3.1. Variations in surface hardness with different standoff distance at different traverse speed
Micro hardness of base material AZ31-B Mg alloy is 93.7 HV0.05. Analysis of measured surface micro-hardness was made at standoff distance(h) = 70mm; 100mm; 120mm; 150mm and traverse speed(v) = 1000mm/min; 2000mm/min; 3000mm/min; 4000mm/min with number of passes = 2 and water jet pressure p = 100 MPa. Table 4. shows the measured micro-hardness and surface roughness values of the peened and Unpeened surfaces of AZ31-B Mg alloy. Figure 3. shows the variations in the measured results on the effect of different standoff distance and traverse speed on the strengthening of material was analyzed. A significant improvement in hardness was observed compared to the base material. Surface hardness showed a tendency to increase with increase in standoff distance to a 132.8 HV0.05.
Table 4
Variation of Micro-Hardness and Surface Roughness of Parameter settings
Experiment No | Water Jet Pressure (MPa) | Standoff Distance (mm) | Traverse Speed (mm/min) | NOP | Micro Hardness (HV0.05) | Surface Roughness (Ra) |
Unpeened | Base Material | 93.7 | 0.962 |
PE1 | 100 | 70 | 4000 | 2 | 110.4 | 1.1 |
PE2 | 100 | 100 | 4000 | 2 | 116.2 | 0.977 |
PE3 | 100 | 120 | 4000 | 2 | 112 | 0.94 |
PE4 | 100 | 150 | 4000 | 2 | 110 | 0.83 |
PE5 | 100 | 70 | 3000 | 2 | 94.2 | 1.86 |
PE6 | 100 | 100 | 3000 | 2 | 116.6 | 1.38 |
PE7 | 100 | 120 | 3000 | 2 | 132.8 | 1.157 |
PE8 | 100 | 150 | 3000 | 2 | 124.1 | 0.816 |
PE9 | 100 | 70 | 2000 | 2 | 95.2 | 3.37 |
PE10 | 100 | 100 | 2000 | 2 | 96.6 | 2.71 |
PE11 | 100 | 120 | 2000 | 2 | 99.2 | 1.433 |
PE12 | 100 | 150 | 2000 | 2 | 114.9 | 0.774 |
PE13 | 100 | 70 | 1000 | 2 | 94.1 | 8.1 |
PE14 | 100 | 100 | 1000 | 2 | 95.4 | 4.04 |
PE15 | 100 | 120 | 1000 | 2 | 94.9 | 1.69 |
PE16 | 100 | 150 | 1000 | 2 | 99.3 | 0.734 |
Evaluation of results confirmed the occurrence of improvement of microhardness on the higher standoff distance (h = 70mm to h = 150mm). The maximum micro-hardness recorded was 132.8HV0.05 at h = 120mm v = 3000mm/min; NOP = 2. Increase in the standoff distance (h) from 70mm to 150mm, resulted in the impinging of water jet on the target surface in the form of individual clusters of water droplets. This created cyclic water hammer pressure action [28] on the surface which permitted as a compressive load on the subsurface and preceding the movement of dislocation of slip boundaries and planes. This resulted in the maximum gradient of work hardening effect on surface layers.
A gradual increase in the micro-hardness of peened surface was seen from 95.2 HV0.05 to 114.9 HV0.05 from the traverse speed of nozzle from v = 1000 mm/min to 4000 mm/min at the standoff distance (h) = 70mm and 100mm. This was due to the characteristic of water from the nozzle to the discrete formation of water jet cluster which induced plastic deformation in the subsurface layer. However, at the standoff distance h = 120mm and h = 150mm with traverse speed v = 3000mm/min and v = 4000mm/min, there was a decrease in the micro-hardness of peened region decreases from 132.8 HV0.05 to 110 HV0.05. This was due to the aerodynamic interaction of water jet, resulting in a substantial reduction on the formation of water droplet cluster, causing variations in axial velocity fluctuation of compression load by water droplets there was also a big reduction in revelation period of interaction of the cluster of water droplets with material surface at higher traverse speed [30]. This confirmed the parametric variant h = 120mm with v = 3000mm/min, that allowed a maximum compressible load on the surface in the form of water droplet clusters, leading to induction of elastic-plastic strain to the subsurface. Above h = 120mm, the intensity of water droplets caused a reduction in the shock pressure wave over the material surface resulting in a smaller deformation effect on the subsurface despite variations in the traverse speed from 1000mm/min to 4000mm/min.
