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This paper studies the mixed element method for the boundary value problem of the biharmonic equation Δ 2 u = f {Δ²u=f} in two dimensions. We start from a u ∼ ∇ u ∼ ∇ 2 u ∼ div ∇ 2 u {u~∇ u~∇²u∇²u} formulation that is discussed in [4] and construct its stability on H 0 1 ( Ω ) × H ~ 0 1 ( Ω ) × L ¯ sym 2 ( Ω ) × H - 1 ( div , Ω ) {H¹₀(Ω)̃¹₀(Ω)̄sym^% {2}(Ω)× H⁻¹(div,Ω)} . Then we utilise the Helmholtz decomposition of H - 1 ( div , Ω ) {H⁻¹(div,Ω)} and construct a new formulation stable on first-order and zero-order Sobolev spaces. Finite element discretisations are then given with respect to the new formulation, and both theoretical analysis and numerical verification are given.
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Li et al. (2017) studied this question.
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