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Meshless interface tracking for the simulation of dendrite envelope growth

Mitja Jančič, Miha Založnik, Gregor Kosec

TL;DR

This work presents Meshless Interface Tracking (MIT) as a sharp, moving-boundary alternative to Phase-Field Interface Capturing (PFIC) for the Grain Envelope Model (GEM) of dendritic solidification. MIT uses h-adaptive, meshless node distributions with RBF-FD discretizations and boundary-node envelopes to propagate the grain envelope directly, avoiding phase-field smoothing artefacts. The approach is validated in 2D, showing agreement with PFIC in principal results while achieving higher envelope-detail and reduced node counts near the front; it also demonstrates favorable computational scaling with envelope refinement. Overall, MIT offers high-accuracy, artifact-free front tracking for mesoscopic GEM simulations and provides a robust reference framework for validating PFIC-based approaches in dendritic growth and grain-interaction studies.

Abstract

The growth of dendritic grains during solidification is often modelled using the Grain Envelope Model (GEM), in which the envelope of the dendrite is an interface tracked by the Phase Field Interface Capturing (PFIC) method. In the PFIC method, an phase-field equation is solved on a fixed mesh to track the position of the envelope. While being versatile and robust, PFIC introduces certain numerical artefacts. In this work, we present an alternative approach for the solution of the GEM that employs a Meshless (sharp) Interface Tracking (MIT) formulation, which uses direct, artefact-free interface tracking. In the MIT, the envelope (interface) is defined as a moving domain boundary and the interface-tracking nodes are boundary nodes for the diffusion problem solved in the domain. To increase the accuracy of the method for the diffusion-controlled moving-boundary problem, an \h-adaptive spatial discretization is used, thus, the node spacing is refined in the vicinity of the envelope. MIT combines a parametric surface reconstruction, a mesh-free discretization of the parametric surfaces and the space enclosed by them, and a high-order approximation of the partial differential operators and of the solute concentration field using radial basis functions augmented with monomials. The proposed method is demonstrated on a two-dimensional \h-adaptive solution of the diffusive growth of dendrite and evaluated by comparing the results to the PFIC approach. It is shown that MIT can reproduce the results calculated with PFIC, that it is convergent and that it can capture more details in the envelope shape than PFIC with a similar spatial discretization.

Meshless interface tracking for the simulation of dendrite envelope growth

TL;DR

This work presents Meshless Interface Tracking (MIT) as a sharp, moving-boundary alternative to Phase-Field Interface Capturing (PFIC) for the Grain Envelope Model (GEM) of dendritic solidification. MIT uses h-adaptive, meshless node distributions with RBF-FD discretizations and boundary-node envelopes to propagate the grain envelope directly, avoiding phase-field smoothing artefacts. The approach is validated in 2D, showing agreement with PFIC in principal results while achieving higher envelope-detail and reduced node counts near the front; it also demonstrates favorable computational scaling with envelope refinement. Overall, MIT offers high-accuracy, artifact-free front tracking for mesoscopic GEM simulations and provides a robust reference framework for validating PFIC-based approaches in dendritic growth and grain-interaction studies.

Abstract

The growth of dendritic grains during solidification is often modelled using the Grain Envelope Model (GEM), in which the envelope of the dendrite is an interface tracked by the Phase Field Interface Capturing (PFIC) method. In the PFIC method, an phase-field equation is solved on a fixed mesh to track the position of the envelope. While being versatile and robust, PFIC introduces certain numerical artefacts. In this work, we present an alternative approach for the solution of the GEM that employs a Meshless (sharp) Interface Tracking (MIT) formulation, which uses direct, artefact-free interface tracking. In the MIT, the envelope (interface) is defined as a moving domain boundary and the interface-tracking nodes are boundary nodes for the diffusion problem solved in the domain. To increase the accuracy of the method for the diffusion-controlled moving-boundary problem, an \h-adaptive spatial discretization is used, thus, the node spacing is refined in the vicinity of the envelope. MIT combines a parametric surface reconstruction, a mesh-free discretization of the parametric surfaces and the space enclosed by them, and a high-order approximation of the partial differential operators and of the solute concentration field using radial basis functions augmented with monomials. The proposed method is demonstrated on a two-dimensional \h-adaptive solution of the diffusive growth of dendrite and evaluated by comparing the results to the PFIC approach. It is shown that MIT can reproduce the results calculated with PFIC, that it is convergent and that it can capture more details in the envelope shape than PFIC with a similar spatial discretization.
Paper Structure (19 sections, 16 equations, 18 figures, 1 table, 2 algorithms)

This paper contains 19 sections, 16 equations, 18 figures, 1 table, 2 algorithms.

Figures (18)

  • Figure 1: Schematic illustration of the main concepts of the GEM.
  • Figure 2: Example h-refined domain discretization. Additionally, example stencils on Dirichlet (green), Neumann (red) boundary and in the interior (blue) are shown.
  • Figure 4: Example of surface reconstruction accompanied with normal vectors computed from the reconstructed spline $\gamma$ of degree $k\in \left \{1, 2, 3,4\right \}$. For clarity, the encircled area is zoomed in and shown on the right. We also show the normal directions in the right figure.
  • Figure 5: Parametric domain used to evaluate the accuracy of surface reconstruction (left) and reconstruction quality analysis (right) in terms of maximum radius error (top right) and maximum normal angle error (bottom right).
  • Figure 6: Presentation of the isotropic growth case.
  • ...and 13 more figures