In addition, water jet peening at single pass created small plastic strain along the peening path. When the nozzle moved in ‘S’ shaped path for second passes in the peened region, the step over distance of water jet (Dc) triggered residual stress formation through plastic deformation. But the kinetic energy of the water jet in this second pass with higher in value of step over distance of water jet (Dc=1mm) did not have the ability to influence the plastic deformation on subsurface layer followed by the first pass water jet peening region. A further increase in the number of passes (NOP = 4 and 6), rather than this formation of elastic-plastic strain in subsurface, visible erosion and grooves was observed on the surface level. This was due to the continuous impact of high-pressure water jet on same peening path in the successive passes.
3.2. Variation of surface roughness with different standoff distance at different traverse speed
The effect of variation in the standoff distance on the surface roughness of the peened material at water jet pressure of p = 100MPa with two number of passes is shown in Fig. 4. Initial surface roughness (Ra) of the base material measured was 0.962µm. Following the water jet peening surface treatment process, the maximum surface roughness recorded was 8.1µm at standoff distance (h) = 70mm with traverse speed (v) = 1000mm/min. Decrease in surface roughness value (Ra) with increase in standoff distance (h = 70mm to h = 150mm) at high water jet pressure (p = 100MPa) was seen. This nature of surface was due to the characteristics of water jet under different parametric conditions. Compared to the standoff distance of h = 150mm, the effect of cyclic impact energy of water droplets on the material was quite high in the standoff distance of h = 70mm. This permitted longitudinal and compressive waves to the impact region, initiating compressive longitudinal waves, with the ability to interact with the microstructural discontinuities and resulting in the improvement in the roughness of the material.
With a reduction in the standoff distance(h) from 150mm to 70 mm, there was an increase in the magnitude of individual water droplet energy causing improved roughness (Ra) in the peened region from 0.734µm to 8.1µm. Surface roughness drift was similar at traverse speed (v) with variations from 1000mm/min to 3000mm/min. The maximum average surface roughness value (Ra) was recorded at traverse speeds(v) = 1000mm/min; 2000mm/min; 3000mm/min was 8.1µm; 3.37 µm; 1.86 µm respectively. This similar roughened surface seen by Stanford [12] is suitable for dental implants.
This was due to the exposure period of high-pressure water jet with a material surface. Reduction in traverse speed (v) produced the maximum number of water droplets and caused machining action on the surface. It also created surface abrasion on the material. At a higher standoff distance (h = 150mm), there was reduction in the effect of kinetic energy of water droplet due to the divergence of water jet stream. It forced a smaller effect of cyclic load on the material surface, creating smooth surface roughness value in the range of 0.734 to 0.83, which was 13.2 % lower than the unpeened material surface roughness. This confirmed the absence of occurrence of significant peening action on the surface above a certain standoff distance even at low traverse speed.
The usage of two passes caused a higher hydraulic impact with abrasion in surface asperities with a reduction in the standoff distance. Initial jet passes water jet originated micro cracks without any shearing effect [31] on the material surface and with no formation of greater and deeper craters. There were no changes in the effect of roughness. But, at successive passes start of initiation of some new cracks was seen which easily propagated previous cracks, leading to the removal of an increased material rate at the surface. As a result, a significant improvement in roughness was observed, leading to the combination of surface material erosion and micro cracks leading to material fatigue.
