Accepted Manuscript Effects of laser remelting speeds on microstructure, immersion corrosion, and electrochemical corrosion of arc–sprayed amorphous Al–Ti–Ni coatings Haixiang Chen, Dejun Kong PII:
S0925-8388(18)33140-2
DOI:
10.1016/j.jallcom.2018.08.252
Reference:
JALCOM 47340
To appear in:
Journal of Alloys and Compounds
Received Date: 14 February 2018 Revised Date:
23 August 2018
Accepted Date: 26 August 2018
Please cite this article as: H. Chen, D. Kong, Effects of laser remelting speeds on microstructure, immersion corrosion, and electrochemical corrosion of arc–sprayed amorphous Al–Ti–Ni coatings, Journal of Alloys and Compounds (2018), doi: 10.1016/j.jallcom.2018.08.252. This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.
ACCEPTED MANUSCRIPT
Effects of laser remelting speeds on microstructure, immersion corrosion, and electrochemical corrosion of arc–sprayed amorphous Al–Ti–Ni coatings
RI PT
Chen Haixiang, Kong Dejun College of Mechanical Engineering, Changzhou University, Changzhou 213164, P.R. China
*Correspondent: Kong Dejun, Ph. D., Professor, Tel: 86–051981169810, Fax: 86–051981169812,
M AN U
SC
E–mail: kong–
[email protected].
Abstract: An arc–sprayed amorphous Al–Ti–Ni coating on S355 structural steel was processed using a laser remelting (LR). The surface and cross–section morphologies, chemical compositions, phases and residual stresses of obtained Al–Ti–Ni coatings at the LR speeds of 5, 10, and 15 mm/s were analyzed
TE D
using a field emission scanning electron microscope (FESEM), energy dispersive spectrometer (EDS), X–ray diffractometer (XRD), and X–ray diffraction stress tester, respectively, and the effects of LR speeds on their immersion corrosion and potentiodynamic polarization curves of Al–Ti–Ni coatings in
EP
3.5% NaCl solution were also investigated to analyze the mechanism of corrosion resistance. The results
AC C
show that the metallurgical bonding is formed at the Al–Ti–Ni coating interface due to the interdiffusions and recombinations of Al, Ti, Ni, Fe, Cr and Mn. The Al–Ti–Ni coatings at the different LR speeds obtain a certain amount of amorphous phases, which are detected as AlFe, AlFe3, AlCrFe2, Ni2MnAl, and AlNi phases. The residual stresses of as–obtained Al–Ti–Ni coatings at the LR speeds of 5, 10, and 15 mm/s are –12 ± 8, 43.9 ± 3, and –34.4 ± 8 MPa, respectively, of which the tensile residual stress exacerbates the immersion corrosion and the compressive stress restrains the crack expansion.. The corrosion potentials of Al–Ti–Ni coatings at the LR speeds of 5, 10, and 15 mm/s are –1.046, –1.106,
1
ACCEPTED MANUSCRIPT and –0.986 V, respectively, which shift positively than S355 steel and effectively increase the corrosion resistance of substrate, the electrochemical corrosion resistance of Al–Ti–Ni coating at the LR speed of 15 mm/s is the best among the three kinds of coating.
RI PT
Keywords: arc spraying; laser remelting (LR); residual stress; immersion corrosion; electrochemical corrosion
SC
1 Introduction
M AN U
As a structural steel, S355 on offshore platforms continually serves in atrocious ocean environment, which is extremely vulnerable to pitting and further produce corrosive cracks [2, 3], therefore, immersion corrosion is one of main reasons for its failure [1]. Further more, offshore platforms are impossible to maintain regularly as a ship because they are far away from the coast, once the corrosion degradation of S355 steel occurs, which will lead to
TE D
incalculable economic losses and casualties. Therefore, the development of anti–corrosion coating on offshore platforms has important scientific significance.
Al coating with low cost, high specific strength and good corrosion resistance is widely deposited on S355 steel
EP
to provide a cathodic protection on offshore platforms [4], which can rapidly form the passive film due to the high
AC C
activity of Al. Unfortunately, a number of chloride ions are presented in seawater, the thin and instable passive film easily suffers from severe pitting. Compared with the traditional Al coating, amorphous Al coating with the unique atom arrangement of long– and short–range disorders is no corrosion sensitive defects such as grain boundary, dislocation and secondary phase, its corrosion resistance is higher than crystal coating [5, 6], which has become the new ideal material for application in anti–corrosion coating [7]. However, the amorphous Al belongs to the marginal glass formers, which requires a very rapid cooling rate (105–106 K/s) to avoid crystallization [6], its application is inevitablely restricted by the limited amorphous forming ability of conventional manufacturing
2
ACCEPTED MANUSCRIPT methods [9]. At present, amorphous Al has been paid wide attentions at China and abroad [8], its fabrication methods have become the research hot spots, whose critical problem is to design appropriate alloy compositions and optimize fabrication methods for increasing the amorphous forming ability [10]. Researches have shown that
RI PT
Ti and Ni elements incorporated into the Al coating can increase its amorphous forming ability [11–13], the about researches of Al–Ti–Ni coating have rarely reported.
Arc spraying with simple operation, high efficiency, and low cost has become an economical and effective
SC
method to fabricate the Al coating [14]. However, the sprayed Al coating is typical lamellar structure with the
M AN U
mechanical bonding at the coating interface, the internal porosity originated from the unmelted Al particles easily forms the corrosion pitting in seawater, which greatly reduces its immersion corrosion resistance [15]. Laser remelting (LR) combines laser technology with surface treatment, which has advantages of sufficient energy, fast heating and rapid cooling rate (105 –1010 K/s) [9, 16], the Al coating is completely melted to eliminate the above
TE D
arc spraying defects and form metallurgical bonding with the substrate. At the same time, the LR with higher cooling rate easily meets the critical cooling rate of amorphous Al and forms the nonequilibrium microstructure to promote amorphous formation [17]. LR speed directly determines the heating time of laser energy on the Al
EP
coating [18], the high LR speed shortens the interaction time between the laser energy and the substrate, which
AC C
reduces the input energy and leads to the Al coating not to be completely melted; while the low LR speed leads to the Al coating suffer a severe warp. Thus, it is essential to investigate a suitable LR speed for fabricating amorphous Al coating, Zhang et al [19] analyzed the effects of laser power on the microstructure and properties of laser cladded Co–based amorphous composite coatings; Mahamood et al [20] researched the influence of scanning speed on the microstructure and microhardness of Ti alloy produced by laser deposition; Li et al [21] researched the effect of remelting scanning speed on the amorphous forming capability of Ni–based alloy using a laser cladding and LR. However, there are few reports about the effects of LR speed on the morphology and
3
ACCEPTED MANUSCRIPT comprehensive properties of arc–sprayed Al–Ti–Ni coating. In this study, arc–sprayed Al–Ti–Ni coatings on S355 steel were remelted at the LR speeds of 5, 10, and 15 mm/s. The purpose was to investigate the effects of LR speeds on the microstructure, immersion corrosion and
RI PT
electrochemical corrosion of amorphous Al–Ti–Ni coatings in 3.5 % NaCl solution, which provided a theoretical basis for the application of amorphous Al–Ti–Ni coatings on offshore platforms.
