Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method
The work presented in this thesis is concerned with the dynamical behavior of a CBandola's acoustical box at low resonances -- Two models consisting of two and three coupled oscillators are proposed in order to analyse the response at the first two and three resonances, respectively -- These mo...
- Autores:
-
Rodríguez Gómez, Sara Elena
- Tipo de recurso:
- Fecha de publicación:
- 2012
- Institución:
- Universidad EAFIT
- Repositorio:
- Repositorio EAFIT
- Idioma:
- spa
- OAI Identifier:
- oai:repository.eafit.edu.co:10784/8533
- Acceso en línea:
- http://hdl.handle.net/10784/8533
- Palabra clave:
- Bandola Andina Colombiana
MÉTODO DE ELEMENTOS FINITOS
ANÁLISIS NUMÉRICO
ACÚSTICA EN MÚSICA
INSTRUMENTOS DE CUERDA
ONDAS ACÚSTICAS
VIBRACIÓN - MEDICIONES
ONDAS SONORAS
Finite element method
Numerical analysis
Music - Acoustics and physics
Stringed instruments
Acoustic waves
Vibration - Measurement
- Rights
- License
- Acceso abierto
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REPOEAFIT2 |
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|
dc.title.spa.fl_str_mv |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method |
title |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method |
spellingShingle |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method Bandola Andina Colombiana MÉTODO DE ELEMENTOS FINITOS ANÁLISIS NUMÉRICO ACÚSTICA EN MÚSICA INSTRUMENTOS DE CUERDA ONDAS ACÚSTICAS VIBRACIÓN - MEDICIONES ONDAS SONORAS Finite element method Numerical analysis Music - Acoustics and physics Stringed instruments Acoustic waves Vibration - Measurement |
title_short |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method |
title_full |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method |
title_fullStr |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method |
title_full_unstemmed |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method |
title_sort |
Numerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element method |
dc.creator.fl_str_mv |
Rodríguez Gómez, Sara Elena |
dc.contributor.advisor.none.fl_str_mv |
Guarín Zapata, Nicolás |
dc.contributor.author.none.fl_str_mv |
Rodríguez Gómez, Sara Elena |
dc.subject.spa.fl_str_mv |
Bandola Andina Colombiana |
topic |
Bandola Andina Colombiana MÉTODO DE ELEMENTOS FINITOS ANÁLISIS NUMÉRICO ACÚSTICA EN MÚSICA INSTRUMENTOS DE CUERDA ONDAS ACÚSTICAS VIBRACIÓN - MEDICIONES ONDAS SONORAS Finite element method Numerical analysis Music - Acoustics and physics Stringed instruments Acoustic waves Vibration - Measurement |
dc.subject.lemb.spa.fl_str_mv |
MÉTODO DE ELEMENTOS FINITOS ANÁLISIS NUMÉRICO ACÚSTICA EN MÚSICA INSTRUMENTOS DE CUERDA ONDAS ACÚSTICAS VIBRACIÓN - MEDICIONES ONDAS SONORAS |
dc.subject.keyword.spa.fl_str_mv |
Finite element method Numerical analysis Music - Acoustics and physics Stringed instruments Acoustic waves Vibration - Measurement |
description |
The work presented in this thesis is concerned with the dynamical behavior of a CBandola's acoustical box at low resonances -- Two models consisting of two and three coupled oscillators are proposed in order to analyse the response at the first two and three resonances, respectively -- These models describe the first resonances in a bandola as a combination of the lowest modes of vibration of enclosed air, top and back plates -- Physically, the coupling between these elements is caused by the fluid-structure interaction that gives rise to coupled modes of vibration for the assembled resonance box -- In this sense, the coupling in the models is expressed in terms of the ratio of effective areas and masses of the elements which is an useful parameter to control the coupling -- Numerical models are developed for the analysis of modal coupling which is performed using the Finite Element Method -- First, it is analysed the modal behavior of separate elements: enclosed air, top plate and back plate -- This step is important to identify participating modes in the coupling -- Then, a numerical model of the resonance box is used to compute the coupled modes -- The computation of normal modes of vibration was executed in the frequency range of 0-800Hz -- Although the introduced models of coupled oscillators only predict maximum the first three resonances, they also allow to study qualitatively the coupling between the rest of the computed modes in the range -- Considering that dynamic response of a structure can be described in terms of the modal parameters, this work represents, in a good approach, the basic behavior of a CBandola, although experimental measurements are suggested as further work to verify the obtained results and get more information about some characteristics of the coupled modes, for instance, the phase of vibration of the air mode and the radiation e ciency |
publishDate |
2012 |
dc.date.issued.none.fl_str_mv |
2012 |
dc.date.available.none.fl_str_mv |
2016-05-26T15:08:22Z |
dc.date.accessioned.none.fl_str_mv |
