Abstract

In the framework of wave propagation, finite difference time domain (FDTD) algorithms, yield high computational time. We propose to use morphing algorithms to deduce some approximate wave pictures of their interactions with fluid-solid structures of various shapes and different sizes deduced from FDTD computations of scattering by solids of three given shapes: triangular, circular and elliptic ones. The error in theL2norm between the FDTD solution and approximate solution deducedviamorphing from the source and destination images are typically less than 1% if control points are judiciously chosen. We thus propose to use a morphing algorithm to deduce approximate wave pictures: at intermediate time steps from the FDTD computation of wave pictures at a time step before and after this event, and at the same time step, but for an average frequency signal between FDTD computation of wave pictures with two different signal frequencies. We stress that our approach might greatly accelerate FDTD computations as discretizations in space and time are inherently linkedviathe Courant–Friedrichs–Lewy stability condition. Our approach requires some human intervention since the accuracy of morphing highly depends upon control points, but compared to the direct computational method our approach is much faster and requires fewer resources. We also compared our approach to some neural style transfer (NST) algorithm, which is an image transformation method based on a neural network. Our approach outperforms NST in terms of theL2norm, Mean Structural SIMilarity, expected signal to error ratio.

Highlights

  • Numerical simulations for elastodynamic wave propagation in complex media require huge computing resources and even with parallel computing resources, the computations may last many hours or many days

  • We describe the application of morphing to the same kind of waves scattered by an aluminum lens of a given thickness at different time steps

  • We explore the abilities of the morphing to face setting modifications

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Summary

Introduction

Numerical simulations for elastodynamic wave propagation in complex media require huge computing resources and even with parallel computing resources, the computations may last many hours (for 2D configurations) or many days (in 3D). Elastodynamic waves play a key role in well-established research topics including medical imaging [1] and site-city interactions [2], at small and large scales, respectively. Research in SM is based upon bold analogies with electromagnetic metamaterials [11], that.

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