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International Journal of Modern Engineering Research (IJMER)
              www.ijmer.com               Vol.3, Issue.2, March-April. 2013 pp-788-792      ISSN: 2249-6645



                Surface Properties of the Stainless Steel X10 CrNi 18/10
                  after Aplication of Plasma Polishing in Electrolyte

                               D. Vaňa, 1 Š. Podhorský, 2 M. Hurajt, 3 V. Hanzen4
                        1234
                           Department of Welding and Foundry, Slovak Technical University, Slovakia

Abstract: The first part of the paper deals with surface properties of the stainless steel specimen after plasma polishing
in electrolyte. The plasma polishing technology is considered as a more environmental friendly alternative to the common
electrochemical polishing process (electropolish). The electrolyte solutions use no acids or toxicants, low concentrated
water solutions of various salts are used instead. The surface roughness, the gloss level and the thickness of removed layer
are in the focus, as well as their dependence upon the treatment time. The results are then compared to the surface
properties of specimens treated by standard electrochemical polishing. The specimens of the same material, the same shape
and the same surface state have been used for both polishing technologies. Finally, the differences between those polishing
processes and the differences between the properties of the polished surfaces are discussed.

Keywords: electrolyte, plasma, polishing, stainless steel

                                                      I. INTRODUCTION
          Polishing of stainless steels is widely used, mainly in order to improve the corrosion resistance of its surface as well
as to reduce the surface roughness. Polishing is the most common surface finishing operation of stainless steel products
in the field of medical, pharmaceutical, food or chemical industry. The corrosion resistance improvement is not the only
benefit of the polishing process, but the surface also becomes smoother and more resistant to dirt, bacteria, rot, etc. [2, 3].
          Surface polishing in acids mixture under the influence of electric current, e.g. the electrochemical polishing, known
as electro- polishing, is the most commonly used polishing method for surface finishing of complexly shaped industrial
parts. A new polishing technology, the plasma polishing in electrolyte has been developed as an alternative to the standard
electrochemical polishing. This paper deals with some properties of stainless steel surface treated by the plasma polishing
process in electrolyte. Especially the surface roughness reduction, the rise of gloss level and the material removal rate are
examined.

                                   II. THE PRINCIPLE OF THE PLASMA POLISHING
          The metal part, to be treated, is immersed into the electrolyte and is connected to the plus pole of the electric current
supply. So the treated part is the anode. The second electrode is connected to the minus pole of the power supply. As it can
be seen on the Fig. 1, the principal scheme of this process is similar to the electro-chemical polishing at first glance. The
main differences are in the voltage value and in the chemical composition of the electrolyte. The high concentrated mixture
of acids is displaced by low-concentrated water solution of chemically neutral salts. A water-steam film is forming on the
entire treated surface due to high value of the voltage between electrodes. The film is electrically nonconductive and it
separates the metal surface from the electrolyte. In this way the electric current is broken so the electric circuit gets
disconnected. But if the voltage between the electrodes is high enough (a few hundreds of volts), the water-steam film
becomes ionized due to high value of the electric field in the thin film. In this case, the electric current flows through the
water-steam film in the form of glow discharge. In this way, the discharge act on the metal surface in this process. The
                                                                  discharge always runs toward the peaks of the surface profile
                                                                  in the form of thin columns since the distance between the
                                                                  electrodes (metal – wall of electrolyte) is here shortest. In this
                                                                  way the surface peak is quickly removed. When the material
                                                                  of the peak is removed, the column of discharge moves
                                                                  to another surface peak where the thickness of the water-
                                                                  steam layer is less. In this way the surface becomes smoother.
                                                                  If a proper chemical composition of the electrolyte and
                                                                  suitable parameters of the process are used, the treated
                                                                  surface becomes glossy [4].
                                                                            One of the advantages of this technology is in the
                                                                  possibility to treat metal parts with complex and irregular
                                                                  shape. Furthermore, there is no shielding effect as it is in the
                                                                  case of electrochemical polishing. The next advantage of the
         Fig. 1 The principal scheme of the process;              plasma polishing process is in the harmless composition
                                                                  of the     electrolyte.     The    electrolytes    are      based
  1 – treated specimen, 2 – electrolyte solution, 3 – work
                                                                  on environmental friendly solution of various salts. The
  vessel, 4 – ionized water-steam film, 5 – power supply.         solutions of concentrations 4 ÷ 6% are prepared by dissolving

                                                             www.ijmer.com                                               788 | Page
International Journal of Modern Engineering Research (IJMER)
              www.ijmer.com              Vol.3, Issue.2, March-April. 2013 pp-788-792      ISSN: 2249-6645

granulate in the water without extra demand on its quality. In the spent solution, iron is bound in the form of oxides. [2, 3].

