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Due to the temperature difference at the interface of the bubble and surrounding fluid, Marangoni convection causes fluid flow during solidification. Most of previous works on simulation of bubble-dendrite interactions ignore the Marangoni effect while it can have a significant effect especially in microgravity conditions where natural convection is absent. The Pore Formation and Mobility Investigation (PFMI) experiments at International Space Station (ISS) have shown that pores and bubbles adhered to the ampoule walls can change the morphology of dendrites and affect the growth kinetics. We used our numerical models to simulate the Marangoni effect and bubble-dendrite interactions during solidification of binary alloys. Effect of Marangoni convection on dendrite growth and bubble-dendrite interactions under microgravity and terrestrial conditions were studied.
A Phase Filed (PF)-Lattice Boltzmann (LB) model was developed to simulate in bubble-dendrite interactions. Using the developed model, interaction of growing dendrites with a big bubble attached to a wall was simulated. The bubble diameter was about two times as big as the primary dendrite arm spacing, similar to what is observed in PFMI-15 experiment. The simulation considered Marangoni convection in the absence of gravity. The results showed that the dendrite branch in vicinity of the bubble grow slower compared to the dendrites far from the bubble. Also side branching is enhanced in the vicinity of the bubble.
Two dimensional (2D) models are usually unable to capture all features of microstructures that are determinative in many materials properties, especially when fluid flow is involved. It is known that melt flow can significantly alter the growth kinetics by affecting solutal gradient around the dendrites, and moving the bubbles. While melt convection is blocked by dendrite arms in 2D simulations, flow can go around the 3D arms which results in a different bubble distribution and dendritic morphology. Studies have shown that the growth of dendrites in 3D is considerably different from 2D. Therefore, in order to obtain correct physical results, it is necessary to perform the simulations in 3D.
The thermocapillary flow field associated with a bubble in PFMI-15 experiment was investigated. The flow path was tracked by following miniature detached dendrite branches that made circular routes from the interface, through the bulk liquid, and back, and showed that a flow field which extended 4.5 mm into the melt had average velocity of ~0.1 mm/s and another one that extended 2.5 mm averaged ~0.4 mm/s. We followed similar tracer dendrite branches as they enter from the melt into the mushy-zone and after traversing certain distance in the mush come back out into the melt. This observation showed that the flow speed in the mushy region is higher than that in the bulk melt, which was puzzling and was considered for our numerical simulations. Another interesting observation from the PFMI videos was that the tracer dendrite branches invariably accelerated as they approached the solid/liquid (S/L) interface.
We performed large-scale three-dimensional (3D) simulations of dendrite growth using our LB code and generates the geometries of the dendrites. Then, the results were imported into COMSOL (commercial Finite Element Analysis software) to study the effect of Marangoni convection and formation of flow streams in the presence of bubble. Our simulation results show that, in the presence of the bubble, convection near the S/L interface is stronger and the maximum flow velocity is observed near the bubble/liquid interface. The same trends can be seen in PFMI videos as well. The tracer dendrite branches slow down as they distance from the interface and accelerate on their return. The results also showed that the velocity magnitude is larger in front of the bubble in the case when only Marangoni convection is responsible for convection (micro-gravity conditions). We also performed simulations for terrestrial conditions in which free convection due to gravity was the main factor controlling the flow velocity, while Marangoni effect was not significant.
The fluid velocities simulated in COMSOL were imported back to our 3D LBM model for dendritic growth to investigate the effect of induced Marangoni convection on the morphology of dendrites. We observed that the induced Marangoni convection changes the temperature field. The temperature profile was not linear ahead of dendrite tip; the melt near the bubble had a higher temperature. The Marangoni convection is responsible for the relatively higher temperature near the bubble. Also, the growth rate decreases in the dendrites closer to the bubble.
