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According to Eq. (88), the first order chemical potentials are continuous across the interface.
All strain components are continuous across the interfaces due to the compatibility requirement in deformation.
The interfaces are treated as perfectly bonded in the most of the existing research works, where the traction and displacement vectors are continuous across the interfaces.
We demonstrate that if the localisation residuals are neglected, as originally proposed by Eringen, the asymptotic stress tensor and its normal derivative are continuous across the crack.
It is assumed that the electrical field inside the crack faces is equal to zero and the magnetic quantities are continuous across the crack faces.
In standard finite element spaces, due to the non-alignment, the functions are continuous across the interface and thus not appropriate for the approximation of the discontinuous pressure.
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The assumed displacements and stresses for each layer are taken to be continuous across the layer thickness; and satisfy the continuity conditions at the interfaces between the layers.
This space is continuous across the midline [25].
Since is continuous across the free boundary, then for any.
The tetrahedral sheet was continuous across the ribbons but with apices pointing up and down in adjacent ribbon [22].
However, in steady state, horizontal currents must be continuous across the boundary between low and high conductivity regions.
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