                                                   III. THE SPECIMENS
          A rolled sheet of austenitic stainless steel X10 CrNi 18/8 has been used for specimens. The specimens
of dimensions 50 mm × 50 mm × 3 mm has been cut from the sheet using water jet cutter. Two holes of diameter 5 mm were
drilled to fix the specimen to its holder during polishing. The surface of the specimens was not treated e.g. it was in crude
(rolled) state. Due to untreated surface layer the initial (before polishing) gloss level of the specimen had the value of 7.5 GU
only. Its average initial value of the surface roughness Ra was 1.7 µm.

                                        IV. THE EXPERIMENTAL PROCEDURE
         The experiment has been focused on the effect of plasma polishing upon the treated surface’s properties. The
properties have been examined are: the gloss level, the surface roughness and the layer thickness removal Δh. To know the
exact material removal rate is important when precise machine parts with tight tolerances are polished. The total treatment
time lasted 5 minutes and was divided into a few intervals to get the surface properties dependence on the treatment time.
After each polishing step the examined properties were measured always on the same spot on the specimen. The conditions
and the process parameters were kept on constant values during each plasma-polishing step. The electrolytic solution
of concentration 6 % has been used at temperature 65°C and the immersion depth of the specimen was 100 mm.




                                                                Fig. 2 The surface roughness measurement on a specimen
Fig. 3 The gloss level measurement on a specimen
                                                                               using surface tester TR 200
          For exact gloss level assessment of the treated specimen a gloss-meter of the type Novo Curve (Rhopoint
Instruments, UK) has been used. The gloss meter uses 60° measurement angle and it conforms to ASTM D523 and to ISO
2813. The gloss level has been measured at the geometric centre of the specimen (Fig. 2) five times and the average values
of these data are in third column of the TABLE 2. Surface tester of type TR 200 (Fig.3) has been used to evaluate the surface
roughness. The resolution of used surface tester is 0.01 µm and it conforms to DIN4772. The tested area was the same as
in the case of the gloss level measurements. The surface roughness of Ra has been measured five times at the same spot, the
average values are in the TABLE 1, as well.
          The thickness hT and the exact weight
                                                    Table 1 Properties of the specimen #1 after each plasma-polishing step;
of the specimens mT have been measured after
each plasma-polishing treatment step, e.g. after          T           RaT          GT         mT          hT         ∆ℎ 𝑇
the treatment time T, to evaluate the value of          [min]        [µm]        [GU]         [g]        [µm]       [µm/min]
the layer thickness removal hT. The value of             0          1.69          8.8      55.379        —            —
layer thickness removal can be calculated as             0.5         1.51         32.8      55.332       1.09         2.18
the difference between thickness of specimen              1          1.38         66.4      55.270       2.53         2.53
before and after polishing. Since this value is          1.5         1.23         87.4      55.222       3.64         2.43
near the resolution and accuracy of common                2          1.06         98.8      55.181       4.59         2.30
digital micrometres, such results are not                2.5         1.00        137.3      55.134       5.67         2.27
precise enough. Therefore, the material                   3          0.98        157.7      55.087       6.76         2.20
removal rate is calculated from the weight                4          0.88        205.7      55.016       8.41         2.10
difference of the specimen before and after               5          0.78        201.7      54.935      10.28         2.06
polishing and the value of the layer thickness      T – time of treatment, Ra – surface roughness, G – gloss level, m –weight
removal is computed from this value using              of the specimen, h – layer thickness removal, ∆hT – speed of layer
own software, developed for this specific                                       thickness removal
purpose. The balance of type PB 303-S
(Mettler-Toledo) with resolution 1 mg has been used. The measured values of the specimen’s weight and the calculated data
are given in TABLE 1. The layer thickness removal is the thickness of the removed material layer from one side of the treated
surface, not the specimen’s thickness difference. The speed of layer thickness removal ∆ℎ has been calculated from the value

                                                            www.ijmer.com                                              789 | Page
International Journal of Modern Engineering Research (IJMER)
              www.ijmer.com              Vol.3, Issue.2, March-April. 2013 pp-788-792      ISSN: 2249-6645

of the layer thickness removal divided by the appropriate treatment time T. These data can be found in the last column of the
TABLE 1.

