On the dynamic buckling of very slender structures to self-weight

We present a mathematical and experimental study of the dynamic buckling of very slender structures due to their self-weight. Modern materials and powerful new analysis methods are leading to the design of very slender tall structures that may be prone to instability issues. Elastic stability of suc...

Full description

Bibliographic Details
Main Authors: Brasil Reyolando, Orbolato Leandro, Pádua Eduardo
Format: Article
Language:English
Published: EDP Sciences 2018-01-01
Series:MATEC Web of Conferences
Online Access:https://doi.org/10.1051/matecconf/201821103002
id doaj-5b872be249204763bdff22bc2c5eb439
record_format Article
spelling doaj-5b872be249204763bdff22bc2c5eb4392021-02-02T06:07:48ZengEDP SciencesMATEC Web of Conferences2261-236X2018-01-012110300210.1051/matecconf/201821103002matecconf_vetomacxiv2018_03002On the dynamic buckling of very slender structures to self-weightBrasil ReyolandoOrbolato LeandroPádua EduardoWe present a mathematical and experimental study of the dynamic buckling of very slender structures due to their self-weight. Modern materials and powerful new analysis methods are leading to the design of very slender tall structures that may be prone to instability issues. Elastic stability of such structures is a problem inside the scope of the Non-Linear Dynamics Analysis Methods. An indicator of instability is when the structure’s free vibration frequency approaches null value. Two main factors affect these frequency results. First the stiffness, composed of elastic stiffness, always positive and non-zero, that diminishes rapidly with height, and the geometric stiffness, negative for compressive forces, whose absolute value grows as the structure gets taller and heavier. Second, the mass, that also grows with the height of the structures. To access this behaviour, we first present a simple one-degree-of-freedom mathematical model derived with Rayleigh’s Method, adopting a cubic polynomial as shape function. Next, comparisons are made with results of an experimental set up composed of a variable length cantilever vertical aluminium bar. These models reasonably agree with analytical close solutions available in the literature.https://doi.org/10.1051/matecconf/201821103002
collection DOAJ
language English
format Article
sources DOAJ
author Brasil Reyolando
Orbolato Leandro
Pádua Eduardo
spellingShingle Brasil Reyolando
Orbolato Leandro
Pádua Eduardo
On the dynamic buckling of very slender structures to self-weight
MATEC Web of Conferences
author_facet Brasil Reyolando
Orbolato Leandro
Pádua Eduardo
author_sort Brasil Reyolando
title On the dynamic buckling of very slender structures to self-weight
title_short On the dynamic buckling of very slender structures to self-weight
title_full On the dynamic buckling of very slender structures to self-weight
title_fullStr On the dynamic buckling of very slender structures to self-weight
title_full_unstemmed On the dynamic buckling of very slender structures to self-weight
title_sort on the dynamic buckling of very slender structures to self-weight
publisher EDP Sciences
series MATEC Web of Conferences
issn 2261-236X
publishDate 2018-01-01
description We present a mathematical and experimental study of the dynamic buckling of very slender structures due to their self-weight. Modern materials and powerful new analysis methods are leading to the design of very slender tall structures that may be prone to instability issues. Elastic stability of such structures is a problem inside the scope of the Non-Linear Dynamics Analysis Methods. An indicator of instability is when the structure’s free vibration frequency approaches null value. Two main factors affect these frequency results. First the stiffness, composed of elastic stiffness, always positive and non-zero, that diminishes rapidly with height, and the geometric stiffness, negative for compressive forces, whose absolute value grows as the structure gets taller and heavier. Second, the mass, that also grows with the height of the structures. To access this behaviour, we first present a simple one-degree-of-freedom mathematical model derived with Rayleigh’s Method, adopting a cubic polynomial as shape function. Next, comparisons are made with results of an experimental set up composed of a variable length cantilever vertical aluminium bar. These models reasonably agree with analytical close solutions available in the literature.
url https://doi.org/10.1051/matecconf/201821103002
work_keys_str_mv AT brasilreyolando onthedynamicbucklingofveryslenderstructurestoselfweight
AT orbolatoleandro onthedynamicbucklingofveryslenderstructurestoselfweight
AT paduaeduardo onthedynamicbucklingofveryslenderstructurestoselfweight
_version_ 1724301950237802496