SC
2 Experimental
M AN U
2.1 Sample preparation
The substrate was European standard S355 structural steel with the chemical composition (wt, %). C 0.17, Si 0.55, Mn 0.94. P 0.035, Cr 0.065, S 0.035, Ni 0.065, Mo 0.30, the rest was Fe. The substrate was ground with 400# sandpaper, coarsened with corundum and cleaned with acetone, and then dried in air. The Al wire packaged
TE D
Ti–Ni powder with the diameter of 2 mm was used for arc spraying, its sketch of wire cross–section is shown in Fig.1. The arc spraying was conducted on an AS400 type intelligent digital arc spraying device, the specific parameters of arc–spraying process are shown in Tab.1. After arc spraying twice, the thickness of Al–Ti–Ni
EP
coating was 450–600 µm.
AC C
The LR test was conducted on a ZKSX–2008 type fiber–coupled laser spraying system, Ar gas was employed as protective gas during the LR test, technical parameters: laser power of 1000 W, spot diameter of 4 mm, overlap ratio of 50 %, respective speed of 5, 10, and 15 mm/s, and Ar gas speed of 15 L/min. After the LR test, the sample was cut into the dimensions of 15 mm × 15 mm × 5 mm. 2.2 Characterization methods The morphologies and chemical compositions of obtained coatings were analyzed using a SUPRA55 type field–emission scanning electron microscope (FESEM) and its configured energy dispersive spectrometer (EDS),
4
ACCEPTED MANUSCRIPT the phases were also analyzed using a D/MAX2500 type PC X–ray diffractometer (XRD), and the residual stresses were analyzed on an X350–A type X–ray diffraction stress tester with the inclination fixed 2ψ method, Cu target–Kα radiation was selected for measuring residual stress, diffraction face of (422), respective incident angle
RI PT
of 0, 15, 25 and 35 o, stress constant of –179 MPa/o, scanning angle 2θ of 145–162 o, scanning step angle of 0.1 o, counting time of 0.5 s, tube voltage of 25.0 kV, tube current of 10.0 mA, and collimated tube diameter of 1 mm. According to Prague equation, residual stress (σ) was
∆(2θ ) ∆ sin 2 ψ
(
)
SC
σ =k
(1)
M AN U
where k was the stress constant, which was related to the coating material; θ was the scanning angle; ψ was the incident angle of X–ray.
The immersion corrosion was performed in a YQW–250 type immersion corrosion chamber in accordance with the GB 6458–86 neutral salt spraying (NSS) protocol, 3.5 % NaCl solution was used to simulate the immersion
TE D
corrosion in seawater. Technological parameters: pH of 6.5 – 7.2, temperature of 26 ± 7 oC, immersion time of 720 h. The morphologies, element distributions and phases of Al–Ti–Ni coatings after the immersion corrosion
EP
test were analyzed using a FESEM, EDS, and XRD, respectively. The electrochemical performance test was conducted on a CHI660E type electrochemical workstation with the
AC C
conventional three–electrode system, and the platinum plate and mercury/calomel–saturated KCl were as the counter electrode and reference electrode, respectively. The sample with the area of 10 mm × 10 mm was exposed in 3.5 % NaCl solution as the working electrode, and the other surfaces were coated and soaked for 15 min before the electrochemical corrosion test, its specific parameters are shown in Tab.2.
3 Analysis and discussion 3.1 Characterizations of surfaces and cross–sections
5
ACCEPTED MANUSCRIPT 3.1.1 Morphologies and EDS analysis of Ti–Ni powder The morphology of Ti–Ni powder is shown in Fig.2 (a). The particle A was Ti with the irregular shape, its surface was loose and rough; while the particle B was Ni with the flat–ball–like shape, its surface was compact
RI PT
and flat. The EDS analysis result of Ti–Ni powder is shown in Fig.2 (b). The Ti–Ni powder was primarily composed of Ti and Ni elements, the C and O elements were also detected, which originated form the absorptive products in the air. The EDS analysis results of Ti and Ni particles are shown in Fig.2 (c)–(d). The Ti and Ni
SC
particles were the constituent elements of Ti–Ni powder, while the C and O elements were the impurity elements;
M AN U
the Pt came from the sputtering gold on the powder surface to enhance its electrical conductivity during the SEM test.
3.1.2 Plane scan analysis of Al–Ti–Ni coating surfaces
The morphology of Al–Ti–Ni coating surface at the LR speed of 5 mm/s is shown in Fig.3 (a). The coating
TE D
surface was rough and porous, which reduced the density of coating surface. The laser working modes between the conduction mode and the keyhole mode were able to convert with the critical value, when the laser energy was lower than that of conduction mode, the low LR speed increased the energy absorbed by the unit volume, which
EP
was conducive to melting the arc–sprayed Al–Ti–Ni coating completely and improved its density; conversely,
AC C
when the laser energy was higher than that of conduction mode, the coating surface temperature was higher than the gasification temperature of Al and led to an intense evaporation of Al, the produced recoil pressure and Marangoni convection caused the decrease of molten pool to form the porosity [22]. At the LR speed of 5mm/s, the input energy was excessive to satisfy the melting of Al–Ti–Ni coating, and the gas originated from the evaporation of Al had no enough time to escape due to the rapid solidification of molten pool, forming the porosity on the coating surface. Some white spherical particles were presented on the coating surface, which was because the high energy led to longer residence time of molten pool, leading to more and more metal and carbon
6
ACCEPTED MANUSCRIPT diffuse into the liquid molten pool and subsequently formed the super saturation. With the continuous and excessive input of laser energy, there was more and more particles precipitation in the rapid solidification process [23]. The result of plane scan analysis is shown in Fig.3 (b). The Al content was low due to the high temperature
were evenly distributed on the coating surface, as shown in Fig.3 (c)–(f).
