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Statements

Subject Item
n2:RIV%2F00216305%3A26110%2F05%3APU51478%21RIV06-GA0-26110___
rdf:type
skos:Concept n10:Vysledek
dcterms:description
If a solid is loaded by a kind of mechanical stress (compression, tensile stress, bending, mechanical shocks, shearing, notching, material fibre breakage etc.), cracks are generated in it which in turn results in a non-uniform distribution of the electric charge over the crack walls, which are getting charged by opposite sign charges. In consequence of the charge oscillatory motion corresponding to the acoustic emission (AE) taking place simultaneously with the crack generation, a time-varying electricdipole is formed. In this way, the cracks make up the source of an electromagnetic field, which can be detected in both the material neighbourhood and, in some cases, a remote region. If a solid is loaded by a kind of mechanical stress (compression, tensile stress, bending, mechanical shocks, shearing, notching, material fibre breakage etc.), cracks are generated in it which in turn results in a non-uniform distribution of the electric charge over the crack walls, which are getting charged by opposite sign charges. In consequence of the charge oscillatory motion corresponding to the acoustic emission (AE) taking place simultaneously with the crack generation, a time-varying electricdipole is formed. In this way, the cracks make up the source of an electromagnetic field, which can be detected in both the material neighbourhood and, in some cases, a remote region. If a solid is loaded by a kind of mechanical stress (compression, tensile stress, bending, mechanical shocks, shearing, notching, material fibre breakage etc.), cracks are generated in it which in turn results in a non-uniform distribution of the electric charge over the crack walls, which are getting charged by opposite sign charges. In consequence of the charge oscillatory motion corresponding to the acoustic emission (AE) taking place simultaneously with the crack generation, a time-varying electricdipole is formed. In this way, the cracks make up the source of an electromagnetic field, which can be detected in both the material neighbourhood and, in some cases, a remote region.
dcterms:title
Theoretical Analysis of Mechanical Load Induced Micro-crack Generation in Concruction Materials Teoretické studium vzniku mikrotrhlin při mechanickém zatěžování Theoretical Analysis of Mechanical Load Induced Micro-crack Generation in Concruction Materials
skos:prefLabel
Theoretical Analysis of Mechanical Load Induced Micro-crack Generation in Concruction Materials Theoretical Analysis of Mechanical Load Induced Micro-crack Generation in Concruction Materials Teoretické studium vzniku mikrotrhlin při mechanickém zatěžování
skos:notation
RIV/00216305:26110/05:PU51478!RIV06-GA0-26110___
n4:strany
205-209
n4:aktivita
n11:P
n4:aktivity
P(GD103/05/H044), P(GP102/02/D073)
n4:dodaniDat
n9:2006
n4:domaciTvurceVysledku
n8:3502465 n8:3037932
n4:druhVysledku
n16:D
n4:duvernostUdaju
n7:S
n4:entitaPredkladatele
n19:predkladatel
n4:idSjednocenehoVysledku
546589
n4:idVysledku
RIV/00216305:26110/05:PU51478
n4:jazykVysledku
n18:eng
n4:klicovaSlova
Micro-crack, mechanical stress, electromagnetic emission, acoustic emission
n4:klicoveSlovo
n5:electromagnetic%20emission n5:acoustic%20emission n5:mechanical%20stress n5:Micro-crack
n4:kontrolniKodProRIV
[63DA2A45D4FD]
n4:mistoKonaniAkce
Prague
n4:mistoVydani
Praha
n4:nazevZdroje
Proocedings of International Workshop Physical and Material Engineering 2005
n4:obor
n13:BM
n4:pocetDomacichTvurcuVysledku
2
n4:pocetTvurcuVysledku
2
n4:projekt
n14:GP102%2F02%2FD073 n14:GD103%2F05%2FH044
n4:rokUplatneniVysledku
n9:2005
n4:tvurceVysledku
Koktavý, Pavel Štefková, Markéta
n4:typAkce
n21:EUR
n4:zahajeniAkce
2005-09-12+02:00
s:numberOfPages
5
n15:hasPublisher
Vysoké učení technické v Brně
n12:isbn
80-01-03290-6
n17:organizacniJednotka
26110