2004
DOI: 10.1111/j.1365-246x.2004.02289.x
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Mixed-grid and staggered-grid finite-difference methods for frequency-domain acoustic wave modelling

Abstract: S U M M A R YWe compare different finite-difference schemes for two-dimensional (2-D) acoustic frequencydomain forward modelling. The schemes are based on staggered-grid stencils of various accuracy and grid rotation strategies to discretize the derivatives of the wave equation. A combination of two O( x 2 ) staggered-grid stencils on the classical Cartesian coordinate system and the 45 • rotated grid is the basis of the so-called mixed-grid stencil. This method is compared with a parsimonious staggered-grid m… Show more

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Cited by 284 publications
(188 citation statements)
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“…The 2D scalar wave equation shown in Equation 1 can be rewritten as (Liu and Tao, 1997;Hustedt et al, 2004)…”
Section: Perfectly Matched Layermentioning
confidence: 99%
“…The 2D scalar wave equation shown in Equation 1 can be rewritten as (Liu and Tao, 1997;Hustedt et al, 2004)…”
Section: Perfectly Matched Layermentioning
confidence: 99%
“…The advantage of the direct-solver approach is that, once the decomposition is performed, equation (15) is efficiently solved for multiple sources using forward and backward substitutions (Marfurt, 1984). This approach has been shown to be efficient for 2D forward problems (Hustedt et al, 2004;Jo et al, 1996;Stekl & Pratt, 1998). However, the time and memory complexities of the LU factorization, and its limited scalability on large-scale distributed memory platforms, prevents the use of the direct-solver approach for large-scale 3D problems (i.e., problems involving more than ten millions of unknowns) (Operto et al, 2007).…”
Section: Time-domain or Frequency-domain Approachesmentioning
confidence: 99%
“…If the source is excited only within the element containing the source, a checker-board pattern is superimposed on the wavefield solution. This pattern results from the fact that one cell out of two is excited in the DG formulation because the DG stencil does not embed a staggered-grid structure (the unexcited grid is not stored in staggered-grid FD methods; see Hustedt et al (2004) for an illustration). To overcome this problem, the source can be distributed over several elements of the mesh or P 1 interpolation can be used in the area containing the sources and the receivers, while keeping P 0 interpolation in the other parts of the model .…”
Section: Boundary Conditions and Source Implementationmentioning
confidence: 99%
See 1 more Smart Citation
“…The system of three first-order equations is recast into one second-order equation and two first-order equations. This transformation and acoustic/electromagnetic analogy [2] allow to simulate electromagnetic wave propagation using finite-difference frequency-domain schemes initially developed for seismic modeling in visco-acoustic approximation [3]. This formulation leads to the system A(m)H y = s where the discrete wave operator A(m) contains the subsurface parameters m while H y and s are respectively the magnetic wavefield and the discretized source terms.…”
Section: Theoretical Basics On Forward and Inverse Problemsmentioning
confidence: 99%