Matrix basis for plane and modal waves in a Timoshenko beam

Plane waves and modal waves of the Timoshenko beam model are characterized in closed form by introducing robust matrix basis that behave according to the nature of frequency and wave or modal numbers. These new characterizations are given in terms of a finite number of coupling matrices and closed f...

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Main Authors: Julio Cesar Ruiz Claeyssen, Daniela de Rosso Tolfo, Leticia Tonetto
Format: Article
Language:English
Published: The Royal Society 2016-01-01
Series:Royal Society Open Science
Subjects:
Online Access:https://royalsocietypublishing.org/doi/pdf/10.1098/rsos.160825
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spelling doaj-3e1594bc9a8a407da691b572357dfffa2020-11-25T04:04:21ZengThe Royal SocietyRoyal Society Open Science2054-57032016-01-0131110.1098/rsos.160825160825Matrix basis for plane and modal waves in a Timoshenko beamJulio Cesar Ruiz ClaeyssenDaniela de Rosso TolfoLeticia TonettoPlane waves and modal waves of the Timoshenko beam model are characterized in closed form by introducing robust matrix basis that behave according to the nature of frequency and wave or modal numbers. These new characterizations are given in terms of a finite number of coupling matrices and closed form generating scalar functions. Through Liouville’s technique, these latter are well behaved at critical or static situations. Eigenanalysis is formulated for exponential and modal waves. Modal waves are superposition of four plane waves, but there are plane waves that cannot be modal waves. Reflected and transmitted waves at an interface point are formulated in matrix terms, regardless of having a conservative or a dissipative situation. The matrix representation of modal waves is used in a crack problem for determining the reflected and transmitted matrices. Their euclidean norms are seen to be dominated by certain components at low and high frequencies. The matrix basis technique is also used with a non-local Timoshenko model and with the wave interaction with a boundary. The matrix basis allows to characterize reflected and transmitted waves in spectral and non-spectral form.https://royalsocietypublishing.org/doi/pdf/10.1098/rsos.160825plane wavesmodal wavestimoshenko beammatrix basiscracked beamfundamental response
collection DOAJ
language English
format Article
sources DOAJ
author Julio Cesar Ruiz Claeyssen
Daniela de Rosso Tolfo
Leticia Tonetto
spellingShingle Julio Cesar Ruiz Claeyssen
Daniela de Rosso Tolfo
Leticia Tonetto
Matrix basis for plane and modal waves in a Timoshenko beam
Royal Society Open Science
plane waves
modal waves
timoshenko beam
matrix basis
cracked beam
fundamental response
author_facet Julio Cesar Ruiz Claeyssen
Daniela de Rosso Tolfo
Leticia Tonetto
author_sort Julio Cesar Ruiz Claeyssen
title Matrix basis for plane and modal waves in a Timoshenko beam
title_short Matrix basis for plane and modal waves in a Timoshenko beam
title_full Matrix basis for plane and modal waves in a Timoshenko beam
title_fullStr Matrix basis for plane and modal waves in a Timoshenko beam
title_full_unstemmed Matrix basis for plane and modal waves in a Timoshenko beam
title_sort matrix basis for plane and modal waves in a timoshenko beam
publisher The Royal Society
series Royal Society Open Science
issn 2054-5703
publishDate 2016-01-01
description Plane waves and modal waves of the Timoshenko beam model are characterized in closed form by introducing robust matrix basis that behave according to the nature of frequency and wave or modal numbers. These new characterizations are given in terms of a finite number of coupling matrices and closed form generating scalar functions. Through Liouville’s technique, these latter are well behaved at critical or static situations. Eigenanalysis is formulated for exponential and modal waves. Modal waves are superposition of four plane waves, but there are plane waves that cannot be modal waves. Reflected and transmitted waves at an interface point are formulated in matrix terms, regardless of having a conservative or a dissipative situation. The matrix representation of modal waves is used in a crack problem for determining the reflected and transmitted matrices. Their euclidean norms are seen to be dominated by certain components at low and high frequencies. The matrix basis technique is also used with a non-local Timoshenko model and with the wave interaction with a boundary. The matrix basis allows to characterize reflected and transmitted waves in spectral and non-spectral form.
topic plane waves
modal waves
timoshenko beam
matrix basis
cracked beam
fundamental response
url https://royalsocietypublishing.org/doi/pdf/10.1098/rsos.160825
work_keys_str_mv AT juliocesarruizclaeyssen matrixbasisforplaneandmodalwavesinatimoshenkobeam
AT danieladerossotolfo matrixbasisforplaneandmodalwavesinatimoshenkobeam
AT leticiatonetto matrixbasisforplaneandmodalwavesinatimoshenkobeam
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