deposition of plasma spray coating using industrial waste

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199 Deposition of Plasma Spray Coating using industrial waste with low grade ore mineral S C MISHRA* and S PRAHARAJ National Institute of Technology, Rourkela, India. *Corresponding author: - [email protected] Received : 5.6.11 , Accepted 19.7.11 Abstract . In spite of its extensive advantages, plasma sprayed coatings suffer from major hindrance due to the high cost of the spray grade powders. In the present investigation, attempts has been made to explore the possibility of using some low grade ore mineral and industrial wastes as coating material, with an aim to reduce the cost of raw material used for coating. Conventional atmospheric plasma spray technique is used to develop coatings of fly ash (an industrial waste) mixed with quartz (a low grade ore mineral) on mild steel and copper substrates. Coatings are characterized with adhesion tests, phase composition analysis, & surface morphology using scanning electron microscopy. This work establishes that, Fly ash-quartz mixture can be used as a potential coating material suitable for depositing plasma spray coating. This work opens up a new pathway for value added utilization of this industrial waste and low grade ore mineral. Keywords: Fly ash, plasma sprayed coating, ceramic coating, industrial waste utilization 1. Introduction Thick ceramic overlay coatings of greater than 50 µm thickness are used for a remarkable number of applications (Matejka and Benko, 1989). In recent years, large number of studies have been carried out on deposition of ceramic coatings on metal components to combat wear, thermal shock etc. (Bandopadhyaya, 2000; Song et al.,1998). Plasma spraying which finds a lot of applications due to its versatility for coating deposition on wide range of materials (metallic and non metallic), hence more suitable for high melting point materials viz. refractory ceramics, cermets etc. (Satpathy et al.,2007; Fauchais, 1996). For a long time, Silica and aluminous-silicate bricks are preferred as refractory materials in many industrial applications, due to their high wear resistance and load bearing capacity at high temperatures (Sidhu et al., 2007). During the last decade, although a large number of investigations have been Orissa Journal of Physics ISSN 0974-8202 Vol. 18, No.2 August 2011 pp. 199-206 © Orissa Physical Society

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Page 1: Deposition of Plasma Spray Coating using industrial waste

199

Deposition of Plasma Spray Coating using industrial waste with low grade ore mineral

S C MISHRA* and S PRAHARAJ National Institute of Technology, Rourkela, India. *Corresponding author: - [email protected]

Received : 5.6.11 , Accepted 19.7.11

Abstract . In spite of its extensive advantages, plasma sprayed coatings suffer from major hindrance due to the high cost of the spray grade powders. In the present investigation, attempts has been made to explore the possibility of using some low grade ore mineral and industrial wastes as coating material, with an aim to reduce the cost of raw material used for coating. Conventional atmospheric plasma spray technique is used to develop coatings of fly ash (an industrial waste) mixed with quartz (a low grade ore mineral) on mild steel and copper substrates. Coatings are characterized with adhesion tests, phase composition analysis, & surface morphology using scanning electron microscopy. This work establishes that, Fly ash-quartz mixture can be used as a potential coating material suitable for depositing plasma spray coating. This work opens up a new pathway for value added utilization of this industrial waste and low grade ore mineral. Keywords: Fly ash, plasma sprayed coating, ceramic coating, industrial waste utilization

1. Introduction

Thick ceramic overlay coatings of greater than 50 µm thickness are used for a remarkable number of applications (Matejka and Benko, 1989). In recent years, large number of studies have been carried out on deposition of ceramic coatings on metal components to combat wear, thermal shock etc. (Bandopadhyaya, 2000; Song et al.,1998). Plasma spraying which finds a lot of applications due to its versatility for coating deposition on wide range of materials (metallic and non metallic), hence more suitable for high melting point materials viz. refractory ceramics, cermets etc. (Satpathy et al.,2007; Fauchais, 1996).

