Abstract
We consider the rapid solidification of a molten YSZ particle, by solving the so-called hyperbolic equations for heat and mass transfer. The hyperbolic model predicts the interface undercooling (due to thermal and solutal effects) and velocity as a function of time, as well as the yttria redistribution within the solid phase. Results are then compared to corresponding ones that we obtained from a parabolic model, to assess the extent to which YSZ solidification is influenced by nonequilibrium effects. Results indicate that these effects are limited to the early part of the solidification process when undercooling is most significant. At this stage, the interface velocity is unsteady, and solute redistribution is most evident. As solidification decelerates, the nonequilibrium effects wane and solidification can then be properly modeled as an equilibrium process.
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig1_HTML.jpg)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig2_HTML.gif)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig3_HTML.gif)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig4_HTML.gif)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig5_HTML.gif)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig6_HTML.gif)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig7_HTML.gif)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig8_HTML.gif)
![](http://media.springernature.com/m312/springer-static/image/art%3A10.1007%2Fs11666-008-9238-5/MediaObjects/11666_2008_9238_Fig9_HTML.gif)
Similar content being viewed by others
Abbreviations
- C :
-
concentration (wt.%)
- C 0 :
-
initial concentration (wt.%)
- C p :
-
specific heat capacity (J kg−1 K−1)
- b :
-
splat thickness (m)
- D :
-
mass diffusivity (m2 s−1)
- h :
-
heat transfer coefficient (W m−2 K−1)
- J C :
-
concentration flux (wt.% m s−1)
- k f :
-
nonequilibrium partition coefficient
- k e :
-
equilibrium partition coefficient
- m :
-
slope of nonequilibrium liquidus (K wt.%−1)
- m e :
-
slope of equilibrium liquidus (K wt.%−1)
- Q :
-
latent heat of solidification (J kg−1)
- T :
-
temperature (K)
- T m :
-
equilibrium melting temperature (K)
- T 0 :
-
initial temperature (K)
- V D :
-
mass diffusion velocity (m s−1)
- V i :
-
interface velocity (m s−1)
- α:
-
thermal diffusivity (m2 s−1)
- κ:
-
thermal conductivity (W m−1 K−1)
- μ:
-
linear kinetics coefficient (m s−1 K−1)
- ρ:
-
density (kg m−3)
- τ:
-
relaxation time (s)
- i:
-
interface
- j:
-
solid or liquid phase
- −:
-
liquid interface
- + :
-
solid interface
References
Chae Y.K., Mostaghimi J., Yoshida T. (2000) Deformation and Solidification Process of a Super-cooled Droplet Impacting on the Substrate Under Plasma Spraying Conditions. Sci. Technol. Adv. Mat. 1:147-156
Wang G.-X., Goswami R., Sampath S., Prasad V. (2004) Understanding the Heat Transfer and Solidification of Plasma-sprayed Yttria-partially Stabilized Zirconia Coatings. Mater. Manuf. Process. 19:259-272
Streibl T., Vaidya A., Friis M., Srinivasan V., Sampath S. (2006) A critical assessment of particle temperature distributions during plasma spraying: Experimental results for YSZ. Plasma Chem. Plasma P. 26:53-72
Clarke D.R., Levi C.G. (2003) Materials design for the next generation thermal barrier coatings. Annu. Rev. Mater. Res. 33:383-417
H. Liu, M. Bussmann, and J. Mostaghimi, A Comparison of Hyperbolic and Parabolic Models of Phase Change of a Pure Metal, in press, Int. J. Heat Mass Tran., 2008. doi:10.1016/j.ijheatmasstransfer.2008.08.030
Mullis A.M. (1997) Rapid solidification within the framework of a hyperbolic conduction model. Int. J. Heat Mass Tran. 40:4085-4094
Sobolev S.L. (1997) Rapid solidification under local nonequilibrium conditions. Phys. Rev. 55:6845-6854
