Current Trends and Open Problems in Computational Mechanics 2022
DOI: 10.1007/978-3-030-87312-7_19
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Locking-Free Mixed Finite Element Methods and Their Spurious Hourglassing Patterns

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Cited by 2 publications
(6 citation statements)
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“…Furthermore, the too soft bending behavior of H1/P0E6T (see Section 5.2) is resembled by the comparably soft behavior (low eigenvalue) of mode 7. The 3D results described for H1/P0E6T and H1U/F12 are inline with the observation by Hille et al 59 for the elasto-plastic material. Both elements show hourglassing in such simulations.…”
Section: F I G U R E 13supporting
confidence: 90%
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“…Furthermore, the too soft bending behavior of H1/P0E6T (see Section 5.2) is resembled by the comparably soft behavior (low eigenvalue) of mode 7. The 3D results described for H1/P0E6T and H1U/F12 are inline with the observation by Hille et al 59 for the elasto-plastic material. Both elements show hourglassing in such simulations.…”
Section: F I G U R E 13supporting
confidence: 90%
“…The element is implemented as described by Pfefferkorn and Betsch 16 and closely related to the improved EAS version by Simo et al 5 H1/P0 (Q1/P0): Mixed pressure element by Simo et al 80 based on a Hu–Washizu functional with elementwise constant pressure field. H1/P0E6T (Q1/P0E2T): Combination of H1/P0 and H1/E9T which was proposed by Armero 54 for 2D plane strain problems (Q1/P0E2T). A 3D extension (H1/P0E6T) has recently been proposed by Hille et al 59 H1/S18 (Q1/S5): Assumed stress element as proposed by Pian and Sumihara 74 and Pian and Tong 86 for linear elasticity in 2D and 3D, respectively. An extension to nonlinear problems can, for example, be found in the work of Viebahn et al 29 However, we use the inverse stress strain relation for a Neo‐Hookean material model proposed by Pfefferkorn et al 19 instead of the numeric procedure in aforementioned reference.…”
Section: Numerical Investigationsmentioning
confidence: 99%
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