RI PT
evaporation, while the Fe content was high due to the element diffusion from the substrate. The Al, Ti, Ni and Fe
The morphology of Al–Ti–Ni coating surface at the LR speed of 10 mm/s is shown in Fig.4 (a). The coating
SC
surface was uneven, showing a certain extent of structural fluctuation. Under the action of high laser energy, the
M AN U
coating surface was rapidly heated and melted to form the molten pool. The liquid metal flew from the edge of molten pool into the bottom due to the large gradient, density and viscosity between the center and the edge of molten pool, then forming the undulation after a rapid solidification process. The result of plane scan analysis is shown in Fig.4 (b). Compared to the result of Al–Ti–Ni coating at the LR speed of 5 mm/s, the Al content
TE D
increased due to the decrease of input heat, which reduced the evaporation of Al. The Al was uniformly distributed on the coating surface, as shown in Fig.4 (c). The Ti, Ni and Fe were enriched on the small range, as shown in Fig.4 (d)–(f).
EP
The morphology of Al–Ti–Ni coating surface at the LR speed of 15 mm/s is shown in Fig.5 (a). The coating
AC C
surface was flat and continuous with no obvious porosity and cracks. The high energy laser caused the liquid possess the adequate suitable energy to move to the equilibrium position, which was conducive to forming the homogeneous structure. The result of plane scan analysis is shown in Fig.5 (b). The high content of Al was detected on the coating surface, which was the same as that at the LR speed of 10 mm/s. The Al, Ti, Ni and Fe were enriched on the coating surface with the different degrees, as shown in Fig.5 (c)–(f). 3.1.3 Plane scan analysis of Al–Ti–Ni coating cross–sections The morphology of Al–Ti–Ni coating cross–section at the LR speed of 5 mm/s is shown in Fig.6 (a). The
7
ACCEPTED MANUSCRIPT cross–section was flat, with no obvious cracks. The result of plane scan analysis is shown in Fig.6 (b). The Al, Ti, Ni, Fe, Cr, C and O were detected on the coating–substrate cross–section, among them, the Al, Ti and Ni were the constituent elements of Al–Ti–Ni coating, and the Fe, Cr and C originated from the substrate, while the O was the
RI PT
impurity element. The Al, Ti, and Ni were evenly distributed on the Al–Ti–Ni coating cross–section with the high content, as shown in Fig.6 (c)–(e). There was obvious diffusion of Fe element from the substrate into the Al–Ti–Ni coating, which was the result of Fe diffusion between the coating and the substrate, as shown in Fig.6 (f).
SC
The morphology of Al–Ti–Ni coating cross–section at the LR speed of 10 mm/s is shown in Fig.7 (a). There
M AN U
were also no obvious porosity and cracks on Al–Ti–Ni coating cross–section. The result of plane scan analysis is shown in Fig.7 (b). The coating–substrate cross–section was composed of Al, Ti, Ni, Fe, Cr and C, among them, the Al, Ti and Ni were the constituent elements of Al–Ti–Ni coating, and the Fe, Cr and C came form the elements of substrate. The Al, Ti and Ni appeared obvious atoms–enriched zones on the Al–Ti–Ni coating cross–section,
TE D
which were diffused into the substrate to a lesser extent, as shown in Fig.7 (c)–(e). The Fe was distributed on the substrate cross–section, and obviously diffused into the Al–Ti–Ni coating at the interface, as shown in Fig.7 (f). The morphology of Al–Ti–Ni coating cross–section at the LR speed of 15 mm/s is shown in Fig.8 (a). The
EP
Al–Ti–Ni coating covered on the substrate with a good density and continuity. The result of plane scan analysis is
AC C
shown in Fig.8 (b). The constituent elements of Al–Ti–Ni coating– substrate cross–section were the same as those at the laser LR speed of 5 mm/s. The Al with the high content was uniformly distributed on the Al–Ti–Ni coating cross–section, as shown in Fig.8 (c). The apparent enrichment of Ti and Ni on the coating cross–section exhibited a small degree of diffusion into the substrate, as shown in Fig.8 (d)–(e). The Fe was obviously diffused in the coating, which was similar to those at the LR speeds of 5 and 10 mm/s, as shown in Fig.8 (f). 3.1.4 XRD analysis The XRD analysis of Al–Ti–Ni coatings at different scanning speeds is shown in Fig.9. The Al–Fe intermetallic
8
ACCEPTED MANUSCRIPT compounds (AlFe, AlFe3), AlCrFe2, Ni2MnAl, and AlNi were detected on the XRD patterns. The high energy laser led to the intermetallic diffusion at the coating interface, which formed the compounds and developed effective metallurgical reactions between the Al–Ti–Ni coating and the substrate, enhancing the interfacial bonding strength o
and 60–70 o, indicating that the
RI PT
[24–26]. The amorphous peaks of Al–Ti–Ni coatings were observed at 30–40
ordered crystal structure of coating was destroyed. The radius sequence of chemical elements was Ti (0.147 nm) > Al (0.143 nm) > Ni (0.125 nm) > Fe (0.124 nm), the significant difference among the atomic sizes increased the
SC
difficulty of rearranging atoms on the microscale, which favored the formation of amorphous structure [27]. The
M AN U
Al–Ti–Ni coatings had weakly diffusion peaks at 40–50 o, which superimposed with the high intensity diffraction peaks of AlNi, AlFe3, AlFe, Ni2MnAl, and AlCrFe, indicating that the arc–sprayed Al–Ti–Ni coatings after the LR test were a complex structure of crystal, amorphous and compound phases. Because the heating rate of affected zone was lower than the critical heating rate, which avoided the crystallization [28], the crystal phases existed in
TE D
the Al–Ti–Ni coating. The diffraction peaks on the angle range of Al–Ti–Ni coatings were similar, but the peak intensity at the LR speed of 15 mm/s decreased obviously, which increased the amorphous content. For amorphous phases, the cooling rate was an important factor for inhibiting the nucleation and growth of grains. The
EP
cooling rate at the different LR speeds endowed the different amorphous forming ability for Al–Ti–Ni coating, the
AC C
high cooling rate was beneficial to forming amorphous structure. This was because the formation of amorphous structure needed extremely rapid cooling rate and less retention time at the melting state [21]. The input energy for molten pool was large and the cooling rate was relatively small at the low LR speed, in which the grain had more time to form and grow up. Conversely, the high LR speed decreased the input heat, which resulted in the less residence time in molten state and increased the cooling rate, thus enlarging the tendency to form the amorphous structure [29]. As a result, the Al–Ti–Ni coating at the LR speed of 15 mm/s formed more amorphous phases during the LR test.