3.3. Multi-response Optimization Technique TOPSIS
Selection of critical factors between different output responses is a tedious process. Inappropriate choice of input responses may lead to surface damage or machining action rather than peening performance. Based on this consideration, selection of optimal input response setting is significant. Amongst different optimization techniques, TOPSIS method is preferable for finding better input responses in manufacturing industries It is closer to the ideal one suggested by Rao [27].
In this study, TOPSIS did relationship assessment between the input responses and the output responses as with the Hardness and Roughness of peened Surface of AZ31 Mg alloy. The basic methodology of TOPSIS involves the choice of input responses that simultaneously find the shortest distance from a Positive Ideal solution that maximizes positive criteria and farthest from a Negative Ideal solution that maximizes negative criteria based on the assumption of weightage to each response. Reference to the steps involved in the TOPSIS has been made by earlier researchers. Table 5, indicates the weightage of Input responses and the ranking of alternatives. The highest closeness coefficient value was obtained under the water jet pressure 100 MPa, SOD = 120mm; TS = 3000mm/min and NOP = 2. Analysis of Surface morphology and topographical features of corroded region of unpeened and PE7 was done for further discussion on the basis of optimal experimental conditions.
Table 5
Weightage of Input Responses and Ranking of Alternatives of TOPSIS
Experiment No | Positive Ideal Solution | Negative Ideal Solution | Closeness Coefficient value | Rank |
Unpeened | 1.0404 | 0.0178 | 0.0169 | 17 |
PE1 | 0.7434 | 0.3761 | 0.3359 | 8 |
PE2 | 0.6703 | 0.5055 | 0.4300 | 4 |
PE3 | 0.7292 | 0.4112 | 0.3606 | 7 |
PE4 | 0.7651 | 0.3661 | 0.3236 | 9 |
PE5 | 0.9946 | 0.0888 | 0.0819 | 15 |
PE6 | 0.6392 | 0.5166 | 0.4470 | 3 |
PE7 | 0.5430 | 0.8785 | 0.6180 | 1 |
PE8 | 0.6022 | 0.6826 | 0.5313 | 2 |
PE9 | 0.9217 | 0.2089 | 0.1848 | 11 |
PE10 | 0.9156 | 0.1677 | 0.1548 | 12 |
PE11 | 0.9171 | 0.1351 | 0.1284 | 13 |
PE12 | 0.6999 | 0.4760 | 0.4048 | 5 |
PE13 | 0.8689 | 0.5762 | 0.3987 | 6 |
PE14 | 0.8978 | 0.2614 | 0.2255 | 10 |
PE15 | 0.9877 | 0.0795 | 0.0745 | 16 |
PE16 | 0.9474 | 0.1257 | 0.1172 | 14 |
3.4. Effect of optimal parameter setting in 3D surface Topography
The 3D surface topography of the water jet peened surface PE7 was selected using the Multi-objective optimization TOPSIS result, it exposed the peaks and valleys in optimal experiment parametric conditions. Topographical changes were observed from the peened surface as indicated by multiple colours in surface topography as shown in Fig. 5. Ra and Rq are the main parameters to quantify surface roughness for load bearing capacity, but area parameters could provide more information for surface texture. 3D surface parameter values were obtained from the respective peened surface profiles mentioned in Table 6. Surface topology parameters selected in this study were Arithmetic mean height (Sa); Root mean square height value (Sq); Skewness (Ssk); Kurtosis (Sku). The focus of the study is on a surface topography selected for surface contact application like cell adhesion and assessment of the performance of the components.
Graphical results Fig. 6 show, the smooth surface topography obtained in Unpeened over PE7 unpeened surface. This was confirmed by Sa value recorded, namely, 1.459µm to the untreated material surface. A similar surface pattern was reported by Rosa et al. [32] This was due to the effect of the traverse speed(v) 3000mm/min with standoff distance (h) 120mm. It provides threshold energy for a uniform erosion of the materials in the peening region and caused a lower value of roughened surface on the material. Peened region recorded Sq was 2.97µm. This was due to high water jet pressure (p) = 100Mpa with successive passes. It permitted minimum energy for the creation of surface waviness on the peened region [33], leading to the desired roughened surface layer directly associated with the surface energy of the implant and later on affecting the protein absorption and wettability of the surface. Surface wettability enhanced cell adhesion, cell proliferation and prevent premature failure of implant.
