Next Article in Journal
Electrochemical Performance of Iron Oxide Nanoflakes on Carbon Cloth under an External Magnetic Field
Next Article in Special Issue
Investigation of Microstructure, Nanohardness and Corrosion Resistance for Oxi-Nitrocarburized Low Carbon Steel
Previous Article in Journal
Effect of Rolling Temperature on the Microstructure and Mechanical Properties of Mg-2Zn-0.4Y Alloy Subjected to Large Strain Rolling
Previous Article in Special Issue
Hydrothermal Surface Treatment of Biodegradable Mg-Materials
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

General Regression Model for Predicting Surface Topography after Abrasive Blasting

by
Dagmar Draganovská
1,*,
Gabriela Ižaríková
2,
Anna Guzanová
1 and
Janette Brezinová
1
1
Department of Mechanical Technology and Materials, Technical University of Košice, Mäsiarska 74, 040 01 Košice, Slovakia
2
Department of Applied Mathematics and Informatics, Technical University of Košice, Letná 9, 042 00 Košice, Slovakia
*
Author to whom correspondence should be addressed.
Metals 2018, 8(11), 938; https://doi.org/10.3390/met8110938
Submission received: 26 October 2018 / Revised: 7 November 2018 / Accepted: 9 November 2018 / Published: 13 November 2018
(This article belongs to the Special Issue Surface Treatment Technology of Metals and Alloys)

Abstract

:
Abrasive blasting modifies the surface state of pre-treated materials in terms of surface irregularities. Bearing in mind that the roughness characteristics affect the components functionality, it is essential to study and evaluation the surface state of pre-treated materials. The paper deals with evaluation of relation between individual parameters of roughness of the blasted surfaces by the correlation analysis. Based on the measured values on the surfaces which were blasted by various types of blasting devices, the correlation matrix was set and the standard of statistic importance of correlation between the monitored parameters was determined from it. The correlation coefficient was also set. There were found regression models using ANOVA (ANalysis Of Variance). Based on the analysis of the results were also proposed sets of roughness parameters, which can be used in the assessment of the blasted surfaces.

