A probabilistic crack band model for quasibrittle fracture
Identifikátory výsledku
Kód výsledku v IS VaVaI
<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F00216305%3A26110%2F16%3APU122692" target="_blank" >RIV/00216305:26110/16:PU122692 - isvavai.cz</a>
Výsledek na webu
<a href="http://dx.doi.org/10.1115/1.4032692" target="_blank" >http://dx.doi.org/10.1115/1.4032692</a>
DOI - Digital Object Identifier
<a href="http://dx.doi.org/10.1115/1.4032692" target="_blank" >10.1115/1.4032692</a>
Alternativní jazyky
Jazyk výsledku
angličtina
Název v původním jazyce
A probabilistic crack band model for quasibrittle fracture
Popis výsledku v původním jazyce
This paper presents a new crack band model (CBM) for probabilistic analysis of quasi-brittle fracture. The model is anchored by a probabilistic treatment of damage initiation, localization, and propagation. This model regularizes the energy dissipation of a single material element for the transition between damage initiation and localization. Meanwhile, the model also takes into account the probabilistic onset of damage localization inside the finite element (FE) for the case where the element size is larger than the crack band width. The random location of the localization band is related to the random material strength, whose statistics is described by a finite weakest link model. The present model is applied to simulate the probability distributions of the nominal strength of different quasibrittle structures. It is shown that for quasibrittle structures direct application of the conventional CBM for stochastic FE simulations would lead to mesh-sensitive results. To mitigate such mesh dependence, it is essential to incorporate the strain localization mechanism into the formulation of the sampling distribution functions of material constitutive parameters.
Název v anglickém jazyce
A probabilistic crack band model for quasibrittle fracture
Popis výsledku anglicky
This paper presents a new crack band model (CBM) for probabilistic analysis of quasi-brittle fracture. The model is anchored by a probabilistic treatment of damage initiation, localization, and propagation. This model regularizes the energy dissipation of a single material element for the transition between damage initiation and localization. Meanwhile, the model also takes into account the probabilistic onset of damage localization inside the finite element (FE) for the case where the element size is larger than the crack band width. The random location of the localization band is related to the random material strength, whose statistics is described by a finite weakest link model. The present model is applied to simulate the probability distributions of the nominal strength of different quasibrittle structures. It is shown that for quasibrittle structures direct application of the conventional CBM for stochastic FE simulations would lead to mesh-sensitive results. To mitigate such mesh dependence, it is essential to incorporate the strain localization mechanism into the formulation of the sampling distribution functions of material constitutive parameters.
Klasifikace
Druh
J<sub>imp</sub> - Článek v periodiku v databázi Web of Science
CEP obor
—
OECD FORD obor
20102 - Construction engineering, Municipal and structural engineering
Návaznosti výsledku
Projekt
<a href="/cs/project/GJ15-19865Y" target="_blank" >GJ15-19865Y: Diskrétní modely lomového porušení: adaptivní zjemňování diskretizace, hnací síla trhliny a napětí na hranici</a><br>
Návaznosti
P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)
Ostatní
Rok uplatnění
2016
Kód důvěrnosti údajů
S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů
Údaje specifické pro druh výsledku
Název periodika
JOURNAL OF APPLIED MECHANICS-TRANSACTIONS OF THE ASME
ISSN
0021-8936
e-ISSN
1528-9036
Svazek periodika
83
Číslo periodika v rámci svazku
5
Stát vydavatele periodika
US - Spojené státy americké
Počet stran výsledku
7
Strana od-do
1-7
Kód UT WoS článku
000374149400005
EID výsledku v databázi Scopus
2-s2.0-84959449514