Chemical composition of ASTM F139 austenitic stainless-steel biomaterial – in percentage weight.
The purpose of present work is to study the biotribological behavior of a mechanically and laser marked biomaterial. Sliding wear tests were conducted on ASTM F139 austenitic stainless-steel specimen, with polypropylene and AISI 316 L austenitic stainless-steel balls, as counterbodies. During wear experiments, a liquid chemical composition was continuously fed between the specimen and the ball. The coefficient of friction acting on the tribological system “specimen – liquid chemical composition – ball” and the wear volume of the wear craters were calculated, and results were analyzed. The results have shown that the biotribological behavior of ASTM F139 austenitic stainless steel was influenced by mechanical or laser marking process, and its wear resistance was dependent on the kind of counterbody.
- austenitic stainless steel
- laser treatment
- wear resistance
- wear volume
- coefficient of friction
The “ball-cratering wear test” has gained large acceptance at universities and research centers as it is widely used in studies focusing on the wear behavior of different materials [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20]. Figure 1 presents a schematic diagram of the principle of wear test, where a rotating ball is forced against the tested specimen and liquid solution supplied between the specimen and the ball during the experiments.
The aim of the “ball-cratering wear test” is to generate “wear craters” on the surface of the specimen. Figure 2 presents an image of such crater, together with an indication of the crater diameter (d) (Figure 2a) and the wear volume (V) (Figure 2b ). The wear volume is determined as a function of “d,” using Eq. (1) , where R is the radius of the ball.
In other line of research, the concept of “biotribology” has gained important spotlight in the area, including research works addressing the biotribological behavior of materials [23, 24, 25, 26, 27, 28, 29] used in the manufacturing of human body elements. Consequently, different laboratory techniques have been employed to reproduce conditions where there are friction and consequent wear of parts of the human mechanical structure with relative movement.
However, wear tests conducted under the “ball-cratering” technique present advantages in relation to other types of tribological procedures, as it favors the desired analysis of the tribological behavior. Therefore, considering the need of tribological characterization of biomaterials and the capacity that the “ball-cratering wear test” method presents to this goal, the purpose of this work is to study the biotribological behavior of mechanically and laser-marked ASTM F139 austenitic stainless-steel biomaterial.
2. Experimental details
2.1 Ball-cratering wear test equipment
Equipment with free-ball mechanical configuration (Figure 3a) was used for the sliding wear tests. Two load cells were used in the tribometer: one load cell to control the “normal force – N” applied on the specimen (Figure 3b) and the other load cell to measure the “tangential force – T” developed during the experiments (Figure 3c).
“Normal” and “tangential” force load cells have a maximum capacity of 50 N and an accuracy of 0.001 N. The values of N and T were registered by a data acquisition system, in real time, during the sliding wear tests.
The tested specimen was an ASTM F139 austenitic stainless-steel biomaterial, marked mechanically and with a nanosecond Q-switched Nd: YAG laser. Its chemical composition is presented in Table 1.
|Chemical element||% (in weight)|
Balls of polypropylene and AISI 316 L austenitic stainless steel, with diameter of D = 25.4 mm (D = 1″ – standard size), were adopted as counterbodies.
To simulate the fluid present in the human body, a chemical liquid solution of PBS – Phosphate Buffered Solution – was inserted between the specimen and the ball. It was composed by the materials mentioned in Table 2.
Table 3 shows the hardness (H) of the materials used in this work (specimen and test balls).
|Material||Hardness – H|
|Specimen||ASTM F139 austenitic stainless steel||180 HV|
|Test ball||Polypropylene||55 – Shore D|
|AISI 316 L austenitic stainless steel||318 HV|
2.3 Ball-cratering wear tests and data acquisition
Table 4 presents the test conditions defined for the sliding wear experiments conducted in this research.