1. Introduction

The priority purpose of surface treatment is to protect the surface against degradation by corrosion, fatigue and wear. Further priorities are the acquisition of new functional properties of surfaces and aesthetics of products. To meet such an objective, the surfaces need to be pre-treated. The pre-treatment method depends on requirements imposed on the product. In principle, it comes to obtain the required characteristics, such as creation of suitable topography of surface, obtaining the requested purity of surface, etc.
Abrasive blasting, more commonly known as sandblasting, is the operation of forcibly propelling a stream of abrasive material against a surface under high pressure to smooth a rough surface, roughen a smooth surface, shape a surface or remove surface contaminants. A pressurized fluid, typically compressed air, or a centrifugal wheel is used to propel the blasting material (often called the media). The first abrasive blasting process was patented by Benjamin Chew Tilghman on 18 October 1870 [1]. Shot peening or blasting are techniques always in direct competition with mechanical treatments such as burnishing [2], with very good results in mold finishing [3]. Isotropic finishing is key in brakes, applications in which other cinematically defined methods origin roughness with defined patters. This is a source of problems in several fields of application. Authors [4] worked on the elimination of the surface spiral pattern after turning operation, which is a challenge to avoid braking problems at the early life of the component.
Another significant positive feature of the abrasive blasting technology, in a relation to a subsequent coating application, is the increase in the actual size of surface area. This creates favourable conditions for the increased adhesion of coatings. In evaluating the actual size of the blasted surface, it is necessary to consider its microscopic and submicroscopic unevenness. By microscopic unevenness, we mean a set of the blasting abrasive notches on the surface of base material, having the character of intersecting fracture surfaces. Submicroscopic unevenness are the result of the different deformation ability of the individual particles of the blasting abrasive which may be caused by a different grain orientation. Furthermore, the blasted surface can also be characterized by a surface volume. The surface volume can be defined as the volume between the imaginary plane passing through the highest peaks and the actual surface area of the base material, per unit of nominal area. It is important to investigate the size of surface volume arisen after the impact of the blasting abrasive of particular material and shape [5].
The original condition of surface before pre-treatment is determined primarily by its origin of production, storage conditions, or, in case of renovation, its previous quarrying. All the factors mentioned, but also many more, affect the condition of surface, mainly its purity and roughness.
The schematic classification of blasting effects on the substrate is shown in Figure 1.
The result of application of blasting technology is affected by:
-
The choice of appropriate blasting abrasives—high level of durability, accurate shape and size of particles and minimal unwanted side effect of particles,
-
the use of appropriate blasting devices—the effort is to produce blasting devices which would work automatically with a programmed process of blasting,
-
optimization of technological parameters of blasting—determination of optimal technological parameters which lies in a correct selection of transition of grit blasting abrasives through the nozzle and the correct level of surface coverage by blasting abrasives. Furthermore, in choosing the right kind, shape and size of blasting abrasives, its speed and the angle of hitting the blasted surface,
-
secondary impact of surface blasting—roughening the surface, hardening the surface, changing mechanical properties of the surface and underground layers,
-
increase the economy of blasting which is closely related to the optimization of technological parameters of blasting (blasting time), service life of grit blasting equipment and abrasives used in its exposed parts.
The blasted surface quality is important for achieving corrosion resistance of coating [6,7,8]. D. Whitehouse in [9,10] brings new look on some issues relating to surfaces interacting with another in many tribological situations. S. Bagherifard [11] assessed surface roughness of low alloy steel shot peened using three shot diameters and velocities. Authors also viewed models of peened surfaces with 100% coverage.
Large particles concentrate considerable energy in the place of impact which triggers the deformation of impurities (oxides, hydroxides, dust etc.) and base material layers resulting in its hardening. Spherical particle which hits base material creates marks the edges of which rise above the metal surface. Due to tension caused by pressure and moving in the place of impact, the impurities gets disintegrated and largely peeled off the metal. Sharp shape particles penetrate the surface layer and get stuck in the base material causing impurities are embedded in the surface layer, too. They also give rise to pressure strain. If the strain is enough to overcome the adhesion, the layers of dirt get peeled off and lifted. Further impact of particle will cause the bursting of disturbed dirt from the base metal. Compared with large particles, the effect of small particles, i.e., particles with less kinetic energy, is of a different nature. Small particles do not cause such a great microplastic deformation of the base metal as the large ones do. However, they give rise to a more steady distribution of the pressure strain. Since the number of particles per weigh unit of grit blasting medium with smaller particles is larger than in large particles, the density of impact will be significantly greater and will trigger considerable pressure strain right in the dirt layer, causing the release of impurities from the metal surface.
To achieve optimum blasting process, correct size and shape of the particles of the grit blasting abrasives (density impact) is important on one hand, and suitable kinetic energy of the particles on the other hand. Selecting appropriate type of grit blasting abrasive is also of importance. It is mainly the mutual ratio of particles hardness of the grit blasting abrasives against the base material. Increase in size and hardness of grit blasting particles increases removal ability blasting abrasives as well as the roughness of blasted metal surface. The particles hit the surface at a certain angle which makes them slip down the surface thus triggering abrasive effect on the surface. The number of marks after the particles impact on the cleaned surface increases with the amount of grit blasting abrasive required for complete removal of small residual waste impurities. Due to the fact that the surface must be blasted for a really long time, until the residues are completely eliminated, which sometimes causes blasting through the surface of the base material resulting in its hardening (side-effect of blasting). D. Kirk [12] deals with the term of surface coverage and solving the problem, how to reach 100% surface coverage in shot peening process, how to predict and control surface coverage in multipass shot peening. D. Wiklund [13] deals with influence of different steel surface treatment of friction conditions during stamping. D. Zhu [14] proposed a method how to characterize relation between micro topography of metal surface and fatigue of the metal. C. Nouguier-Lehon in [15] investigated impact depth of zirconium oxide balls in ultrasonic shot peening of copper tube. Author found good agreement between finite element simulations and experimental results of impact depth and distribution of impacts measured using confocal microscope.
Blasting abrasives are loose materials of granular nature consisting of different large particles (polydispersion). There are mainly two types of blasting media used-metallic and non-metallic ones. Metal blasting abrasives can be in in three different forms:
-
Blasting abrasive of spherical shape, known as shot,
-
blasting abrasive of irregular sharp shape—grit,
-
blasting abrasive of a roller shape, its height is equal to its diameter—chopped wire.
The most widespread abrasives are metal ones, on the basis of iron. They can be heat treated or galvanized. Out of metal blasting abrasives, the most used are cast iron grit, steel shot and chopped wire. The shape of particle of blasting abrasives used determines the resulting surface relief [5,16,17,18,19]. Surface has rounded small peaks after the blasting with grit or sharp notches after grit (Figure 2).
In addition to the above ferrous blasting abrasives, blasting abrasives of non-ferrous nature are used for many reasons, too. Their use is specific to a certain kind of pre-treated material and work. Out of non-metallic blasting abrasives, the most spread are blasting abrasives of mineral origin, both natural and artificial, in particular, corundum (Al2O3—man-made or natural hard crystallized alumina), natural garnet, glass beads as well as secondary raw materials, e.g., different slag from metallurgical processes. All of the above types of non-metallic blasting abrasives have a lower specific weight in comparison with metal blasting abrasives, cause less deformation of the base material as well as lower surface roughness. They also feature low durability and therefore are mainly used for single blasting.
When assessing technical surface, its specific properties as well as the properties of coating—base material interface need to be considered. They are, in several cases, different from the properties of the base material including mechanical, physical, chemical and physical-chemical properties which are researched and assessed by a variety of special methods.
The evaluation of blasting surface properties can be done in terms of:
-
Surface topography,
-
degree of purity and degree of coverage,
-
microhardness,
-
changes of mechanical and technological properties,
-
residual tension and structural changes,
-
physical—chemical properties.
From the point of view topography, blasted surface can be defined as non-oriented (Figure 3).
Surface topography of blasted material depends on:
-
Properties of blasted material (mainly its hardness). Material exhibiting higher hardness, when being blasted, will not be as much affected as soft material in terms of surface topography.
-
the type of used blasted abrasive. Hard blasting abrasives with larger diameter of particles harden the surface more than particles of small diameter. The ratio of blasting abrasive hardness to the hardness of blasted metal is important from the point of view of qualitative impact on surface and also in terms of removal of metal material itself,
-
the same blasted abrasive invokes different topography for various parameters of blasting (landing speed, angle of impact, etc.) [20,21,22].
M.N. Durakbasa in [23] investigated surface roughness on flat and spherical specimens prepared using different machining processes with periodic and random profiles. Author compared results reached using stylus profilometer, confocal laser scanning microscope and infinite focus microscope. H. Zhu [24] monitored development of surface roughness at different stages of wear and proposed specific parameter reflecting both fractal dimension and scale coefficient of rough surfaces.
The aim of the paper is to create a mathematical model describing the relationship between the surface roughness parameters of the blasted surface. The obtained model can serve for predicting roughness parameters on the metal surface after abrasive blasting. Monitoring of the achieved roughness of steel surfaces is an important part of ensuring repeatability and reproducibility of the pre-treatment process. From the very principle of the blasting process, it follows that the repeated use of blasting abrasives leads to irreversible changes in their shape, dimensions, depletion of their plasticity and thus the change of their mechanical properties, which results in a change in the resulting topography of the surface. Breaking of the abrasive grains causes surface contamination by dust particles, decreasing of roughness values, and consequently a change in the adhesion of subsequently applied coatings. It is therefore important to monitor roughness parameters during the surface preparation process.

