Download e-book for iPad: A geometric approach to free boundary problems by Luis Caffarelli, Sandro Salsa

By Luis Caffarelli, Sandro Salsa

ISBN-10: 0821837842

ISBN-13: 9780821837849

Loose or relocating boundary difficulties look in lots of parts of research, geometry, and utilized arithmetic. a customary instance is the evolving interphase among a pretty good and liquid section: if we all know the preliminary configuration good adequate, we must always have the ability to reconstruct its evolution, particularly, the evolution of the interphase. during this publication, the authors current a sequence of principles, equipment, and methods for treating the main easy problems with the sort of challenge. particularly, they describe the very primary instruments of geometry and genuine research that make this attainable: homes of harmonic and caloric measures in Lipschitz domain names, a relation among parallel surfaces and elliptic equations, monotonicity formulation and stress, and so on. The instruments and concepts awarded right here will function a foundation for the research of extra advanced phenomena and difficulties. This e-book turns out to be useful for supplementary examining or can be a very good self sufficient examine textual content. it's appropriate for graduate scholars and researchers attracted to partial differential equations.

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U+ (x) ≥ c d(x, F (u) , x ∈ Ω+ (u) and sup u+ ≥ C r Br (x0 ) x0 ∈ F (u) . Let’s see what are the minimal assumptions to achieve this kind of results. A parallel with viscosity solutions of elliptic equations Lv = Tr(A(x)D2 v) = 0 is in order. A linear growth and the non degeneracy for u+ correspond to having a Harnack inequality (controlled growth) for v and this is true, for instance, if L is strictly elliptic (A(x) ≥ λI) and A is bounded measurable. 43 44 3. THE REGULARITY OF THE FREE BOUNDARY For our free boundary problem, the parallel requirement is that 0 < c < u+ ν ≤ C in the viscosity sense.

Put e¯ = γδe1 + e, where e1 ∈ span{e, ν}, |e1 | = 1, e1 , e = 0, γ ≤ 13 C1 (μ, θ0 ), and let σ:σ ¯ = σ + ρ(σ)σ 1 , σ ∈ ∂Γ(θ, e)} Sμ = {¯ where |σ 1 | = 1, σ 1 , σ = 0, σ 1 ∈ span{e, σ}. Then, if γ = γ(μ, θ0 ) is small enough, for every σ ¯ ∈ ∂Sμ , α( σ ¯ , e¯ ) ≥ θ + γδ ≡ θ¯ . 4. LIPSCHITZ FREE BOUNDARIES ARE C 1,γ 58 ¯ e¯) with Thus Sμ ⊂ Sμ and contains the cone Γ( θ, π π ¯ − θ ≤ (1 − γ) −θ . 3. 2 holds also if we fix any θ , θ2 ≤ θ < θ and put, for every ¯ , e), σ ∈ Γ(θ π E(σ) = − α(σ, ν) − (θ − θ ) 2 ρ(σ) = |σ| sin θ − θ + μE(σ) Sμ = Bρ(σ) (σ) ¯ ,e) σ∈Γ(θ The constant λ still depends only on μ and θ0 .

We write 1 1 u uε Δw = ε BR ε Now, by the linear growth of u: 1 − ε u uε wν dσ + ∂BR ∂BR 1 ε w Δ(u uε ) . BR u uε wν dσ ≥ c0 R and, for σ small, 1 ε u uε Δw ≤ − BR u+ ≤ c¯σR < BσR c0 R. 2 Hence 1 1 |∇u|2 ≥ ε BR ∩{0

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A geometric approach to free boundary problems by Luis Caffarelli, Sandro Salsa


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