|Normal force – NPP||Ball of polypropylene||0.05 N|
|Normal force – N316L||Ball of AISI 316 L austenitic stainless steel||0.40 N|
|Test ball rotational speed – n||75 rpm|
|Tangential sliding velocity – v||0.1 m/s|
|Test time – t||10 min|
|Sliding distance – S||60 m|
Following values of normal force (N) for the sliding wear experiments: NPP = 0.05 N and N316L = 0.40 N were defined as a function of density (ρ) of the ball material – polypropylene ⇒ρPP = 0.91 g/cm3 and AISI 316 L austenitic stainless steel ⇒ρ316L = 8 g/cm3. The rotational speed (n) of ball was 75 rpm. For n = 75 rpm and D = 25.4 mm, the tangential sliding velocity (v) of the ball is 0.1 m/s. Wear tests were conducted under a test time (t) of 10 min. With 0.1 m/s tangential sliding velocity and 10 min (600 s) test time, a sliding distance (S) of 60 m was calculated between the ball and the specimen.
All experiments were conducted without interruption, and the chemical liquid solution of PBS – Phosphate Buffered Solution – was fed between the specimen and the ball during the tests, under a frequency of 1 drop/10 s. Both the normal force (N) and the tangential force (T) were monitored and registered constantly. Finalizing the sliding wear tests, the diameters (d) of the wear craters were measured by optical microscopy, and their surfaces were analyzed by scanning electron microscopy.
3. Results and discussion
3.1 Scanning electron microscopy
Figure 4 shows a scanning electron micrograph of the surface of a wear crater generated during the sliding wear tests.
Occurrence of grooves, due to sliding movement between the ball and the specimen, was observed in the scanning electron micrograph. The result presented in Figure 4 is in qualitative agreement with the literature , where it is reported that the action of grooves on the surface of a material is characterized as a common tribological behavior of two metallic materials under relative movement.
3.2 Wear volume behavior
Figure 5 presents the behavior of the specimen in terms of wear volume (V) for the following conditions: mechanically and laser-marked specimen and different types of balls (counterbodies).
In addition, Figure 5 shows a decrease in wear volume under laser marking process for both types of counterbodies. Decrease in wear volume is related to increase in local hardness of the specimen. Increase of hardness can be attributed to the action of laser on specimen surface. In relation to specimen marked mechanically, the possible increase of local hardness could have occurred due to local surface hardening.
However, the increase of local hardness caused by laser marking is higher than the local hardness caused by mechanical marking, justifying the results presented in Figure 5.
3.3 Coefficient of friction behavior
Figure 6 shows the behavior of the coefficient of friction (μ) for the conditions, which the specimen is marked mechanically and marked with laser, and for the different types of balls – counterbodies.
In the present tribological conditions, coefficient of friction was found lower for the wear tests conducted against polypropylene ball than AISI 316 L austenitic stainless-steel ball counterbodies.
The following conclusions can be drawn from the results obtained in this research, regarding to tribological behavior of ASTM F139 austenitic stainless steel:
tribological behavior was influenced by the type of the marking process – “mechanical” or “laser” – applied for the investigated biomaterial;
wear volume was found to be dependent on the normal force acting on the specimen, that is, they were dependent on the type of counterbody – ball of polypropylene or ball of AISI 316 L austenitic stainless steel; and
coefficient of friction was found dependent on the type of ball; the lower values of μ were observed under the use of polypropylene ball.
diameter of the wear crater (mm) diameter of the test ball (mm) hardness (HV) test ball rotational speed (rpm) normal force (applied on the specimen) (N) radius of the test ball (mm) sliding distance (m) test time (min) tangential force (developed during the wear tests) (N) tangential sliding velocity of the test ball (m/s) wear volume of the wear crater (mm3) coefficient of friction density (g/cm3)
diameter of the wear crater (mm)
diameter of the test ball (mm)
test ball rotational speed (rpm)
normal force (applied on the specimen) (N)
radius of the test ball (mm)
sliding distance (m)
test time (min)
tangential force (developed during the wear tests) (N)
tangential sliding velocity of the test ball (m/s)
wear volume of the wear crater (mm3)
coefficient of friction