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Localization of cracks arising from mechanical loading of solids

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F00216305%3A26220%2F08%3APU77192" target="_blank" >RIV/00216305:26220/08:PU77192 - isvavai.cz</a>

  • Result on the web

  • DOI - Digital Object Identifier

Alternative languages

  • Result language

    čeština

  • Original language name

    Lokalizace trhlin vznikajících při mechanickém zatěžování pevných látek

  • Original language description

    Simultaneous measurement of electromagnetic (EME) and acoustic (AE) emission signals resulting from mechanical loading of solids can be used to localize the arising cracks. In the 2D case, the localization methods are usually based on identifying intersection points of the circles drawn around the AE sensors (provided the time of the crack generation is known from the EME signal measurement) or hyperbolas, whose foci are situated in the AE sensors (when only AE signals are measured). When these methodsare applied, the mechanical wave propagation velocity in the material under investigation must be known. However, if an excessive number of AE sensors is used, the different circle or hyperbola intersection points are not identical. In fact, these intersection points are only marking the boundaries of the region of probable crack generation. The information provided for the point in question in this way is not unambiguous. Therefore, to support the arising crack localization efforts, a n

  • Czech name

    Lokalizace trhlin vznikajících při mechanickém zatěžování pevných látek

  • Czech description

    Simultaneous measurement of electromagnetic (EME) and acoustic (AE) emission signals resulting from mechanical loading of solids can be used to localize the arising cracks. In the 2D case, the localization methods are usually based on identifying intersection points of the circles drawn around the AE sensors (provided the time of the crack generation is known from the EME signal measurement) or hyperbolas, whose foci are situated in the AE sensors (when only AE signals are measured). When these methodsare applied, the mechanical wave propagation velocity in the material under investigation must be known. However, if an excessive number of AE sensors is used, the different circle or hyperbola intersection points are not identical. In fact, these intersection points are only marking the boundaries of the region of probable crack generation. The information provided for the point in question in this way is not unambiguous. Therefore, to support the arising crack localization efforts, a n

Classification

  • Type

    D - Article in proceedings

  • CEP classification

    BM - Solid-state physics and magnetism

  • OECD FORD branch

Result continuities

  • Project

    <a href="/en/project/GA103%2F06%2F0708" target="_blank" >GA103/06/0708: Acoustic and electromagnetic emission in materials research</a><br>

  • Continuities

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)

Others

  • Publication year

    2008

  • Confidentiality

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Data specific for result type

  • Article name in the collection

    Defektoskopie 2008

  • ISBN

    978-80-214-3759-3

  • ISSN

  • e-ISSN

  • Number of pages

    8

  • Pages from-to

  • Publisher name

    Česká společnost pro nedestruktivní testování

  • Place of publication

    Brno

  • Event location

    Brno

  • Event date

    Nov 4, 2008

  • Type of event by nationality

    EUR - Evropská akce

  • UT code for WoS article