Semi-discrete Matrix Free Formulation of 3D Full Waveform Elastic Modeling and Inversion

Author(s):  
S. Moore ◽  
S. Zhuk ◽  
D.S. Chunduri ◽  
T. Tchrakian ◽  
E. van den Berg ◽  
...  
2017 ◽  
Author(s):  
Olga Podgornova ◽  
Scott Leaney ◽  
Smaine Zeroug ◽  
Lin Liang

Geophysics ◽  
2019 ◽  
Vol 84 (5) ◽  
pp. R783-R792 ◽  
Author(s):  
Debanjan Datta ◽  
Piyoosh Jaysaval ◽  
Mrinal Sen ◽  
Adrien F. Arnulf

In most full-waveform inversion (FWI) problems, sufficient prior information is available to constrain the velocity of certain parts of the model, e.g., the water column or, in some cases, near-surface velocities. We take advantage of this situation and develop a fast Schur-complement-based forward modeling and inversion approach by partitioning the velocity model into two parts. The first part consists of the constrained zone that does not change during the inversion, whereas the second part is the anomalous zone to be updated during the inversion. For this decomposition, we partially factorize the governing system of linear equations by computing a Schur complement for the anomalous zone. The Schur complement system is then solved to compute the fields in the anomalous zone, which are then back substituted to compute the fields in the constrained region. For each successive modeling steps with new anomalous zone velocities, the corresponding Schur complement is easily computed using simple algebra. Because the anomalous part of the model is comparatively smaller than the whole model, considerable computational savings can be achieved using our Schur approach. Additionally, we showed that the Schur complement method maintains the accuracy of standard frequency-domain finite difference formulations, but this comes at a slightly higher peak memory requirement. Our FWI workflow shows reduced runtime by 15%–57% depending upon the depth of the water column without losing any accuracy compared to the standard method.


Geophysics ◽  
2011 ◽  
Vol 76 (5) ◽  
pp. A37-A44 ◽  
Author(s):  
Margherita Maraschini ◽  
Daniele Boiero ◽  
Sebastiano Foti ◽  
Laura Valentina Socco

Starting from the nondimensionalization of equations of motion we partition the set of the velocity models in equivalence classes, such that the full waveform of an element in a given class can be calculated from the full waveform of any other element in the same class by scaling model parameters. We give a formal derivation of the seismic wavefield scale properties and we prove their capability through the use of numerical examples. Besides this, we introduce how the scale properties can be used to save computational time in full waveform modeling and inversion. In forward modeling we can use them for the calculation of the full waveform of any model in the same equivalence class of a model whose full waveform has been previously calculated. In full waveform inversion, scale properties can be used for full waveform matching: Given an experimental seismogram and a synthetic one, we can choose, in the same class of the synthetic model, another element whose waveform is closer to the experimental one.


Geophysics ◽  
1987 ◽  
Vol 52 (3) ◽  
pp. 279-288 ◽  
Author(s):  
Michael W. Asten

Modeling of transient electromagnetic soundings requires consideration of the full bipolar transmitter waveform in order to obtain full measurement accuracy from field instruments. The full‐waveform transient may be computed using existing impulse‐response forward algorithms followed by a convolution procedure with truncation and residual estimation after an even number of terms, which results in average increases in run time of about 80 percent. Simple calculations based on approximations for the behavior of transient decay over (a) a conductive layer over a resistive basement, (b) a homogeneous half‐space, and (c) a resistive layer over a conductive basement show that the effect of the full waveform is greatest at sample times near the end of the transmitter off‐time, and for the case of a conductive basement. Failure to consider the full waveform is expected to yield errors in the amplitude of the computed transient in the range of 4 to 100 percent or more, depending upon the sample time and type of earth model. Examples of soundings over moderately conductive coal measures and highly conductive cindered coal show that failure to use the full waveform yields depths and resistivities biased to erroneously high values. The bias is small in the former case, but produces substantial errors in the latter case. Depth to the electrical basement of 300 to 400 m may be estimated to accuracies of approximately 5 percent by computer inversion to three‐layer or four‐layer models.


2011 ◽  
Author(s):  
Gianluca Fiandaca ◽  
Esben Auken ◽  
Aurélie Gazoty ◽  
Anders Vest Christiansen

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