                                                      V. THE RESULTS
          Graphical representation of the obtained data is shown on Fig. 4. The value of surface roughness Ra decreases by
the treatment time nonlinearly, initially it declines quickly but then this decline slows down. So the roughness falls more
quickly at the beginning of the polishing process. Using regression analysis of the measured data the following relation has
been found:
      𝑅𝑎 = 1.68 − 0.35𝑇 + 0.036 𝑇 2 [𝜇𝑚, 𝑚𝑖𝑛]                                                                                   (1)
          The gloss level of the treated surface rises almost linearly by the treating time during the first four minutes (Fig. 4).
After the maximal value is reached, there is no evident change of the gloss level. This relation can be described in the
interval 0 to 5 minutes by the following equation:
     𝐺 = 10.8 + 39.6 𝑇 + 8.8 𝑇 2 − 1.8 𝑇 3 [𝐺𝑈, 𝑚𝑖𝑛]                                                                            (2)
          The layer thickness removal shown in Fig. 4 seems to be constant by the treatment time at first glance, but as it can
be seen in TABLE 1 the values slightly decrease except the first value. The following equation has been used to describe this
dependence in the range of 1 ÷ 5 minutes:
    ∆ℎ = −0.12 + 2.52 𝑇 − 0.09𝑇 2 [𝜇𝑚, 𝑚𝑖𝑛]                                                                                     (3)
          This equation is not valid in the first minute of treatment, where the value of the layer thickness removal is less. It
can be explained by the fact, that the initial specimen’s surface had been covered by an oxide film. Metal oxides are
electrically nonconductive so it takes longer to remove them for the plasma-polishing process. A graphical presentation
of the dependence of the layer thickness removal hT upon the treatment time T is shown on the Fig. 5.




  Fig. 5 Surface roughness, gloss level and layer thickness removal           Fig. 4 Dependence of the layer thickness removal
                 dependence upon the treatment time                                    speed upon the treatment time

                              VI. COMPARISON TO THE STANDARD ELECTROPOLISH
The plasma-polishing technology is an alternative to the commonly used electrochemical polishing process, known simply as
―electropolish‖. There is the question, how the surface parameters will differ if the same samples are processed by both
polishing methods. Therefore a few specimens have been polished electrochemically, as well. The specimens of the same
material, the same shape and the same surface state as it was in the case of plasma-polishing have been used. The electrolyte
solution for electrochemical polishing consisted of 64% H 3PO4, 13% H2SO4 and 23% H2O [5, 6]. The temperature of the
electrolyte has been kept during polishing at 60°C. Four specimens (specimen #2 to #5) have been processed 3 minutes, each
at different value of the electric current density: 40 A.dm-2, 50 A.dm-2, 60 A.dm-2 and 72 A.dm-2.




                                                             www.ijmer.com                                              790 | Page
International Journal of Modern Engineering Research (IJMER)
              www.ijmer.com             Vol.3, Issue.2, March-April. 2013 pp-788-792      ISSN: 2249-6645

Table 2 The measured and calculated properties of the specimens before and after 3 minutes of electrochemical polishing
 Specimen        Ra0        Ra3        Ra3        G0            G3         t0        m0         m3          h3       ∆𝒉 𝑻
   No.          [m]       [m]         []       [GU]          [GU]      [mm]        [g]        [g]        [m]     [µm/min]
     2          1.67       1.46        -12.6       8.8          116.0    2.8638     55.672     55.202       10.9       3.62
     3          1.87       1.50        -19.8       8.8          141.6    2.8202     54.967     55.202       12.9       4.30
     4          1.86       1.45        -22.0       8.8          148.5    2.8488     55.609     54.408       14.9       4.98
     5          1.75       1.28        -26.9       8.8          184.4    2.8132     54.792     54.056       17.0       5.67


          The measurement procedure of the specimens’
parameters and the data processing was the same as it was
described for the case of plasma-polishing. The measured
data can be found in the TABLE 2. Subscript 0 is used for
values measured before polishing (processing time T =
0 min), and subscript 3 is used for values measured after 3
minute of polishing (T = 3 min). The values of the layer
thickness removal h for each specimen, calculated from
the specimens’ weight difference are also in in TABLE 2, as
well as the relative values of the surface roughness
reduction Ra. The results obtained for the specimen #1,
which have been treated 3 minutes by plasma-polishing
process, are graphically compared to the results obtained
                                                                   Fig. 6 Surface roughness reduction of the specimens after
for the next four specimens (#2 to #5), which have been
                                                                                     3 minutes of treatment
treated electrochemically also 3 minutes. Fig. 6 shows the
relative surface roughness reduction Ra of the treated
specimens. It is obvious, that the plasma-polishing process
is much more efficient in surface flattening than the
traditional electrochemical polishing process, regardless
the used anodic current density. The value of Ra decreases
by 42 % when plasma-polishing has been used, the highest
decrement of Ra in the case of electrochemical polishing is
for the highest used value of anodic current density and its
value is 27 % only.
   The surface gloss levels of the specimens are compared
in Fig. 7. As it can be seen on the figure, the reached gloss
level of the polished surface is proportional to the electric
current density used during electrochemical process. At its
highest value (72 A.dm-2) the gloss level is little higher
                                                                   Fig. 7 Surface gloss level of the specimens reached after3
than the gloss level of the plasma-polished specimen. The
                                                                                      minutes of treatment
values of layer thickness removal from the specimens’
surface after 3 minutes of treatment are compared at Fig. 8.
This value is also proportional to the anodic current density
in the case of electrochemical polishing as it was for the
gloss level or for the surface roughness declension. As it is
evident in the picture, all these values are much higher than
as the value of layer thickness removal of plasma polished
specimen. After 3 minutes of treatment, the plasma-
polishing process removes 6.76 μm thick layer of the metal
from the treated surface only.

