no code implementations • 15 Dec 2023 • Carlos E. Pérez De Jesús, Alec J. Linot, Michael D. Graham
In this work we exploit the symmetries of the Navier-Stokes equations (NSE) and use simulation data to find the manifold where the long-time dynamics live, which has many fewer degrees of freedom than the full state representation, and the evolution equation for the dynamics on that manifold.
no code implementations • 10 Oct 2023 • C. Ricardo Constante-Amores, Alec J. Linot, Michael D. Graham
Additionally, we explore a modified approach where the system alternates between spaces of states and observables at each time step -- this approach no longer satisfies the linearity of the true Koopman operator representation.
no code implementations • 28 Jan 2023 • Alec J. Linot, Kevin Zeng, Michael D. Graham
The high dimensionality and complex dynamics of turbulent flows remain an obstacle to the discovery and implementation of control strategies.
no code implementations • 11 Jan 2023 • Alec J. Linot, Michael D. Graham
For comparison, we show that the models outperform POD-Galerkin models with $\sim$2000 degrees of freedom.
no code implementations • 1 May 2022 • Kevin Zeng, Alec J. Linot, Michael D. Graham
We show that the ROM-based control strategy translates well to the true KSE and highlight that the RL agent discovers and stabilizes an underlying forced equilibrium solution of the KSE system.
no code implementations • 29 Mar 2022 • Alec J. Linot, Joshua W. Burby, Qi Tang, Prasanna Balaprakash, Michael D. Graham, Romit Maulik
We present a data-driven modeling method that accurately captures shocks and chaotic dynamics by proposing a novel architecture, stabilized neural ordinary differential equation (ODE).
no code implementations • 31 Aug 2021 • Alec J. Linot, Michael D. Graham
Then the ODE, in these coordinates, is approximated by a NN using the neural ODE framework.
1 code implementation • 20 Dec 2019 • Alec J. Linot, Michael D. Graham
A data-driven framework is developed to represent chaotic dynamics on an inertial manifold (IM), and applied to solutions of the Kuramoto-Sivashinsky equation.