On the isospectral beams
The free undamped infinitesimal transverse vibrations of a thin straight beam are modelled by a forth-order differential equation. This paper investigates the families of fourth-order systems which have one spectrum in common, and correspond to four different sets of end-conditions. The analysis is...
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Format: | Article |
Language: | English |
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Texas State University
2005-04-01
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Series: | Electronic Journal of Differential Equations |
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Online Access: | http://ejde.math.txstate.edu/conf-proc/12/g1/abstr.html |
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author | Kazem Ghanbari |
author_facet | Kazem Ghanbari |
author_sort | Kazem Ghanbari |
collection | DOAJ |
description | The free undamped infinitesimal transverse vibrations of a thin straight beam are modelled by a forth-order differential equation. This paper investigates the families of fourth-order systems which have one spectrum in common, and correspond to four different sets of end-conditions. The analysis is based on the transformation of the beam operator into a fourth-order self-adjoint linear differential operator. This operator is factorized as a product $L=H^{*}H$, where $H$ is a second-order differential operator of the form $H=D^2+rD+s$, and $H^{*}$ is its adjoint operator. |
first_indexed | 2024-12-20T10:58:29Z |
format | Article |
id | doaj.art-a37b7a1548aa4cdc9445e48373cfd808 |
institution | Directory Open Access Journal |
issn | 1072-6691 |
language | English |
last_indexed | 2024-12-20T10:58:29Z |
publishDate | 2005-04-01 |
publisher | Texas State University |
record_format | Article |
series | Electronic Journal of Differential Equations |
spelling | doaj.art-a37b7a1548aa4cdc9445e48373cfd8082022-12-21T19:43:06ZengTexas State UniversityElectronic Journal of Differential Equations1072-66912005-04-01Conference125764On the isospectral beamsKazem GhanbariThe free undamped infinitesimal transverse vibrations of a thin straight beam are modelled by a forth-order differential equation. This paper investigates the families of fourth-order systems which have one spectrum in common, and correspond to four different sets of end-conditions. The analysis is based on the transformation of the beam operator into a fourth-order self-adjoint linear differential operator. This operator is factorized as a product $L=H^{*}H$, where $H$ is a second-order differential operator of the form $H=D^2+rD+s$, and $H^{*}$ is its adjoint operator.http://ejde.math.txstate.edu/conf-proc/12/g1/abstr.htmlIsospectral, Euler-Bernoulli equation for the vibrating beam, beam operator |
spellingShingle | Kazem Ghanbari On the isospectral beams Electronic Journal of Differential Equations Isospectral, Euler-Bernoulli equation for the vibrating beam, beam operator |
title | On the isospectral beams |
title_full | On the isospectral beams |
title_fullStr | On the isospectral beams |
title_full_unstemmed | On the isospectral beams |
title_short | On the isospectral beams |
title_sort | on the isospectral beams |
topic | Isospectral, Euler-Bernoulli equation for the vibrating beam, beam operator |
url | http://ejde.math.txstate.edu/conf-proc/12/g1/abstr.html |
work_keys_str_mv | AT kazemghanbari ontheisospectralbeams |