9
ACCEPTED MANUSCRIPT 3.1.5 Residual stress analysis The residual stresses of Al–Ti–Ni coatings at the different LR speeds are shown in Fig.10. The residual stresses of amorphous Al–Ti–Ni coatings at the LR speeds of 5, 10 and 15 mm/s were –12.2 ± 8 MPa (Fig.10 (a)), 43.9 ± 3
RI PT
MPa (Fig.10 (b)) and –34.4 ± 8 MPa (Fig.10 (c)), respectively. The residual stresses after the LR test mainly came from that the temperature distribution was extremely uneven due to its local input heat, which led to the slower cooling rate in molten pool center and faster peripheral cooling, forming the temperature gradient from the centre
SC
to the edge of molten pool. The molten pool shrunk and restricted with the surrounding metal in the rapid
after solidification. 3.2 Corrosion characterizations 3.2.1 Corrosion morphologies
M AN U
solidification process, leading to constraining the deformation and forming the residual stresses in the coating
TE D
Fig.11 (a) shows the corrosion morphology of Al–Ti–Ni coating at the LR speed of 5 mm/s. The obvious corrosion cracking was presented on the Al–Ti–Ni coating surface, the longitudinal cracks were tended along the surface perpendicular to the Al–Ti–Ni coating, which extended flexurally and connected with the secondary
EP
cracks. The cracks were mainly originated from the defects, such as pitting [31]. On one hand, the porosity on
AC C
Al–Ti–Ni coating surface (Fig.3 (a)) provided the pathway for the penetration of corrosive media and formed the pitting in the initial period of immersion corrosion. The stress was concentrated on the local zones of pitting [32, 33]; On the other hand, the pitting was the source of corrosion crack, whose sensitivity was proportional to the sizes of pitting. With the increase of pitting sizes, the stress concentration on the pitting zones was more obvious [34]. The compressive stress of –12.2 ± 8 MPa in Fig.10 (a) was not enough to restrict the crack growth, more pitted porosity was formed and maintained growth up during the continuous immersion corrosion, eventually connected with each other. When the local stress around the pitting exceeded the certain critical stress, the stress
10
ACCEPTED MANUSCRIPT concentration occurred on the groove position, which was transferred from the pitting to the crack [35]. The corrosion products on the cracks were loose, leading to the corrosion condition of local electrolyte was maintained, and the corrosion pitting was further connected. The result of plane scan analysis is shown in Fig.11 (b). The Al
RI PT
maintained a low content, which was unevenly distributed on the coating, as shown in Fig.11 (c). The Ti and Ni were also unevenly distributed on the coating surface, forming the atoms–rich zones on the Al–poor zones, as shown in Fig.11 (d)–(e).
SC
Fig.12 (a) shows the corrosion morphology of Al–Ti–Ni coating at the LR speed of 10 mm/s. The corrosion was
M AN U
uneven on the coating, there were more corrosion cracks and large shedded areas. Compared with that at the LR speed of 5 mm/s, the corrosion degree was severer. The penetration and diffusivity of corrosive Cl– with the small atom radius was enhanced due to the tensile stress of 43.9 ± 3 MPa in Fig.10 (b), which promoted the forming of microcracks and accelerated the local corrosion sensitivity near the defects and the dissolution of Al in
TE D
microcracks, so the high corrosion speed led to the larger crack width [36]. The cracks on Al–Ti–Ni coating surface were connected with the increase of corrosion time, once the bonding strength among the Al–Ti–Ni coatings due to the mechanical interlocking reactions was less than the local tensile stress, the adhesive loss and
EP
spalling occurred on the coating surface [37]. The result of plane scan analysis is shown in Fig.12 (b). Compared
AC C
with that in Fig.4 (b), the mass fraction of Al decreased, indicating that the Al was dissolved into 3.5% NaCl solution. The Al was unevenly distributed on the coating surface, forming the atom–rich zones, as shown in Fig.12 (c). The Ti and Ni were also unevenly distributed, and the atoms–rich zones were formed on the Al atom–poor zones, as shown in Fig.12 (d)–(e).
Fig.13 (a) shows the corrosion morphology of Al–Ti–Ni coating at the LR speed of 15 mm/s. The corrosion cracks were covered by the corrosion products, and the microdefects on the coating surface were the preferred location of corrosion. The microcracks reacted with the corrosive media and produced the dense corrosion
11
ACCEPTED MANUSCRIPT products, which were deposited on the microcrack surfaces, preventing the electrolyte infiltration to a certain extent. The compressive stress of Al–Ti–Ni coating in Fig.10 (c) was also conducive to closuring of coating cracks and slowing down the invasion of aggressive ions into the Al–Ti–Ni coating, which prevented further corrosion.
RI PT
The result of plane scan analysis is shown in Fig.13 (b). Compared with that in Fig.5 (b), the Al content also decreased, indicating that the Al was dissolved. The Al, Ti, and Ni contents were unevenly distributed on the coating surface, as shown in Fig.13 (c)–(e).
SC
3.2.2 XRD analysis after corrosion
M AN U
The XRD spectra of amorphous Al–Ti–Ni coatings at the different LR speeds after the immersion corrosion test are shown in Fig.14 (a). The detected phases of Al–Ti–Ni coatings were similar, which were composed of AlNi, AlFe3, AlFe, Ni2MnAl and AlCrFe2, and the trend of peak broadening at 30–40 o and 60–70 o showed the presence of amorphous phases. Compared with those in Fig.9, there was no new phases formed, indicating that their phase
TE D
compositions were stable. The XRD results showed that the effect of phase compositions on the corrosion resistance was small, while the content of amorphous phase had the greater influence on their corrosion resistance. 3.2.3 Electrochemical Corrosion
EP
The potentiodynamic polarization curves of Al–Ti–Ni coatings at the different LR speeds and S355 steel in
AC C
3.5 % NaCl solution are shown in Fig.15. The polarization curves of Al–Ti–Ni coatings had similar shape, indicating there was the same corrosion process in the initial immersion period. At the initial period of anodic polarization, the current density increased with the increase of potentials, the coatings occurred the anodic dissolution reaction. With the potentials continuously increased, the corrosion current changed slowly, the anodic polarization curve on the range did not obey the Talfel law. As the polarization potentials continuously increased, the anode currents increased sharply. Due to the increasing potentials, the migration rate of anions in 3.5 % NaCl solution also increased, and the Cl– easily penetrated the passivation film on the Al–Ti–Ni coating, leading to
12
ACCEPTED MANUSCRIPT easily reaching the pitting potential. The corresponding electrochemical parameters of Al–Ti–Ni coatings such as corrosion potential (Ecorr) and corrosion current density (icorr) were obtained from the polarization curves. The corrosion potentials of Al–Ti–Ni coatings at the LR speeds of 5, 10, 15 mm/s were –1.046, –1.106, and –0.986 V,
RI PT
respectively. Compared with the –1.426 V of S355 steel, the corrosion potentials of Al–Ti–Ni coatings shifted positively, suggesting that the Al–Ti–Ni coating enhanced the corrosion resistance of substrate, this was attributed to the formed amorphous structures with high chemical stability and the complex phase of intermetallic
SC
compounds after the LR test. The corrosion occurred preferentially at the grain boundary location, while the
M AN U
amorphous structure inhibited the Cl– penetration into the coating due to the lack of defects, such as grain boundaries, dislocations and second particles at a certain extent [39], the intermetallic compounds increased the corrosion potential and delayed the corrosion rate [9], effectively improving the corrosion resistance of Al–Ti–Ni coatings.
