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Effect of the Raw Material and Coating Process Conditions on the Densification of 8 wt% Y2O3-ZrO2 Thermal Barrier Coating by Atmospheric Plasma Spray 원문보기

한국세라믹학회지 = Journal of the Korean Ceramic Society, v.53 no.6, 2016년, pp.628 - 634  

Oh, Yoon-Suk (Engineering Ceramic Center, Korea Institute of Ceramic & Engineering Technology) ,  Kim, Seong-Won (Engineering Ceramic Center, Korea Institute of Ceramic & Engineering Technology) ,  Lee, Sung-Min (Engineering Ceramic Center, Korea Institute of Ceramic & Engineering Technology) ,  Kim, Hyung-Tae (Engineering Ceramic Center, Korea Institute of Ceramic & Engineering Technology) ,  Kim, Min-Sik (R&D Center, Sewon Hardfacing Co. LTD.) ,  Moon, Heung-Soo (R&D Center, Sewon Hardfacing Co. LTD.)

Abstract AI-Helper 아이콘AI-Helper

The 8 wt% yttria($Y_2O_3$) stabilized zirconia ($ZrO_2$), 8YSZ, a typical thermal barrier coating (TBC) for turbine systems, was fabricated under different starting powder conditions and coating parameters by atmospheric plasma spray (APS) coating process. Four different starti...

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제안 방법

  • 8YSZ granules were prepared by spray drying method, and size, shape of the granules were affirmed to vary with differences in the process variables for preparation of granules. Also, by utilizing as-received individual granules, coatings were prepared by atmospheric plasma spray method for consideration of the effects of granule conditions on the coating structures. In the case of donut-type granules, relatively denser structures were formed in comparison with the spherical granules, which was presumably due to a difference in the specific surface areas of splat in contact with the substrate.
  • For phase analysis of the granules prepared by spray drying and the coating specimens produced by atmospheric plasma spray method, the samples were analyzed by measuring diffraction peaks using an X-ray diffractometer (X-ray diffraction, Rigaku SmartLab, Rigaku, JAPAN) in the range of 2θ = 5 ~ 80° under the conditions of 40 kV, 200 mA and Cu-Kα radiation at the scanning speed of 2°/min. Also, for the granule powders and the coating samples, microstructures were observed using FESEM (Field Emission Scanning electron microscope, Jeol 7100F, JEOL, Japan) under the acceleration voltage conditions of 10 and 5 kV, respectively. In the case of coating samples, samples for observation of cross sections were produced by mounting in epoxy, drying for more than 12 h, polishing of side face to 100 µm with the use of diamond suspension, followed by cleaning in acetone for 20 minutes and drying in a dryer under the temperature condition higher than 80℃ for more than 12 h.
  • By mixing two types of raw materials, i.e. zirconia (ZrO2, particle diameter (D50): 0.3 µm, purity: 99.5%, Zhonglong Hightech Limited, China) powder and yttria (Y2O3, particle diameter (D50): 5 µm, purity: 99.999%, Feilong International Group Co., ltd, China) powder and using a spray dry method, granulated powder of 8wt% yttria stabilized zirconia (8YSZ) for atmospheric plasma spray was prepared.
  • By using a particle size analyzer (Beckman Coulter LS Particle Size Analyzer, LS 13 320), particle size analysis was conducted for the granulated powders prepared. For phase analysis of the granules prepared by spray drying and the coating specimens produced by atmospheric plasma spray method, the samples were analyzed by measuring diffraction peaks using an X-ray diffractometer (X-ray diffraction, Rigaku SmartLab, Rigaku, JAPAN) in the range of 2θ = 5 ~ 80° under the conditions of 40 kV, 200 mA and Cu-Kα radiation at the scanning speed of 2°/min.
  • For phase analysis of the granules prepared by spray drying and the coating specimens produced by atmospheric plasma spray method, the samples were analyzed by measuring diffraction peaks using an X-ray diffractometer (X-ray diffraction, Rigaku SmartLab, Rigaku, JAPAN) in the range of 2θ = 5 ~ 80° under the conditions of 40 kV, 200 mA and Cu-Kα radiation at the scanning speed of 2°/min.
  • 5. Representatively, coatings formed from two types of granules with different particle sizes were selected together with a coating prepared from a commercial spray powder product as comparison data for the comparative analysis. For all granule powders observed in the range of 2θ = 5 ~ 80°, similar diffraction patterns could be observed.
  • Also, among the process conditions for spray drying, the inlet temperature was maintained at about 180℃, and the outlet temperature at about 70 ~ 80℃, and the process conditions for size control of granules were secured by varying disc(atomizer) speed from 6000 to 12,000 rpm. To grant strength and to control the extent of densification for as-received granulated powders with different particle sizes and shapes, classification was made after heat treatment in air atmosphere at 1400℃/4 h and 1600℃/4 h, respectively. In Fig.

대상 데이터

  • Here, the mixing ratio for Ar:He gases was set to be 45/5 NLPM by volumetric ratio, and the powder feeding rate was maintained at 30 g/min. Detailed conditions for the top coating process are shown in Table 1. As the coating apparatus used for such atmospheric plasma spray, Triplex proTM 200 product of Oerlikon Metco Company (Switzerland) was employed. Process flow chart for the entire manufacturing of bond coating and top coating is shown in Fig.
  • As a material for bond coating, a commercial alloy material of Ni-Co-Cr-Al-Y composition (Amdry 386-2, particle diameter: 5 ~ 63 µm, Ni23-Co20Cr12.5Al0.5Y) was used.
  • At first, granules were prepared by the spray dry method after undergoing the primary and the secondary mixing processes using a ball mill. The spray dryer employed was domestically-produced DIE FCNM-026R (Dong Jin Spray Drying Technology) model. At this time, upon the secondary mixing process, shape of granules was controlled by varying feeding conditions for the binder (PVA, Polyvinyl alcohol) and the flocculant (NaOH).