P.K. Galenko and D.A. Danilov, Linear Morphological Stability Analysis of the Solid-Liquid Interface in Rapid Solidification of a Binary System, J. Phys. Rev. E, 2004, 69, p 051608, 1-13
Galenko P.K., Danilov D.A. (1997) Local nonequilibrium effect on rapid dendritic growth in a binary alloy melt. Phys. Lett. A 235:271-280
L. Bianchi, F. Blein, P. Lucchese, M. Vardelle, A. Vardelle, and P. Fuchais, Effect of Particle Velocity and Substrate Temperature on Alumina and Zirconia Splat Formation, Thermal Spray Industrial Applications, C. Berndt and S. Sampath, Ed., (Materials Park, OH), ASM International, 1994, p 569-574
M. Fukomoto, Y. Huang, and M. Ohwatari, Flattening Mechanism in Thermal Sprayed Particle Impinging on Flat Substrate, Thermal Spray Meeting the Challenges of the 21st Century, C. Coddet, Ed., (Materials Park, OH), ASM International, 1998, p 401-406
Pasandideh-Fard M., Pershin V., Chandra S., Mostaghimi J. (2002) Splat shapes in a thermal spray coating process: simulations and experiments. J. Therm. Spray Techn. 11:206-217
Kurz W., Fisher D.J. (1998) Fundamentals of solidification, 4th Ed. Trans Tech Publications, Aedermannsdorf, pp. 63-89
Wang G.-X., Matthys E.F. (1996) Modeling of nonequilibrium surface melting and resolidification for pure metals and binary alloys. J. Heat Transf. 118:944-951
C. Li, J. Li, and W. Wong, The Effect of Substrate Preheating and Surface Organic Covering on Splat Formation, Thermal Spray Meeting the Challenges of the 21st Century, C. Coddet, Ed., (Materials Park, OH), ASM International, 1998, p 473-480
J. Pech, B. Hannoyer, A. Denoirjean, and P. Fauchais, Influence of Substrate Preheating Monitoring on Alumina Splat Formation in DC Plasma Process, Thermal Spray Surface Engineering via Applied Research, C. Berndt, Ed., (Materials Park, OH), ASM International, 2000, p 759-765
Salimi Jazi H.R., Mostaghimi J., Coyle T., Chandra S., Lau C.Y., Rosenzweig L., Moran E. (2007) Effect of droplet characteristics and substrate surface topography on the final morphology of plasma sprayed zirconia single splat. J. Therm. Spray Techn 16:291-299
Aziz M.J., Kaplan T. (1998) Continuous growth model for interface motion during alloy solidification. Acta Metall. 36:2335-2347
Aziz M.J., Boettinger W.J. (1994) On the transition from short-range diffusion-limited to collision-limited growth in alloy solidification. Acta Metall. Mater. 42:527-537
Cattaneo C. (1948) Sulla conduzione del calore. Atti Sem. Mat. Fis. Univ. Modena 3:83-101
Galenko P.K., Danilov D.A. (1999) Model for free dendritic alloy growth under interfacial and bulk phase nonequilibrium conditions. J. Cryst. Growth 197:992-1002
Xiong H.-B., Zheng L.-L., Streibl T.A. (2006) Critical assessment of particle temperature distributions during plasma spraying: Numerical studies for YSZ. Plasma Chem. Plasma P 26:53-72
Author information
Authors and Affiliations
Corresponding author
Additional information
This article is an invited paper selected from presentations at the 2008 International Thermal Spray Conference and has been expanded from the original presentation. It is simultaneously published in Thermal Spray Crossing Borders, Proceedings of the 2008 International Thermal Spray Conference, Maastricht, The Netherlands, June 2-4, 2008, Basil R. Marple, Margaret M. Hyland, Yuk-Chiu Lau, Chang-Jiu Li, Rogerio S. Lima, and Ghislain Montavon, Ed., ASM International, Materials Park, OH, 2008.
Rights and permissions
About this article
Cite this article
Liu, H., Bussmann, M. & Mostaghimi, J. The Effect of Undercooling on Solidification of YSZ Splats. J Therm Spray Tech 17, 646–654 (2008). https://doi.org/10.1007/s11666-008-9238-5
Received:
Revised:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s11666-008-9238-5