Основные понятия
The authors present an approach to coupling mixed-dimensional continua by employing the mathematically enriched linear Cosserat micropolar model, where the kinematical reduction to lower dimensional domains leaves the fundamental degrees of freedom intact, enabling intrinsic agreement of the degrees of freedom at the interface.
Аннотация
The paper introduces the linear isotropic Cosserat micropolar model in three dimensions and subsequently reduces it to shell, plate, and beam models using kinematical assumptions and integration. The resulting reduced models all share the same kinematical degrees of freedom, namely displacements and rotations, enabling intrinsic coupling at interfaces of mixed dimensionality.
The derivation of the reduced models is performed using tangential differential calculus, which allows for a direct implementation in automated solvers of partial differential equations. The coupling itself is achieved by restricting the bulk fields to codimensional domains using consistent Sobolev trace operators, yielding a mixed-dimensional action functional.
The authors present numerical examples involving a three-dimensional silicone-rubber block reinforced with a curved graphite shell, a three-dimensional silver block reinforced with a graphite plate and beams, and intersecting silver shells reinforced with graphite beams.
Статистика
The internal energy functional of the three-dimensional Cosserat micropolar model is given by Eq. (2.15).
The internal energy functional of the Cosserat shell model is given by Eq. (3.35).
The internal energy functional of the Cosserat plate model is given by Eq. (3.38).
The internal energy functional of the Cosserat beam model is given by Eq. (4.15).
Цитаты
"The coupling itself is then achieved by restricting the bulk fields to codimensional domains using consistent Sobolev trace operators, yielding a mixed-dimensional action functional."
"We emphasise that the resulting reduced models in this work do not coincide with the standard linear Naghdi shell or the Reissner–Mindlin plate formulations, nor with the traditional definition of the Cosserat rod in the case of the beam formulations."