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When using the improved max approximator, but not area weighting, the resulting barrier potential can be negative (i.e., attractive instead of repulsive). This only occurs in cases of parallel edges using the mollified formulation. The issue does not occur when using area weighting.
Background
Edge-edge mollification is still used, but not mentioned in the Convergent IPC paper. The original mollified edge-edge energy is
and $E \cap x$ is the set of edges that contain $x$ as an end-point. The function $m$ is our edge-edge mollification function
$$
m = \begin{cases}-\frac{1}{\epsilon_{\times}^2} c^2+\frac{2}{\epsilon_{\times}} c & c<\epsilon_{\times}, \ 1 & c \geq \epsilon_{\times},\end{cases}
$$
where $c= |e_1 \times e_2 |^2$ and $\epsilon_{\times}=10^{-3} |\bar{e}_1|^2 |\bar{e}_2|^2.$
Environment (please complete the following information):
OS and Version: macOS
Compiler and Version: Apple clang version 16.0.0
The text was updated successfully, but these errors were encountered:
When using the improved max approximator, but not area weighting, the resulting barrier potential can be negative (i.e., attractive instead of repulsive). This only occurs in cases of parallel edges using the mollified formulation. The issue does not occur when using area weighting.
Background
Edge-edge mollification is still used, but not mentioned in the Convergent IPC paper. The original mollified edge-edge energy is
The improved max approximator with mollification is
where
and$E \cap x$ is the set of edges that contain $x$ as an end-point. The function $m$ is our edge-edge mollification function
where$c= |e_1 \times e_2 |^2$ and $\epsilon_{\times}=10^{-3} |\bar{e}_1|^2 |\bar{e}_2|^2.$
Environment (please complete the following information):
The text was updated successfully, but these errors were encountered: