Corrosion–Erosion Of13Cr24Mn0.44 Stainless Steel
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Corrosion–erosion wear behaviors of 13Cr24Mn0.44N stainless steel insaline–sand slurry
Zhou Guanghong, Ding Hongyan , Zhang Yue, Li Nianlian
Faculty of Mechanical Engineering, Huaiyin Institute of Technology, Huaian, Jiangsu 223003, China
a r t i c l e i n f o
Available online 21 December 2009
Keywords:
Stainless steel
Corrosion–erosion wear
Wear mechanism
Synergism
a b s t r a c t
The corrosion–erosion wear behaviors of austenitic stainless steels, 316L and 13Cr24Mn0.44N, were
investigated in water–sand slurry and saline–sand slurry, respectively. The corrosion–erosion wear
mass-loss was measured to evaluate the influence of medium and materials. The worn surface andcorrosion–erosion wear mechanism were analyzed using a scanning electron microscopy and a non-
contact optical profilometer. Results show that the corrosion–erosion wear mass-loss of
13Cr24Mn0.44N is lower than that of 316L in both the slurries. The relative wear resistance increases
with the increasing of the impingement velocity and arrives at maximum of 1.6. The dominant wear
mechanism of 13Cr24Mn0.44N is abrasive wear in the water–sand slurry, whereas it becomes abrasive
wear associated with little corrosive pitting in the saline–sand slurry. As the impingement velocity
increased all the synergism ratios exhibit a tendency of increase, among which the synergism ratio of
13Cr24Mn0.44N is always lower than that of 316L at any given velocity. The results indicate that
13Cr24Mn0.44N possesses a predominant anti-corrosion–erosion wear property.
& 2009 Elsevier Ltd. All rights reserved.
1. Introduction
Austenitic stainless steels are widely used in many compo-
nents where corrosion resistance is crucial, such as slurry
handling in food and chemical industries [1,2]. When used in
such fields, they often undergo tribocorrosion or mechanical
action of hard particles. Generally, the total metal removal is not
simply the sum of the corrosion and the wear measured in
separate experiments. The interaction of erosion with corrosion
could significantly affect entire mass-loss due to the synergism
between mechanical and electrochemical effect. For example, if a
corrosive solution carries the particles, the surface damage due to
corrosion increases as a consequence of synergistic mechanisms
between corrosion and erosion [3–7]. The synergistic effect
between erosion and corrosion has been receiving more and
more attention in recent years. Many studies have showed thatcorrosion is accelerated by wear and the wear may be also
accelerated by corrosion [8–12].
Recently high nitrogen stainless steels have been paid a special
attention due to its good combination of strength, ductility,
toughness, weldability, localized corrosion resistance and tribo-
logical properties [13–16]. Particularly, it has been shown that
nitrogen additions improve the resistance to pitting and crevice
corrosion of stainless steels in solutions containing chloride ions
(Cl) [17]. In addition, high manganese stainless steels have
excellent work hardening effect [18–21]. Mills’ study has shownthat CrMnN steel possesses superior wear corrosion resistance
and good cavitation erosion resistance compared with the 304
stainless steel [18].
In our earlier work, a new type austenitic stainless steel with
high manganese and moderate nitrogen, 13Cr24Mn0.44N, has
been developed [22]. The aim of this work is to study the
corrosion–erosion wear behaviors of 13Cr24Mn0.44N submitted
to liquid impingement accompanied by corrosion–erosion condi-
tion. Reference experiment has also been conducted with com-
mercially used 316L stainless steel under same conditions.
2. Experimental procedures
2.1. Materials and mediums
The 13Cr24Mn0.44N stainless steel used here was developed
by Shanghai Research Institute of Materials. The steel ingot was
firstly austenized at 1050 1C for 1 h, and then oil-quenched, and
lastly annealed at 850 1C for 1 h to relieve internal stresses. The
hardness of 13Cr24Mn0.44N, after annealing treatment, is about
197HV. The rectangular specimens (20mm10mm2mm)
were cut-out using electrical discharge method. It was ground
to an average surface roughness Ra of 1.6mm. Reference experi-
ment was also conducted with commercially used 316L stainless
ARTICLE IN PRESS
Contents lists available at ScienceDirect
journal homepage: www.elsevier.com/locate/triboint
Tribology International
0301-679X/$- see front matter & 2009 Elsevier Ltd. All rights reserved.
doi:10.1016/j.triboint.2009.12.021
Corresponding author. Tel.: +86 517 83559196; fax: +86 517 83559041.