2. Materials and Methods

2.1. The Base Materials

The base material was non-alloy high quality structural steel S235JR, thickness 2 mm. The chemical composition of the base material is shown in Table 1.

2.2. Modification of Surface Topography by Blasting

Four types of blasting abrasives were used for modification of the surface topography. There were:
-
Conventional blasting abrasives:
1. Steel grit (hereinafter SG) with the particle size of 0.71 mm. SG is produced by crushing steel shot. The advantage of this abrasive lies in its durability and impact resistance. The chemical composition of SG is shown in Table 2.
2. Steel shot (SS) with the particle size of 0.9 mm. SS is made of hypoeutectoid specially treated steel by spraying the melt through nozzles to the shape of a shot that falls into the water tank. Next, the shot is dried and separated into the particle size fractions on the separation unit. It has a fine homogeneous structure of tempered martensite, which exhibits optimal resilient elasticity and resistance to material fatigue. The chemical composition of SS is shown in Table 2.
3. Corundum (C) with the particle size of 0.9 mm. It’s a sharp, angular blasting abrasive. It is produced by melting bauxite in induction furnace at 1600 °C. Despite the content of silicon compounds, it is safe for health. The chemical composition of C is shown in Table 3.
-
Non-conventional blasting abrasives:
4. Demetalized steel slag (DSS) with the particle size of 0.9 mm. It is a secondary raw material, produced as a by-product of steel production. The chemical composition of DSS is shown in Table 4.
Table 5 is summary table regarding the applied abrasives.
The blasting was pneumatic air-blast device by equipment TJVP 320, producer Škoda, Plzeň, Czech Republic. The samples were blasted with abrasives at working pressure of 0.6 MPa, nozzle diameter was 1.2 mm, blasting angle 75° and the distance of the nozzle from the substrate was 200 mm.
The measurement of the roughness was by the profilometer Surftest SJ—301, Mitutoyo, Tokyo, Japan. Settings in roughness measurement:
  • A measured profile: R
  • a filter: GAUSS,
  • a sampling length l (λc): 0.8 mm
  • a number of sampling lengths: N = 5
  • an evaluation length ln: 4 mm
  • a number of measured profiles: 50.
Within experimental works evaluated by STN EN ISO 4287 system, surfaces blasted by different types of blasting abrasives were evaluated, with the use of set of variables attempting to sufficiently define specifics of considered surfaces. The blasting surfaces which have the same Ra value can be fully different in terms on of their profile. It is necessary to add another parameters, which enable the more precise distinction of differences in blasting surfaces. [25,26] The measured parameters were:
-
The middle arithmetic deflection of elaborated profile on the basic length (Ra),
-
the overall height of the profile on the elaborated length (Rt),
-
the biggest height of profile on the basic length (Rz),
-
the middle separation of disparities on the basic length (RSm),
-
the average number of peaks per the average (RPc),
-
the developed length of the profile (Rlo).
For the visualization of assessed surfaces and setting of surface volume, also 3D analysis was realized by the laser microscope of Olympus LEXT OLS 3000, LM, Tokyo, Japan.
The surface volume is an important quantity which has an importance while assessing blasted surfaces regarding a set number of coated material. A method which was applied for calculating a surface volume of individual surfaces is based on implementing 3D visualization of assessed surfaces with a MATLAB software utilization.

2.3. Statistical Evaluation of Blasted Surface Topography

Values of individual roughness parameters were assessed by the correlation analysis in Statistica program. A correlation analysis was used to study the relationship between the individual roughness parameters. The correlation represents the degree of dependence between two or more variables. The output of the correlation analysis is the correlation matrix of the correlation coefficients for all the variables.
If the correlation coefficient represents the linear dependence between the two variables, then its second power gives the coefficient of determination. The coefficient of determination indicates to what extent (in per cent) the change of one variable affects the other. The correlation coefficient can varies from −1 to 1. The numeric value indicates the strength of dependence and the sign determines the direct or inverse dependence. If the correlation coefficient (its absolute value) varies between values of 0.5 to 0.7, it is a significant dependence. When it varies in the range of 0.7 to 0.9 then the dependence is high and above value of 0.9 there is a very tight correlation. The positive sign of the correlation coefficient means direct dependence, negative sign means indirect dependence.
Correlation is statistically significant when the significance indicator (p-value) is lower than the significance level (1% or 5%). Significant correlations are marked red (at significance level—5%).
Correlation matrix and matrix charts were used for tested types of blasting abrasives. Regression models were set using the ANOVA [27]. Regression or ANOVA can be the key to define DOEs [28]. The principle of the experiment is shown in Figure 4.

