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...

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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
id REPOEAFIT2_21be76d2017c1c349f55db50ae6f5da9
oai_identifier_str oai:repository.eafit.edu.co:10784/8533
network_acronym_str REPOEAFIT2
network_name_str Repositorio EAFIT
repository_id_str
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
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bitstream.checksumAlgorithm.fl_str_mv MD5
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repository.name.fl_str_mv Repositorio Institucional Universidad EAFIT
repository.mail.fl_str_mv repositorio@eafit.edu.co
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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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