                  VII. DISCUSSION
Analysing the above results of the accomplished
experiments a few conclusions can be drawn. The plasma-
polishing process removes the material from the treated
surface starting to remove the top of the surface profile’s      Fig. 8 The values of the layer thickness removal from the
peaks. Even a little amount of the material has been                  specimens’ surface after 3 minutes of treatment
removed when the process starts, it corresponds to a
relatively high value of layer thickness removal – marked
as h1 shown in Fig. 8. After the tops of the surface profile
peaks are disappeared and the process removes the next
same amount of the material as in the previous case, e.g. S2 = S1 on the Fig. 8, the thickness of this removed layer h2 is
much less as the thickness of the prior layer h1. Therefore the value of the layer thickness removal falls down quickly at the
                                                           www.ijmer.com                                             791 | Page
International Journal of Modern Engineering Research (IJMER)
                www.ijmer.com              Vol.3, Issue.2, March-April. 2013 pp-788-792      ISSN: 2249-6645

beginning of the treatment and then it continually slows down probably to a constant value. The material removing progress
is more complex if the treated surface is covered by a layer of oxides or any other dirt. Since this topmost layer of metal-
oxides is electrically nonconductive it takes longer for plasma-polishing process to remove them. It explains the low material
removal speed at the beginning of the treatment on the Fig. 5. As soon as the topmost layer is removed the surface
roughness decreases according to above described theory.




      Fig. 9 Surface profile of the treated metal during                       Fig. 10 Surface profile of the treated metal during
                      plasma polishing                                                     electrochemical polishing

           The material removal process during plasma polishing is different as it is in the case of standard electrolytic
polishing, when the material from the surface is removed by anodic dissolution – Fig. 10. An anodic film forms on the
treated surface during electrochemical polishing. The anodic film has lower electric conductivity then the surrounding
electrolytic solution and the process of surface flattering is based on different velocity of anodic dissolving through this
layer. Anodic dissolving is more intensive on the peaks of surface profile, where the anodic film is thinner so the electrical
resistance is lower. Therefore the velocity of anodic dissolving v1 is faster here than on the ―valleys‖ of the surface profile –
v2. In this way, the metal is being removed not only on the peaks of the surface profile, but from whole surface although with
different speed. This is the reason why it takes longer to reduce the surface roughness (Fig. 6) and why the thickness of layer
removed from the surface is much higher (Fig. 8) then as it in the case of plasma-polishing, where the metal is removed
mainly from the surface profile’s peaks.

                                                      VIII. CONCLUSION
           Surface properties of the specimens made from stainless steel X10 CrNi 18/10 have been plasma polished
in electrolyte. The resulting properties of the polished surface depend on the treatment time. The gloss level rapidly increases
during the first four minutes as it is described by the equation (2). The surface roughness reduction is most significant during
the first four minutes, as well. The equation (1) will be useful to calculate the needful processing time when the desired value
of the surface roughness is in focus. To calculate the dimension changes, for example when the precision machine parts are
plasma-polished, the equation (3) can be used. All above equations can be also used for other stainless steels, although the
resulting values may slightly differ.
           The plasma polishing process is more efficient at surface roughness reduction than the common electrochemical
polishing process. Furthermore, the value of the layer thickness removal is much less in the case of plasma polishing process.
It can be supposed that this value will not depends on the spent state of the electrolytic solution such as it is in the state
of electrochemical process. But this expectation must be confirmed experimentally in the next.