3. Results and Discussion

The measurement results are shown in Table 6. Ra parameter is the basic and most common evaluated that is why it was used as the basis for comparison of surfaces. All evaluated surfaces featured comparable parameter Ra, the types of surfaces were correctly chosen and can be compared mutually. Profilographs of surfaces with Abbot—Fireston curves of material proportion for all evaluated types of surfaces are in Figure 5.
On the basis of performed measurements and their results, differences in their granularity caused by the use of different shapes of blasting abrasives (sharp shape or spherical) can be stated. Best rugged surface was achieved in blasting with sharp particles (corundum), where parameter RSm has reached the lowest value among the evaluated surfaces (or parameter RPc the highest). On the contrary, the lowest surface roughness was recorded for spherical particle (shot). Boxplot (average and 1.96 standard deviation) for roughness parameters is shown in Figure 6.
Differences are also evident from the waveforms of curves of material proportion profiles, where the main difference can be observed in the upper section of cut—40%. The smallest material proportion can be reported for surface blasted with round blasting abrasive. Out of surfaces blasted with sharp shape blasting abrasive, the smallest material proportion is reported for blasting with grit, followed by surface blasted with demetalized steelmaking slag and finally the surface blasted with corundum.
In a comprehensive assessment of surfaces topography, the evaluation of only Ra parameter is not enough. For the same values of parameter Ra, the nature and smoothness of blasted surfaces differs. Due to this, the evaluation of surface needs to implement a set of parameters of roughness out of which following combinations can be recommended:
-
Ra, Rz, RSm
-
Ra, Rz, RPc or
-
Ra, Rz, Rlo.
These allow you to effectively distinguish differences in topography of blasted surfaces from the point of view of other follow-up technologies, respectively to evaluate previous effects that had led to their creation.
At a mutual visual comparing of assessed surfaces, a difference is visible as in a character of surfaces blasted by various TP types. The different character of blasting surface is shown on Figure 7. At such types an uneven surface is reached, resulting by an incidental fall of particles—blasting abrasives. A surface blasted by a sharp blasting abrasives—steel and corundum grit and DOT does not show such uniformity as at blasting by round particles. Notches are on the surface in a various orientation, intersected mutually and a notable part of holes and juts is sharp. From utilized sharp TP, the most segmented surface was detected at the surface blasted by a steel grit, what corresponds moreover with the results achieved by 2D measurement of RPc and RSm parameters. At blasting by round blasting abrasives—a steel shot, more uniformed surface modification was achieved, which is created by intersected round juts. Holes create round areas which are bounded—lined by angular juts.
Values of the surface volume achieved at individual surfaces are displayed in Table 7. The biggest surface volume was recorded at blasting by the steel grit and the smallest at utilizing the shot, what corresponds also with a tendency of roughness quantities. Such fact in compliance with a recommendation that under functional coatings an angular type—grit is used as a suitable blasting abrasives, where a surface achieves a bigger segmentation as a surface obtained by the shot which is more suitable under protection coatings.
There were observed six parameters of roughness (Ra, Rz, Rt, RSm, Rlo, RPc), i.e., the correlation matrix has a size of 6 × 6, it is the matrix of correlation coefficients for all pairs of parameters. The paired correlation coefficient measures the dependence between the two variables mutually. In Figure 8, Figure 9, Figure 10 and Figure 11, significant dependencies are indicated in red.
Figure 8 shows the correlation matrix and matrix graphs of the individual roughness parameters for the surface blasted with steel grit. There is statistically significant correlation between all monitored parameters, with the exception of Rlo-RSm and Rlo-RPc pairs. There is a strong direct dependence between the Rz-Ra and Rz-Rt pairs, and a strong indirect dependence between RPc-RSm. Between parameters Ra-Rz-Rt-RSm-Rlo, there is always a direct dependence. There is an indirect dependence between RPc and the other parameters, the strongest in RPc-RSm pair.
Figure 9 shows the correlation matrix and matrix graphs of the individual roughness parameters for the surface blasted with steel shot. There is statistically significant correlation between the observed parameters, with the exception of Ra-RSm, Ra-RPc, Rz-RSm and Rz-RPc pairs. Between parameters Rz-Ra, Rz-Rt and Rz-Rlo are strong direct dependencies. Between parameters Ra-Rz-Rt-RSm-Rlo, there is always a direct dependence, with the exception of Rlo-RSm. Between RPc and other parameters are indirect dependencies, except for Rlo-RPc, between RPc-RSm parameters, there is the strongest dependency (r = −0.9782).
Correlation matrix and graphs of corundum (Figure 10) show a significant correlation between the observed parameters except for Ra-RSm and Ra-RPc. There is a very close dependence between RPc-RSm. Rz-Ra and Rz-Rt feature a high dependence. Rz-Ra and Rz-Rt feature a strong direct dependence, while RPc-RSm feature a strong indirect dependence. There is an indirect dependence between RPc and other parameters, with the exception of Rlo where there is no dependency.
Correlation matrix and graphs of demetalized steelmaking slag (Figure 11) show a statistically significant correlation between the monitored parameters except for Rlo-RSm and Rlo-RPc. There is a very close dependence between RPc-RSm. Rz-Ra and Rz-Rt feature a high dependence. Parameters Rz-Ra and Rz-Rt feature a strong direct dependence and a strong indirect dependence exists between RPc-RSm. There is an indirect dependence between RPC and other parameters.
Correlation matrices and graphs suggest that parameters of surfaces prepared with the use of blasting abrasives:
-
Sharp shaped (grit, corundum, demetalized steelmaking slag devices) show a high direct dependence between Rz-Ra and Rz-Rt parameters,
-
spherical shaped (shot) show that there is also a high direct relationship between Rz-Ra and Rz-Rt parameters, but a high direct dependence between Rz and Rlo parameters,
-
RPc and RSm parameters feature a high indirect dependence for both shapes of blasting abrasives.
With the use of ANOVA, regression models were set. Ra value was chosen as a dependent variable. Other surface roughness characteristics were considered as independent variables (1)
Ra = f (Rz, Rt, RSm, Rlo, RPc),
General regression model can be written in the following form (2)
Ra = a0 + a1Rz + a2Rt + a3RSm + a4Rlo + a5RPc,
where a0 is the locating constant that expresses the expected level of the dependent variable at zero value of the independent variable, a1–a5 are regression coefficients expressing by how many units of measure the dependent variable changes when the independent variable changes by one unit of measure.
The relevance of proposed model is tested by means of ANOVA, based on p-values, the estimated models are statistically significant, (p < α, α = 0.05). Regression models for Ra variable and p-values are in Table 8.
To evaluate the significance of a locating constant and the regression coefficients, p-values are used. Statistically significant changes are shown in the Table 9 which also implies that Rz and Rlo are statistically significant for all types of blasting abrasives (statistical significance marked in bold).
3D graphs in Figure 12 show the relationship between a mean arithmetic deviation of the profile at the base length Ra, maximum height of the profile on the base length Rz and total height of the profile on the evaluated length Rt. If Rz rises, Ra rises too. Ra values are the highest for corundum blasting and lowest for steel grit blasting.
Measured values of the observed parameters in blasting with various blasting abrasives were compared using Kruskal–Wallis test and subsequently by the multiple comparison method, post hoc analysis, Table 10. The Kruskal–Wallis test is a nonparametric test, and is used when the assumptions of one-way ANOVA are not met. Both the Kruskal–Wallis test assess for significant differences on a continuous dependent variable by a categorical independent variable (with two or more groups). At the significance level of 0.05, zero hypothesis of the mean values conformity is rejected, i.e., the type of blasting abrasives influences the value of monitored parameters. Statistically significant differences detected by post hoc analysis are indicated in the Table 10. Statistically significant differences are not found in standardized Rz and Rt parameters for steel grit blasting and demetalized steelmaking slag blasting and for the non-standardized Rlo parameters for steel grit and corundum blasting (use of bold in the Table 10).

