2009
DOI: 10.1002/nme.2524
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A time‐staggered partitioned coupling algorithm for transient heat conduction

Abstract: SUMMARYWe present a time-staggered partitioned coupling algorithm for transient heat conduction finite element simulations. This algorithm divides a large structural mesh into a number of smaller subdomains, solves the individual subdomains separately and couples the solutions to obtain the response to the original problem. The proposed algorithm is a mixed multi-timestep algorithm and enables arbitrary time integration schemes and meshes to be coupled with different timesteps in the various subdomains. In thi… Show more

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Cited by 27 publications
(9 citation statements)
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“…The use of different time-steps in different subdomains is referred to as multi-time-stepping or subcycling. Some representative works in this direction are [12][13][14]. But many of the prior efforts on mixed methods and multi-time-stepping suffer from one or more of the following deficiencies: (i) The method cannot handle multiple subdomains.…”
Section: Introductionmentioning
confidence: 99%
“…The use of different time-steps in different subdomains is referred to as multi-time-stepping or subcycling. Some representative works in this direction are [12][13][14]. But many of the prior efforts on mixed methods and multi-time-stepping suffer from one or more of the following deficiencies: (i) The method cannot handle multiple subdomains.…”
Section: Introductionmentioning
confidence: 99%
“…A more detailed description of the modelling approaches can be found in [3]. Besides adaptivity techniques in both, the spatial and temporal domain and an in Section 22: Scientific computing time integrated heat source, the computational domain is, based on [4], split into sub-domains Ω i , leading to:…”
Section: Thermal Model and Multi-time-steppingmentioning
confidence: 99%
“…The respective parts in black correspond to the weak form of the thermal problem for the sub-domains (κ, f and q denote the thermal conductivity, a heat source and boundary fluxes), whereas the red parts arise due to the weak imposition of the constraints on the interface Γ, that aim to set the jumps of the temperatures as well as the jumps of the fluxes to zero (l denotes the smallest edge length of the mesh and η a penalty parameter used for the weak imposition). In the present approach the interface terms a treated explicit in time, which decouples the sub-domains and allows for a separate integration in time [4].…”
Section: Thermal Model and Multi-time-steppingmentioning
confidence: 99%
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“…The proposed methods were not A‐stable and made use of stabilization techniques that often depended on arbitrary constants. In 14, the authors presented similar algorithms with implicit–explicit coupling, in order to use explicit integrators with fine time steps in stiff mesh regions and implicit integrators with coarse time steps in non‐stiff mesh regions. They employed the generalized‐α method 15 and the classical fourth‐order RK scheme to analyze the implications of different time integrators.…”
Section: Introductionmentioning
confidence: 99%