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Regularization of the collision in the electromagnetic two-body problem.
Efrain Buksman Hollander1, Jayme De Luca
1Universidade Federal de São Carlos, Departamento de Física, Rodovia Washington Luis, km 235, Caixa Postal 676, São Carlos, São Paulo 13565-905, Brazil.
Chaos (Woodbury, N.Y.)
|December 1, 2004
Summary
This study presents a regular differential equation for simulating the collision of two equal-mass bodies in relativistic electrodynamics. It uses a novel numerical method to accurately calculate collision orbits, ensuring stable, non-runaway solutions for this complex conservative system.
Area of Science:
- Theoretical Physics
- Computational Physics
- Electrodynamics
Background:
- Relativistic action-at-a-distance electrodynamics involves complex two-body interactions.
- Simulating collisions in such systems presents mathematical challenges due to singularities.
- Historical context includes foundational work by Dirac, Wheeler, and Feynman.
Purpose of the Study:
- To derive a regular differential equation for the collision of two equal-mass bodies.
- To develop a stable numerical method for calculating collision orbits.
- To analyze the physics of this conservative dynamical system.
Main Methods:
- Derivation of a regular differential equation using Poincaré invariance and energy constants.
- Definition of finite variables and derivatives at the point of collision.
- Numerical calculation of collision orbits via a self-consistent minimization method.
Main Results:
- A regularized differential equation applicable to two-body collisions in relativistic electrodynamics.
- Successful numerical computation of collision orbits using a stable, non-runaway solution selection method.
- Demonstration of finite variables and derivatives at the collision point.
Conclusions:
- The derived regular equation provides a robust method for studying relativistic two-body collisions.
- The numerical approach ensures stability and accuracy in simulating complex dynamical systems.
- This work advances the understanding of covariant time-symmetric two-body dynamics.