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Supremum norm stability for forced heat problems

Statement

Assume Countable Choice. Let Ω⊆Rn be nonempty, bounded and open, T>0, and let real u,v∈C2,1(Ω‾×[0,T]) solve ut−Δu=f, vt−Δv=g with f,g∈C(Ω‾×[0,T]). Put a=∥u(⋅,0)−v(⋅,0)∥∞, bt=sup⁡∂Ω×[0,t]∣u−v∣, and m(s)=max⁡Ω‾∣f(⋅,s)−g(⋅,s)∣. Then for 0<t≤T, sup⁡Ω‾×[0,t]∣u−v∣≤max⁡(a,bt)+∫0tm(s)ds, and hence also the bound with a+bt in place of the maximum.

Facts & Assumptions

Given: Countable Choice, a bounded open Ω⊆Rn, T>0, real u,v∈C2,1(Q‾) on Q=Ω×(0,T] with ut−Δu=f and vt−Δv=g in Q for continuous f,g, and 0<t≤T.

[A1]

Countable Choice is the ambient hypothesis (The Axiom of Countable Choice (ACω)).

[F1]

Cylinder convention and parabolic boundary: the class C2,1(Q‾), the closed cylinder Ω‾×[0,T] and ∂p(Ω×(0,t])=(Ω‾×{0})∪(∂Ω×[0,t]) are those of Parabolic cylinder and parabolic boundary.

[F2]

Comparison: if U,V∈C2,1(Q‾) with Q=Ω×(0,t], Ut−ΔU≤Vt−ΔV in Q and U≤V on ∂pQ, then U≤V on Q‾ (Comparison and uniqueness for the bounded-cylinder heat problem).

[F4]

Fundamental theorem of calculus, first part: if φ is continuous on [0,t], then s↦∫0sφ is differentiable with derivative φ (The first fundamental theorem: if f is integrable on [a,b] and continuous at c, then F′(c)=f(c); in particular a continuous f has F as a primitive), continuity on a compact interval supplying the integrability used to form the integral (A continuous function on [a,b] is Riemann integrable, by Heine-Cantor and Riemann's criterion).

[F5]

The Laplacian is Δw=∑i∂i∂iw (The Laplacian of a C2 function and of a C2 vector field), the partial derivatives being those of Directional derivatives and partial derivatives of a map U⊆Rm→Rn; a function of the time variable alone has all its x-partial derivatives 0, and ±m is an admissible forcing for the comparison principle.

Proof

Given: Countable Choice, bounded Ω, T>0, solutions u,v∈C2,1(Q‾) of ut−Δu=f, vt−Δv=g, continuous f,g, and 0<t≤T.

1.1A1F1F3given

Put w:=u−v and Qt:=Ω×(0,t]. Then w∈C2,1(Qt‾) with wt−Δw=f−g in Qt, and on the parabolic boundary of Qt one has ∣w∣≤a on Ω‾×{0} and ∣w∣≤bt on ∂Ω×[0,t] by the definitions of a and bt; moreover the function s↦m(s)=max⁡Ω‾∣f(⋅,s)−g(⋅,s)∣ is well defined on [0,t] and continuous there: it is a maximum of a continuous function on the compact Ω‾ for each s by [F3], and given ε>0, uniform continuity of f and g on the compact Q‾ [F3] gives δ>0 such that ∣f(x,s)−f(x,s0)∣<ε/2 and ∣g(x,s)−g(x,s0)∣<ε/2 for all x∈Ω‾ whenever ∣s−s0∣<δ, whence ∣m(s)−m(s0)∣≤ε.

2.1step 1.1F4F5given

Let M:=max⁡(a,bt)≥0 and for s∈[0,t] put W+(s):=M+∫0sm(σ) dσ and W−(s):=−M−∫0sm(σ) dσ, viewed as functions of (s,x). By [F4] and the continuity of m from step 1.1, both are of class C2,1(Qt‾) with (W±)t−ΔW±=±m: the time derivative is ±m(s) by [F4] and every x-partial derivative vanishes because W± depends on s alone, so ΔW±=0 by [F5]. On the parabolic boundary of Qt one has W−≤−M≤w≤M≤W+, since ∣w∣≤M there by step 1.1.

3.1step 1.1step 2.1F2given

Comparison applied twice. For the pair (U,V)=(w,W+): wt−Δw−(W+,t−ΔW+)=(f−g)−m≤0 in Qt and w≤W+ on ∂pQt by step 2.1, so [F2] gives w≤W+ on Qt‾. For the pair (U,V)=(W−,w): W−,t−ΔW−−(wt−Δw)=−m−(f−g)≤0 in Qt and W−≤w on ∂pQt by step 2.1, so [F2] gives W−≤w on Qt‾. Therefore ∣w(s,x)∣≤M+∫0sm(σ) dσ for every (s,x)∈[0,t]×Ω‾.

4.1step 3.1given∎

Since s↦∫0sm is nondecreasing on [0,t] (the integrand is nonnegative), step 3.1 gives ∣u−v∣≤M+∫0tm on Ω‾×[0,t], hence sup⁡Ω‾×[0,t]∣u−v∣≤max⁡(a,bt)+∫0tm(s) ds. Finally max⁡(a,bt)≤a+bt, so the same estimate holds with a+bt in place of the maximum.

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