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Imperfect interface between the inclusions and the matrix has a significant influence on the macro properties of the composites.
We observed no correlation between Atlastin 3 and vRNPs staining (Supplementary Fig. 4d), but Sec23 and Sec31A localized frequently between the inclusions and the ER, and even co-localized with NP in specific spots (Fig. 5c, Supplementary Fig. 4e).
The bonds between the inclusions and the interphases as well as between the interphases and the matrix are assumed to be perfect.
The results have shown that the interfacial bonding between the inclusions and the matrix controls the crack path through the composite and determines whether or not an inclusion will act as a bridge and consequently provide a toughening effect.
Furthermore, Weng's approximate model of interfacial debonding between the inclusions and the matrix is installed, because of its very simple criterion for the initiation of debonding to simulate progressive debonding phenomena.
By computing the energy histories for the system when subject to a blast load, we show that there is a transfer of energy between the inclusions and the surrounding mortar.
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Moreover, the magnetoelastic stresses at the interface between the inclusion and the matrix are presented with figures.
The problem is reduced to a system of singular integral equations, with the differences in interface stresses between the inclusion and the matrix as the unknown functions.
Comparisons are made between the inclusion and exclusion of self-induced and forced fluctuating pressures, as well as the fidelity required in computing the temperature distributions.
Further, in the case when the bonding between the inclusion and the matrix is assumed to be imperfect, we show that for the stress distribution inside the inclusion to be uniform, the inclusion must be elliptical.
A thin homogeneous viscoelastic interphase between the inclusion and the matrix is used to model the more realistic bonding state between them.
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