Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p

Storn J (2024)
Journal of Scientific Computing 99(2): 35.

Zeitschriftenaufsatz | Veröffentlicht | Englisch
 
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Abstract / Bemerkung
**Abstract**

We introduce a numerical scheme that approximates solutions to linear PDE’s by minimizing a residual in the $$W^{-1,p'}(\Omega )$$ W - 1 , p ( Ω ) norm with exponents $$p> 2$$ p > 2 . The resulting problem is solved by regularized Kačanov iterations, allowing to compute the solution to the non-linear minimization problem even for large exponents $$p\gg 2$$ p 2 . Such large exponents remedy instabilities of finite element methods for problems like convection-dominated diffusion.

Erscheinungsjahr
2024
Zeitschriftentitel
Journal of Scientific Computing
Band
99
Ausgabe
2
Art.-Nr.
35
ISSN
0885-7474
eISSN
1573-7691
Page URI
https://pub.uni-bielefeld.de/record/3005506

Zitieren

Storn J. Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p. Journal of Scientific Computing. 2024;99(2): 35.
Storn, J. (2024). Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p. Journal of Scientific Computing, 99(2), 35. https://doi.org/10.1007/s10915-024-02494-5
Storn, Johannes. 2024. “Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p”. Journal of Scientific Computing 99 (2): 35.
Storn, J. (2024). Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p. Journal of Scientific Computing 99:35.
Storn, J., 2024. Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p. Journal of Scientific Computing, 99(2): 35.
J. Storn, “Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p”, Journal of Scientific Computing, vol. 99, 2024, : 35.
Storn, J.: Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p. Journal of Scientific Computing. 99, : 35 (2024).
Storn, Johannes. “Solving Minimal Residual Methods in $$W^{-1,p'}$$ with Large Exponents p”. Journal of Scientific Computing 99.2 (2024): 35.
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2025-07-23T09:30:51Z
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