4. Conclusions

The innovative contribution of the research work is characterization of the surface topography of surfaces created by blasting using four types of blasting abrasives. Authors created a mathematical model of relationships between roughness parameters of the blasted surface. The obtained model can serve for the prediction of roughness parameters on the metal surface after abrasive blasting and to ensure repeatability and reproducibility of blasted surfaces topography. On the basic of the realized measurements and their analyses it can be stated that:
-
From the point of view of consistent differentiation of the surface topography, apart from the Ra parameter, parameter Rz seems to be suitable one as an additional parameter. Parameter Rt is not necessary to evaluate vertical parameters. The surface, in terms of roughness, can be evaluated by standardized/normalized (RSm) and non-standardized/normalized (RPc) parameters. Parameter RSm represents the inverse RPc value, thus the surface can be evaluated with the use of any of them.
-
For all types of blasting rains, the strongest direct dependence is detected at Rz-Rt pair and the strongest indirect dependence was monitored for RPc-RSm pair. Those dependencies are in compliance with a definition of individual roughness parameters. A statistically non-notable correlation for those types of blasting particles was shown between parameters RSm-Rlo and RPc-Rlo for steel grift, Ra-RSm, Ra-RPc, Rz-RSm and Rz-RPc for steel shot, Ra-RSm and Ra-RPc pre corundum, Rlo-RSm and Rlo-RPc for demetalized steelmaking slag.
-
By realized measurements and 3D visualization of blasted surfaces a presumption was proved that abrasive particles make after the fall in a base material their prints which are dependent on their shape and size, by which a detection of surface complexity was achieved—thus its various segmentation. The particle shape of blasting abrasives (round or angular) has thus a notable effect in the process of blasting and is one of the attributes for an achieved topography of blasted surface, surface volume size, and further characteristics as well.
-
From the point of view of achieved surface volume, the biggest value was recorded at blasting by the steel grit and the smallest was when using the shot what corresponds with a tendency of roughness quantities. Thus it is possible to state a recommendation that under functional coatings an angular type—grit is a suitable blasting abrasives, where a surface achieves a bigger segmentation as a surface obtained by the shot which is suitable rather under protection coatings.

