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Phase Field Modeling of the Tetragonal-to-Monoclinic Phase Transformation in Zirconia Matthew Trappett 1, Morgan Diefendorf 2 Mahmood Mamivand 2 Mechanical and Biomedical Engineering 1Department of , Utah Valley University 2Department of Mechanical and Biomedical Engineering, Boise State University

Introduction Methods Results

The tetragonal to monoclinic phase transformation (T M) in • Phase Field Equations zirconia is an important contributor to the failure of nuclear MOOSE fuel rods used in nuclear power plants. A model of this • Material Properties process has been developed using a phase field method by Input File for Mamivand et al. Our goal is to apply this model using the • Energy Functions Processing MOOSE framework. MOOSE, multi-physics object oriented software environment, is a valuable tool for modeling T M because: Phase Field Method: • Automatic parallelization • Mathematical model used for moving boundary Figure 4: Zirconia • Finite Element Framework problems. Figure 5: Current TM using COMSOL. • Plug-n-physics modules • Minimizes and accounts for all the energies. results using MOOSE. • Free and open source • Ginzburg-Landau Kinetic Equation implemented into MOOSE kernels to define the phase field model: Figure 1. Zirconia Conclusion

cladding crack. ƞ , , 1, … MOOSE is capable of modeling T M in zirconia with ƞ , an approach more valuable than classical methods. This could provide important insight for development of rods for prevention of cracking.

Figure 2. TEM micrograph of Future Works partially transformed t-ZrO 2. • Continue fixing parameters in MOOSE to represent Objectives TM zirconia structure as shown in figure 2. • Run MOOSE code on the • Understand MOOSE framework and it’s phase field Figure 3. MOOSE code module. at Idaho utilizes coupled and implicit National Lab to generate multi-physics solvers to • Learn phase field method of martensitic T M in large quantities of data. calculate solutions which zirconia. • Apply and Figure 6. Falcon can be viewed using the AI to Supercomputing System • Implement the T M of zirconia into MOOSE. built in GUI, Peacock. accumulated data for located at INL. further elucidation.

[1] Mamivand, M., Zaeem, M. A., Kadiri, H. E., & Chen, L. (2013). Phase field modeling of the [3] Derek R. Gaston and Cody J. Permann and John W. Peterson and Andrew E. Slaughter and tetragonal-to-monoclinic phase transformation in zirconia. Acta Materialia,61(14), 5223-5235. David Andr and Yaqi Wang and Michael P. Short and Danielle M. Perez and Michael R. Tonks This work was supported by the National Science doi:10.1016/j.actamat.2013.05.015 and Javier Ortensi and Ling Zou and Richard C. Martineau. (2015). Physics-based multiscale Foundation via the REU Site: Materials for Society at [2] Brian Alger and David Andr and Robert W. Carlsen and Derek R. Gaston and Fande Kong and coupling for full core nuclear reactor , Annals of Nuclear Energy. Boise State University (DMR 1658076). Alexander D. Lindsay and Jason M. Miller and Cody J. Permann and John W. Peterson and Andrew [4] Mamivand, M., Zaeem, M., Kadiri, H. Phase Field Modeling of Tetragonal to Monoclinic E. Slaughter and Roy Stogner. (2019). MOOSE Web Page, https://mooseframework.org Transformation in Zirconia. Mississippi State University