TE D
The corrosion current density of Al–Ti–Ni coatings after the LR test was 10–6–10–9 A/cm2, which were more than 10–4 A/cm2 of substrate. Generally speaking, the higher Ecorr usually meant better chemical stability, while the lower icorr meant lower corrosion rate [38]. Compared with that at the LR speed of 15 mm/s, the Al–Ti–Ni coatings
EP
at the LR speeds of 5 and 10 mm/s had inactive Ecorr and greater icorr, indicating that their corrosion resistance was
AC C
relatively poor. Therefore, there was severe corrosion in Figs.11 (a) and 12 (a). The Al–Ti–Ni coating at the LR speed of 15 mm/s showed the highest Ecorr and the lowest icorr, indicating the best corrosion resistance among three kinds of Al–Ti–Ni coatings, which was consistent with the lower corrosion degree in Fig.13 (a). The corrosion resistance of Al–Ti–Ni coating at the LR speed of 15 mm/s was the best among three kinds of coatings due to its high contents of amorphous structure and excellent surface morphology, which were benefit to reducing the active center of corrosion and improved its corrosion resistance.
13
ACCEPTED MANUSCRIPT 4 Conclusions (1) The Al, Ti and Ni of Al–Ti–Ni coatings and the Fe, Mn, and Cr of substrate at the different LR speeds are diffused to generate the intermetallic compounds of AlFe3, AlFe, AlCrFe2, Ni2MnAl, and AlNi, which forms
RI PT
metallurgical bonding at the coating interface. (2) The phases of Al–Ti–Ni coatings at the LR speeds of 5, 10 and 15 mm/s are composed of crystal, amorphous and intermetallic compound phases, the increased LR speed is beneficial to forming amorphous
SC
phases.
M AN U
(3) The residual stresses of Al–Ti–Ni coating at the LR speeds of 5, 10 and 15 mm/s are –12 ± 8, 43.9 ± 3 and –34.4 ± 8 MPa, of which the compressive stress is benefit to restraining the crack expansion, while the tensile residual stress accelerates the occurrence and process of immersion corrosion.
(4) The corrosion potentials of Al–Ti–Ni coatings at the LR speeds of 5, 10 and 15 mm/s are –1.046, –1.106 and
TE D
–0.986 V, respectively, the corrosion degree of Al–Ti–Ni coating at the LR speed of 15 mm/s is the lightest, which
EP
is due to the higher amorphous content and excellent surface morphology.
Acknowledgments
AC C
Financial support for this research by the Key Research and Development Project of Jiangsu Province (BE2016052) is gratefully acknowledged.
References
[1] Chun YJ, Hong ZX, Xing HS, Oleg G. Experimental and numerical study on collapse of aged jacket platforms caused by corrosion or fatigue cracking. Engineering Structures, 2016, 112: 14–22 [2] Adedipe O, Brennan F, Kolios A. Review of corrosion fatigue in offshore structures: Present status and challenges in the offshore wind sector. Renewable and Sustainable Energy Reviews, 2016, 61: 141–154 [3] Bhandari J, Khan F, Abbassi R, Garaniya V, Ojeda R. Modelling of pitting corrosion in marine and offshore steel structures – A technical review. Journal of Loss Prevention in the Process Industries, 2015, 37: 39–62 [4] Yang HB, Qian Z, Zhang GJ, Nie JF, Liu XF. The grain refinement performance of B–doped TiC on Zr–containing Al alloys. Journal of Alloys and Compounds, 2018, 731: 774–783
14
ACCEPTED MANUSCRIPT [5] Hosaka T, Yoshihara S, Amanina I, Donald BJM. Influence of grain refinement and residual stress on corrosion behavior of AZ31 magnesium alloy processed by ECAP in RPMI–1640 medium. Procedia Engineering. 2017, 184: 432–441 [6] Zhang JF, Liu M, Song JB, Deng CM, Deng CG. Microstructure and corrosion behavior of Fe–based amorphous coating prepared by HVOF. Journal of Alloys and Compounds, 2017, 721: 506–511 [7] Liu JT, Hou JX, Zhang XR, Guo J, Xu LF, Fan GJ. Influence of remelting treatment on corrosion behavior of amorphous alloys. Rare Metal Materials and Engineering. 2017, 46(2): 296–300 [8] Cheng JB, Wang BL, Liu Q, Liang XB. In–situ synthesis of novel Al–Fe–Si metallic glass coating by arc spraying. Journal of
RI PT
Alloys and Compounds. 2017, 716: 88–95
[9] Tan CL, Zhu HM, Kuang TC, Shi J, Liu HW, Liu ZW. Laser cladding Al–based amorphous–nanocrystalline composite coatings on AZ80 magnesium alloy under water cooling condition. Journal of Alloys and Compounds, 2017, 690: 108–115
[10] Zhang CL, Lv P, Cai J, Zhang YW, Xia H, Guan QF. Enhanced corrosion property of W–Al coatings fabricated on aluminum using surface alloying under high–current pulsed electron beam. Journal of Alloys and Compounds, 2017, 723: 258–265 Zhao SF, Lu SY, Yang GN, Chen SQ, Yao KF. Effects of Cu addition on the glass forming ability and
SC
[11] Gu JL, Shao Y,
corrosion resistance of Ti–Zr–Be–Ni alloys. Journal of Alloys and Compounds, 2017, 725: 573–579 [12] Sichani HR, Salehi M, Edris H, Farani MT. The effect of APS parameter on the microstructural, mechanical and corrosion properties of plasma sprayed Ni–Ti–Al intermetallic coatings. Surface and Coatings Technology, 2017, 309: 959–968
Alloys and Compounds, 2016, 661: 294–305
M AN U
[13] Sina H, Surreddi KB, Iyengar S. Phase evolution during the reactive sintering of ternary Al–Ni–Ti powder compacts. Journal of
