Images reconstruction for well to well tomography with Levenberg Marquardt method

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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...

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Detalles Bibliográficos
Autores: Chambi Chambi, Juan, Carita Montero, Raul, Berrocal Tito, Mariella
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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spelling 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
repository.name.fl_str_mv
repository.mail.fl_str_mv
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score 13.754011
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