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Joint fill-distance and kernel-width refinement for value and derivative consistency
Statement
Assume the hypotheses of Explicit cellwise error for kernel value and gradient quadrature and let f∈C³(R^d) have bounded derivatives. There are constants C₀,C₁, independent of ε,h and the interior point x, such that
Thus ε→0 and h/ε²→0 suffice for both value and derivative errors to vanish uniformly at interior points. Constants depend only on the fixed kernel, dimension, and cell regularity.
Facts & Assumptions
Given: An admissible kernel, a cell rule with the fill-radius and local-volume bounds of Meshfree cell quadrature and fill radius, h≤ε≤1, an interior point, and f∈C³ with bounded f and derivatives through order three.
Second-order convolution bias for an interior C² field: |S_εf−f|≤(m₂/2)ε²||D²f||∞.
Second-order bias for the kernel particle gradient: |D_εf−∇f|≤(m₃/6)ε²||D³f||∞.
Explicit cellwise error for kernel value and gradient quadrature: the value and derivative quadrature errors are bounded by the two displayed h-terms.
Proof
Add and subtract S_εf(x): |Q⁰_{ε,h}f−f|≤|Q⁰_{ε,h}f−S_εf|+|S_εf−f|. Apply [F1] and the first bound in [F3] to obtain the first inequality after increasing constants.
Add and subtract D_εf(x): |Q¹_{ε,h}f−∇f|≤|Q¹_{ε,h}f−D_εf|+|D_εf−∇f|. Apply [F2] and the second bound in [F3] to obtain the second inequality.
If ε→0 and h/ε²→0, then ε²→0, h/ε²→0, and h/ε≤h/ε² because ε≤1. Every term on the right sides of steps 1.1 and 1.2 therefore tends to zero uniformly at the stated interior points.
Depends on
Used by
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Sources
- Volker Springel, Smoothed Particle Hydrodynamics in Astrophysics, Annual Review of Astronomy and Astrophysics 48 (2010), author full text (standard reference, not scraped)
- Benjamin Seibold, MIT OpenCourseWare 18.336, Numerical Methods for Partial Differential Equations, Lecture 25: Particle Methods (Spring 2009) (standard reference, not scraped)