E-mail address: [email protected] (H. Ding).
Tribology International 43 (2010) 891–896
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steel. The chemical compositions of the experimental materials
are listed in Table 1. A strongly saline–sand slurry was used as the
corrosive medium consisting of 5 wt% NaCl solution, 10wt% river–
sand (SiO2 particles, 250–325mm, 2200–2300 HV) and distilled
water. Comparison test was also performed in the slurry only
consisting of 10 wt% river–sand and distilled water, namely
water–sand slurry. All tests were performed at room tempera-
ture and with the medium exposed to air.
2.2. Erosion–corrosion wear test
The wear experiments were performed in a modified solid
particle slurry corrosion–erosion wear apparatus. The impinge-
ment velocity can be well controlled by a motor. The specimens
were mounted in holders at the edge of the impeller, in which the
impingement angle can be adjusted. The impeller was connected
to a rotating spindle by a bar. It is schematically shown in Fig. 1.
For each test, the slurry pot was filled with 1200 ml aqueous
solution, either water–sand slurry or saline–sand slurry.
All the experimental materials were firstly ground by SiC paper
in 240 grit and degreased in acetone. Specimens were then
cleaned by ethanol and air-dried after abraded by SiC paper from
600 to 1000 grit step by step. The experiments were conducted at
three velocities of 100, 500 and 1000r/min for 2 h at room
temperature. After completion of tests, the specimens wereultrasonically cleaned in acetone. Later, their surface character-
istics and mechanical properties were investigated. Note that
three replicate tests were conducted for each specimen.
2.3. Characterization
The microstructure of the 13Cr24Mn0.44N was observed by
optical microscope (OM, Zeiss Axio, Germany) and was deter-
mined by using X-ray diffraction (XRD, D8-Advance Bruker,
Germany). The hardness was measured at 0.98 N for 10 s by a
digital microhardness meter (HXD-1000TMC, China); the mea-
surement was repeated for 5 times and the hardness value in this
paper was the average. The corrosion–erosion wear surface and
its 3D-morphology were observed and analyzed using scanningelectron microscopy (SEM, Hitachi 3000N, Japan) and non-contact
optical profilometer (Micro-XAM ADE, USA). Wear weight-loss
was measured by an electronic balance with sensitivity of 0.1 mg.
The corrosion–erosion wear resistance was evaluated by wear
mass-loss ratio (DM 0), which was calculated from the following
equation:
DM 0 ¼ M 0M
M 0ð1Þ
Where, M 0 is the weight of materials before corrosion–erosion
wear and M stands for the weight of specimen after corrosion–
erosion wear.
Besides, the relative wear resistance (e) was employed to
evaluate the corrosion–erosion wear-ability of 13Cr24Mn0.44N
versus that of 316L, which can be calculated as:
e ¼ W s=W c ð2Þ
Where, W s is the mass-loss of 316L; W c is that of 13Cr24Mn0.44N
under the corresponding condition.
To investigate the synergism ratio (Z) between corrosion–
erosion and wear, the amount of synergy DM cw can be calcu-
lated according to a typical corrosion wear model as following
equation [23]:
DM c -w ¼ M corr M water ð3Þ
Where, M corr is the entire mass-loss after corrosion–erosion in the
saline–sand slurry; M water stands for the mass-loss after abradedin the water–sand slurry. Therefore, the synergism ratio Z, i.e.,
contribution of DM cw to M corr can be calculated as the following
equation:
Z ¼ DM c -w
M corr ¼
M corr M water
M corr ð4Þ
3. Results and discussion
3.1. Microstructure of the 13Cr24Mn0.44N stainless steel
The microstructure of 13Cr24Mn0.44N austenitic stainless
steels is shown in Fig. 2. It presents a typical austenitemicrostructure, which is confirmed further by XRD (Fig. 3). The
peak of the spectrum pattern shows that the structure of
13Cr24Mn0.44N is single austenite phase. In addition, some
twin-crystal structure was also presented in Fig. 2. Previous study
[24] has proved that element Mn in stainless steels is helpful for
the formation of twin-crystal structure.
