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A square-root global error bound for projected Euler with certified projection tolerances

Statement

Assume the hypotheses of Existence and uniqueness for projected dynamics and convergence of projection Euler under countable and dependent choice, including Countable Choice and Dependent Choice, and let x be its unique solution. Let D be any finite bound for the diameter of C, set M=∥f(0,x0)∥2+L(T+D),C0=8M2+L2(1+M)2T,Kerr=C0Te(2L+1)T. For h=T/N, let Xh be the affine interpolant of the exact projection Euler recurrence. If a complete run of Projected Euler with certified inexact projection solves returns nodes x~k with certified residuals sup⁡z∈C⟨x~k+hf(tk,x~k)−x~k+1,z−x~k+1⟩≤εk2, and X~h is their affine interpolant, then sup⁡0≤t≤T∥X~h(t)−x(t)∥2≤Kerrh+eLT∑k=0N−1εk. In particular, the exact-projection branch has uniform error O(h). Certified projection errors with ∑kεk=O(h) retain that rate; no rate follows from an uncertified solver tolerance alone.

Facts & Assumptions

Given: The data, Countable Choice and Dependent Choice assumptions of Existence and uniqueness for projected dynamics and convergence of projection Euler under countable and dependent choice, and a completed inexact projected-Euler run with the residual certificates in the Statement.

[A1]

The Axiom of Countable Choice (ACω) is assumed as in [F1] to obtain the exact solution x; the estimates use no additional countable choices.

[A2]

The axiom of dependent choice: a relation in which every element is related to something admits an N-indexed chain is assumed as in [F1] to obtain the exact solution x; the estimates use no additional dependent choices.

[F1]

Existence and uniqueness for projected dynamics and convergence of projection Euler under countable and dependent choice: there is a unique absolutely continuous x satisfying f(t,x)−x˙∈NC(x) almost everywhere.

[F4]

A certified projection variational residual bounds the projection error: a feasible candidate with variational residual at most ε2 is within distance ε of its exact projection.

[F5]

Projected Euler with certified inexact projection solves: a completed run returns feasible nodes with the residual certificates specified in the algorithm Definition.

[F7]

The product of two absolutely continuous functions is absolutely continuous and Fundamental theorem of calculus for absolutely continuous functions: products of AC components are AC with the product derivative a.e., and the derivative integrates to the endpoint difference.

[F10]

Gronwall's integral inequality with variable and constant coefficients: if u≥0 is continuous and u(t)≤A+∫0tbu for constants A,b≥0, then u(t)≤Aebt.

[F11]

Projected contact dynamics and explicit projection Euler step: the outward cone is NC(x)={n:⟨n,z−x⟩≤0 for every z∈C}, and an exact projection step satisfies xk+1=PC(xk+hf(tk,xk)).

Proof

1.1A1A2F1F3F6F8F11F12givenchoosealgebra

By [F12], compactness makes C closed, so the projection and normal-cone hypotheses in [F11] and [F3] apply to the stated set. Let Xh be the exact affine Euler interpolant, Xˉh(t)=xk+1 on [tk,tk+1), Fh(t)=f(tk,xk), and nh=Fh−X˙h. The projection variational inequality in [F11] gives nh(t)∈NC(Xˉh(t)). Nonexpansiveness [F3] gives ∥X˙h∥2≤M and ∥Xˉh−Xh∥2≤hM, so ∥nh∥2≤2M. For the exact solution put n(t)=f(t,x(t))−x˙(t)∈NC(x(t)). At almost every differentiability point, x(t+s)∈C on both sides of t; the normal inequality with z=x(t+s), divided by positive and negative s and passed to the limit, gives ⟨n(t),x˙(t)⟩=0. Hence ∥x˙(t)∥22=⟨f(t,x(t)),x˙(t)⟩, so Cauchy–Schwarz [F8] gives ∥x˙(t)∥2≤M and ∥n(t)∥2≤2M.

1.2F3F4F5F9givenalgebrainduction

By [F4] and [F5], each inexact node is within εk of the exact projection of its own unprojected input. Comparing it with the exact node and using [F3] and the state-Lipschitz bound gives ∥x~k+1−xk+1∥2≤(1+hL)∥x~k−xk∥2+εk. Iteration from the common initial point yields max⁡k∥x~k−xk∥2≤(1+hL)N∑kεk. By [F9], (1+hL)N≤eNhL=eLT.

2.1F1F2F6F7F8step 1.1givenalgebra

Put eh=Xh−x and Eh=∥eh∥22. By [F6]–[F7], Eh is absolutely continuous and Eh′=2⟨X˙h−x˙,eh⟩ almost everywhere. Monotonicity [F2] at Xˉh and x gives ⟨nh−n,Xˉh−x⟩≥0. Since ∥Xˉh−Xh∥2≤hM and ∥nh−n∥2≤4M, differentiation yields 12Eh′≤LEh+Lh(1+M)Eh+4M2h. Indeed, ∥Fh−f(t,x)∥2≤L(h+∥xk−x(t)∥2)≤L(∥eh∥2+h(1+M)) using the within-step displacement bound; [F8] bounds its inner product with eh.

3.1F7F10step 2.1givenalgebra

Since (Eh−Lh(1+M))2≥0, we have Lh(1+M)Eh≤12Eh+12L2(1+M)2h2. Thus Eh′≤(2L+1)Eh+8M2h+L2(1+M)2h2≤(2L+1)Eh+C0h, since h≤T. Integrating the inequality and using Eh(0)=0 gives Eh(t)≤C0hT+(2L+1)∫0tEh(s) ds. By [F10], sup⁡tEh(t)≤C0hTe(2L+1)T, hence sup⁡t∥Xh(t)−x(t)∥2≤Kerrh.

4.1step 3.1step 1.2givenalgebra∎

On each mesh cell, X~h−Xh is the affine interpolation of its endpoint errors, so its norm is at most the larger endpoint norm. The triangle inequality with step 3.1 gives sup⁡t∥X~h(t)−x(t)∥2≤Kerrh+eLT∑kεk, which is the claimed estimate. If εk=0 all k, or if their sum is O(h) along a refining mesh, the stated O(h) rate follows.

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