                                                             REFERENCES
[1]    M. Murgaš, J. Solár, Š. Podhorský, I. Novotný: Boundary of possibilities of plasma-electrolytic technology at reducing of a metal
       surface roughness, Proc. International conference CO-MAT-TECH 2000, Bratislava, SK, 2000, 183-188.
[2]    D. Vaňa, Š. Podhorský: Electrolytic-plasma polishing of stainless steel in electrolyte, IN: TEAM, Trnava, 2011, 243-246.
[3]    R. Tóth, Š. Podhorský: Electrolytic-plasma cleaning and surface conditioning of casting, IN: ActaMetallurgica, 5, 1999, 192-196.
[4]    Š. Podhorský, R. Šuba, R. Tóth: Metalic surfaces treated by plasma discharge in electrolyte. In: Funkčné povrchy v strojárstve 2007
       v krajinách V4: Trenčín, Alexander Dubček University of Trenčín, 2007, 138-143.
[5]    E. S. Lee: Machining Characteristics of the Electro polishing of Stainless Steel (STS316L). IN: Int J Adv Manuf Technol, Springer-
       Verlag London Limited (2000) 16, 591–599.
[6]    V. Číhal, Korozivzdorné oceli a slitiny (Prague, Academia, 1999).




                                                                 www.ijmer.com                                                792 | Page

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Bg32788792

  • 1. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-788-792 ISSN: 2249-6645 Surface Properties of the Stainless Steel X10 CrNi 18/10 after Aplication of Plasma Polishing in Electrolyte D. Vaňa, 1 Š. Podhorský, 2 M. Hurajt, 3 V. Hanzen4 1234 Department of Welding and Foundry, Slovak Technical University, Slovakia Abstract: The first part of the paper deals with surface properties of the stainless steel specimen after plasma polishing in electrolyte. The plasma polishing technology is considered as a more environmental friendly alternative to the common electrochemical polishing process (electropolish). The electrolyte solutions use no acids or toxicants, low concentrated water solutions of various salts are used instead. The surface roughness, the gloss level and the thickness of removed layer are in the focus, as well as their dependence upon the treatment time. The results are then compared to the surface properties of specimens treated by standard electrochemical polishing. The specimens of the same material, the same shape and the same surface state have been used for both polishing technologies. Finally, the differences between those polishing processes and the differences between the properties of the polished surfaces are discussed. Keywords: electrolyte, plasma, polishing, stainless steel I. INTRODUCTION Polishing of stainless steels is widely used, mainly in order to improve the corrosion resistance of its surface as well as to reduce the surface roughness. Polishing is the most common surface finishing operation of stainless steel products in the field of medical, pharmaceutical, food or chemical industry. The corrosion resistance improvement is not the only benefit of the polishing process, but the surface also becomes smoother and more resistant to dirt, bacteria, rot, etc. [2, 3]. Surface polishing in acids mixture under the influence of electric current, e.g. the electrochemical polishing, known as electro- polishing, is the most commonly used polishing method for surface finishing of complexly shaped industrial parts. A new polishing technology, the plasma polishing in electrolyte has been developed as an alternative to the standard electrochemical polishing. This paper deals with some properties of stainless steel surface treated by the plasma polishing process in electrolyte. Especially the surface roughness reduction, the rise of gloss level and the material removal rate are examined. II. THE PRINCIPLE OF THE PLASMA POLISHING The metal part, to be treated, is immersed into the electrolyte and is connected to the plus pole of the electric current supply. So the treated part is the anode. The second electrode is connected to the minus pole of the power supply. As it can be seen on the Fig. 1, the principal scheme of this process is similar to the electro-chemical polishing at first glance. The main differences are in the voltage value and in the chemical composition of the electrolyte. The high concentrated mixture of acids is displaced by low-concentrated water solution of chemically neutral salts. A water-steam film is forming on the entire treated surface due to high value of the voltage between electrodes. The film is electrically nonconductive and it separates the metal surface from the electrolyte. In this way the electric current is broken so the electric circuit gets disconnected. But if the voltage between the electrodes is high enough (a few hundreds of volts), the water-steam film becomes ionized due to high value of the electric field in the thin film. In this case, the electric current flows through the water-steam film in the form of glow discharge. In this way, the discharge act on the metal surface in this process. The discharge always runs toward the peaks of the surface profile in the form of thin columns since the distance between the electrodes (metal – wall of electrolyte) is here shortest. In this way the surface peak is quickly removed. When the material of the peak is removed, the column of discharge moves to another surface