English

Explicit Discrete Solution for Some Optimization Problems and Estimations with Respect to the Exact Solution

Numerical Analysis 2026-03-13 v1 Numerical Analysis

Abstract

We consider two steady-state heat conduction systems called, SS and SαS_\alpha, in a multidimensional bounded domain DD for the Poisson equation with source energy gg. In one system, we impose mixed boundary conditions (temperature bb on the boundary Γ1\Gamma_1, heat flux qq on Γ2\Gamma_2 and an adiabatic condition on Γ3\Gamma_3). In the other system, the condition on Γ1\Gamma_1 is replaced by a convective heat flux condition with coefficient α\alpha. For each of these systems, we consider three associated optimization problems (Pi)(P_{i}) and (Piα)(P_{i\alpha }), i=1,2,3i=1,2,3, where the variable is the source energy gg, the heat flux qq and the environmental temperature bb, respectively. In the particular case where DD is a rectangle, the explicit continuous optimization variables and the corresponding state of the systems are known. In the present work, by using a finite difference scheme, we obtain the discrete systems (Sh)({S^h}) and (Sαh){(S^h_\alpha)} and discrete optimization problems (Pih){(P^h_i)} and (Piαh){(P^h_{i \alpha})}, i=1,2,3i=1,2,3, where hh is the space step in the discretization. Explicit discrete solutions are found, and convergence and estimation errors results are proved when hh goes to zero and when α\alpha goes to infinity. Moreover, some numerical simulations are provided in order to test theoretical results. Finally, we note that the use of a three-point finite-difference approximation for the Neumann or Robin boundary condition at the boundary improves the global order of convergence from O(h)O(h) to O(h2)O(h^2).

Keywords

Cite

@article{arxiv.2603.11313,
  title  = {Explicit Discrete Solution for Some Optimization Problems and Estimations with Respect to the Exact Solution},
  author = {Julieta Bollati and Mariela C. Olguin and Domingo A. Tarzia},
  journal= {arXiv preprint arXiv:2603.11313},
  year   = {2026}
}
R2 v1 2026-07-01T11:15:34.694Z