Images reconstruction for well to well tomography with Levenberg Marquardt method
Descripción del Articulo
The Cross-Borehole-Seismic Tomography is a seismic method most used for the determination of subsurface structure of the land. This method involves placing in a borehole the seismic wave generating sources, and in another borehole the receiver as waves detector. The tomographic image reconstructed f...
Autores: | , , |
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Formato: | artículo |
Fecha de Publicación: | 2013 |
Institución: | Universidad Nacional Mayor de San Marcos |
Repositorio: | Revistas - Universidad Nacional Mayor de San Marcos |
Lenguaje: | español |
OAI Identifier: | oai:ojs.csi.unmsm:article/8680 |
Enlace del recurso: | https://revistasinvestigacion.unmsm.edu.pe/index.php/fisica/article/view/8680 |
Nivel de acceso: | acceso abierto |
Materia: | Inverse problem Cross-Borehole-Seismic Tomography Levenberg Marquardt method. Problema inverso tomografía pozo a pozo método Levenberg Marquardt. |
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Images reconstruction for well to well tomography with Levenberg Marquardt methodReconstrucción de imágenes para tomografía de pozo a pozo con el método de Levenberg MarquardtChambi Chambi, JuanCarita Montero, RaulBerrocal Tito, MariellaInverse problemCross-Borehole-Seismic TomographyLevenberg Marquardt method.Problema inversotomografía pozo a pozométodo Levenberg Marquardt.The Cross-Borehole-Seismic Tomography is a seismic method most used for the determination of subsurface structure of the land. This method involves placing in a borehole the seismic wave generating sources, and in another borehole the receiver as waves detector. The tomographic image reconstructed from Cross-Borehole-Seismic Tomography is obtained by considering a parameter called slowness which is reverse speed with which the seismic waves travel, slowness S varies depending on the geological structure. We consider direct waves traveling from one borehole to another and we obtain an approximation of the following linear system as MS = T , where M is a matrix and is related to the discretization domain, S is the vector formed by the slowness of each discretized domain element and T is the arrival time of the first wave coming from source to detector. For the evaluation of the algorithms we design underground structures, which get the data from the detectors. To obtain more realistic data, we added random noise to 3.0%. With these data we proceed to rebuild the soil properties.La tomografía de pozo a pozo es uno de los métodos sísmicos más usados para la determinación de la estructura de los subsuelos. Este método consiste en colocar en un pozo las fuentes que generan las ondas sísmicas, y en otro pozo los receptores de las ondas. La imagen reconstruida en la tomografía de pozo a pozo es obtenida al considerar el parámetro denominado lentitud, que es la inversa de la velocidad con la que viajan las ondas sísmicas, la lentitud S varía según la estructura geológica del medio de propagación. Considerando ondas directas que viajan de un pozo a otro, realizamos una aproximación lineal para obtener S como MS = T , donde M es una matriz y está relacionado con la discretización del dominio, S es el vector formado por la lentitud de cada elemento discretizado del dominio y T es el tiempo de llegada de la primera onda desde la fuente al detector. Para la evaluación de los algoritmos diseñamos estructuras de subsuelos, de los cuales obtenemos los datos de los detectores. Para obtener datos más realísticos, se les agrega un ruido aleatorio hasta 3.0%. Con esos datos se procede a reconstruir las propiedades del suelo.Universidad Nacional Mayor de San Marcos2013-12-31info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionapplication/pdfhttps://revistasinvestigacion.unmsm.edu.pe/index.php/fisica/article/view/868010.15381/rif.v16i02.8680Revista de Investigación de Física; Vol. 16 No. 02 (2013); 1-9Revista de Investigación de Física; Vol. 16 Núm. 02 (2013); 1-91728-29771605-7724reponame:Revistas - Universidad Nacional Mayor de San Marcosinstname:Universidad Nacional Mayor de San Marcosinstacron:UNMSMspahttps://revistasinvestigacion.unmsm.edu.pe/index.php/fisica/article/view/8680/7534Derechos de autor 2013 Juan Chambi Chambi, Raul Carita Montero, Mariella Berrocal Titohttps://creativecommons.org/licenses/by-nc-sa/4.0info:eu-repo/semantics/openAccessoai:ojs.csi.unmsm:article/86802020-09-03T20:21:52Z |
dc.title.none.fl_str_mv |
Images reconstruction for well to well tomography with Levenberg Marquardt method Reconstrucción de imágenes para tomografía de pozo a pozo con el método de Levenberg Marquardt |
title |
Images reconstruction for well to well tomography with Levenberg Marquardt method |
spellingShingle |