이론/모형

  • As a comparison item with the prepared granules, reference coating samples were prepared by using commercial YSZ powder (204B-XCL, Sulzer Metco) and atmospheric plasma spray method. Prior to preparation of the coating samples, bond coating was formed by HVOF (High Velocity Oxyfuel deposition, JP5000, PRAXAIR, USA) method to increase adhesion to the 8YSZ top coating.
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참고문헌 (19)

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  2. T. A. Taylor, D. L. Appleby, A. E. Weatherill, and J. Griffiths, "Plasma-Sprayed Yttria-Sabilized Zirconia Coatings: Structure-Prpperty Relationships," Surf. Coat. Technol., 43 470-80 (1990). 

  3. S. Sampath, U. Schulz, M. O. Jarligo, and S. Kuroda, "Processing Science of Advanced Thermal-Barrier Systems," MRS Bull., 37 [10] 903-10 (2012). 

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  5. A. Vaidya, V. Srinivasan, T. Streibl, M. Friis, W. Chi, and S. Sampath, "Process Maps for Plasma Spraying of Yttria-Stabilized Zirconia: An Integrated Approach to Design, Optimization and Reliability," Mater. Sci. Eng. A, 497 239-53 (2008). 

  6. A. Kulkarni, A. Vaidya, A. Goland, S. Sampath, and H. Herman, "Processing Effects on Porosity-Property Correlations in Plasma Sprayed Yttria-Stabilized Zirconia Coatings," Mater. Sci. Eng. A, 359 100-11 (2003). 

  7. N. Curry, N. Markocsan, X. H. Li, A. Tricoire, and M. Dorfman, "Next Generation Thermal Barrier Coatings for the Gas Turbine Industry," J. Therm. Spray Technol., 20 [1-2] 108-15 (2011). 

  8. C. Kim, Y. S. Heo, T. W. Kim, and K. S. Lee, "Fabrication and Characterization of Zirconia Thermal Barrier Coatings by Spray Drying and Atmospheric Plasma Spraying," J. Korean Ceram. Soc., 50 [6] 326-32 (2013). 

  9. S. I. Jung, J. H. Kim, J. H. Lee, Y. G. Jung, U. G. Paik, and K. S. Lee, "Microstructure and Mechanical Properties of Zirconia-based Thermal Barrier Coatings with Starting Powder Morphology," Surf. Coat. Technol., 204 [6] 802-6 (2009). 

  10. P. Carpio, A. Borrell, M. D. Salvador, A. Gomez, E.Martinez, and E. Sanchez, "Microstructure and Mechanical Properties of Plasma Spraying Coatings from YSZ Feedstocks Comprising Nano- and Submicron-Sized Particles," Ceram. Int., 41 4108-17 (2015). 

  11. S. Mihm, T. Duda, H. Gruner, G. Thomas, and B. Dzur, "Method and Process Development of Advanced Atmospheric Plasma Spraying for Thermal Barrier Coatings," J. Therm. Spray Technol., 21 [3-4] 400-8 (2009). 

  12. Y. Tan, V. Srinivasan, T. Nakamura, S. Sampath, P. Bertrand, and G. Bertrand, "Optimizing Compliance and Thermal Conductivity of Plasma Sprayed Thermal Barrier Coatings via Controlled Powders and Processing Strategies," J. Therm. Spray Technol., 21 [5] 950-62 (2012). 

  13. F. Tang, L. Ajdelsztajn, G. E. Kimb, V. Provenzano, and J. M. Schoenung, "Effects of Variations in Coating Materials and Process Conditions on the Thermal Cycle Properties of NiCrAlY/YSZ Thermal Barrier Coatings," Mater. Sci. Eng. A, 425 94-106 (2006). 

  14. H. Guo, S. Kuroda, and H. Murakami, "Microstructures and Properties of Plasma-Sprayed Segmented Thermal Barrier Coatings," J. Am. Ceram. Soc., 89 [4] 1432-39 (2006). 

  15. J. Go, Y. G. Jung, S. Kim, and U. G. Paik, "Analysis of Thermoelastic Characteristics for Vertical-Cracked Thermal Barrier Coatings Through Mathematical Approaches," Surf. Coat. Technol., 206 1615-20 (2011). 

  16. Z. Lu, M. S. Kim, S. W. Myoung, J. H. Lee, Y. G. Jung, I. S. Kim, and C. Y. Jo, "Thermal Stability and Mechanical Properties of Thick Thermal Barrier Coatings with Vertical Type Cracks," Trans. Nonferrous Met. Soc. China, 24 s29-35 (2014). 

  17. M. Karger, R. Vassen, and D. Stover, "Atmospheric Plasma Sprayed Thermal Barrier Coatings with High Segmentation Crack Densities: Spraying Process, Microstructure and Thermal Cycling Behavior," Surf. Coat. Technol., 206 16-23 (2011). 

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  19. W. J. Lee, Y. S. Oh, S. M. Lee, H. T. Kim, D. S.Lim, and S. W. Kim, "Fabrication and Characterization of 7.5 wt% $Y_2O_3-ZrO_2$ Thermal Barrier Coatings Deposited by Suspension Plasma Spray," J. Korean Ceram. Soc., 51 [6] 598-604 (2014). 

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