Основні поняття
The authors present a computational framework for efficiently obtaining multidimensional phase-space solutions of systems of non-linear coupled differential equations using high-order implicit Runge-Kutta Physics-Informed Neural Networks (IRK-PINNs).
Анотація
The authors introduce a versatile algorithm based on time-discrete implicit Runge-Kutta Physics-Informed Neural Networks (IRK-PINNs) to effectively solve a broad range of differential equations, including those describing particle trajectories in physical systems.
Key highlights:
- The IRK-PINN scheme is adapted to handle phase-space coordinates as functions, enabling efficient simulation of particle motion in external fields.
- The approach is particularly useful for explicitly time-independent and periodic force fields, as the phase-space manifold remains unchanged after a single time step propagation.
- The algorithm is validated by generating accurate results for both functional PDEs and equations of motion, including Keplerian orbits in a central Gaussian potential and charged particle motion in a periodic electric field.
- The IRK-PINN method outperforms conventional low-order Runge-Kutta methods, especially for stiff problems and high-frequency oscillations.
- Further work is needed to address the challenge of divergent trajectories, which limits the algorithm's applicability to certain dynamical systems like the Coulomb potential.
Статистика
The force exerted on a particle with charge q by an external electric field E(x, t) is given by F(x, t) = qE(x, t).
The electric field, characterized by an angular frequency ω and incident angle α relative to the x-axis, is represented by the function E(x, t) = (A cos(ωt) cos(α), A cos(ωt) sin(α)), where A denotes the field's amplitude.
The differential equation of motion can be expressed as N[χ] = −(˙x, E(x)).
Цитати
"PINNs can be effectively employed using continuous and discrete representations of time. The time-continuous approach uses space and time variables as inputs, and learn to satisfy the differential equations across the entire domain of interest. This can be impractical without data distributed across multiple time slices. In addition, time-continuous PINNs also encounter difficulties with high-frequency oscillations and stiff problems, lacking a clear strategy to deal with them."
"The discrete-time PINNs learn to model changes within a fixed discrete time step, utilizing only spatial information from a single time slice. This approach improves the accuracy in solving stiff problems by leveraging the A-stability of implicit Runge-Kutta (IRK) methods."