For a long time, Silica and aluminous-silicate bricks are preferred as refractory materials in many industrial applications, due to their high wear resistance and load bearing capacity at high temperatures (Sidhu et al., 2007). During the last decade, although a large number of investigations have been

Orissa Journal of Physics

ISSN 0974-8202

Vol. 18, No.2 August 2011 pp. 199-206

© Orissa Physical Society

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S C Mishra and S Praharaj

Orissa Journal of Physics, Vol. 18, No.2, August 2011 200

carried out for development of plasma spray ceramic coatings, not much effort has been made to use low-grade raw materials for such purposes (Sampath et al., 1990). In the recent past, efforts have been made to deposit fly ash coating on metal substrates by premixing with aluminum powder (Mishra et al., 2000). Fly ash premixed with Titania bearing ore mineral has also been found successful in depositing thermal spray coatings on metals (Mishra et al., 2008). In the present investigation, attempts have been made to develop plasma spray coatings utilizing industrial waste i.e. fly ash with addition of a low grade mineral i.e. quartz to deposit alumino-silicate composite coatings. Fly ash along with quartz (plentily available in India) can be a cost effective substitute for conventional extenders for high performance (industrially useful) coatings (Tiwari and Saxena, 1999). Thus the soul objective of this work is to reduce the cost of the spray grade powders (i.e. raw material) required for thermal spray coating. In this paper, coatings are deposited on metal substrates using atmospheric plasma spraying system, at different operating power levels of the plasma torch.

Deposition efficiency, which is an important factor that determines the techno-economics of the process, was evaluated for the coatings. To characterize the coatings, Coating interface bond strength is measured using coating pull out method confirming to ASTM C-633 standard. To ascertain the phases present and phase changes / transformation taking place during plasma spraying, X-ray diffractograms are taken on the raw material and on coatings. The coating quality and behavior depends on coating morphology and inter-particle bonding of the sprayed powders. So the surface morphology of the coatings is studied using Scanning Electron Microscope.

2. Materials and Method

Fly ash +40% quartz are mixed in a planetary ball mill for 3 hours to get a homogeneous mixture. The particle size of the powders is in the range of 40 to 100 micron. Commercially available copper and mild steel are chosen as substrate materials. The circular discs specimens of 1 inch dia and 3mm thick are grit blasted at a pressure of 3 kg/cm2 using alumina grits. The standoff distance in blasting is kept between 120-150 mm. to get the average roughness of the substrates ~6.8 µm. The grit blasted specimens are cleaned with acetone and spraying is carried out immediately after cleaning. Conventional 40kW atmospheric plasma spray (APS) system is used. The plasma input power is varied from 11 to 21 kW by controlling the gas flow rate, voltage and the arc current. The operating parameters during coating deposition are given in table 1.

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Orissa Journal of Physics, Vol. 18, No.2, August 2011 201

Table 1. Operating parameters of the plasma spray unit.

Operating Parameters Values

Plasma Arc Current (amp)

Arc Voltage (volt)

Plasma Gas (Argon) Flow Rate (Lpm)

Secondary Gas (N2) Flow Rate (Lpm)

Carrier Gas (Argon) Flow Rate (Lpm)

Powder Feed Rate (gm/min)

Torch to Base Distance TBD(mm)

280-500

40-45

28

3

12

15

100

The coating adhesion strength is measured by coating pullout test using a special zig for holding the sample. The test was performed as per ASTM C-633 standard. XRD analysis of the coatings is done using Ni-filtered Cu-Kα radiation. The surfaces morphology of all coatings is investigated with JEOL JSM-6480 LV scanning electron microscope in secondary electron imaging mode.