peak where the thickness of the water- steam layer is less. In this way the surface becomes smoother. If a proper chemical composition of the electrolyte and suitable parameters of the process are used, the treated surface becomes glossy [4]. One of the advantages of this technology is in the possibility to treat metal parts with complex and irregular shape. Furthermore, there is no shielding effect as it is in the case of electrochemical polishing. The next advantage of the Fig. 1 The principal scheme of the process; plasma polishing process is in the harmless composition of the electrolyte. The electrolytes are based 1 – treated specimen, 2 – electrolyte solution, 3 – work on environmental friendly solution of various salts. The vessel, 4 – ionized water-steam film, 5 – power supply. solutions of concentrations 4 ÷ 6% are prepared by dissolving www.ijmer.com 788 | Page
  • 2. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-788-792 ISSN: 2249-6645 granulate in the water without extra demand on its quality. In the spent solution, iron is bound in the form of oxides. [2, 3]. III. THE SPECIMENS A rolled sheet of austenitic stainless steel X10 CrNi 18/8 has been used for specimens. The specimens of dimensions 50 mm × 50 mm × 3 mm has been cut from the sheet using water jet cutter. Two holes of diameter 5 mm were drilled to fix the specimen to its holder during polishing. The surface of the specimens was not treated e.g. it was in crude (rolled) state. Due to untreated surface layer the initial (before polishing) gloss level of the specimen had the value of 7.5 GU only. Its average initial value of the surface roughness Ra was 1.7 µm. IV. THE EXPERIMENTAL PROCEDURE The experiment has been focused on the effect of plasma polishing upon the treated surface’s properties. The properties have been examined are: the gloss level, the surface roughness and the layer thickness removal Δh. To know the exact material removal rate is important when precise machine parts with tight tolerances are polished. The total treatment time lasted 5 minutes and was divided into a few intervals to get the surface properties dependence on the treatment time. After each polishing step the examined properties were measured always on the same spot on the specimen. The conditions and the process parameters were kept on constant values during each plasma-polishing step. The electrolytic solution of concentration 6 % has been used at temperature 65°C and the immersion depth of the specimen was 100 mm. Fig. 2 The surface roughness measurement on a specimen Fig. 3 The gloss level measurement on a specimen using surface tester TR 200 For exact gloss level assessment of the treated specimen a gloss-meter of the type Novo Curve (Rhopoint Instruments, UK) has been used. The gloss meter uses 60° measurement angle and it conforms to ASTM D523 and to ISO 2813. The gloss level has been measured at the geometric centre of the specimen (Fig. 2) five times and the average values of these data are in third column of the TABLE 2. Surface tester of type TR 200 (Fig.3) has been used to evaluate the surface roughness. The resolution of used surface tester is 0.01 µm and it conforms to DIN4772. The tested area was the same as in the case of the gloss level measurements. The surface roughness of Ra has been measured five times at the same spot, the average values are in the TABLE 1, as well. The thickness hT and the exact weight Table 1 Properties of the specimen #1 after each plasma-polishing step; of the specimens mT have been measured after each plasma-polishing treatment step, e.g. after T RaT GT mT hT ∆ℎ 𝑇 the treatment time T, to evaluate the value of [min] [µm] [GU] [g] [µm] [µm/min] the layer thickness removal hT. The value of 0 1.69 8.8 55.379 — — layer thickness removal can be calculated as 0.5 1.51 32.8 55.332 1.09 2.18 the difference between thickness of specimen 1 1.38 66.4 55.270 2.53 2.53 before and after polishing. Since this value is 1.5 1.23 87.4 55.222 3.64 2.43 near the resolution and accuracy of common 2 1.06 98.8 55.181 4.59 2.30 digital micrometres, such results are not 2.5 1.00 137.3 55.134 5.67 2.27 precise enough. Therefore, the material 3 0.98 157.7 55.087 6.76 2.20 removal rate is calculated from the weight 4 0.88 205.7 55.016 8.41 2.10 difference of the specimen before and after 5 0.78 201.7 54.935 10.28 2.06 polishing and the value of the layer thickness T – time of treatment, Ra – surface roughness, G – gloss level, m –weight removal is computed from this value using of the specimen, h – layer thickness removal, ∆hT – speed of layer own software, developed for this specific thickness removal purpose. The balance of type PB 303-S (Mettler-Toledo) with resolution 1 mg has been used. The measured values of the specimen’s weight and the calculated data are given in TABLE 1. The layer thickness removal is the thickness of the removed material layer from one side of the treated surface, not the specimen’s thickness difference. The speed of layer thickness removal ∆ℎ has been calculated from the value www.ijmer.com 789 | Page
