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![Page 1: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/1.jpg)
Multiscale Models for Microstructure Evolution
and Response
R. B. HaberCenter for Process Simulation and DesignUniversity of Illinois at Urbana–Champaign
ITR/AP DMR 01-21695
NSF Division of Materials ResearchITR Computational Materials
WorkshopJune 17-19, 2004 Urbana, IL
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Recent progress
Modeling Solidification Microstructures
Cryopreservation of biological materials
2D - 3D transition in directional solidification
Spacetime Discontinuous Galerkin Methods
Adaptive O(N) method for hyperbolic PDEsVisualization & parallel implementationFracture and dewetting under shock loading
Additional topicsShape and topology optimization of microstructurePhase field crystalsAtomistic / continuum coupling strategy
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Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
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Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
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Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
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cess
Sim
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![Page 5: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/5.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
r Pro
cess
Sim
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tion &
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![Page 6: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/6.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
r Pro
cess
Sim
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tion &
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![Page 7: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/7.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
r Pro
cess
Sim
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tion &
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![Page 8: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/8.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
r Pro
cess
Sim
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tion &
D
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QuickTime™ and aVideo decompressor
are needed to see this picture.
![Page 9: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/9.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
r Pro
cess
Sim
ula
tion &
D
esi
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QuickTime™ and aVideo decompressor
are needed to see this picture.
![Page 10: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/10.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
r Pro
cess
Sim
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![Page 11: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/11.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
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Sim
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![Page 12: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/12.jpg)
Modeling Solidification Microstructures
J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
Cente
r fo
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![Page 13: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/13.jpg)
Austenite-Martensite phase transition in shocked shape-memory alloys
Discontinuous fields play central roleshocks --- use SDG method for elastodynamicsphase boundary kinetics --- use SDG method for Hamilton–Jacobi equations
“Standard numerical methods, such as shock capturing schemes and finite element methods, cannot be applied directly to the sharp interface model. Undercompressive waves such as phase interfaces turn out to be very sensitive to numerical dissipation, regularization, mesh refinements, etc. …” – LeFloch
M A
time
SM AShock
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Spacetime discontinuous Galerkin finite element method
Distinguishing features of SDG method
discontinuous basis functionsspacetime interpolation time
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Tent PitcherAdaptive spacetime meshing
Given a space mesh, Tent Pitcher constructs a spacetime mesh such that the slope of every facet is bounded to satisfy causality
Patches (”tents”) of tetrahedra are created and solved one at a time to yield an O(N) method with rich parallel structure
Individual patches are refined by a newest vertex method on the space mesh to produce a nonconforming spacetime grid
tent–pitching sequence
newest-vertex refinement strategy
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Parallel Solution Strategy
Built on top of Finite Element Framework within the Charm++ parallel programming environment
Provides domain decomposition into “chunks”, transparent message passing, and dynamic load balancing
Chunks run Tent Pitcher in parallel; physics code “thinks” it is serial
Good scaling and processor utilization
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Pixel-Exact Rendering of Spacetime Data Sets
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High-Performance and Hi-Fidelity Rendering
Techniques
Programmable GPUs post-process physics data at pixel level
Heavily pipelined and 16 x parallel
Discontinuity anti-aliasing
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Crack-tip Wave Scattering Example
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Crack-tip Wave Scattering Example
QuickTime™ and aMPEG-4 Video decompressor
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Crack-tip Wave Scattering Example
QuickTime™ and aMPEG-4 Video decompressor
are needed to see this picture.
![Page 22: Multiscale Models for Microstructure Evolution and Response R. B. Haber Center for Process Simulation and Design University of Illinois at Urbana– Champaign.](https://reader035.fdocuments.in/reader035/viewer/2022062511/551c1e7b5503469e4f8b59fd/html5/thumbnails/22.jpg)
Crack Propagation Examplewith Cohesive Interface
QuickTime™ and aMPEG-4 Video decompressor
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Shock Scattering by Stiff Circular Inclusions in a
Composite Material
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Particle Dewetting in a Shocked Composite
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Continuing Work on SDG Methods
Code optimizations, combine parallel and adaptive (near term)
Inclined tent poles to track moving interfaces (and shocks?)
Extend SDG method to three dimensions
Combine elastodynamics with conservation laws solver to address shocked SMAs
Model dislocation density evolution in thin films (new proposal with Acharya et al.)
Applications to Schrödinger equation
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Shape and Topology Optimization of Material Microstructures M. Bendsøe, R. Haber, J. Norato and D. Tortorelli
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Phase Field Crystals J. Dantzig, B. Athreya, A. Chang, L. Kale and K. Wang
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Atomistic / Continuum Coupling in Spacetime R. Haber, D.Johnson, B. Kraczek, C. Xia
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Thanks to CPSD/MCC team
CS: Jeff Erickson, Michael Garland, Laxmikant Kale, Damrong Guoy, Shuo-Heng Chung, Shripad Thite, Yuan Zhou, Mark Hills, K. Wang
T&AM: Reza Abedi, Morgan Hawker, Yong Fan, Jayandran Palaniappan, Chunguang Xia
Math: Katarina Jegdic, Bob Jerrard, Boris Petracovici, John Sullivan
M&IE: Jon Dantzig, Dan Tortorelli, Julian Norato, B. Athreya, A. Chang
MatSE/Physics: Duane Johnson, Brent Kraczek
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