Julien Diaz
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Julien Diaz has a total of 24 co-authors. Here are the top co-authors by number of shared publications:
Hélène Barucq
5 shared publications- Hélène Barucq
Makutu, Inria, TotalEnergies Universite de Pau et des Pays de l'Adour, CNRS Pau France
5 shared publications - Abdelaâziz Ezziani
Laboratory MAEGE FSJES Aïn Sebaâ, Hassan II University of Casablanca, Casablanca, Morocco
4 shared publications - Caroline Baldassari
French Institute for Research in Computer Science and Automation
3 shared publications - Henri Calandra
Centre Scientifique et Technique Jean Féger TOTAL avenue de Larribau F-64000 Pau France
3 shared publications Patrick Joly
INRIA Rocquencourt, Domaine de Voluceau, 78153 Le Chesnay, France
3 shared publications
Latest Publications
- 1 November 2021
- Published by Elsevier in Journal of Computational Physics
- Vol. 445
Time domain analysis and localization of a non-local PML for dispersive wave equations
- 1 November 2021
- Published by Elsevier in Journal of Computational Physics
- Vol. 445
Time domain analysis and localization of a non-local PML for dispersive wave equations
- 1 September 2021
- Published by Elsevier in Journal of Computational Physics
- Vol. 441
Local strategies for improving the conditioning of the plane-wave Ultra-Weak Variational Formulation
- 1 September 2021
- Published by Elsevier in Journal of Computational Physics
- Vol. 441
Local strategies for improving the conditioning of the plane-wave Ultra-Weak Variational Formulation
- 5 February 2021
- Published by Wiley in International Journal for Numerical Methods in Engineering
- Vol. 122 (12) , 3015-3043
Implementation of hybridizable discontinuous Galerkin method for time‐harmonic anisotropic poroelasticity in two dimensions
We apply a hybridizable discontinuous Galerkin (HDG) method to numerically solve two‐dimensional anisotropic poroelastic wave equations in the frequency domain given by Biot theory. The motivation for choosing HDG method comes from the complexity of the considered equations and the high number of unknowns. The HDG method possesses all the advantages of discontinuous Galerkin method (hp‐adaptivity, accuracy, ability to model complex tectonics, etc.) without a drastic increase in the number of degrees of freedom. After a description of its implementation, we illustrate the accuracy of the proposed method by comparisons with analytical solutions. We then perform a sensitivity analysis of the method as a function of stabilization parameters and frequency, and show in particular that there exists optimal values of these parameters in order to obtain a very good level of accuracy. We also show the ability of the method to reproduce the different types of poroelastic waves including the slow Biot wave.
- 5 February 2021
- Published by Wiley in International Journal for Numerical Methods in Engineering
- Vol. 122 (12) , 3015-3043
Implementation of hybridizable discontinuous Galerkin method for time‐harmonic anisotropic poroelasticity in two dimensions
We apply a hybridizable discontinuous Galerkin (HDG) method to numerically solve two‐dimensional anisotropic poroelastic wave equations in the frequency domain given by Biot theory. The motivation for choosing HDG method comes from the complexity of the considered equations and the high number of unknowns. The HDG method possesses all the advantages of discontinuous Galerkin method (hp‐adaptivity, accuracy, ability to model complex tectonics, etc.) without a drastic increase in the number of degrees of freedom. After a description of its implementation, we illustrate the accuracy of the proposed method by comparisons with analytical solutions. We then perform a sensitivity analysis of the method as a function of stabilization parameters and frequency, and show in particular that there exists optimal values of these parameters in order to obtain a very good level of accuracy. We also show the ability of the method to reproduce the different types of poroelastic waves including the slow Biot wave.
- 5 January 2019
- Published by Springer Nature
- p. 145-153
Trefftz-Discontinuous Galerkin Approach for Solving Elastodynamic Problem
- 5 January 2019
- Published by Springer Nature
- p. 145-153
Trefftz-Discontinuous Galerkin Approach for Solving Elastodynamic Problem
- 1 July 2015
- Published by Elsevier in Computer Methods in Applied Mechanics and Engineering
- Vol. 291, 240-265
Multi-level explicit local time-stepping methods for second-order wave equations
- 1 July 2015
- Published by Elsevier in Computer Methods in Applied Mechanics and Engineering
- Vol. 291, 240-265
Multi-level explicit local time-stepping methods for second-order wave equations
- 1 September 2014
- Published by EDP Sciences in ESAIM: Proceedings and Surveys
- Vol. 45, 67-74
High-Order Time Discretization of The Wave Equation by Nabla-P Scheme.
