2022
DOI: 10.1007/s10704-022-00634-2
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Adaptive modelling of dynamic brittle fracture - a combined phase field regularized cohesive zone model and scaled boundary finite element approach

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Cited by 28 publications
(2 citation statements)
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“…The field variables are constructed from Equation (39) with boldufalse(ξ,ηfalse)=[]ufalse(ξ,ηfalse)1emvfalse(ξ,ηfalse)boldpfalse(ξ,ηfalse)$$ \mathbf{u}\left(\xi, \eta \right)=\left[u\left(\xi, \eta \right)\kern1em v\Big(\xi, \eta \Big)\right]\equiv \mathbf{p}\left(\xi, \eta \right) $$ representing the displacement field and ϕfalse(ξ,ηfalse)boldpfalse(ξ,ηfalse)$$ \phi \left(\xi, \eta \right)\equiv \mathbf{p}\left(\xi, \eta \right) $$ representing the phase field variable. The discretization of the coupled governing equations follows similarly from that presented in Reference 71 where the general form of shape functions replace the scaled boundary shape functions for the displacement field.…”
Section: Numerical Examplesmentioning
confidence: 99%
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“…The field variables are constructed from Equation (39) with boldufalse(ξ,ηfalse)=[]ufalse(ξ,ηfalse)1emvfalse(ξ,ηfalse)boldpfalse(ξ,ηfalse)$$ \mathbf{u}\left(\xi, \eta \right)=\left[u\left(\xi, \eta \right)\kern1em v\Big(\xi, \eta \Big)\right]\equiv \mathbf{p}\left(\xi, \eta \right) $$ representing the displacement field and ϕfalse(ξ,ηfalse)boldpfalse(ξ,ηfalse)$$ \phi \left(\xi, \eta \right)\equiv \mathbf{p}\left(\xi, \eta \right) $$ representing the phase field variable. The discretization of the coupled governing equations follows similarly from that presented in Reference 71 where the general form of shape functions replace the scaled boundary shape functions for the displacement field.…”
Section: Numerical Examplesmentioning
confidence: 99%
“…A staggered solution scheme is adopted to solve the coupled equations. The phase field variable is assumed to be constant over a cell and is averaged from the phase field values at the nodes, similar to the approach adopted in Reference 71.…”
Section: Numerical Examplesmentioning
confidence: 99%