[14] Zhou JX, Yang MC, Wang RQ, Pang XM. Annealing behavior of aluminum coating prepared by arc spraying on P355NL1 steel. Surface and Coatings Technology, 2017, 330: 53–60
[15] Bai Y, Li XB, Xing LK, Wang ZH, Li Y. A novel non–skid composite coating with higher corrosion resistance. Ceramics International, 2017, 43 (17): 15095–15106
[16] Wang L, Yao JH, Hu Y, Song SY. Suppression effect of a steady magnetic field on molten pool during laser remelting. Applied
TE D
Surface Science, 2015, 351: 794–802
[17] Cai ZB, Cui XF, Liu Z, Li Y, Dong ML, Jin G. Microstructure and wear resistance of laser cladded Ni–Cr–Co–Ti–V high–entropy alloy coating after laser remelting processing. Optics and Laser Technology, 2018, 99: 276–281 [18] Zhang JY, Long Y, Liao SX, Lin HT, Wang CY. Effect of laser scanning speed on geometrical features of Nd: YAG laser machined holes in thin silicon nitride substrate. Ceramics International, 2017, 43 (3): 2938–2942
EP
[19] Zhang L, Wang CS, Han LY, Dong C. Influence of laser power on microstructure and properties of laser clad Co–based amorphous composite coatings, Surfaces and Interfaces, 2017, 6: 18–23 [20] Mahamood RM, Akinlabi ET. Scanning speed influence on the microstructure and micro hardness properties of titanium alloy
AC C
produced by laser metal deposition Process. Materialstoday: Proceedings, 2017, 4 (4): 5206–5214 [21] Li RF, Jin YJ, Li ZG, Zhu YY, Wu MF. Effect of the remelting scanning speed on the amorphous forming ability of Ni–based alloy using laser cladding plus a laser remelting process. Surface and Coatings Technology, 2014, 259 (c): 725–731 [22] Han QQ, Setchi R, Lacan F, Gu DD, Evans SL. Selective laser melting of advanced Al–Al2O3 nanocomposites: Simulation, microstructure and mechanical properties. Materials Science and Engineering A, 2017, 698: 162–173 [23] Wang CW, Zhou H, Zhang ZH, Zhao Y, Zhang P, Cong DL, Meng C, Tan FX. Tensile property of a hot work tool steel prepared by biomimetic coupled laser remelting process with different laser input energies. Applied Surface Science, 2012, 258 (22): 8732–8738 [24] Cai ZB, Cui XF, Liu Z, Li Y, Dong ML, Jin G. Microstructure and wear resistance of laser cladded Ni–Cr–Co–Ti–V high–entropy alloy coating after laser remelting processing. Optics and Laser Technology, 2018, 99: 276–281 [25] Pariona MM, Teleginski V, Santo KD, Santos ELR, Camargo LAADO, Riva R. AFM study of the effects of laser surface remelting on the morphology of Al–Fe aerospace alloys. Materials Characterization, 2012, 74: 64–76 [26] Wu C, Li, YK Xie SH. Micro–structure, mechanical properties and comparison of monolithic and laminated Ti–B4C composite
15
ACCEPTED MANUSCRIPT with Al doped. Journal of Alloys and Compounds, 2018, 733: 1–5 [27] Sun LL, Pang SJ, Liu Y, Xiong HP, Zhang T. A Ti–Zr–Cu–Ni–Co–Fe–Al–Sn amorphous filler metal for improving the strength of Ti–6Al–4V alloy brazing joint. Progress in Natural Science: Materials International. 2017, 27(6): 687–694 [28] Lu YZ, Huang GK, Wang YZ, Li HG, Qin ZX, Lu X. Crack–free Fe–based amorphous coating synthesized by laser cladding. Materials Letters, 2018, 210: 46–50 [29] Li RF, Li ZG, Huang J, ZhuYY. Dilution effect on the formation of amorphous phase in the laser cladded Ni–Fe–B–Si–Nb coatings after laser remelting process. Applied Surface Science, 2012, 258 (20): 7956–7961
RI PT
[30] Seung CY, Kyoung JC, Taeho K, Si HK, Ju YK, Ji HK. Microstructural evolution and stress–corrosion–cracking behavior of thermally aged Ni–Cr–Fe alloy. Corrosion Science, 2016, 111: 39–51
[31] Lavigne O, Gamboa E, Luzin V, Law M. Analysis of intergranular stress corrosion crack paths in gas pipeline steels; straight or inclined. Engineering Failure Analysis, 2018, 85: 26–35
[32] Hao WK, Liu ZY, Wu W, Li XG, Du CW, Zhang DW. Electrochemical characterization and stress corrosion cracking of E690
SC
high strength steel in wet–dry cyclic marine environments. Materials Science and Engineering A, 2018, 710: 318–328 [33] Peng YW, Chen CM, Li XY, Gong JM, Jiang Y, Liu Z. Effect of low–temperature surface carburization on stress corrosion cracking of AISI 304 austenitic stainless steel. Surface and Coatings Technology, 2017, 328: 420–427 [34] Yang ZX, Kan B, Li JX, Su YJ, Qiao LJ. Hydrostatic pressure effects on stress corrosion cracking of X70 pipeline steel in a
M AN U
simulated deep–sea environment. International Journal of Hydrogen Energy, 2017, 42 (44): 27446–27457 [35] Hou Q, Liu ZY, Li CT, Li XG. The mechanism of stress corrosion cracking of alloy 690TT in a caustic solution containing lead. Corrosion Science, 2017, 128: 154–163
[36] Xi X, Yang ST.Time to surface cracking and crack width of reinforced concrete structures under corrosion of multiple rebars. Construction and Building Materials, 2017, 155: 114–125
[37] Zhu WJ, François R, Zhang CP, Zhang DL. Propagation of corrosion–induced cracks of the RC beam exposed to marine environment under sustained load for a period of 26 years. Cement and Concrete Research, 2018, 103: 66–76
TE D
