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PDEs on moving surfaces via the closest point method and a modified grid based particle method

Numerical Analysis · Submitted 1 Nov 2019

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Here we propose solving PDEs on moving surfaces using a combination of the CPM and a modification of the grid based particle method (Leung and Zhao, J. Comput.

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arXiv ID1911.00458 (version 1)
Pith IDLFVJO77M, Pith's permanent record of this paper and its review
CitationA. Petras, S.J. Ruuth. "PDEs on moving surfaces via the closest point method and a modified grid based particle method." arXiv:1911.00458 (2019). https://pith.science/paper/LFVJO77M
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What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.13 · human participants 0.02 · controlled comparison 0.04 · randomized assignment 0.01 · states quantitative result 0.07 · compares with prior results 0.27 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

Partial differential equations (PDEs) on surfaces arise in a wide range of applications. The closest point method (Ruuth and Merriman, J. Comput. Phys. 227(3):1943-1961, [2008]) is a recent embedding method that has been used to solve a variety of PDEs on smooth surfaces using a closest point representation of the surface and standard Cartesian grid methods in the embedding space. The original closest point method (CPM) was designed for problems posed on static surfaces, however the solution of PDEs on moving surfaces is of considerable interest as well. Here we propose solving PDEs on moving surfaces using a combination of the CPM and a modification of the grid based particle method (Leung and Zhao, J. Comput. Phys. 228(8):2993{3024, [2009]). The grid based particle method (GBPM) represents and tracks surfaces using meshless particles and an Eulerian reference grid. Our modification of the GBPM introduces a reconstruction step into the original method to ensure that all the grid points within a computational tube surrounding the surface are active. We present a number of examples to illustrate the numerical convergence properties of our combined method. Experiments for advection-diffusion equations that are strongly coupled to the velocity of the surface are also presented.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Partial differential equations (PDEs) on surfaces arise in a wide range of applications. background 1.00 0.04 0.02 asserted 1.00
s1 The closest point method (Ruuth and Merriman, J. Comput. background 0.92 0.04 0.02 unclear 0.64
s2 Phys. 227(3):1943-1961, [2008]) is a recent embedding method that has been used to solve a variety of PDEs on smooth surfaces using a closest point representation of the surface and standard Cartesian grid methods in the embedding space. background 1.00 0.04 0.04 asserted 1.00
s3 The original closest point method (CPM) was designed for problems posed on static surfaces, however the solution of PDEs on moving surfaces is of considerable interest as well. gap 0.81 0.06 0.05 asserted 1.00
s4 Here we propose solving PDEs on moving surfaces using a combination of the CPM and a modification of the grid based particle method (Leung and Zhao, J. Comput. contribution 0.91 0.79 0.38 asserted 0.95
s5 Phys. 228(8):2993{3024, [2009]). background 0.53 0.06 0.04 unclear 0.77
s6 The grid based particle method (GBPM) represents and tracks surfaces using meshless particles and an Eulerian reference grid. background 0.64 0.07 0.03 asserted 1.00
s7 Our modification of the GBPM introduces a reconstruction step into the original method to ensure that all the grid points within a computational tube surrounding the surface are active. method 0.64 0.93 0.12 asserted 1.00
s8 We present a number of examples to illustrate the numerical convergence properties of our combined method. contribution 0.66 0.93 0.14 asserted 0.96
s9 Experiments for advection-diffusion equations that are strongly coupled to the velocity of the surface are also presented. contribution 0.62 0.91 0.07 asserted 0.97

What kind of paper the classifier reports this is: method or tool 1.00 · evidence from simulation or computation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

Partial differential equations (PDEs) on surfaces arise in a wide range of applications. The closest point method (Ruuth and Merriman, J. Comput. Phys. 227(3):1943-1961, [2008]) is a recent embedding method that has been used to solve a variety of PDEs on smooth surfaces using a closest point representation of the surface and standard Cartesian grid methods in the embedding space. The original closest point method (CPM) was designed for problems posed on static surfaces, however the solution of PDEs on moving surfaces is of considerable interest as well. Here we propose solving PDEs on moving surfaces using a combination of the CPM and a modification of the grid based particle method (Leung and Zhao, J. Comput. Phys. 228(8):2993{3024, [2009]). The grid based particle method (GBPM) represents and tracks surfaces using meshless particles and an Eulerian reference grid. Our modification of the GBPM introduces a reconstruction step into the original method to ensure that all the grid points within a computational tube surrounding the surface are active. We present a number of examples to illustrate the numerical convergence properties of our combined method. Experiments for advection-diffusion equations that are strongly coupled to the velocity of the surface are also presented.

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