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Explicit local Lipschitz bound for the regularized SPH vector field

Statement

Let K be a nonempty compact convex subset of the positive-density domain of Fixed-width regularized conservative SPH particle system. Use ||z||#=max_i{|q_i|,|v_i|,|e_i|}, M=Σ_im_i, V=sup_{z∈K}max_i|v_i|, K₁=||∇W_ε||∞, K₂=||D²W_ε||∞, and a(ρ,e)=P(ρ,e)/ρ². Define A₀=max_{z∈K,1≤i≤N}|a(ρ_i(q),e_i)|, A_ρ=max_{z∈K,1≤i≤N}|∂ρa(ρ_i(q),e_i)|, A_e=max{z∈K,1≤i≤N}|∂_ea(ρ_i(q),e_i)|, and A_Lip=2MK₁A_ρ+A_e. By A continuous real-valued function on a nonempty compact metric space is bounded and attains a greatest and a least value, these maxima are finite and attained, since K is nonempty compact and the functions involved are continuous. Then the full state vector field F is Lipschitz on K with constant

L=max⁡{1, M(2K1ALip+4A0K2), 2MVALipK1+2MA0K1+4MA0VK2}.

Facts & Assumptions

Given: A nonempty compact convex positive-density tube K, the fixed finite masses, a C¹ pressure map P, and a C² kernel W_ε.

[F1]

Fixed-width regularized conservative SPH particle system: ρ_i=Σ_jm_jW_ε(q_i−q_j), A_i=a(ρ_i,e_i), and the q, v and e components of F are the displayed finite sums.

[F2]

Scaling identities for kernel moments and derivatives: ||∇W_ε||∞=K₁ and ||D²W_ε||∞=K₂ are finite for fixed ε.

[F4]

A continuous real-valued function on a nonempty compact metric space is bounded and attains a greatest and a least value: continuous real-valued functions on a nonempty compact metric space are bounded and attain their maxima and minima.

[F5]

The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a): derivatives of the density and pressure-coefficient compositions are given by the chain rule.

Proof

1.1F1F2F3F5F6F7algebraF4

Let z,z′∈K, δ=||z−z′||#, and z(s)=(1−s)z+sz′ for 0≤s≤1; convexity keeps this segment in K. Differentiating ρ_i(q(s)) using [F5] and the finite-sum rule [F6] gives Σ_jm_j∇W_ε(q_i(s)−q_j(s))·(q_i′−q_i−q_j′+q_j), whose absolute value is at most 2MK₁δ by [F1], [F2], and Cauchy-Schwarz [F7]. Along the same segment, A_i(s)=a(ρ_i(q(s)),e_i(s)) has derivative bounded by 2MK₁A_ρδ+A_eδ=A_Lipδ, by [F5]. The one-dimensional mean value inequality [F3] on s∈[0,1] yields |A_i−A_i′|≤A_Lipδ.

2.1F1F2F3F7step 1.1algebra

For the acceleration component, subtract its two finite sums. The coefficient difference contributes at most 2MA_LipK₁δ, and the kernel-gradient difference at most 4MA₀K₂δ because the triangle inequality [F7] gives |(q_i−q_j)−(q_i′−q_j′)|≤2δ and [F3] bounds the change in ∇W_ε by K₂ times its argument change. Thus |v̇_i−v̇_i′|≤M(2A_LipK₁+4A₀K₂)δ.

3.1F1F2F3F7step 1.1algebra∎

For ė_i, the coefficient difference contributes at most 2MVA_LipK₁δ; the relative-velocity difference at most 2MA₀K₁δ by the triangle inequality [F7]; and the kernel-gradient difference at most 4MA₀VK₂δ by [F3]. Also |q̇_i−q̇_i′|≤δ. Taking the maximum of the three component bounds gives the stated L.

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