Abstract:Multiscale methods based on coupled partial differential equations defined on bulk and embedded manifolds are still poorly explored from the theoretical standpoint, although they are successfully used in applications, such as microcirculation and flow in perforated subsurface reservoirs. This work aims at shedding light on some theoretical aspects of a multiscale method consisting of coupled partial differential equations defined on one-dimensional domains embedded into three-dimensional ones. Mathematical iss… Show more
“…Due to its inherent complexity, this is a longstanding problem that needs to be addressed in the short-term to move towards wider clinical adoption of magnetic hyperthermia. A unified magnetic hyperthermia theory should be made possible in the near future, taking advantage of 3D-1D coupling strategies based on topological model reduction [189].…”
Section: Treatment Planning and Dosimetrymentioning
The scientific community has made great efforts in advancing magnetic hyperthermia for the last two decades after going through a sizeable research lapse from its establishment. All the progress made in various topics ranging from nanoparticle synthesis to biocompatibilization and in vivo testing have been seeking to push the forefront towards some new clinical trials. As many, they did not go at the expected pace. Today, fruitful international cooperation and the wisdom gain after a careful analysis of the lessons learned from seminal clinical trials allow us to have a future with better guarantees for a more definitive takeoff of this genuine nanotherapy against cancer. Deliberately giving prominence to a number of critical aspects, this opinion review offers a blend of state-of-the-art hints and glimpses into the future of the therapy, considering the expected evolution of science and technology behind magnetic hyperthermia.
“…Due to its inherent complexity, this is a longstanding problem that needs to be addressed in the short-term to move towards wider clinical adoption of magnetic hyperthermia. A unified magnetic hyperthermia theory should be made possible in the near future, taking advantage of 3D-1D coupling strategies based on topological model reduction [189].…”
Section: Treatment Planning and Dosimetrymentioning
The scientific community has made great efforts in advancing magnetic hyperthermia for the last two decades after going through a sizeable research lapse from its establishment. All the progress made in various topics ranging from nanoparticle synthesis to biocompatibilization and in vivo testing have been seeking to push the forefront towards some new clinical trials. As many, they did not go at the expected pace. Today, fruitful international cooperation and the wisdom gain after a careful analysis of the lessons learned from seminal clinical trials allow us to have a future with better guarantees for a more definitive takeoff of this genuine nanotherapy against cancer. Deliberately giving prominence to a number of critical aspects, this opinion review offers a blend of state-of-the-art hints and glimpses into the future of the therapy, considering the expected evolution of science and technology behind magnetic hyperthermia.
“…The singularity issue was remedied in a series of papers by Köppl and coauthors [12,15,4], in which the authors considered an alternative coupling of the model. This idea was further developed by Laurino and Zunino [16], where the coupled 1D-3D flow model was rigorously rederived. In the new derivation, the 1D equation is coupled to the 3D equation via a cylinder boundary source δ Γ , centered on the (2D) lateral boundary of the cylinder.…”
Section: Introductionmentioning
confidence: 99%
“…More recently, an extended finite element method was formulated for the mixed coupled 1D-3D flow model by Březina and Exner [2]. They take, as their starting point, the strong formulation of the coupled 1D-3D flow model (with a cylinder source [16]), before directly reformulating it as a mixed equation in 1D and 3D.…”
Section: Introductionmentioning
confidence: 99%
“…In this article, we derive a mixed formulation of the coupled 1D-3D flow model, taking the same set of model equations as in [16] as our starting point. Moreover, we follow their procedure of first deriving the variational formulation of the problem and then performing the averaging that leads to a dimensional reduction.…”
In this work, we consider a set of mixed-dimensional PDEs that are used to model e.g. microcirculation, root water uptake and the flow of fluids in a reservoir perforated with wells. To be more precise, we consider here the Poisson equation posed in two distinct domains. The two are then coupled by the use of a filtration law. We show how the mixed framework is a natural setting for this problem, as it allows the two equations to be posed using global variables. Further, the applications we consider are characterized by a scale disparity between the two domains. With this in mind, we perform a physically motivated averaging of the coupling condition. This has the advantage of allowing the solution to be approximated using non-conforming, coarse meshes.
“…Such models are referred to as mixed-dimensional when the network flow is simplified to a family of one-dimensional domains along with the network edges. 1 Moreover, when the coupling between the network and the domain exceeds two topological dimensions, the model is referred to as having a high-dimensional gap [21,19]. A high-dimensional gap thus arises when the flow in the network is connected to a domain of dimension d \geq 2 through its leaf nodes or when the flow in the network is connected to a domain of dimension d \geq 3 through its edges.…”
\bfA \bfb \bfs \bft \bfr \bfa \bfc \bft . In this work, we show the underlying mathematical structure of mixed-dimensional models arising from the composition of graphs and continuous domains. Such models are becoming popular in applications, in particular, to model the human vasculature. We first discuss the model equations in the strong form, which describes the conservation of mass and Darcy's law in the continuum and network as well as the coupling between them. By introducing proper scaling, we propose a weak form that avoids degeneracy. Well-posedness of the weak form is shown through standard Babu\v ska--Brezzi theory. We also develop the mixed formulation finite-element method and prove its well-posedness. A mass-lumping technique is introduced to derive the two-point flux approximation (TPFA) type discretization as well, due to its importance in applications. Based on the Babu\v ska--Brezzi theory, error estimates can be obtained for both the finite-element scheme and the TPFA scheme. We also discuss efficient linear solvers for discrete problems. Finally, we present some numerical examples to verify the theoretical results and demonstrate the robustness of our proposed discretization schemes.\bfK \bfe \bfy \bfw \bfo \bfr \bfd \bfs . mixed-dimensional problems, mixed-formulation, finite-element method \bfA \bfM \bfS \bfs \bfu \bfb \bfj \bfe \bfc \bft \bfc \bfl \bfa \bfs \bfs \bfi fi\bfc \bfa \bft \bfi \bfo \bfn \bfs . 65N30, 65N15, 65N08, 65N22 \bfD \bfO \bfI .
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