2016-05-26T15:08:22Z |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/bachelorThesis |
dc.type.eng.fl_str_mv |
bachelorThesis |
dc.type.coar.fl_str_mv |
http://purl.org/coar/resource_type/c_7a1f |
dc.type.local.spa.fl_str_mv |
Trabajo de grado |
dc.type.hasVersion.eng.fl_str_mv |
acceptedVersion |
dc.identifier.uri.none.fl_str_mv |
http://hdl.handle.net/10784/8533 |
url |
http://hdl.handle.net/10784/8533 |
dc.language.iso.spa.fl_str_mv |
spa |
language |
spa |
dc.rights.coar.fl_str_mv |
http://purl.org/coar/access_right/c_abf2 |
dc.rights.local.spa.fl_str_mv |
Acceso abierto |
rights_invalid_str_mv |
Acceso abierto http://purl.org/coar/access_right/c_abf2 |
dc.coverage.spatial.eng.fl_str_mv |
Medellín de: Lat: 06 15 00 N degrees minutes Lat: 6.2500 decimal degrees Long: 075 36 00 W degrees minutes Long: -75.6000 decimal degrees |
dc.publisher.spa.fl_str_mv |
Universidad EAFIT |
dc.publisher.program.spa.fl_str_mv |
Ingeniería física |
dc.publisher.department.spa.fl_str_mv |
Escuela de Ciencias. Ciencias Básicas |
institution |
Universidad EAFIT |
bitstream.url.fl_str_mv |
https://repository.eafit.edu.co/bitstreams/4f9648d5-4f71-428d-8a59-6a2bded282e9/download https://repository.eafit.edu.co/bitstreams/8b37911d-5b7d-4e26-bad5-67b5a4c40b9b/download |
bitstream.checksum.fl_str_mv |
76025f86b095439b7ac65b367055d40c 329e2f103f84f467022e2086469ccce3 |
bitstream.checksumAlgorithm.fl_str_mv |
MD5 MD5 |
repository.name.fl_str_mv |
Repositorio Institucional Universidad EAFIT |
repository.mail.fl_str_mv |
repositorio@eafit.edu.co |
_version_ |
1814110216108638208 |
spelling |
Guarín Zapata, NicolásRodríguez Gómez, Sara ElenaIngeniero Físicosrh89s@gmail.comMedellín de: Lat: 06 15 00 N degrees minutes Lat: 6.2500 decimal degrees Long: 075 36 00 W degrees minutes Long: -75.6000 decimal degrees2016-05-26T15:08:22Z20122016-05-26T15:08:22Zhttp://hdl.handle.net/10784/8533The work presented in this thesis is concerned with the dynamical behavior of a CBandola's acoustical box at low resonances -- Two models consisting of two and three coupled oscillators are proposed in order to analyse the response at the first two and three resonances, respectively -- These models describe the first resonances in a bandola as a combination of the lowest modes of vibration of enclosed air, top and back plates -- Physically, the coupling between these elements is caused by the fluid-structure interaction that gives rise to coupled modes of vibration for the assembled resonance box -- In this sense, the coupling in the models is expressed in terms of the ratio of effective areas and masses of the elements which is an useful parameter to control the coupling -- Numerical models are developed for the analysis of modal coupling which is performed using the Finite Element Method -- First, it is analysed the modal behavior of separate elements: enclosed air, top plate and back plate -- This step is important to identify participating modes in the coupling -- Then, a numerical model of the resonance box is used to compute the coupled modes -- The computation of normal modes of vibration was executed in the frequency range of 0-800Hz -- Although the introduced models of coupled oscillators only predict maximum the first three resonances, they also allow to study qualitatively the coupling between the rest of the computed modes in the range -- Considering that dynamic response of a structure can be described in terms of the modal parameters, this work represents, in a good approach, the basic behavior of a CBandola, although experimental measurements are suggested as further work to verify the obtained results and get more information about some characteristics of the coupled modes, for instance, the phase of vibration of the air mode and the radiation e ciencyspaUniversidad EAFITIngeniería físicaEscuela de Ciencias. Ciencias BásicasBandola Andina ColombianaMÉTODO DE ELEMENTOS FINITOSANÁLISIS NUMÉRICOACÚSTICA EN MÚSICAINSTRUMENTOS DE CUERDAONDAS ACÚSTICASVIBRACIÓN - MEDICIONESONDAS SONORASFinite element methodNumerical analysisMusic - Acoustics and physicsStringed instrumentsAcoustic wavesVibration - MeasurementNumerical analysis of the modal coupling at low resonances in a Colombian Andean Bandola in C using the finite element methodinfo:eu-repo/semantics/bachelorThesisbachelorThesisTrabajo de gradoacceptedVersionhttp://purl.org/coar/resource_type/c_7a1fAcceso abiertohttp://purl.org/coar/access_right/c_abf2LICENSElicense.txtlicense.txttext/plain; charset=utf-82556https://repository.eafit.edu.co/bitstreams/4f9648d5-4f71-428d-8a59-6a2bded282e9/download76025f86b095439b7ac65b367055d40cMD51ORIGINALSaraElena_RodriguezGomez_2012.pdfSaraElena_RodriguezGomez_2012.pdfTrabajo de gradoapplication/pdf15189501https://repository.eafit.edu.co/bitstreams/8b37911d-5b7d-4e26-bad5-67b5a4c40b9b/download329e2f103f84f467022e2086469ccce3MD5210784/8533oai:repository.eafit.edu.co:10784/85332019-05-07 10:52:39.228open.accesshttps://repository.eafit.edu.coRepositorio Institucional Universidad EAFITrepositorio@eafit.edu.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 |