Process Conditions and Microstructures of Ceramic Coatings by Gas Phase Deposition Based on Plasma Spraying

Plasma spraying at very low pressure (50-200 Pa) is significantly different from atmospheric plasma conditions (APS). By applying powder feedstock, it is possible to fragment the particles into very small clusters or even to evaporate the material. As a consequence, the deposition mechanisms and the resulting coating microstructures could be quite different compared to conventional APS liquid splat deposition. Thin and dense ceramic coatings as well as columnar-structured strain-tolerant coatings with low thermal conductivity can be achieved offering new possibilities for application in energy systems. To exploit the potential of such a gas phase deposition from plasma spray-based processes, the deposition mechanisms and their dependency on process conditions must be better understood. Thus, plasma conditions were investigated by optical emission spectroscopy. Coating experiments were performed, partially at extreme conditions. Based on the observed microstructures, a phenomenological model is developed to identify basic growth mechanisms.

[1]  A. Atkinson,et al.  Microstructure evolution in thin zirconia films: Experimental observation and modelling , 2011 .

[2]  Georg Mauer,et al.  Plasma and Particle Temperature Measurements in Thermal Spray: Approaches and Applications , 2011 .

[3]  Robert Vassen,et al.  Application of Suspension Plasma Spraying (SPS) for Manufacture of Ceramic Coatings , 2008 .

[4]  Ch. Hollenstein,et al.  Modelling and Diagnostics of a Supersonic DC Plasma Jet Expanding at Low Pressure , 2002, International Thermal Spray Conference.

[5]  John A. Thornton,et al.  Influence of substrate temperature and deposition rate on structure of thick sputtered Cu coatings , 1975 .

[6]  D. Stöver,et al.  Thin and Dense Ceramic Coatings by Plasma Spraying at Very Low Pressure , 2009, International Thermal Spray Conference.

[7]  P. Mcmurry,et al.  Hypersonic plasma particle deposition—A hybrid between plasma spraying and vapor deposition , 2006, International Thermal Spray Conference.

[8]  Malko Gindrat,et al.  Vapor Phase Deposition Using Plasma Spray-PVD™ , 2010 .

[9]  K. Reichelt,et al.  Nucleation and growth of thin films , 1988 .

[10]  J. Venables,et al.  Nucleation and growth of thin films , 1984 .

[11]  John A. Thornton,et al.  Influence of apparatus geometry and deposition conditions on the structure and topography of thick sputtered coatings , 1974 .

[12]  Konstantin von Niessen,et al.  Plasma Spray-PVD: A New Thermal Spray Process to Deposit Out of the Vapor Phase , 2011 .

[13]  Russell Messier,et al.  Revised structure zone model for thin film physical structure , 1984 .

[14]  H. Liao,et al.  Very low pressure plasma sprayed alumina and yttria-stabilized zirconia thin dense coatings using a modified transferred arc plasma torch , 2011 .

[15]  R. Kužel,et al.  Ion-assisted sputtering of TiN films , 1990 .

[16]  J. Thornton High Rate Thick Film Growth , 1977 .

[17]  B. Movchan,et al.  STRUCTURE AND PROPERTIES OF THICK CONDENSATES OF NICKEL, TITANIUM, TUNGSTEN, ALUMINUM OXIDES, AND ZIRCONIUM DIOXIDE IN VACUUM. , 1969 .

[18]  M. Krane,et al.  Column Formation in Suspension Plasma-Sprayed Coatings and Resultant Thermal Properties , 2011 .

[19]  P. Fauchais,et al.  Two-temperature transport coefficients in argon–helium thermal plasmas , 2004 .