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Geometrically Higher Order Unfitted Space-Time Methods for PDEs on Moving Domains
Numerical Analysis · Submitted 4 Feb 2022
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim These include studies in different dimensions for different polynomial degrees in space and time, validating the higher order accuracy in both variables.
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The abstract, sentence by sentence
In this paper, we propose new geometrically unfitted space-time Finite Element methods for partial differential equations posed on moving domains of higher order accuracy in space and time. As a model problem, the convection-diffusion problem on a moving domain is studied. For geometrically higher order accuracy, we apply a parametric mapping on a background space-time tensor-product mesh. Concerning discretisation in time, we consider discontinuous Galerkin, as well as related continuous (Petrov-)Galerkin and Galerkin collocation methods. For stabilisation with respect to bad cut configurations and as an extension mechanism that is required for the latter two schemes, a ghost penalty stabilisation is employed. The article puts an emphasis on the techniques that allow to achieve a robust but higher order geometry handling for smooth domains. We investigate the computational properties of the respective methods in a series of numerical experiments. These include studies in different dimensions for different polynomial degrees in space and time, validating the higher order accuracy in both variables.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this paper, we propose new geometrically unfitted space-time Finite Element methods for partial differential equations posed on moving domains of higher order accuracy in space and time. | contribution 1.00 | 0.92 | 0.24 | asserted 0.99 |
| s1 | As a model problem, the convection-diffusion problem on a moving domain is studied. | method 0.44 | 0.65 | 0.03 | asserted 0.98 |
| s2 | For geometrically higher order accuracy, we apply a parametric mapping on a background space-time tensor-product mesh. | method 0.98 | 0.89 | 0.05 | asserted 1.00 |
| s3 | Concerning discretisation in time, we consider discontinuous Galerkin, as well as related continuous (Petrov-)Galerkin and Galerkin collocation methods. | method 0.97 | 0.78 | 0.03 | asserted 0.98 |
| s4 | For stabilisation with respect to bad cut configurations and as an extension mechanism that is required for the latter two schemes, a ghost penalty stabilisation is employed. | method 0.98 | 0.83 | 0.05 | asserted 1.00 |
| s5 | The article puts an emphasis on the techniques that allow to achieve a robust but higher order geometry handling for smooth domains. | contribution 0.90 | 0.43 | 0.18 | asserted 0.87 |
| s6 | We investigate the computational properties of the respective methods in a series of numerical experiments. | method 0.60 | 0.94 | 0.04 | asserted 0.96 |
| s7 | These include studies in different dimensions for different polynomial degrees in space and time, validating the higher order accuracy in both variables. | result 0.47 | 0.94 | 0.19 | asserted 0.98 |
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The paper
Original abstract
In this paper, we propose new geometrically unfitted space-time Finite Element methods for partial differential equations posed on moving domains of higher order accuracy in space and time. As a model problem, the convection-diffusion problem on a moving domain is studied. For geometrically higher order accuracy, we apply a parametric mapping on a background space-time tensor-product mesh. Concerning discretisation in time, we consider discontinuous Galerkin, as well as related continuous (Petrov-)Galerkin and Galerkin collocation methods. For stabilisation with respect to bad cut configurations and as an extension mechanism that is required for the latter two schemes, a ghost penalty stabilisation is employed. The article puts an emphasis on the techniques that allow to achieve a robust but higher order geometry handling for smooth domains. We investigate the computational properties of the respective methods in a series of numerical experiments. These include studies in different dimensions for different polynomial degrees in space and time, validating the higher order accuracy in both variables.
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How the literature uses it
2 arXiv papers cite this in 11 sentences
Papers citing it · 7 sentences without a confident label
Uses its method or tool 1 paper
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We explain the space-time mesh deformation on an arbitrary time slab $Q_n$, $n=1,…,N$, also used in [ref] .
An Accurate and Robust Eulerian Finite Element Method for Partial Differential Equations on Evolving Surfaces · Space-time mesh deformation · 0.92
Uses its data or values 1 paper
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As in [ref] , we take $μ= 0.1$.
Space-time unfitted finite element methods for time-dependent problems on moving domains · An example with topology change · 0.99
Compares with it 1 paper
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In contrast to the results reported in [ref] , we do not see any spurious diffusion starting before the time of first contact even though there is only a single full cell between the two disks at the time slab right before contact (see Figure [ref]).
Space-time unfitted finite element methods for time-dependent problems on moving domains · An example with topology change · 0.94
What it cites · 6 sentences without a confident label
Uses the method or tool of 1 paper
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This does not need to be a continuous discrete function, so that we recommend to apply the previously discussed projection only element-wise and skip the final averaging step, called $P_h$ in [ref] .
Isoparametric unfitted BDF -- Finite element method for PDEs on evolving domains · Discontinuous-in-time deformations and mesh transfer operations · 0.90
Cites as background 1 paper
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In characteristic-based methods also known as semi-Lagrangian methods such as those discussed in [ref] instead of the partial derivative $∂/∂t$ the material derivative $d/dt = ∂/∂t + w·∇$ is approximated.
A fourth-order unfitted characteristic finite element method for solving the advection-diffusion equation on time-varying domains · Approaches in the literature · 0.91
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