Composite boundary-valued solution of the 2.5-D Green's function for arbitrary acoustic media

Theoretically, the Green’s function can be used to calculate the wavefield response of a specified source and the Frechet derivative with respect to the model parameters for crosshole seismic full‐waveform inversion. In this paper, we apply the finite‐element method to numerically compute the 2.5-D Green’s function for an arbitrary acoustic medium by solving a composite boundary‐valued problem in the wavenumber‐frequency domain. The composite boundary condition consists of a 2.5-D absorbing boundary condition for the propagating wave field and a mixed boundary condition for the evanescent field in inhomogeneous media modeling. A numerical experiment performed for a uniform earth (having a known exact solution) shows the accuracy of the computation in the frequency and time domain. An inhomogeneous medium test, involving an embedded low‐velocity layer, demonstrates that the permissible range of ky at each frequency can be determined rationally from the critical wavenumber value of the medium around the sou...

[1]  A. Tarantola Inversion of seismic reflection data in the acoustic approximation , 1984 .

[2]  Jack K. Cohen,et al.  Two and one‐half dimensional Born inversion with an arbitrary reference , 1987 .

[3]  Albert C. Reynolds,et al.  Boundary conditions for the numerical solution of wave propagation problems , 1978 .

[4]  W. Rodi,et al.  Nonlinear waveform tomography applied to crosshole seismic data , 1996 .

[5]  R. Pratt,et al.  INVERSE THEORY APPLIED TO MULTI‐SOURCE CROSS‐HOLE TOMOGRAPHY.: PART 1: ACOUSTIC WAVE‐EQUATION METHOD1 , 1990 .

[6]  R. Pratt,et al.  Short Note A critical review of acoustic wave modeling procedures in 2.5 dimensions , 1995 .

[7]  M. Toksöz,et al.  Diffraction tomography and multisource holography applied to seismic imaging , 1987 .

[8]  P. Williamson,et al.  Frequency-domain acoustic-wave modeling and inversion of crosshole data; Part 1, 2.5-D modeling method , 1995 .

[9]  S. Greenhalgh,et al.  2.5-D acoustic wave modelling in the frequency-wavenumber domain , 1997 .

[10]  B. Kennett,et al.  A 2.5‐D Time‐Domain Elastodynamic Equation For Plane‐Wave Incidence , 1996 .

[11]  U. Das,et al.  RESISTIVITY AND INDUCED POLARIZATION RESPONSES OF ARBITRARILY SHAPED 3‐D BODIES IN A TWO‐LAYERED EARTH* , 1987 .

[12]  Hiroshi Takenaka,et al.  2.5-D modelling of elastic waves using the pseudospectral method , 1996 .

[13]  R. Pratt,et al.  The application of diffraction tomography to cross-hole seismic data , 1988 .

[14]  R. Higdon Absorbing boundary conditions for elastic waves , 1991 .

[15]  Reinhold Ludwig,et al.  Finite-Element Formulation of Acoustic Scattering Phenomena with Absorbing Boundary-Condition in the Frequency-Domain , 1993 .

[16]  Reinhold Ludwig,et al.  Nonlinear Diffractive Inverse Scattering for Multiple-Scattering in Inhomogeneous Acoustic Background Media , 1995 .

[17]  B. Kennett,et al.  AN ALTERNATIVE STRATEGY FOR NON‐LINEAR INVERSION OF SEISMIC WAVEFORMS1 , 1991 .

[18]  T. Dickens Diffraction tomography for crosswell imaging of nearly layered media , 1994 .

[19]  S. Deregowski,et al.  A THEORY OF ACOUSTIC DIFFRACTORS APPLIED TO 2-D MODELS* , 1983 .

[20]  Leiv-J. Gelius Limited-view diffraction tomography in a nonuniform background , 1995 .

[21]  M. Gunzburger,et al.  Boundary conditions for the numerical solution of elliptic equations in exterior regions , 1982 .

[22]  S. Ergintav,et al.  THE USE OF THE HARTLEY TRANSFORM IN GEOPHYSICAL APPLICATIONS , 1990 .