Core Concepts
A novel numerical algorithm is proposed for computing α-dissipative solutions of the Hunter-Saxton equation, where α belongs to W^{1,∞}(R, [0,1)). The method combines a projection operator with a generalized method of characteristics and an iteration scheme to handle the unknown energy loss at wave breaking occurrences.
Abstract
The content presents a new numerical algorithm for computing α-dissipative solutions of the Hunter-Saxton (HS) equation. The HS equation is known to develop singularities in finite time, leading to a loss of uniqueness for weak solutions. To properly describe the solution and its energy, a finite, nonnegative Radon measure is introduced.
The proposed algorithm extends a previous method from the authors, which was limited to constant α. The key challenges addressed here are:
The amount of energy to be removed at wave breaking occurrences cannot be computed a priori, as it depends on the spatial location of the wave breaking. An iteration scheme is introduced to approximate this energy loss.
The possibility of accumulating wave breaking times is handled by extracting a finite sequence of breaking times that acts as a non-uniform temporal discretization. This reduces the computational complexity compared to repeatedly computing the particle trajectories at nearly identical wave breaking times.
The numerical implementation details are provided, including the projection operator, the computation of the wave breaking function, and the time evolution via the iteration scheme. Convergence of the numerical solution in C([0,T], L^∞(R)) for any finite T ≥ 0 is also established.