Images reconstruction for well to well tomography with Levenberg Marquardt method Chambi Chambi, Juan Inverse problem Cross-Borehole-Seismic Tomography Levenberg Marquardt method. Problema inverso tomografía pozo a pozo método Levenberg Marquardt. |
title_short |
Images reconstruction for well to well tomography with Levenberg Marquardt method |
title_full |
Images reconstruction for well to well tomography with Levenberg Marquardt method |
title_fullStr |
Images reconstruction for well to well tomography with Levenberg Marquardt method |
title_full_unstemmed |
Images reconstruction for well to well tomography with Levenberg Marquardt method |
title_sort |
Images reconstruction for well to well tomography with Levenberg Marquardt method |
dc.creator.none.fl_str_mv |
Chambi Chambi, Juan Carita Montero, Raul Berrocal Tito, Mariella |
author |
Chambi Chambi, Juan |
author_facet |
Chambi Chambi, Juan Carita Montero, Raul Berrocal Tito, Mariella |
author_role |
author |
author2 |
Carita Montero, Raul Berrocal Tito, Mariella |
author2_role |
author author |
dc.subject.none.fl_str_mv |
Inverse problem Cross-Borehole-Seismic Tomography Levenberg Marquardt method. Problema inverso tomografía pozo a pozo método Levenberg Marquardt. |
topic |
Inverse problem Cross-Borehole-Seismic Tomography Levenberg Marquardt method. Problema inverso tomografía pozo a pozo método Levenberg Marquardt. |
description |
The Cross-Borehole-Seismic Tomography is a seismic method most used for the determination of subsurface structure of the land. This method involves placing in a borehole the seismic wave generating sources, and in another borehole the receiver as waves detector. The tomographic image reconstructed from Cross-Borehole-Seismic Tomography is obtained by considering a parameter called slowness which is reverse speed with which the seismic waves travel, slowness S varies depending on the geological structure. We consider direct waves traveling from one borehole to another and we obtain an approximation of the following linear system as MS = T , where M is a matrix and is related to the discretization domain, S is the vector formed by the slowness of each discretized domain element and T is the arrival time of the first wave coming from source to detector. For the evaluation of the algorithms we design underground structures, which get the data from the detectors. To obtain more realistic data, we added random noise to 3.0%. With these data we proceed to rebuild the soil properties. |
publishDate |
2013 |
dc.date.none.fl_str_mv |
2013-12-31 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
https://revistasinvestigacion.unmsm.edu.pe/index.php/fisica/article/view/8680 10.15381/rif.v16i02.8680 |
url |
https://revistasinvestigacion.unmsm.edu.pe/index.php/fisica/article/view/8680 |
identifier_str_mv |
10.15381/rif.v16i02.8680 |
dc.language.none.fl_str_mv |
spa |
language |
spa |
dc.relation.none.fl_str_mv |
https://revistasinvestigacion.unmsm.edu.pe/index.php/fisica/article/view/8680/7534 |
dc.rights.none.fl_str_mv |
Derechos de autor 2013 Juan Chambi Chambi, Raul Carita Montero, Mariella Berrocal Tito https://creativecommons.org/licenses/by-nc-sa/4.0 info:eu-repo/semantics/openAccess |
rights_invalid_str_mv |
Derechos de autor 2013 Juan Chambi Chambi, Raul Carita Montero, Mariella Berrocal Tito https://creativecommons.org/licenses/by-nc-sa/4.0 |
eu_rights_str_mv |
openAccess |
dc.format.none.fl_str_mv |
application/pdf |
dc.publisher.none.fl_str_mv |
Universidad Nacional Mayor de San Marcos |
publisher.none.fl_str_mv |
Universidad Nacional Mayor de San Marcos |
dc.source.none.fl_str_mv |
Revista de Investigación de Física; Vol. 16 No. 02 (2013); 1-9 Revista de Investigación de Física; Vol. 16 Núm. 02 (2013); 1-9 1728-2977 1605-7724 reponame:Revistas - Universidad Nacional Mayor de San Marcos instname:Universidad Nacional Mayor de San Marcos instacron:UNMSM |
instname_str |
Universidad Nacional Mayor de San Marcos |
instacron_str |
UNMSM |
institution |
UNMSM |
reponame_str |
Revistas - Universidad Nacional Mayor de San Marcos |
collection |
Revistas - Universidad Nacional Mayor de San Marcos |
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1795238318260092928 |
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13.754011 |
Nota importante:
La información contenida en este registro es de entera responsabilidad de la institución que gestiona el repositorio institucional donde esta contenido este documento o set de datos. El CONCYTEC no se hace responsable por los contenidos (publicaciones y/o datos) accesibles a través del Repositorio Nacional Digital de Ciencia, Tecnología e Innovación de Acceso Abierto (ALICIA).
La información contenida en este registro es de entera responsabilidad de la institución que gestiona el repositorio institucional donde esta contenido este documento o set de datos. El CONCYTEC no se hace responsable por los contenidos (publicaciones y/o datos) accesibles a través del Repositorio Nacional Digital de Ciencia, Tecnología e Innovación de Acceso Abierto (ALICIA).