[38] Xia ZH, Zhang M, Zhang Y, Zhao Y, Liaw PK, Qiao JW. Effects of Ni–P amorphous films on mechanical and corrosion properties of Al0.3CoCrFeNi high–entropy alloys. Intermetallics, 2018, 94: 65–72 [39] Tavoosi M, Barahimi A. Corrosion behavior of amorphous–nanocrystalline Fe–Ni–Cr electrodeposited coatings. Surfaces and
AC C
EP
Interfaces, 2017, 8: 103–111
16
ACCEPTED MANUSCRIPT Tables Tab.1 Technological parameters of arc–sprayed Al–Ti–Ni coating
Parameter
Spraying voltage/V
30–32
Spraying current/A
RI PT
Item
160
Spraying distance/mm
150
0.1
SC
The move speed of arc spraying gun/m•s–1 Spraying angle/o
M AN U
80
0.6
Wire feed rate/cm•min–1
100
Overlap ratio/%
35
AC C
EP
TE D
Spraying pressure/MPa
17
ACCEPTED MANUSCRIPT Tab.2 Test parameters of electrochemical corrosion test
Parameter
Electric potential
–1.5–0
Sweep segment
1
Scanning rate/V/s
0.001
Quiet time/S
2
Sensitivity/A/V
10–0.002
AC C
EP
TE D
M AN U
SC
RI PT
Item
18
ACCEPTED MANUSCRIPT Figures Al wire Φ 2 mm
Ni powder
100 µm
RI PT
Ti powder
AC C
EP
TE D
M AN U
SC
Fig.1 Sketch of Al wire packaged Ti–Ni powder cross–section
19
ACCEPTED MANUSCRIPT 1600
A
C
Ni Ti
Counts/cps
1200
800
BB
Ni
O
400
Pt Pt
(a) Morphology of Ti–Ni powder
0
1
2
Ti Al
Ni
3
7000
3000
Pt
CO
3
4 5 6 Energy/keV
7
8
0
9
10
(c) EDS analysis result of Ti particle
At/% 44.02 52.40 3.58
Ni
M AN U
2
10
Ni
1000
Pt
1
9
SC
Ti
C
0
4000
2000
1000 O
Ti
8
Element Mass/% Ni 78.80 C 19.33 O 1.76
5000
2000
0
Ni
6000
40.10 21.98 37.92
Counts/cps
Counts/cps
3000
68.69 9.49 21.81
7
(b) Plane scan analysis of Ti–Ni powder
Ti Element Mass/% At/%
Ti C O
4 5 6 Energy/keV
RI PT
0
4000
Element Mass/% At/% Ti 16.04 6.09 Ni 19.73 5.87 C 49.77 72.37 O 14.36 15.67
0
1
2
3
4 5 6 Energy/keV
7
8
9
10
(d) EDS analysis result of Ni particle
AC C
EP
TE D
Fig.2 Morphology and plane scan analysis of Ti–Ni powder and EDS analysis of Ni and Ti particles
20
ACCEPTED MANUSCRIPT 8000 Al
Carbides Counts/cps
Element Al Ti Ni Fe C O
O Ti
6000
Fe Ni
4000 C
Mass/% 7.46 5.87 10.97 43.16 14.24 18.30
At/% 7.54 3.34 5.10 21.07 32.31 30.60
2000 Pt
0
10 µm
1
2
3
4 5 6 Energy/keV
Fe
7
8
9
10
(b) Result of plane scan analysis
(c) Al content
M AN U
SC
(a) Plane scanned position
0
Ti
RI PT
Porosity
(d) Ti content
(e) Ni content
(f) Fe content
AC C
EP
TE D
Fig.3 Plane scan analysis of Al–Ti–Ni coating surface at LR speed of 5 mm/s
21
ACCEPTED MANUSCRIPT 50000
Counts/cps
Element Mass/% Al 23.20 Ti 1.82 Ni 0.74 Fe 2.56 Mn 1.19 C 25.01 O 45.48
Al
40000 30000 O Mn Ti
20000
At/% 14.55 0.64 0.21 0.78 0.47 35.25 48.11
10000
100 µm
0
1
Pt Ti
2
3
Fe Mn
4 5 6 Energy/keV
7
8
9
(b) Result of plane scan analysis
10
(c) Al content
M AN U
SC
(a) Plane scanned position
C Fe Ni
RI PT
0
(d) Ti content
(e) Ni content
AC C
EP
TE D
Fig.4 Plane scan analysis of Al–Ti–Ni coating surface at LR speed of 10 mm/s
22
(f)
Fe content
ACCEPTED MANUSCRIPT 50000 Element Al Ti Ni Fe Mn C O
Al
30000 20000
100 µm
C Fe Ni
0
1
Pt Ti
2
3
4 5 6 Energy/keV
Fe Mn
7
8
9
(b) Result of plane scan analysis
10
(c) Al content
M AN U
SC
(a) Plane scanned position
At/% 13.33 0.85 0.24 0.92 0.44 46.20 38.02
O Mn Ti
10000 0
Mass/% 21.87 2.48 0.86 3.12 0.98 33.73 36.98
RI PT
Counts/cps
40000
(d) Ti content
(e) Ni content
AC C
EP
TE D
Fig.5 Plane scan analysis of Al–Ti–Ni coating surface at LR speed of 15 mm/s
23
(f) Fe content
ACCEPTED MANUSCRIPT 40000 Fe Ni
Counts/cps
30000
Al–Ti–Ni coating
Al
O Cr Ti
20000
Element Mass/% Al 5.12 Ti 1.12 Ni 10.97 Fe 55.33 Cr 5.05 C 14.76 O 7.64
C
At/% 5.95 0.74 5.86 31.06 3.05 38.53 14.83
10000 Ti
0
200 µm
1
2
3
4 5 6 Energy / kev
7
8
9
10
(b) Result of plane scan analysis
(c) Al content
M AN U
SC
(a) Cross–section morphology
0
Fe
RI PT
Pt
Substrate
(d) Ti content
(e) Ni content
(f) Fe content
AC C
EP
TE D
Fig.6 Plane scan analysis of Al–Ti–Ni coating cross–section at LR speed of 5 mm/s
24
ACCEPTED MANUSCRIPT
Counts/cps
12000
Al–Ti–Ni coating
Fe Ni
9000
6000
Cr
Element Al Ti Ni Fe Cr Al C
Mass/% At/% 7.94 8.02 1.71 0.97 6.21 2.88 56.63 27.62 Fe 1.13 0.68 26.38 59.83
3000 C
0
200 µm
1
2
Ti 3
4 5 6 Energy / kev
Fe
7
Ni Ni
8
9
(b) Result of plane scan analysis
10
(c) Al content
M AN U
SC
(a) Cross–section morphology
0
Pt
RI PT
Substrate
(d) Ti content
(e) Ni content
(f) Fe content
AC C
EP
TE D
Fig.7 Plane scan analysis of Al–Ti–Ni coating cross–section at LR speed of 10 mm/s
25
ACCEPTED MANUSCRIPT
Counts/cps
Al–Ti–Ni coating
12000 8000 Cr
Element Mass/% At/% Al 7.40 7.52 Ti 1.59 0.91 Ni 6.13 2.86 Fe 56.81 27.89 Fe Cr 1.11 0.67 24.49 55.91 Al C O 2.47 4.23
4000 C
Fe
Pt
Substrate 0
200 µm
1
2
Ni
3
4 5 6 Energy / kev
7
8
9
(b) Result of plane scan analysis
10
(c) Al content
M AN U
SC
(a) Cross–section morphology
0
RI PT
Ni Fe
16000
(d) Ti content
(e) Ni content
(f) Fe content
AC C
EP
TE D
Fig.8 Plane scan analysis of Al–Ti–Ni coating cross–section at LR speed of 15 mm/s
26
Ni2MnAl AlCrFe2 AlFe
AlNi
1200
15000
800 400 0 30 32 34 36 38 40 o 2θ/
10000 5000
0 10 20 30 40 50 60 70 80 90 o 2θ /
(a) At LR speed of 5 mm/s
Ni2MnAl
10000
AlFe
AlCrFe 2
500 0 30 32 34 36 38 40 o 2θ/
(c) At LR speed of 15 mm/s
SC M AN U TE D EP
1000
0 10 20 30 40 50 60 70 80 90 o 2θ/
Fig.9 XRD spectra of Al–Ti–Ni coatings at different LR speeds
27
1500
5000
0 10 20 30 40 50 60 70 80 90 o 2θ/
(b) At LR speed of 10 mm/s
AlFe3
Intensity/a.u.
