Computing zero-group-velocity points in anisotropic elastic waveguides: Globally and locally convergent methods
Daniel A. Kiefer (1), Bor Plestenjak (2), Hauke Gravenkamp (3) and, Claire Prada (1) ((1) Institut Langevin, ESPCI Paris, Universit\'e PSL, CNRS,, Paris, France, (2) Faculty of Mathematics, Physics, University of, Ljubljana, Ljubljana, Slovenia

TL;DR
This paper introduces three numerical methods for accurately computing zero-group-velocity points in anisotropic elastic waveguides, which are crucial for nondestructive testing and structural characterization.
Contribution
It develops a two-parameter eigenvalue model for ZGV points and presents globally convergent, locally convergent, and hybrid algorithms for their computation.
Findings
The globally convergent method finds all ZGV points but is limited to small problems.
The Newton-type method is fast and applicable to larger problems with initial guesses.
The hybrid method combines approaches to handle large problems without initial guesses.
Abstract
Dispersion curves of elastic waveguides exhibit points where the group velocity vanishes while the wavenumber remains finite. These are the so-called zero-group-velocity (ZGV) points. As the elastodynamic energy at these points remains confined close to the source, they are of practical interest for nondestructive testing and quantitative characterization of structures. These applications rely on the correct prediction of the ZGV points. In this contribution, we first model the ZGV resonances in anisotropic plates based on the appearance of an additional modal solution. The resulting governing equation is interpreted as a two-parameter eigenvalue problem. Subsequently, we present three complementary numerical procedures capable of computing ZGV points in arbitrary nondissipative elastic waveguides in the conventional sense that their axial power flux vanishes. The first method is…
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Taxonomy
TopicsNumerical methods in engineering · Electromagnetic Simulation and Numerical Methods · Composite Material Mechanics