Deposition efficiency is evaluated by weighing method (Chen, 2004), which is a widely accepted method:

η = (Gc / Gp) X 100 (1)

Where η is the deposition efficiency, Gc is the weight of coating deposited on the substrate and Gp is the weight expended feedstock

3. Results and Discussions

Figure 1 shows the variation of deposition efficiency of fly ash-quartz coating. It is interesting to note that the deposition efficiency is increased in a sigmoidal fashion with the torch input power which reveals that the coating deposition efficiency is influenced by torch input power. Plasma spray deposition efficiency of a given material depends on its melting point, thermal heat capacity and particle size of the powder etc. At lower power level, the plasma jet temperature is not high enough to melt the entire feed powder (particles) that enter the plasma jet. As the power level is increased, the average plasma temperature increases, thus melting a larger fraction of the feed powder. The spray efficiency therefore increases with increase in input power to the plasma

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torch. However, beyond a certain power level of the torch, temperature of the plasma becomes high enough leading to vaporization/dissociation of the powder particles. Thus there is not much increase in deposition efficiency and coating thickness as well. This tendency is generally observed in deposition of plasma spray coatings. However, the operating power above which the efficiency decrease depends on the chemical nature of the feed material i.e. powder and its particle size, thermal conductivity, in-situ phase transformations etc.

Coating interface bond strength is evaluated and the variation of adhesion strength of the coatings is shown in figure 2. Each data point is the average of five test runs.

05

10152025303540

0 5 10 15 20 25

Torch power input (KW)

Dep

ositi

on e

ffic

ienc

y (%

)

0

1

2

3

4

5

6

7

0 10 20 30

Torch pow er input (KW)

Adh

esio

n st

reng

th (M

Pa)

Mild steel

Copper

Fig 1. Variation of deposition efficiency of flyash-quartz coatings at different power levels.

Fig 2. Variation of coating adhesion strength with power level.

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From the above figure, it is clear that the adhesion strength varies with operating power of the plasma torch. Maximum adhesion strength of 6.12 MPa on mild steel and of 5.802 MPa on copper substrate is recorded on the coatings deposited at 21 kW power level. It can be visualized that, the interface bond strength increases with increase in input power to the torch up to a certain power level and then shows a very little or nominal variation in coating adhesion irrespective of the substrate material. This might be due to the fact that, when the operating power level is increased, larger fraction of particles attain molten state as well as the velocity of the particles also increase. Therefore there is better probability for splat formation i.e. forms a lamellar structure and hence better mechanical inter-locking of molten particles/splats on the substrate leading to increase in adhesion strength (Pawlowski, 1995). But, at a much higher power level fragmentation and vaporization of the particles increases. There is also a greater chance to fly off of smaller particles during in-flight traverse and results almost no increase in adhesion strength of the coatings. Coating adhesion strength is higher in case of mild steel substrate than that of copper substrate, may be due to (I) the difference of thermal conductivity of substrates and also may be due to (II) the thermal expansion coefficient mismatch at the ceramic metal interface (Guilmard et al., 1993). Mechanical interlocking between the coating and the substrate surface is considered to be the most effective contributor of adhesion between them (Safai and Herman, 1977).

The XRD analysis of the raw material and fly ash-quartz coatings were made. The XRD of the feed material shows the presence of quartz, alumina, wustite etc. phases. With increase in coating power level, appearance of some new phases such as mullite, tridymite, cristobolite, γ-alumina, etc. are found. Especially the percentage of mullite and tridamite (high temperature phase of silica) are found to increase with increase in torch input power. It may be due to the availability of high temperature which has accelerated the phase transformations and different phase are formed depending on enthalpy/ environment and transformation conditions (Bullard et al., 1992). As these coatings is consists of mixture of hard oxides, it is expected that a ceramic composite coating from low grade materials could be made which can have better wear resistance properties.

The adhesion strength of the coatings depends on the coating morphology and inter-particle bonding of the sprayed powders. SEM micrographs of Fly ash-quartz coating surfaces are shown in figure.3.