  • 3. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-788-792 ISSN: 2249-6645 of the layer thickness removal divided by the appropriate treatment time T. These data can be found in the last column of the TABLE 1. V. THE RESULTS Graphical representation of the obtained data is shown on Fig. 4. The value of surface roughness Ra decreases by the treatment time nonlinearly, initially it declines quickly but then this decline slows down. So the roughness falls more quickly at the beginning of the polishing process. Using regression analysis of the measured data the following relation has been found: 𝑅𝑎 = 1.68 − 0.35𝑇 + 0.036 𝑇 2 [𝜇𝑚, 𝑚𝑖𝑛] (1) The gloss level of the treated surface rises almost linearly by the treating time during the first four minutes (Fig. 4). After the maximal value is reached, there is no evident change of the gloss level. This relation can be described in the interval 0 to 5 minutes by the following equation: 𝐺 = 10.8 + 39.6 𝑇 + 8.8 𝑇 2 − 1.8 𝑇 3 [𝐺𝑈, 𝑚𝑖𝑛] (2) The layer thickness removal shown in Fig. 4 seems to be constant by the treatment time at first glance, but as it can be seen in TABLE 1 the values slightly decrease except the first value. The following equation has been used to describe this dependence in the range of 1 ÷ 5 minutes: ∆ℎ = −0.12 + 2.52 𝑇 − 0.09𝑇 2 [𝜇𝑚, 𝑚𝑖𝑛] (3) This equation is not valid in the first minute of treatment, where the value of the layer thickness removal is less. It can be explained by the fact, that the initial specimen’s surface had been covered by an oxide film. Metal oxides are electrically nonconductive so it takes longer to remove them for the plasma-polishing process. A graphical presentation of the dependence of the layer thickness removal hT upon the treatment time T is shown on the Fig. 5. Fig. 5 Surface roughness, gloss level and layer thickness removal Fig. 4 Dependence of the layer thickness removal dependence upon the treatment time speed upon the treatment time VI. COMPARISON TO THE STANDARD ELECTROPOLISH The plasma-polishing technology is an alternative to the commonly used electrochemical polishing process, known simply as ―electropolish‖. There is the question, how the surface parameters will differ if the same samples are processed by both polishing methods. Therefore a few specimens have been polished electrochemically, as well. The specimens of the same material, the same shape and the same surface state as it was in the case of plasma-polishing have been used. The electrolyte solution for electrochemical polishing consisted of 64% H 3PO4, 13% H2SO4 and 23% H2O [5, 6]. The temperature of the electrolyte has been kept during polishing at 60°C. Four specimens (specimen #2 to #5) have been processed 3 minutes, each at different value of the electric current density: 40 A.dm-2, 50 A.dm-2, 60 A.dm-2 and 72 A.dm-2. www.ijmer.com 790 | Page
  • 4. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-788-792 ISSN: 2249-6645 Table 2 The measured and calculated properties of the specimens before and after 3 minutes of electrochemical polishing Specimen Ra0 Ra3 Ra3 G0 G3 t0 m0 m3 h3 ∆𝒉 𝑻 No. [m] [m] [] [GU] [GU] [mm] [g] [g] [m] [µm/min] 2 1.67 1.46 -12.6 8.8 116.0 2.8638 55.672 55.202 10.9 3.62 3 1.87 1.50 -19.8 8.8 141.6 2.8202 54.967 55.202 12.9 4.30 4 1.86 1.45 -22.0 8.8 148.5 2.8488 55.609 54.408 14.9 4.98 5 1.75 1.28 -26.9 8.8 184.4 2.8132 54.792 54.056 17.0 5.67 The measurement procedure of the specimens’ parameters and the data processing was the same as it was described for the case of plasma-polishing. The measured data can be found in the TABLE 2. Subscript 0 is used for values measured before polishing (processing time T = 0 min), and subscript 3 is used for values measured after 3 minute of polishing (T = 3 min). The values of the layer thickness removal h for each specimen, calculated from the specimens’ weight difference are also in in TABLE 2, as well as the relative values of the surface roughness reduction Ra. The results obtained for the specimen #1, which have been treated 3 minutes by plasma-polishing process, are graphically compared to the results obtained Fig. 6 Surface roughness reduction of the specimens after for the next four specimens (#2 to #5), which have been 3 minutes of treatment treated electrochemically also 3 minutes. Fig. 6 shows the relative surface roughness reduction Ra of the treated specimens. It is obvious, that the plasma-polishing process is much more efficient in surface flattening than the traditional electrochemical polishing process, regardless the used anodic current density. The value of Ra decreases by 42 % when plasma-polishing has been used, the highest decrement of Ra in the case of electrochemical polishing is for the highest used value of anodic current density and its value is 27 % only. The surface gloss levels of the specimens are compared in Fig. 7. As it can be seen on the figure, the reached gloss level of the polished surface is proportional to the electric current density used during electrochemical process. At its highest value (72 A.dm-2) the gloss level is little higher Fig. 7 Surface gloss level of the specimens reached after3 than the gloss level of the plasma-polished specimen. The minutes of treatment values of layer thickness removal from the specimens’ surface after 3 minutes of treatment are compared at Fig. 8. This value is also proportional to the anodic current density in the case of electrochemical polishing as it was for the gloss level or for the surface roughness declension. As it is evident