3.2. Wear resistance of 316L and 13Cr24Mn0.44N in aqueous slurry
The mass-loss ratios of both the austenitic stainless steels,
316L and 13Cr24Mn0.44N, are shown in Fig. 4. It is clear that the
mass-loss ratio of 316L is always larger than that of
13Cr24Mn0.44N whether after corrosion–erosion in saline–sand
slurry or in water–sand slurry.
Table 1
Chemical compositions of the experimental materials (wt%).
Experimental
material
C Mn Si Ni Cr N Mo V Ti
13Cr24Mn0.44N 0.05 24.62 0.57 0.1 13.18 0.44 – – –
316L 0.035 1.32 0.055 10.40 16.60 – 2.20 0.08 0.02
Fig. 1. Schematic diagram of the modified solid particle slurry erosion–corrosionapparatus.
G. Zhou / Tribology International 43 (2010) 891–896 892
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It is of interest that, the more increase of the impingement
velocity, the more is the difference in mass-loss ratio. To
quantitative analyze the difference wear-loss in two slurries
clearly, the relative wear resistance values e are used and
summarized in Table 2. The value of e increased with the
increasing of the impingement velocity; meanwhile, the e was
always higher in saline–sand slurry than that in water–sand
slurry at same impingement velocity. The biggest e was 1.6 at
1000r/min in saline–sand slurry; therefore, we believed that13Cr24Mn0.44N stainless steels can be applied in strongly saline–
sand slurry at higher impingement velocity, compared with 316L.
The result can be interpreted owing to the different chemical
compositions of the two stainless steels. Firstly, it has been
proved that nitrogen element added into austenitic steels can
simultaneously improve fatigue life, strength, wear and localized
corrosion resistance, attributed to the strong hardening effect of
nitrogen in solid solution [18]. In addition, Ref. [25] pointed out
that higher content of manganese in austenite microstructure
would cause rapid work hardening, attribute to the reorientation
of carbon members of C–Mn couples in the cores of dislocations.The hardness results after erosion wear are listed in Table 3. It
can be found that the increment of the impingement velocity can lead
to a higher hardness, indicating a work-hardening effect occurrence.
Compared with 316L, however, the hardness of 13Cr24Mn0.44N
induced by impingement increased by more than 15% attributed to
the strong hardening effect as discussed above. This result agrees with
previous studies [25,26] satisfactorily.
3.3. Synergism ratios between wear and corrosion of 316L and
13Cr24Mn0.44N
From Fig. 4 one can also see that the mass-loss ratio, whether
for 316L or 13Cr24Mn0.44N, is larger in saline–sand slurry than
that in water–sand slurry. This means the corrosive slurry with
Fig. 2. Microstructure of 13Cr24Mn0.44N.
600
400
200
20 30 40 50 60 70 80
2θ/deg
c p s
(111)
(200)(220)
Fig. 3. XRD spectrum pattern of 13Cr24Mn0.44N.
Fig. 4. Mass-loss ratios of 316L and 13Cr24Mn0.44N at various velocities: (a) in water–sand slurry, (b) in saline–sand slurry.
Table 2
Relative wear resistance of 13Cr24Mn0.44N versus 316L in different slurries at
various velocities.
Slurry 100 (r/min) 500(r/min) 1000 (r/min)
Water–sand 1.29 1.39 1.5
Saline–sand 1.42 1.56 1.6
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hard particles accelerates the wear process, which presents a
positive synergism between wear and corrosion. The synergism
ratios calculated from the mass-loss between the two slurries are
summarized in Table 4.
It can be seen that all the synergism ratios exhibit a tendency
of increase as the velocity increased. However, an exciting result
is that the synergism ratios of 13Cr24Mn0.44N are always lower
than those of 316L at any velocity. This indicates that
13Cr24Mn0.44N has a good anti-corrosion–erosion wear abilitycompared with 316L.