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The coating deposited at 11KW power level (fig 3a) on mild steel substrate, shows a uniform distribution of molten/semi molten particles which have agglomerated to form laths. More amounts of cavitations are observed. Some (open) large pores are found on the inter particle boundaries and triple particle/grain junctions. These may have originated due to the inadequate flow of molten particles during their solidification (Ctibor et al., 2007). Coating made at 15kW (fig.3b), bears a different morphology. Some spheroidal particles are found which might have formed due to breaking and fragmentation of larger particles at a higher power level during their in-flight traverse through the plasma jet and then solidified in the form of spheres due to fast rate of quenching. Deep pores are found but the amount of cavitations is less. In case of coatings made at 18kW

(a) (b)

(d)

Fig. 3 : Surface Morphology of fly ash-quartz coatings deposited at (a) 11kW, (b) 15kW, (c) 18kW and (d) 21kW power levels.

(c)

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(fig.3c), the fragmented particles carry higher thermal energy. So they might have reached the surface in semi molten state and agglomerated to form smaller splats. Cavitation is still less here which might have led to the increase of adhesion strength. At still higher power level i.e. 21kW (fig.3d), much smaller fragmented particles are found and are fused together in semi molten state in lumps to form flattened regions. Amount of cavitations is slightly more than the previous case.

4. Conclusions

From this study it has been found that fly ash with low grade ore mineral (quartz) additions can be used to deposit plasma spray ceramic composite coating on metal substrates. The maximum adherence strength of 6.120 MPa on mild steel substrate and of 5.802 Mpa on copper substrate is recorded in such coatings. Inter-oxide transformations of the raw materials do occur during spray deposition and their amount varies with operating power of the plasma torch. The operating power level of the plasma torch affects the coating morphology and mechanical properties of the coating.

References

[1] D Matejka and B Benko, Plasma spraying of metallic and ceramic materials, (Wiley Interscience, New York, 1989) pp.132

[2] P P Bandopadhyaya, Processing and characterization of plasma sprayed ceramic coatings on steel substrates – Ph.D. Thesis (IIT, Kharagpur, 2000)

[3] Y S Song, J C Han, M H Park, H Rob, K H Loe, E S Byun and S Sasaki, Proc. 15th International Thermal Spray Conference – 29th May, France, pp.225 (1998)

[4] A Satpathy, S C Mishra, P V A Padmanabhan and K P Sree Kumar, Journal of Solid Waste Technology and Management, 33(2), 48 (2007)

[5] P Fauchais, M Verdelle, A Verdelle and L Bianchi, Ceramic International, 22, 295 (1996)

[6] B S Sidhu, H Singh, D Puri and S Prakash, Tribology International, 40, 800 (2007)

[7] S Sampath, H Herman, Protective coatings processing and characterization edited by R M Yazici, (The Minerals, Metals and Material Society, USA, 1990) p.145.

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Orissa Journal of Physics, Vol. 18, No.2, August 2011 206

[8] S C Mishra, K C Rout, P V A Padmanavan and B Mills, Journal of Materials Processing Technology, 102(1-3), 9 (2000)

[9] S C Mishra, A Satpathy, S Das, S Sarkar, PVA Padmanavan and K P Sreekumar, Journal of Manufacturing Engineering, 3(2), 118 (2008)

[10] S Tiwari and M Saxena, Br. Corros. J. 34, 184 (1999)

[11] H Chen, S W Lee, D Hao, Cheran, X. Ding and Ho Cho Chul, Materials Letter, 58, 1241 (2004)

[12] L Pawlowski, The science and engineering of thermal spray coatings (Wiley Interscience, New York, USA, 1995) pp.432.

[13] Y Guilmard, J Denape, J A Petit, Tribology International, 26, 29 (1993)

[14] S Safai, and H Herman, Thin Solid Films, 45, 295 (1977)

[15] D E Bullard, D C Lynch and W G Davenport, Nonequillibrium plasma processing of ores, In: Kaddah, El., (Ed.) Thermal Plasma Applications in Materials and Metallurgical Processing, pp.175-191 (1992)

[16] P Ctibor, K Neufuss, F Zahalka and B Kolman, Wear, 262, 1274 (2007)