Author Contributions

Investigation—D.D., validation—G.I., formal analysis—A.G., supervision—J.B.

Funding

This research was funded by Ministry of Education of the Slovak Republic VEGA No.1/0424/17 and of the Slovak Research and Development Agency APVV-16-0359 and the APC was funded by Slovak Research and Development Agency.

Acknowledgments

This work was supported by scientific grant agency of the Ministry of Education of the Slovak Republic VEGA No.1/0424/17 and of the Slovak Research and Development Agency APVV-16-0359.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Smil, V. Creating the Twentieth Century: Technical Innovations of 1867–1914 and Their Lasting Impact, 1st ed.; Oxford University Press: Oxford, UK, 2005; ISBN 978-0-19-516874-7. [Google Scholar]
  2. Huo, F.; Zhao, H.; Zhao, D. Nanogrinding of Silicon Wafer Using a Novel Vitrified Diamond Wheel. Mater. Manuf. Process 2011, 26, 977–981. [Google Scholar] [CrossRef]
  3. Lacalle, L.N.; Lamikiz, A.; Munoa, J.; Salgado, M.A.; Sanchez, J.A. Improving the high-speed finishing of forming tools for advanced high-strength steels (AHSS). Int. J. Adv. Manuf. Technol. 2006, 29, 49–63. [Google Scholar] [CrossRef]
  4. Rodríguez, A.; López de Lacalle, L.N.; Fernández, A.; Braun, S. Elimination of surface spiral pattern on brake discs. J Zhejiang Univ.-Sci. A Appl. Phys. Eng. 2014, 15, 53–60. [Google Scholar] [CrossRef] [Green Version]
  5. Brezinová, J.; Guzanová, A.; Draganovská, D. Abrasive Blast Cleaning and Its Application, 1st ed.; Trans Tech Publications: Pfaffikon, Switzerland, 2015; p. 107. ISBN 978-3-03835-995-1. [Google Scholar]
  6. Guzanová, A.; Brezinová, J.; Draganovská, D.; Jaš, F. A study of the effect of surface pre-treatment on the adhesion of coatings. J. Adhes. Sci. Technol. 2014, 28, 1–18. [Google Scholar] [CrossRef]
  7. Draganovská, D.; Tomáš, M.; Ižol, P. Evaluation of micro-geometry changes on surfaces after chemical pretreatment. Arch. Mech. Technol. Autom. 2014, 34, 17–24. [Google Scholar]
  8. Momber, A. Blast Cleaning Technology, 1st ed.; Springer: Berlin, Germany, 2008; p. 540. ISBN 978-3-540-73644-8. [Google Scholar]
  9. Whitehouse, D.J. A new look at surface metrology. Wear 2009, 266, 560–565. [Google Scholar] [CrossRef]
  10. Whitehouse, D.J. Surface metrology. Meas. Sci. Technol. 1997, 8, 955–972. [Google Scholar] [CrossRef]
  11. Bagherifard, S.; Ghelichi, R.; Guagliano, M. Numerical and experimental analysis of surface roughness generated by shot peening. Appl. Surf. Sci. 2012, 258, 6831–6840. [Google Scholar] [CrossRef]
  12. Kirk, D. Theoretical principles of shot peening coverage. Shot Peener 2005, 19, 24–26. [Google Scholar]
  13. Wiklund, D.; Wihlborg, A.; Rosén, B.-G. Evaluation of Surface Topography Parameters for Friction Prediction in Stamping. Wear 2004, 257, 1296–1300. [Google Scholar] [CrossRef]
  14. Zhu, D.; Xu, L.; Wang, F.; Liu, T.; Lu, K. Evolution of Metal Surface Topography during Fatigue. Metals 2017, 7, 66. [Google Scholar] [CrossRef]
  15. Nouguier-Lehon, C.; Zarwel, M.; Diviani, C.; Hertz, D.; Zahouani, H.; Hoc, T. Surface impact analysis in shot peening process. Wear 2013, 302, 1058–1063. [Google Scholar] [CrossRef]
  16. Jiang, X.; Whitehouse, D.J. Technological shifts in surface metrology. CIRP Ann. Manuf. Technol. 2012, 61, 815–836. [Google Scholar] [CrossRef]
  17. Whitehouse, D.J. Functional Fractal Analysis of Surfaces. Nanotechnol. Precis. Eng. 2009, 7, 19–28. [Google Scholar]
  18. Wichern, C.M.; Cooman, B.C.D.; Tyne, C.J.V. Surface roughness changes on a hot-dipped galvanized sheet steel during deformation at low strain levels. Acta Mater. 2004, 52, 1211–1222. [Google Scholar] [CrossRef]
  19. Brezinová, J.; Draganovská, D.; Guzanová, A. Blasting-suitable choice of the surface treatment before coatings application. In Conference Proceedings of the 9th Conference on Pigments and Binders, Seč, Czech Republic, 7–8 November 2016; Chemagazín s.r.o.: Pardubice, Czech Republic, 2016. [Google Scholar]
