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Stable $C^1$-conforming finite element methods for a class of nonlinear fourth-order evolution equations

Agus L. Soenjaya, Thanh Tran

Abstract

We propose some finite element schemes to solve a class of fourth-order nonlinear PDEs, which include the vector-valued Landau--Lifshitz--Baryakhtar equation, the Swift--Hohenberg equation, and various Cahn--Hilliard-type equations with source and convection terms, among others. The proposed numerical methods include a spatially semi-discrete scheme and two linearised fully-discrete $C^1$-conforming schemes utilising a semi-implicit Euler method and a semi-implicit BDF method. We show that these numerical schemes are stable in $\mathbb{H}^2$. Error analysis is performed which shows optimal convergence rates in each scheme. Numerical experiments corroborate our theoretical results.

Stable $C^1$-conforming finite element methods for a class of nonlinear fourth-order evolution equations

Abstract

We propose some finite element schemes to solve a class of fourth-order nonlinear PDEs, which include the vector-valued Landau--Lifshitz--Baryakhtar equation, the Swift--Hohenberg equation, and various Cahn--Hilliard-type equations with source and convection terms, among others. The proposed numerical methods include a spatially semi-discrete scheme and two linearised fully-discrete -conforming schemes utilising a semi-implicit Euler method and a semi-implicit BDF method. We show that these numerical schemes are stable in . Error analysis is performed which shows optimal convergence rates in each scheme. Numerical experiments corroborate our theoretical results.
Paper Structure (14 sections, 29 theorems, 221 equations, 6 figures)

This paper contains 14 sections, 29 theorems, 221 equations, 6 figures.

Key Result

Lemma 2.1

For any vector-valued function $\boldsymbol{v}:\Omega\to\mathbb{R}^3$, we have provided that the partial derivatives are well defined.

Figures (6)

  • Figure 1: Order of convergence for experiment 1.
  • Figure 2: Snapshots of the magnetic spin field $\boldsymbol{u}$ (projected onto $\mathbb{R}^2$) at given times in experiment 1. The colours indicate relative magnitude of the vectors.
  • Figure 3: Order of convergence for experiment 2.
  • Figure 4: Snapshots of the magnetic spin field $\boldsymbol{u}$ (projected onto $\mathbb{R}^2$) at given times in experiment 2. The colours indicate relative magnitude of the vectors.
  • Figure 5: Order of convergence for experiment 3.
  • ...and 1 more figures

Theorems & Definitions (59)

  • Lemma 2.1
  • proof
  • Lemma 2.2
  • proof
  • Lemma 2.3
  • proof
  • Lemma 2.4
  • proof
  • Proposition 3.1
  • proof
  • ...and 49 more