3.4. Corrosion–erosion wear mechanism of 316L and
13Cr24Mn0.44N in two slurries
Fig. 5 depicts the SEM images of the worn surface after erosion
wear in both the slurries at the velocity of 1000 r/min. Many
scratch lines along the direction of impingement were observed in
all the cases due to the sharp SiO2 particles. The micro-cut slots of
13Cr24Mn0.44N were relatively narrower and smoother in the
water–sand slurry as shown in Fig. 5(a); in contrast, additional
corrosive pitting and a little of wide deep ditches exhibited in
saline–sand slurry probably caused by impacting hard particles,
as shown in Fig. 5(b). Therefore, the dominant wear mechanism of
13Cr24Mn0.44N is abrasive wear in the water–sand slurry,
whereas it becomes abrasive wear associated with little
corrosive pitting in the saline–sand slurry.As for 316L, the dominant wear mechanism is also abrasive
wear in the water–sand slurry. This can be verified by the SEM
photograph as shown in Fig. 5(c), from which many micro-cut
slots, as well as some impingement pits, were presented. By
Table 4
Synergism ratio (Z) between corrosion and wear of experimental materials at
various velocities.
Materials 100 (r/min) 500 (r/min) 1000 (r/min)
316L 0.21 0.29 0.34
13Cr24Mn0.44N 0.15 0.20 0.28
Fig. 5. SEM image of the surface after erosion in two slurries at high velocity: (a) 13Cr24Mn0.44N, in water–sand slurry, (b) 13Cr24Mn0.44N, in saline–sand slurry,
(c) 316L, in water–sand slurry, (d) 316L, in saline–sand slurry.
Table 3
Hardness (HV) after erosion wear in water–sand slurry at various velocities.
Materials 100 (r/min) 500 (r/min) 1000 (r/min)
316L 378.8 410.8 452.6
13Cr24Mn0.44N 442.8 468.7 592.5
Fig. 6. SEM image of the pitting hole of 316L after erosion in saline–sand slurries
at 1000 r/min.
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contrast, the remarkable pitting corrosion and brittle delamina-
tion took place on the surface when corrosion–erosion wear
conducted in saline–sand slurry, evidenced in Fig. 5(d). Fig. 6
illustrates the higher magnification SEM photograph of the pittinghole after corrosion–erosion in saline–sand slurry. The presence of
plate-like hole in 316L indicated that the corrosive slurry was able
to pass though the surface and locally attack the substrate,
promoting formation of pits and reducing mechanical supporting
ability. The local weak corrosion surface can be continuously
removed by the action of the flow and the presence of solids;
therefore, the brittle delamination may flake from the surface of
the samples.
It is further evidenced by Fig. 7, which shows the 3D-
morphology of the cleaned surface of 316L stainless steel after
corrosion erosion in saline–sand slurry. Obviously the 3D-
morphology (Fig. 7(a), observed from top) was similar to the
SEM image. However, some deep corrosion pittings presented in
another 3D-morphology (Fig. 7(b), observed from side). Thismorphology can also demonstrate that 316L processes a poor
erosion wear resistance in saline–sand slurry, compared with
13Cr24Mn0.44N.
4. Conclusions
The results of the present study on the corrosion–erosion wear
behavior of a new stainless steel 13Cr24Mn0.44N, compared with
the commonly used 316L, in saline–sand slurry and water–sand
slurry, provides a new insight into the synergism between wear
and corrosion. The mass-loss ratio of 316L is always larger than
that of 13Cr24Mn0.44N whether in saline–sand slurry or in
water–sand slurry. The relative wear resistance increases with theincreasing of the impingement velocity and arrives at maximum
of 1.6. Both the stainless steels present a positive synergism
between wear and corrosion. As the impingement velocity
increased all the synergism ratios exhibit a tendency of increase,
among which the synergism ratio of 13Cr24Mn0.44N is always
lower than that of 316L at any given velocity. All above indicates a
predominant anti-corrosion–erosion wear property of high-Mn
austenitic stainless steel. The dominant wear mechanism of
13Cr24Mn0.44N is abrasive wear in the water–sand slurry,
whereas it becomes abrasive wear associated with little corrosive
pitting in the saline–sand slurry. As for 316L, the dominant wear
mechanism is also abrasive wear in the water–sand slurry,
whereas it becomes abrasive wear associated with corrosive
delamination fatigue in the saline–sand slurry.
Acknowledgment
The author would like to acknowledge professor Q.X. Dai for
his help on the preparation of the experimental material.
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