  20. Brown, C.A. Describing Ground Surface Texture Using Contact Profilometry and Fractal Analysis. Wear 1991, 141, 211–226. [Google Scholar] [CrossRef]
  21. Zeng, W.; Jiang, X.; Scott, P.J. Roundness Filtration by Using Robust Regression Filter. Meas. Sci. Technol. 2011, 22, 035108. [Google Scholar] [CrossRef]
  22. Wang, M.; Xi, L.; Du, S. 3D surface form error evaluation using high definition metrology. Precis. Eng. 2014, 38, 230–236. [Google Scholar] [CrossRef]
  23. Durakbasa, M.N.; Osanna, P.H.; Demircioglu, P. The factors affecting surface roughness measurements of the machined flat and spherical surface structures—The geometry and the precision of the surface. Measurement 2011, 44, 1986–1999. [Google Scholar] [CrossRef]
  24. Zhu, H.; Ge, S.; Huang, X.; Zhang, D.; Liu, J. Experimental Study on the Characterization of Worn Surface Topography with Characteristic Roughness Parameter. Wear 2003, 255, 309–314. [Google Scholar] [CrossRef]
  25. ISO 4287: Geometrical Product Specifications (GPS)—Surface Texture: Profile Method Terms, Definitions and Surface Texture Parameters, 1st ed.; ISO: Geneva, Switzerland, 1997.
  26. Draganovská, D.; Ižaríková, G.; Brezinová, J.; Guzanová, A. The Study of Parameters of Surface Roughness by the Correlation Analysis. Mater. Sci. Forum 2015, 818, 15–18. [Google Scholar] [CrossRef]
  27. Ižaríková, G. Monte Carlo Simulation for Anova. Acta Simul. 2016, 2, 11–15. [Google Scholar]
  28. Arnaiz-Gonzalez, A.; Fernández-Valdivielso, A.; Bustillo, A.; López de Lacalle, L.N. Using artificial neural networks for the prediction of dimensional error on inclined surfaces manufactured by ball-end milling. Int. J. Adv. Manuf. Technol. 2016, 83, 847–859. [Google Scholar] [CrossRef]
Figure 1. The schematic classification of blasting effects on the substrate.
Figure 1. The schematic classification of blasting effects on the substrate.
Metals 08 00938 g001
Figure 2. The surface of metallic substrate blasted by polydispersed (a) shot (b) grit.
Figure 2. The surface of metallic substrate blasted by polydispersed (a) shot (b) grit.
Metals 08 00938 g002
Figure 3. The classification of surfaces in terms of surface topography.
Figure 3. The classification of surfaces in terms of surface topography.
Metals 08 00938 g003
Figure 4. The principle of the experiment.
Figure 4. The principle of the experiment.
Metals 08 00938 g004
Figure 5. Profilographs and Abbot—Fireston curves blasting surfaces (a) SG, (b) C, (c) DSS, (d) SS.
Figure 5. Profilographs and Abbot—Fireston curves blasting surfaces (a) SG, (b) C, (c) DSS, (d) SS.
Metals 08 00938 g005
Figure 6. Boxplot (average and 1.96 standard deviation) for roughness parameters.
Figure 6. Boxplot (average and 1.96 standard deviation) for roughness parameters.
Metals 08 00938 g006
Figure 7. Microscopic snapshot of the surface and 3D appearance—blasting surface (a) SG, (b) C, (c) DSS, (d) SS.
Figure 7. Microscopic snapshot of the surface and 3D appearance—blasting surface (a) SG, (b) C, (c) DSS, (d) SS.
Metals 08 00938 g007aMetals 08 00938 g007b
Figure 8. The correlation matrix and the graphs for the steel grit.
Figure 8. The correlation matrix and the graphs for the steel grit.
Metals 08 00938 g008
Figure 9. The correlation matrix and the graphs for the steel shot.
Figure 9. The correlation matrix and the graphs for the steel shot.
Metals 08 00938 g009
Figure 10. The correlation matrix and the graphs for the corundum.
Figure 10. The correlation matrix and the graphs for the corundum.
Metals 08 00938 g010
Figure 11. The correlation matrix and the graphs for the DSS.
Figure 11. The correlation matrix and the graphs for the DSS.
Metals 08 00938 g011
Figure 12. 3D models graphs of the blasting surfaces.
Figure 12. 3D models graphs of the blasting surfaces.
Metals 08 00938 g012aMetals 08 00938 g012b
Table 1. Chemical composition of steel S235JRG2 in wt. %.
Table 1. Chemical composition of steel S235JRG2 in wt. %.
CMnSiPSN
max. 0.19max. 1.50-max. 0.045max. 0.045max. 0.014
Table 2. Chemical composition of steel shot in wt. %.