3
RI PT
5000
15000
1600
AlNi AlFe
Intensity/a.u.
10000
20000
Intensity/a.u.
AlFe AlCrFe2
2000 1500 1000 500 0 30 32 34 36 38 40 o 2θ /
Intensity/a.u.
15000
AlNi AlFe3 Ni2MnAl
AC C
Intensity/a.u.
20000
Intensity/a.u.
ACCEPTED MANUSCRIPT
ACCEPTED MANUSCRIPT
149 0.0
0.2
0.4
0.6
0.8
Sin ϕ 2
150
150 149 0.0
200
300
0.2
0.4
0.6
0.8
2
Sin ϕ
100
153 2θ /
156
159
162
0
147
150
153 2θ/
0
(a) At LR speed of 5 mm/s
×× ×
149 0.0
200
×
150
0.2
0.4
0.6
0.8
2
Sin ϕ
156
159
0
162
147
150
(b) At LR speed of 10 mm/s
156 0
(c) At LR speed of 15 mm/s
M AN U
SC
Fig.10 Residual stress analysis of Al–Ti–Ni coatings at different LR speeds
28
153 2θ/
0
RI PT
150
TE D
147
151
100
EP
0
σ = –34.4 ± 8 MPa ο
×× × ×
0 o 15 o 25 o 35
2 θρ/
151
Counts/cps
×
150
152
o
σ= 43.9 ± 3 MPa ο
×× ×
300
Counts/cps
2θp/
o
151
σ = –12.2 ± 8 MPa
400
152
o
0 o 25 o 35 o 45
AC C
Counts/cps
300
400
152
o
0 o 25 o 35 o 45
2 θ p/
450
159
162
ACCEPTED MANUSCRIPT Al
Element Mass/% Al 9.39 Ti 3.28 Ni 1.12 Fe 6.88 C 51.93 O 27.40
15000
Secondary cracks Counts /cps.
12000 C
9000 O Ti
6000 3000
Ti Ni
Cracks
0
1
Ti
2
3
4 5 6 Energy/ kev.
Fe
Ni
7
8
9
10
RI PT
0
At/% 5.25 1.03 0.29 2.46 65.16 25.81
(b) Result of plane scan analysis
M AN U
SC
(a) Plane scanned position
(c) Al content
(d) Ti content
(e) Ni content
AC C
EP
TE D
Fig.11 Plane scan analysis of Al–Ti–Ni coating at LR speed of 5 mm/s after immersion corrosion test
29
ACCEPTED MANUSCRIPT 25000 Al
Element Al Ti Ni Fe C O
Counts/cps.
20000 15000 C
10000
Mass/% At/% 11.8 6.52 2.04 0.63 1.02 0.26 4.95 1.78 51.78 64.30 28.40 26.51
O Ti
5000 Pt
0
1
2
Ti
3
Fe
4 5 6 Energy/kev.
7
8
9
10
RI PT
0
(b) Result of plane scan analysis
M AN U
SC
(a) Plane scanned position
(c) Al content
(d) Ti content
(e) Ni content
AC C
EP
TE D
Fig.12 Plane scan analysis of Al–Ti–Ni coating at LR speed of 10 mm/s after immersion corrosion test
30
ACCEPTED MANUSCRIPT 20000 Al
Element Al Ti Ni Fe C O
Counts / cps.
16000 12000 8000
Mass/% 14.56 4.82 1.78 6.79 38.23 33.82
At/% 8.82 1.64 0.49 2.57 52.02 34.55
O CTi
4000 Ti
Pt Fe
0
1
Ni
2
3
Ti
4 5 6 Energy/kev.
Fe
7
8
9
10
RI PT
0
(b) Result of plane scan analysis
M AN U
SC
(a) Plane scanned position
(c) Al content
(d) Ti content
(e) Ni content
AC C
EP
TE D
Fig.13 Plane scan analysis of Al–Ti–Ni coating at LR speed of 15 mm/s after immersion corrosion test
31
ACCEPTED MANUSCRIPT
5000
0 30 32 34 36 o38 40 2θ/
10000
40
50 2θ/
60
70
80
90
0 10
20
30
40
o
50 2θ/
(a) At LR speed of 5 mm/s
AlCrFe2
2000 1000 0 30 32 34 36o 38 40 2θ/
AlFe 10000
60
70
80
0 10
90
o
(b) At LR speed of 10 mm/s
20
30
40
50 2θ/
60
(c) At LR speed of 15 mm/s
EP
TE D
M AN U
SC
Fig.14 XRD analysis results of Al–Ti–Ni coatings at different LR speeds after immersion corrosion test
32
70
0
RI PT
30
15000
3000
5000
5000
20
Ni2MnAl AlFe3 AlNi
1000
AlFe
15000
20000
lntensity/a.u.
AlCrFe2
2000
lntensity/a.u.
0 30 32 34 36 38 40 o 2θ/
10000
0 10
AlFe3
20000
1000
Intensity/a.u.
2000
Intensity/a.u.
15000
AlFe3 Ni2MnAl AlFe AlCrFe2
4000
3000
AlNi Ni2MnAl
25000
3000
AC C
Intensity/a.u.
20000
4000
AlNi
Intensity/a.u.
25000
80
90
ACCEPTED MANUSCRIPT 0.5
Al-Ti-Ni coating at LR speed of 15 mm/s
0.0
S355 structural steel
E/V
-0.5 -1.0 -1.5
Al-Ti-Ni coating at LR speed of 5 mm/s
-2.0
Al-Ti-Ni coating at LR speed of 10 mm/s -8
-6 -4 -2 Iogi / (A / cm )
-2
0
RI PT
-2.5 -10
AC C
EP
TE D
M AN U
SC
Fig.15 Polarization curves of Al–Ti–Ni coatings at different LR speeds and substrate
33
ACCEPTED MANUSCRIPT
Highlights (1) The compounds of Al-Fe, AlCrFe2 and Ni2MnAl formA metallurgical bonding at the coating interface. (2) The Al–Ti–Ni coatings after LR are composed of crystal, amorphous and intermetallic compounds.
RI PT
(3) The residual stresses of Al–Ti–Ni coating are compressive stress, restraining its cracking.
AC C
EP
TE D
M AN U
SC
(4) The corrosion potentials of Al–Ti–Ni coatings after LR shift positively, showing high corrosion resistance.