TY - JOUR
T1 - Goal-oriented adaptivity using unconventional error representations for the 1D Helmholtz equation
AU - Darrigrand, Vincent
AU - Pardo, David
AU - Muga, Ignacio
N1 - Publisher Copyright:
© 2015 Elsevier Ltd.
PY - 2015/5/1
Y1 - 2015/5/1
N2 - In this work, the error of a given output functional is represented using bilinear forms that are different from those given by the adjoint problem. These representations can be employed to design novel h, p, and hp energy-norm and goal-oriented adaptive algorithms. Numerical results in 1D show that, for wave propagation problems, the advantages of this new representation are notorious when selecting the Laplace equation as the dual problem. Specifically, the computed upper bounds of the new error representation are sharper than the classical ones used in both energy-norm and goal-oriented adaptive methods, especially when the dispersion (pollution) error is significant.
AB - In this work, the error of a given output functional is represented using bilinear forms that are different from those given by the adjoint problem. These representations can be employed to design novel h, p, and hp energy-norm and goal-oriented adaptive algorithms. Numerical results in 1D show that, for wave propagation problems, the advantages of this new representation are notorious when selecting the Laplace equation as the dual problem. Specifically, the computed upper bounds of the new error representation are sharper than the classical ones used in both energy-norm and goal-oriented adaptive methods, especially when the dispersion (pollution) error is significant.
KW - Error representation
KW - Finite element methods
KW - Goal-oriented adaptivity
KW - Helmholtz equation
UR - http://www.scopus.com/inward/record.url?scp=84926421679&partnerID=8YFLogxK
U2 - 10.1016/j.camwa.2015.03.006
DO - 10.1016/j.camwa.2015.03.006
M3 - Article
AN - SCOPUS:84926421679
SN - 0898-1221
VL - 69
SP - 964
EP - 979
JO - Computers and Mathematics with Applications
JF - Computers and Mathematics with Applications
IS - 9
ER -