Local maximum‐entropy approximation schemes: a seamless bridge between finite elements and meshfree methods
By Marino Arroyo, Magdalena Ortiz. 2006
410 citations recorded by the source corpus.
Subfields: Geophysics, Management, Monitoring, Policy and Law, Mechanics of Materials
View Paper: https://www.semanticscholar.org/paper/b4d678051473d4e99837d11ff813072f034c5f5b
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Geophysics
- Natarajan Sukumar
- Jiun-Shyan Chen
- Timon Rabczuk
- Daniel Millán
- Stéphane P.A. Bordas
- Marino Arroyo
- Hector Gomez
- Thomas Rüberg
In Management, Monitoring, Policy and Law
- Natarajan Sukumar
- Jiun-Shyan Chen
- Timon Rabczuk
- Daniel Millán
- Stéphane P.A. Bordas
- Marino Arroyo
- Hector Gomez
- Thomas Rüberg
In Mechanics of Materials
- Stéphane P.A. Bordas
- Hung Nguyen-Xuan
- Timon Rabczuk
- Trung Nguyen-Thoi
- Guirong Liu
- Sundararajan Natarajan
- Jiun-Shyan Chen
- Natarajan Sukumar
Citations in the corpus
- Free vibration analysis of functionally graded carbon nanotube-reinforced composite plates using the element-free kp-Ritz method in thermal environment (2013, background): “Arroyo and Ortiz [30] reported local maximumentropy approximation schemes which can be considered as a convenient basis for the numerical solution of partial differential equations in the style of mesh-free Galerkin methods.”
- Some basic formulations of the virtual element method (VEM) for finite deformations (2017, background): “, concave ones), harmonic shape functions [15, 16, 17] and max-entropy shape functions [18, 19, 20] need to be computed numerically at the quadrature points element by element.”
- Phase-field modeling of fracture in linear thin shells (2014, positive): “As it was discussed in [39], the locality of the LME basis functions smoothness depends on a nondimensional parameter γ.”
- Isogeometric analysis: An overview and computer implementation aspects (2012, neutral): “approximations [125].”
- Exact imposition of boundary conditions with distance functions in physics-informed deep neural networks (2021, methodology): “A related approach is the local maximum-entropy (max-ent) meshfree method [48] that yield compactly-supported basis functions of exponential form that constitute a partition-ofunity [49], possess linear completeness, and provide a smooth transition from Delaunay basis functions [50] to global maximu”
- Topology optimization using polytopes (2013, background): “, φn are a set of barycentric coordinates, for instance [4,7,12,15,16], which satisfy all the desired properties of a conforming interpolants such as partition of unity, Kronecker-delta, linear completeness and piecewise linear (C0 function) along the edges of e.”
- New perspectives on polygonal and polyhedral finite element methods (2014, methodology): “The dual problem (unconstrained convex minimization) is efficiently solved using Newton’s method [40, 76, 21].”
- Phase‐field modeling and simulation of fracture in brittle materials with strongly anisotropic surface energy (2015, methodology): “We resort here to LME approximants [28], a meshfree method with non-negative and smooth basis functions.”
- A generalized approximation for the meshfree analysis of solids (2011, methodology): “However, it is difficult to extend this method to higher order approximations since the first k moments of arbitrary fixed points do not belong to the moment space given by the convex hull of the nodal points [27, 31].”
- Quadratic maximum-entropy serendipity shape functions for arbitrary planar polygons (2013, methodology): “For a Gaussian nodal prior weight function, the implicit function theorem is invoked to prove the smoothness of non-negative [37] and signed shape functions [1].”
- Optimal transportation meshfree approximation schemes for fluid and plastic flows (2010, methodology): “[38, 39] and references therein) and the shape functions can then be reconstructed from the rearranged nodal sets [27].”
- Smooth, second order, non‐negative meshfree approximants selected by maximum entropy (2009, methodology): “In [1], some properties of the so-called convex approximants (non-negative and reproducing exactly affine functions) were identified.”
- Meshless methods: A review and computer implementation aspects (2008, methodology): “The recent inception of the smoothed finite element method (SFEM) [108,110–112,125,126], regained interest in polygonal interpolation [127] and, in particular, the recent discovery of maximum entropy approximations [123,124] may help bringing some more flexibility to the XFEM.”
- Meshfree Methods: Progress Made after 20 Years (2017, positive): “Convex approximations for meshfree computation based on the principle of maximum entropy (MaxEnt) (Jaynes 1957) to achieve unbiased statistical in fl uence of nodal data have been proposed for the Galerkin solution of PDEs (Arroyo and Ortiz 2006; Sukumar 2004).”