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[[Image:Euclidean Voronoi diagram.svg|thumb|20 points and their Voronoi cells]]
The '''natural element method (NEM)'''<ref>{{cite journal|url=|title=The natural element method in solid mechanics|first1=N.|last1=Sukumar|first2=B.|last2=Moran|first3=T.|last3=Belytschko|date=21 June 1998|journal=International Journal for Numerical Methods in Engineering|volume=43|issue=5|pages=839–887|doi=10.1002/(SICI)1097-0207(19981115)43:5<839::AID-NME423>3.0.CO;2-R|bibcode=1998IJNME..43..839S}}</ref><ref>{{cite journal| title=A new extension of the natural element method for non‐convex and discontinuous problems: the constrained natural element method (C‐NEM)| author1=J. Yvonnet| author2=D. Ryckelynck| author3=P. Lorong| author4=F. Chinesta| publisher=International Journal for Numerical Methods in Engineering| pages=1451–1474}}</ref><ref>{{cite journal|url=https://www.researchgate.net/publication/332678382|title=Large deformation analysis of elastic bodies by nonlinear Petrov–Galerkin natural element method | journal=Advances in Mechanical Engineering | date=April 2019}}</ref> is a [[meshless method]] to solve [[partial differential equation]], where the ''elements'' do not have a predefined shape as in the [[finite element method]], but depend on the geometry.<ref>{{Cite journal |title=Research on Natural Element Method and the application to simulate metal forming processes |
A [[Voronoi diagram]] partitioning the space is used to create each of these elements.
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