Modeling of self-excited stress measurement system

In the paper two types of numerical models of the self-excited acoustical system are presented. This new type of auto-oscillating system is used for stress change measurement in constructions and rock masses. The essence of the self-excited acoustical system is to use a vibration emitter and vibrati...

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Main Authors: Ireneusz Dominik, Krzysztof Lalik, Stanisław Flaga
Format: Article
Language:English
Published: SAGE Publishing 2021-06-01
Series:Journal of Low Frequency Noise, Vibration and Active Control
Online Access:https://doi.org/10.1177/1461348420929456
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spelling doaj-f7f89f840e87477abcb342fa8279b4a52021-06-23T22:33:57ZengSAGE PublishingJournal of Low Frequency Noise, Vibration and Active Control1461-34842048-40462021-06-014010.1177/1461348420929456Modeling of self-excited stress measurement systemIreneusz DominikKrzysztof LalikStanisław FlagaIn the paper two types of numerical models of the self-excited acoustical system are presented. This new type of auto-oscillating system is used for stress change measurement in constructions and rock masses. The essence of the self-excited acoustical system is to use a vibration emitter and vibration receiver placed at a distance, which are coupled with a proper power amplifier, and which are operating in a closed loop with a positive feedback. This causes the excitation of the system. The change of the velocity of wave propagation, which is associated with the change of the resonance frequency in the system is caused by the deformation of the examined material. Stress changes manifest themselves in small but detectable variations of frequency. The first of the presented models was created on the basis of estimating the model parameters by identification of the sensor–conditioner–amplifier–emitter system. The second mathematical model was delivered from the force–charge equation of the piezoelectric transducers: the sensor and the emitter. The model of the loaded beam, which determined the response of any beam point to the force applied to any other beam point is also presented.https://doi.org/10.1177/1461348420929456
collection DOAJ
language English
format Article
sources DOAJ
author Ireneusz Dominik
Krzysztof Lalik
Stanisław Flaga
spellingShingle Ireneusz Dominik
Krzysztof Lalik
Stanisław Flaga
Modeling of self-excited stress measurement system
Journal of Low Frequency Noise, Vibration and Active Control
author_facet Ireneusz Dominik
Krzysztof Lalik
Stanisław Flaga
author_sort Ireneusz Dominik
title Modeling of self-excited stress measurement system
title_short Modeling of self-excited stress measurement system
title_full Modeling of self-excited stress measurement system
title_fullStr Modeling of self-excited stress measurement system
title_full_unstemmed Modeling of self-excited stress measurement system
title_sort modeling of self-excited stress measurement system
publisher SAGE Publishing
series Journal of Low Frequency Noise, Vibration and Active Control
issn 1461-3484
2048-4046
publishDate 2021-06-01
description In the paper two types of numerical models of the self-excited acoustical system are presented. This new type of auto-oscillating system is used for stress change measurement in constructions and rock masses. The essence of the self-excited acoustical system is to use a vibration emitter and vibration receiver placed at a distance, which are coupled with a proper power amplifier, and which are operating in a closed loop with a positive feedback. This causes the excitation of the system. The change of the velocity of wave propagation, which is associated with the change of the resonance frequency in the system is caused by the deformation of the examined material. Stress changes manifest themselves in small but detectable variations of frequency. The first of the presented models was created on the basis of estimating the model parameters by identification of the sensor–conditioner–amplifier–emitter system. The second mathematical model was delivered from the force–charge equation of the piezoelectric transducers: the sensor and the emitter. The model of the loaded beam, which determined the response of any beam point to the force applied to any other beam point is also presented.
url https://doi.org/10.1177/1461348420929456
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AT krzysztoflalik modelingofselfexcitedstressmeasurementsystem
AT stanisławflaga modelingofselfexcitedstressmeasurementsystem
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