We introduce a time adaptive multirate method based on the Dirichlet-Neumann waveform relaxation (DNWR) algorithm for the simulation of two coupled linear heat equations with strong jumps in the material coefficients across the interface. Numerical results are included to illustrate the advantages of the time adaptive approach over the multirate approach and the robustness of the multirate DNWR method with respect to its sibling, the multirate Neumann-Neumann waveform relaxation (NNWR) method introduced in a previous work [3].
Model problemThe unsteady transmission problem reads as follows, where we consider a domain Ω ⊂ R d which is cut into two subdomains Ω = Ω 1 ∪ Ω 2 with transmission conditions at the interface Γ = ∂Ω 1 ∩ ∂Ω 2 :where t ∈ [T 0 , T f ] and n m is the outward normal to Ω m for m = 1, 2. The constants λ 1 and λ 2 are the thermal conductivities on Ω 1 and Ω 2 respectively. D 1 and D 2 are the thermal diffusivities defined by D m = λm αm with α m = ρ m c pm where ρ m represents the density and c pm the specific heat capacity of the material on Ω m , m = 1, 2.
The Dirichlet-Neumann waveform relaxation algorithmThe Dirichlet-Neumann waveform relaxation (DNWR) method introduced in [2] starts with an initial guess g 0 (x, t) on the interface Γ × (T 0 , T f ], and then performs a three-step iteration. At each iteration k, imposing continuity of the solution across the interface, one first finds the local solution u k+1 1 (x, t) on Ω 1 by solving the Dirichlet problem (2). Then, imposing continuity of the heat fluxes across the interface, one finds the local solution u k+1 2