Table 6
Variations in Area Parameters of Unpeened and PE7 of AZ31-B Mg alloy
Area Parameters | Unpeened | PE7 |
Arithmetic mean height | 1.718 | 1.459 |
Root mean square height | 2.35 | 2.971 |
Skewness | -0.771 | -6.589 |
Kurtosis | 4.244 | 62.733 |
Ssk parameter describes the shape of the normal height distribution of a roughness profile. Ssk -6.589 µm was observed, confirming the surface heights with confined valley structures in the vicinity of the peened region. This was happening due to the effect of traverse speed with high standoff distance in successive passes. At a standoff distance h = 120mm, each water droplet had sufficient kinetic energy for creating surface abrasion in material surface through the removal of material shatters in the minimal level. In addition, traverse speed v = 3000mm/min created a transition region [35] of water jet column that supported the creation of a uniform surface pattern over the peening region. Successive passes induced critical energy of water jet to produce a majority of peaks and valleys closer to the surface of peened region. This combined effect of parameters setting permitted maximum negative skewness values to the unpeened profile. This type of pattern considered favourable for high load bearing capacity provided with a good bonding ratio for any contact type application, was confirmed by the percentage of relative material ratio roughness (Rmr%) shown in Fig. 7. This measured the load bearing and wear resistance of the peened surface. The graph shows improvement in the Rmr value of peened surface over unpeened pattern leads for providing better surface for cell adhesion. This was confirmed by the result obtained by Yuvaraj et al. [10] on-surface milling process on SS304 using AWJ.
Variations in the Sku values for Exp 1 and Exp 8 indicate the uniform presence and absence of peaks and valleys in surface texture. PE7 shows a high Sku value of 62.733µm. This formation confirmed by red colour in Fig. 5, indicates the excessive projection of peaks with deeper valleys are particularly in PE7. This nature of surface created was due to high standoff distance with high traverse speed. It caused a reduction in the intensity of water jet pressure producing inordinate peak and valleys near the peened region.
3.5. Effect of Optimal setting of WJP parameters on XRD Analysis
Figure 8. shows the XRD diffraction patterns of unpeened and peened (PE7) AZ31B Mg alloy at optimized parameter settings. and both the peened and unpeened AZ31B Mg samples as mainly composed of α-Mg while the β-Mg17Al12 phase is insignificant, due to the presence of a low content of Aluminium in the alloy. XRD plot show no new diffraction peaks in the peened surface confirming the absence of any new formation of crystals generated after peening. Figure 9. reveals the Intensity of diffraction peak, [002] and [101] of peened surface (PE7) as lower than that of the unpeened surface. Changes in the intensity of the diffraction peaks could be the result of the lower surface finish of the peened surface over the unpeened surface, which became a favourable condition for achieving better ooseointegration and cell growth in body fluid condition. The similar trend obtained by yuvaraj [38] et al. compared the surface integrity of Aluminium alloy with CAAWJM and AWJ cutting process. The position of the diffraction peak at [002] crystalline plane became smooth and was shifted slightly to a higher angle after the WJP process. FWHM values obtained using Jade software data analysis were 0.1360 and 0.1730 for unpeened and PE7 surface respectively, obtained using the Jade Software data analysis. The broadened diffraction peak could be the result of grain refinement [37] and an increase in the micro-strain rate on the material surface layer of AZ31B Mg alloy after WJP, which was further confirmed through the estimation of the grain size of peened and unpeened AZ31B Mg surface by Debye-Scherrer formula:
D = Kλ/β cos θ------------------(1)
Where,
D is average crystallite size (nm)
λ stands for X-ray wavelength (0.15046 nm)
β is the FWHM of diffraction peak (radian)
θ is half of diffraction angle (degree)
K is a constant with value set to 0.89 from the XRD experimental data.