Table 2. Chemical composition of steel shot in wt. %.
CMnSiPS
SG0.75–1.200.60–1.100.70–1.10max. 0.04max. 0.04
SS0.95–1.200.70–1.100.80–1.10max. 0.04max. 0.04
Table 3. Chemical composition of corundum in wt. %.
Table 3. Chemical composition of corundum in wt. %.
Al2O3SiO2Fe2O3CaOTiO2
95.50max. 1.40max. 0.60max. 0.201.5–3.0
Table 4. Chemical composition of DSS in wt. %.
Table 4. Chemical composition of DSS in wt. %.
CaOSiO2Al2O3Fe2O3MgOMnOSO3
45.8013.501.7028.106.153.840.95
Table 5. Used types of blasting abrasives.
Table 5. Used types of blasting abrasives.
Types of Blasting AbrasivesAbbreviationThe Particle Size [mm]ShapeMaterial
steel gritSG0.71gritmetalic
steel shotSS0.9shotmetalic
corundumC0.9shotnon-metalic
demetalized steel slagDSS0.9shotnon-metalic
Table 6. The average and standard deviation for roughness parameters.
Table 6. The average and standard deviation for roughness parameters.
Roughness ParametersSGSSDSSC
Ra [µm]10.32 ± 0.7811.71 ± 0.9011.23 ± 0.8912.46 ± 1.00
Rz [µm]69.32 ± 6.7262.10 ± 4.7670.49 ± 5.7880.85 ± 7.58
Rt [µm]87.43 ± 11.8774.94 ± 6.4487.32 ± 10.03102.40 ± 13.54
RSm [µm]306.29 ± 41.14535.71 ± 75.38390.89 ± 59.07357.30 ± 49.21
RPc [number/cm]33.28 ± 4.5019.01 ± 2.5126.07 ± 3.3128.50 ± 3.86
Rlo [mm]2.83 ± 0.022.60 ± 0.012.77 ± 0.022.83 ± 0.03
Table 7. Surface volume of evaluated surfaces.
Table 7. Surface volume of evaluated surfaces.
Surface Blasted withSurface Volume [× 108 µm3]
SS5.81
SG7.95
C7.42
DSS6.78
Table 8. Regressions models, p-value (Ra).
Table 8. Regressions models, p-value (Ra).
Blasting AbrasivesRegression Modelp-Value
SGRa = −11.620 + 0.121Rz − 0.033Rt−0.003RSm + 6.838Rlo − 0.059RPc2.94 × 10−27
SSRa = −45.884 + 0.106Rz − 0.002Rt−0.005RSm + 21.622Rlo − 0.136RPc3.61 × 10−17
CRa = −36.111 + 0.060Rz + 0.003Rt + 0.004RSm + 14.912Rlo + 0.003RPc1.42 × 10−22
DSSRa = −30.905 + 0.117Rz − 0.027Rt − 0.003RSm + 14.667Rlo − 0.118RPc7.12 × 10−23
Table 9. Test locating constant and regression coefficients, p-value (Boltface—statistically significant variables).
Table 9. Test locating constant and regression coefficients, p-value (Boltface—statistically significant variables).
Blasting AbrasivesInterceptRzRtRSmRloRPc
SG0.11282.64 × 10−131.33 × 10−50.29060.01140.0399
SS0.06430.00060.92920.24430.03260.2473
C0.00040.00040.70020.55561.67 × 10−50.9714
DSS0.0056.87 × 10−90.00250.43410.00030.1409
Table 10. Kruskal–Wallis test of the blasting surfaces.
Table 10. Kruskal–Wallis test of the blasting surfaces.
RaKruskal–Wallis Test: H = 170.5216, p = 0.000RzKruskal–Wallis Test: H = 213.6769, p = 0.000
SGSSDSSCSGSSDSSC
SG 0.0000.0000.000SG 0.0001.00000.000
SS0.000 0.01610.0002SS0.000 0.0000.000
DSS0.0000.0161 0.000DSS1.00000.000 0.000
C0.0000.00020.0000 C0.0000.0000.000
RtKruskal–Wallis Test: H = 193.8189, p = 0.000RSmKruskal–Wallis Test: H = 273.8240, p = 0.000
SGSSDSSCSGSSDSSC
SG 0.0001.00000.000SG 0.0000.0000.000
SS0.000 0.00000.000SS0.000 0.0000.000
DSS1.00000.000 0.000DSS0.0000.000 0.0149
C0.0000.0000.000 C0.0000.0000.0149
RloKruskal–Wallis Test: H = 319.4280, p = 0.000RPcKruskal–Wallis Test: H = 273.9025, p = 0.000
SGSSDSSCSGSSDSSC
SG 0.0000.0001.0000SG 0.0000.0000.000
SS0.000 0.0000.000SS0.000 0.0000.000
DSS0.0000.000 0.000DSS0.0000.000 0.0149
C1.00000.0000.000 C0.0000.0000.0149

Share and Cite

MDPI and ACS Style

Draganovská, D.; Ižaríková, G.; Guzanová, A.; Brezinová, J. General Regression Model for Predicting Surface Topography after Abrasive Blasting. Metals 2018, 8, 938. https://doi.org/10.3390/met8110938

AMA Style

Draganovská D, Ižaríková G, Guzanová A, Brezinová J. General Regression Model for Predicting Surface Topography after Abrasive Blasting. Metals. 2018; 8(11):938. https://doi.org/10.3390/met8110938

Chicago/Turabian Style

Draganovská, Dagmar, Gabriela Ižaríková, Anna Guzanová, and Janette Brezinová. 2018. "General Regression Model for Predicting Surface Topography after Abrasive Blasting" Metals 8, no. 11: 938. https://doi.org/10.3390/met8110938

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop