FeS
Fe1-x
S
Fe
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Fig. 11. Cross-section morphologies of corrosion product scale on X65 steel
immersed in SC CO2-saturated NaCl solution without (a, b) and with 50 ppm H2S (c,
d) at 10 MPa and 80 °C.
(a)
(d)(c)
(b)
Epoxy
Matrix
Scale
Epoxy
Matrix
Scale
Epoxy
Matrix
Scale
Epoxy
Matrix
Scale
Outer layer
Inner layer
Original steel surface
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Fig. 12. Raman spectra of the inner layer scale on X65 steel formed in SCCO2-saturated NaCl solution without H2S at 10 MPa and 80 °C.
200 400 600 800 1000 1200 14000
200
400
600
800
1000
1200
1400
1600
Intensity,a.u.
Wavenumbers shift, cm-1
182
282
731
1084
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Fig. 13. Surface morphologies of the corroded X65 steel exposed to different systems
at 10 MPa and 80 °C after the removal of corrosion products: (a) in SC CO2 phase
without H2S; (b) in SC CO2 phase with 50ppm H2S; (c) in aqueous phase without H2S;
(d) in aqueous phase with 50 ppm H2S.
(a)
(d)(c)
(b)
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Fig. 14. The depth of localized corrosion pits on X65 steel measured by profile meter
exposed to different systems at 10 MPa and 80 °C after the removal of corrosion
products.
0 1 2 3 4 5-30
-20
-10
0
10
20
Dept
h,
m
Distance, mm
SC CO2 phase - no H
2S
10.6 m
0 1 2 3 4 5
-300
-200
-100
0
100
Depth,
m
Distance, mm
Aqueous phase - 50 ppm H2S
81.4 m
0 1 2 3 4 5
-300
-200
-100
0
100
D
epth,
m
Distance, mm
Aqueous phase - no H2S
316 m
0 1 2 3 4 5-30
-20
-10
0
10
20
Depth
, m
Distance, mm
SC CO2 phase - 50 ppm H
2S
20.4 m
(a)
(d)(c)
(b)
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0
2
4
6
8
10
12
Localizedcorrosionrate,mm/y
no H2S
50 ppm H2S
SC CO2 phase Aqueous phase
0.29 0.48
9.19
2.45
Fig. 15. Localized corrosion rates of X65 steel exposed to both SC CO2 and aqueous phases with 50 ppm and without H2S at 10 MPa and 80 °C for 10d.
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Fig. 16. Schematic of the crack and spallation of corrosion product scale in the
dynamic aqueous phase without H2S at 10 MPa and 80 °C.
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Fig. 17. Schematic of the crack and spallation of corrosion product scale in the
dynamic aqueous phase containing H2S at 10 MPa and 80 °C.
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Table 1 Compositions of CO2 streams transported in the existing pipelines (vol%)
Pipelines A [13-15] B
[16]
C
[14-1
5]
D
[16]
E
[15]
F
[14,
17]
G
[14]
H
[14-1
5]
CO2 85-95 93-96 95 96 96.8-97.4
98.5 98.7-99.4
99.7
CH4 2-15
(C6H14)
0.5-2 1-5 0.7 1.7 0.2 0.3 -
N2 <0.5 3-5 4 <300 0.6-0.9 1.3 0.3 0.3
H2S (ppmv) <260 150 20 9000 - <26 Trace -
CO - - - 0.1 - - - -
O2 (ppmv) - - - <70 - <14 - -
SOx - - - - - - - -
NOx - - - - - - - -
H2 - 3-5 - Trace - - - -Ar - 3-5 - - - - - -
H2O (ppmv) 122 Saturat
ed
630 20 315 630 418 -
Source Anthropog
enic
Natural Natur
al
Anthropoge
nic
Natural Natur
al
Natural Natur
al
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Table 2 CO2 quality specifications
DYNAMIS
CO2 quality
recommendati
on
Alstom CO2
quality tolerances
IPCC CO2 quality specification Kinder
Morgan
specificati
on
Coal fired plants Gas fired plants
Concentration Low HighPost-combust
ion capture
Pre-combus
tion captureOxy-fuel
Post-combu
stion capture
Pre-combus
tion capture
Oxy-fu
elCO2
(vol.%)>95.5 >90 >95 ≥95
H2O
(ppmv)500 <10 <600 ≤630
H2S
(ppmv)200 <100
<
150000 100-6000 0 0 <100 0
≤20
ppmw
SOx
(ppmv)100 <100 <1500 <100 0 5000 <100 0 <100
≤35
ppmw
NOx
(ppmv)100 <100 <1500 <100 0 100 <100 0 <100
CO
(ppmv)2000 <100
<
400000 300-4000 0 0 400 0
O2 (ppmv)
EOR:100-1000
; Aquifer: <4
v%
<10 <1000 <10 ppmw
CH4
(vol.%)
EOR <2;
Aquifer <4<4 <5
N2, Ar, H2 <4 (all <4 <4 N2: ≤4
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(vol.%) non-condensab
le gases)
Others
(ppmv)
Particulates
(mg/N m3):
Low <0.1; High
<10
(EOR/Storage)
N2/Ar/O2:
100
N2/Ar/O2:
300-6000
N2/Ar/O
2: 37000
N2/Ar/O2:
100
N2/Ar/O2:
13000
N2/Ar/
O2:
41000
Total
sulfur: ≤
35 ppmw;
Hydrocarb
on: ≤ 5
vol.%
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Table 3 Experimental conditions
Temperature
(°C)
Pressure
(MPa)
Flow
rate
(m/s)
H2S
(ppm)
Immersion
time (d)
Water-saturatedCO2 (SC CO2
phase80 10 1
0
10
50
CO2-saturated
water (Aqueous
phase)
0
50
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Table 4 Experimental formulas for calculation of the equilibrium constants
Formula Solubility
limit
Ref.
K sp, FeCO3= 10-59.3498-0.041377T K -
2.1963T K
+24.5724logT K +2.518 I 0.5-0.657 I
1.58×10-10 [51]
K sp,FeS= 102848.770
T K -6.347 + log K a,1
1.58×10-5 [52]