- 1 September 2014
- Published by EDP Sciences in ESAIM: Proceedings and Surveys
- Vol. 45, 67-74
High-Order Time Discretization of The Wave Equation by Nabla-P Scheme.
- Open Access
- 27 January 2014
- Published by Brazilian Society for Computational and Applied Mathematics (SBMAC) in TEMA (São Carlos)
- Vol. 15 (3) , 301-310
Equivalent Boundary Conditions for Heterogeneous Acoustic Media
In this work, we have worked on possibilities to model artificial boundaries needed in the simulation of wave propagation in acoustic heterogeneous media. Our motivation is to restrict the computational domain in the simulation of seismic waves that are propagated from the earth and transmitted to the stratified heterogeneous media composed by ocean and atmosphere. Two possibilities were studied and compared in computational tests: the use of absorbing boundary conditions on an artificial boundary in the atmosphere layer and the elimination of the atmosphere layer using an equivalent boundary condition that mimics the propagation of waves through the atmosphere.
- 27 January 2014
- Published by Brazilian Society for Computational and Applied Mathematics (SBMAC) in TEMA (São Carlos)
- Vol. 15 (3) , 301-310
Open AccessEquivalent Boundary Conditions for Heterogeneous Acoustic Media
In this work, we have worked on possibilities to model artificial boundaries needed in the simulation of wave propagation in acoustic heterogeneous media. Our motivation is to restrict the computational domain in the simulation of seismic waves that are propagated from the earth and transmitted to the stratified heterogeneous media composed by ocean and atmosphere. Two possibilities were studied and compared in computational tests: the use of absorbing boundary conditions on an artificial boundary in the atmosphere layer and the elimination of the atmosphere layer using an equivalent boundary condition that mimics the propagation of waves through the atmosphere.
- Open Access
- 17 April 2013
- Published by EDP Sciences in ESAIM: Mathematical Modelling and Numerical Analysis
- Vol. 47 (3) , 903-932
Stability analysis of the Interior Penalty Discontinuous Galerkin method for the wave equation
We consider here the Interior Penalty Discontinuous Galerkin (IPDG) discretization of the wave equation. We show how to derive the optimal penalization parameter involved in this method in the case of regular meshes. Moreover, we provide necessary stability conditions of the global scheme when IPDG is coupled with the classical Leap–Frog scheme for the time discretization. Numerical experiments illustrate the fact that these conditions are also sufficient.
- 17 April 2013
- Published by EDP Sciences in ESAIM: Mathematical Modelling and Numerical Analysis
- Vol. 47 (3) , 903-932
Open AccessStability analysis of the Interior Penalty Discontinuous Galerkin method for the wave equation
We consider here the Interior Penalty Discontinuous Galerkin (IPDG) discretization of the wave equation. We show how to derive the optimal penalization parameter involved in this method in the case of regular meshes. Moreover, we provide necessary stability conditions of the global scheme when IPDG is coupled with the classical Leap–Frog scheme for the time discretization. Numerical experiments illustrate the fact that these conditions are also sufficient.
- 1 January 2012
- Published by Global Science Press in Communications in Computational Physics
- Vol. 11 (2) , 674-690
Micro-Differential Boundary Conditions Modelling the Absorption of Acoustic Waves by 2D Arbitrarily-Shaped Convex Surfaces
Micro-Differential Boundary Conditions Modelling the Absorption of Acoustic Waves by 2D Arbitrarily-Shaped Convex Surfaces - Volume 11 Issue 2 - Hélène Barucq, Julien Diaz, Véronique Duprat
- 1 January 2012
- Published by Global Science Press in Communications in Computational Physics
- Vol. 11 (2) , 674-690
Micro-Differential Boundary Conditions Modelling the Absorption of Acoustic Waves by 2D Arbitrarily-Shaped Convex Surfaces
Micro-Differential Boundary Conditions Modelling the Absorption of Acoustic Waves by 2D Arbitrarily-Shaped Convex Surfaces - Volume 11 Issue 2 - Hélène Barucq, Julien Diaz, Véronique Duprat