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Abstracts for Journals and Proceedings
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Lenart R, Eshraghi M, Felicelli SD. "Modeling Dendritic Solidification in Microgravity and Terrestrial Conditions." TMS 2018. 147th Annual Meeting,The Minerals, Metals and Materials Society, Phoenix, AZ, March 11-15, 2018. TMS 2018. 147th Annual Meeting, The Minerals, Metals and Materials Society, Phoenix, AZ, March 11-15, 2018. http://www.programmaster.org/PM/PM.nsf/ApprovedAbstracts/2227C45F068F04B58525814F0069B533?OpenDocument ; accesed 9/12/18. , Mar-2018
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Abstracts for Journals and Proceedings
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Dorari E, Eshraghi M, Felicelli SD. "A Lattice Boltzmann Model with Multiple Grids and Time Steps for Dendritic Solidification." TMS 2018. 147th Annual Meeting,The Minerals, Metals and Materials Society, Phoenix, AZ, March 11-15, 2018. TMS 2018. 147th Annual Meeting,The Minerals, Metals and Materials Society, Phoenix, AZ, March 11-15, 2018. http://www.programmaster.org/PM/PM.nsf/ApprovedAbstracts/7B273D2B32519A748525814D007BBB36?OpenDocument ; accessed 9/12/18. , Mar-2018
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Abstracts for Journals and Proceedings
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Dorari E, Eshraghi M, Felicelli SD. "Simulation of Dendritic Solidification Using Multiple-Grid Lattice Boltzmann Model." Presentation at ASME 2017 International Mechanical Engineering Congress and Exposition, Tampa, Florida, November 3–9, 2017. ASME 2017 International Mechanical Engineering Congress and Exposition, Tampa, Florida, November 3–9, 2017. , Nov-2017
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Abstracts for Journals and Proceedings
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Nabavizadeh SA, Eshraghi M, Felicelli SD, Tewari SN. "Marangoni Effects on Bubble-Dendrite Interactions Under Microgravity and Terrestrial Conditions." 33rd Annual Meeting of the American Society for Gravitational and Space Research, Seattle, WA, October 25-28, 2017. 33rd Annual Meeting of the American Society for Gravitational and Space Research, Seattle, WA, October 25-28, 2017. , Oct-2017
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Abstracts for Journals and Proceedings
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Nabavizadeh SA, Eshraghi M, Felicelli SD. "A Phase-Field Lattice Boltzmann Model for Bubble-Dendrite Interaction During Solidification of Binary Alloys." TMS 2018. 147th Annual Meeting, The Minerals, Metals and Materials Society, Phoenix, AZ, March 11-15, 2018. TMS 2018. 147th Annual Meeting, The Minerals, Metals and Materials Society, Phoenix, AZ, March 11-15, 2018. http://www.programmaster.org/PM/PM.nsf/ApprovedAbstracts/9F686A7810F5FFBF8525814F000C07A4?OpenDocument ; accessed 9/12/18. , Mar-2018
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Articles in Peer-reviewed Journals
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Dorari E, Eshraghi M, Felicelli SD. "A multiple-grid-time-step lattice Boltzmann method for transport phenomena with dissimilar time scales: Application in dendritic solidification." Applied Mathematical Modelling. 2018 Oct;62:580-94. https://doi.org/10.1016/j.apm.2018.06.023 , Oct-2018
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Dissertations and Theses
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Upadhyay SR. (Supriya R. Upadhyay) "Spurious Grain Formation during Directional Solidification in Microgravity." Master’s Thesis, Cleveland State University, May 2018. , May-2018
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Papers from Meeting Proceedings
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Nabavizadeh SA, Eshraghi M, Felicelli SD. "Feasibility Study of Different Pseudopotential Multiphase Lattice Boltzmann Methods for Dendritic Solidification." ASME 2017 International Mechanical Engineering Congress and Exposition, Tampa, Florida, November 3–9, 2017. In: ASME 2017 International Mechanical Engineering Congress and Exposition. Volume 14: Emerging Technologies; Materials: Genetics to Structures; Safety Engineering and Risk Analysis, Tampa, Florida, USA, November 3–9, 2017. Paper No. IMECE2017-71019, V014T11A033; 7 pages. https://doi.org/10.1115/IMECE2017-71019 , Nov-2017
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