Grain sizes for the peened and unpeened surfaces calculated were 43.489nm and 51.263nm respectively, confirming the refinement of the grain size of the Water jet peening treatment without abrasives through their effect on the surface on a nano scale level through severe plastic deformation [6].
3.6. Effect of Optimal setting of WJP parameters on Corrosion performance
The potentio dynamic polarization curves of Unpeened and PE7 in SBF solution are shown in Fig. 10. Determination of Corrosion potential (Ecorr), corrosion current density (icorr) and polarization resistance (Rp) was done using the Tafel extrapolation [28][36] method, details are provided in Table 7.
Table 7
Calculated Values of Ecorr, Icorr, and Corrosion Rate of Unpeened and PE7
Experiments | Ecorr (V) | Icorr (µA/cm2) | RP (Ω cm2) | Corrosion rate (µm/Year) |
Exp 1 | -0.16279 | 0.013292 | 1.5419*105 | 0.31106 |
Exp 8 | -0.32044 | 0.004067 | 7.4169*105 | 0.047259 |
In the case of the Unpeened surface, a sharp rise in cathodic polarization curve with increase in corrosion potential indicating the development of hydrogen evolution and magnesium dissolution was observed. The passive region was confirmed by the anodic branches of the polarization curves, indicating the natural formation form the passive films on the sample surface [7], when the alloy samples were exposed to a corrosive medium.
Tafel behavior was observed for PE7 with surface roughness of 1.157 Ra, and the steady increase in the current on the anodic potential region indicated the WJP AZ31-Mg alloys exhibiting wider passive regions than the as-received ones. PE7 was seen exhibiting its ability to hinder the corrosion effect. This could be the result of the strengthening effect at the grain boundaries due to the WJP process, despite a higher surface roughness value. Grain boundaries are highly susceptible to corrosion as they tend to possess high surface energy creating an anodic region with respect to the grain region. WJP treatment resulted in the refinement of surface and a plentiful grain boundary [25]. The newly developed refined grain boundaries showed a tendency to slow down the corrosion process in comparison with the coarse grain structure [31] due to the presence of Al content in grain boundary, acting as a kinetic barrier [34]. This was confirmed by EDAX result showed a higher presence of Al content in the corroded region of peened over the unpeened surface in Table 8.
PE7 indicates the formation of an immediate passive surface layer which is relatively stable and compact when exposed to SBF solution. The immediate passive layer might cause a reduction in the corrosion rate on AZ31-B Mg alloy due to its increased specific surface area and surface activity over the unpeened surface which slowed down the reaction with chloride ions. This phenomenon was further confirmed through the presence of the wider potentio-dynamic polarization curve for the peened surface as seen in Fig. 10. A similar trend was observed by Liu et al [19] following the analysis of the corrosion behavior of magnesium alloys using shot peening. Better corrosion inhibiting nature was observed as the effect of surface roughness up to a certain limit, and reduction in the micro galvanic corrosion between the grain boundary and grain region for the WJP surfaces.
Table 8
Presence of Ions in corrode region Unpeened and PE7 in SBF Fluid
Weight % | O | Mg | Al | P | Cl | K | Ca |
Unpeened | 55.27 | 39.91 | 0.42 | 0.32 | 2.95 | 0.19 | 0.93 |
PE7 | 36.49 | 36.78 | 2.2 | 14.34 | 0.49 | 0.02 | 9.69 |
With increase in the number of passes (NOP = 2) in the case of peening process, there was preponderance of the smooth regions on the corroded surface. There was also a significant reduction in the number of pits compared to the unpeened surface, wherein pit formation was much narrower for the peened surface (PE7). This was confirmed by the microstructure view of corroded region of Unpeened surface and peened surface shown in Fig. 11. These observations, along with the results of the potentio-dynamic polarization measurements, indicate SOD = 120mm; TS = 3000mm/min; NOP = 2, the highest corrosion resistance for the peened surface (PE7) through the WJP process at optimized parameters.