in the picture, all these values are much higher than as the value of layer thickness removal of plasma polished specimen. After 3 minutes of treatment, the plasma- polishing process removes 6.76 μm thick layer of the metal from the treated surface only. VII. DISCUSSION Analysing the above results of the accomplished experiments a few conclusions can be drawn. The plasma- polishing process removes the material from the treated surface starting to remove the top of the surface profile’s Fig. 8 The values of the layer thickness removal from the peaks. Even a little amount of the material has been specimens’ surface after 3 minutes of treatment removed when the process starts, it corresponds to a relatively high value of layer thickness removal – marked as h1 shown in Fig. 8. After the tops of the surface profile peaks are disappeared and the process removes the next same amount of the material as in the previous case, e.g. S2 = S1 on the Fig. 8, the thickness of this removed layer h2 is much less as the thickness of the prior layer h1. Therefore the value of the layer thickness removal falls down quickly at the www.ijmer.com 791 | Page
  • 5. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-788-792 ISSN: 2249-6645 beginning of the treatment and then it continually slows down probably to a constant value. The material removing progress is more complex if the treated surface is covered by a layer of oxides or any other dirt. Since this topmost layer of metal- oxides is electrically nonconductive it takes longer for plasma-polishing process to remove them. It explains the low material removal speed at the beginning of the treatment on the Fig. 5. As soon as the topmost layer is removed the surface roughness decreases according to above described theory. Fig. 9 Surface profile of the treated metal during Fig. 10 Surface profile of the treated metal during plasma polishing electrochemical polishing The material removal process during plasma polishing is different as it is in the case of standard electrolytic polishing, when the material from the surface is removed by anodic dissolution – Fig. 10. An anodic film forms on the treated surface during electrochemical polishing. The anodic film has lower electric conductivity then the surrounding electrolytic solution and the process of surface flattering is based on different velocity of anodic dissolving through this layer. Anodic dissolving is more intensive on the peaks of surface profile, where the anodic film is thinner so the electrical resistance is lower. Therefore the velocity of anodic dissolving v1 is faster here than on the ―valleys‖ of the surface profile – v2. In this way, the metal is being removed not only on the peaks of the surface profile, but from whole surface although with different speed. This is the reason why it takes longer to reduce the surface roughness (Fig. 6) and why the thickness of layer removed from the surface is much higher (Fig. 8) then as it in the case of plasma-polishing, where the metal is removed mainly from the surface profile’s peaks. VIII. CONCLUSION Surface properties of the specimens made from stainless steel X10 CrNi 18/10 have been plasma polished in electrolyte. The resulting properties of the polished surface depend on the treatment time. The gloss level rapidly increases during the first four minutes as it is described by the equation (2). The surface roughness reduction is most significant during the first four minutes, as well. The equation (1) will be useful to calculate the needful processing time when the desired value of the surface roughness is in focus. To calculate the dimension changes, for example when the precision machine parts are plasma-polished, the equation (3) can be used. All above equations can be also used for other stainless steels, although the resulting values may slightly differ. The plasma polishing process is more efficient at surface roughness reduction than the common electrochemical polishing process. Furthermore, the value of the layer thickness removal is much less in the case of plasma polishing process. It can be supposed that this value will not depends on the spent state of the electrolytic solution such as it is in the state of electrochemical process. But this expectation must be confirmed experimentally in the next. REFERENCES [1] M. Murgaš, J. Solár, Š. Podhorský, I. Novotný: Boundary of possibilities of plasma-electrolytic technology at reducing of a metal surface roughness, Proc. International conference CO-MAT-TECH 2000, Bratislava, SK, 2000, 183-188. [2] D. Vaňa, Š. Podhorský: Electrolytic-plasma polishing of stainless steel in electrolyte, IN: TEAM, Trnava, 2011, 243-246. [3] R. Tóth, Š. Podhorský: Electrolytic-plasma cleaning and surface conditioning of casting, IN: ActaMetallurgica, 5, 1999, 192-196. [4] Š. Podhorský, R. Šuba, R. Tóth: Metalic surfaces treated by plasma discharge in electrolyte. In: Funkčné povrchy v strojárstve 2007 v krajinách V4: Trenčín, Alexander Dubček University of Trenčín, 2007, 138-143. [5] E. S. Lee: Machining Characteristics of the Electro polishing of Stainless Steel (STS316L). IN: Int J Adv Manuf Technol, Springer- Verlag London Limited (2000) 16, 591–599. [6] V. Číhal, Korozivzdorné oceli a slitiny (Prague, Academia, 1999). www.ijmer.com 792 | Page