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Backstepping Neural Operators for $2\times 2$ Hyperbolic PDEs

Shanshan Wang, Mamadou Diagne, Miroslav Krstić

TL;DR

The paper addresses stabilization of 2×2 coupled linear hyperbolic PDEs using backstepping and introduces DeepONet-based neural operators to approximate the coupled Goursat-form kernel PDEs that arise in this setting. By proving continuity of the plant-to-kernel mapping and the existence of arbitrarily accurate DeepONet approximations, it shows that learned gains can guarantee stabilization (GES) when used in boundary feedback, and semi-global practical exponential stability (SG-PES) when the full output-feedback law is learned. The approach dramatically speeds up gain computation and is validated through simulations on a representative 2×2 system, with explicit stability bounds that quantify the impact of approximation error. The work thus blends proof-based Lyapunov analysis with data-driven neural operators to enable fast, reliable neural control of infinite-dimensional systems, with potential applications in oil drilling, traffic dynamics, and fluid/flow models.

Abstract

Deep neural network approximation of nonlinear operators, commonly referred to as DeepONet, has proven capable of approximating PDE backstepping designs in which a single Goursat-form PDE governs a single feedback gain function. In boundary control of coupled PDEs, coupled Goursat-form PDEs govern two or more gain kernels-a PDE structure unaddressed thus far with DeepONet. In this paper, we explore the subject of approximating systems of gain kernel PDEs for hyperbolic PDE plants by considering a simple counter-convecting $2\times 2$ coupled system in whose control a $2\times 2$ kernel PDE system in Goursat form arises. Engineering applications include oil drilling, the Saint-Venant model of shallow water waves, and the Aw-Rascle-Zhang model of stop-and-go instability in congested traffic flow. We establish the continuity of the mapping from a total of five plant PDE functional coefficients to the kernel PDE solutions, prove the existence of an arbitrarily close DeepONet approximation to the kernel PDEs, and ensure that the DeepONet-approximated gains guarantee stabilization when replacing the exact backstepping gain kernels. Taking into account anti-collocated boundary actuation and sensing, our $L^2$-Globally-exponentially stabilizing (GES) approximate gain kernel-based output feedback design implies the deep learning of both the controller's and the observer's gains. Moreover, the encoding of the output-feedback law into DeepONet ensures semi-global practical exponential stability (SG-PES). The DeepONet operator speeds up the computation of the controller gains by multiple orders of magnitude. Its theoretically proven stabilizing capability is demonstrated through simulations.

Backstepping Neural Operators for $2\times 2$ Hyperbolic PDEs

TL;DR

The paper addresses stabilization of 2×2 coupled linear hyperbolic PDEs using backstepping and introduces DeepONet-based neural operators to approximate the coupled Goursat-form kernel PDEs that arise in this setting. By proving continuity of the plant-to-kernel mapping and the existence of arbitrarily accurate DeepONet approximations, it shows that learned gains can guarantee stabilization (GES) when used in boundary feedback, and semi-global practical exponential stability (SG-PES) when the full output-feedback law is learned. The approach dramatically speeds up gain computation and is validated through simulations on a representative 2×2 system, with explicit stability bounds that quantify the impact of approximation error. The work thus blends proof-based Lyapunov analysis with data-driven neural operators to enable fast, reliable neural control of infinite-dimensional systems, with potential applications in oil drilling, traffic dynamics, and fluid/flow models.

Abstract

Deep neural network approximation of nonlinear operators, commonly referred to as DeepONet, has proven capable of approximating PDE backstepping designs in which a single Goursat-form PDE governs a single feedback gain function. In boundary control of coupled PDEs, coupled Goursat-form PDEs govern two or more gain kernels-a PDE structure unaddressed thus far with DeepONet. In this paper, we explore the subject of approximating systems of gain kernel PDEs for hyperbolic PDE plants by considering a simple counter-convecting coupled system in whose control a kernel PDE system in Goursat form arises. Engineering applications include oil drilling, the Saint-Venant model of shallow water waves, and the Aw-Rascle-Zhang model of stop-and-go instability in congested traffic flow. We establish the continuity of the mapping from a total of five plant PDE functional coefficients to the kernel PDE solutions, prove the existence of an arbitrarily close DeepONet approximation to the kernel PDEs, and ensure that the DeepONet-approximated gains guarantee stabilization when replacing the exact backstepping gain kernels. Taking into account anti-collocated boundary actuation and sensing, our -Globally-exponentially stabilizing (GES) approximate gain kernel-based output feedback design implies the deep learning of both the controller's and the observer's gains. Moreover, the encoding of the output-feedback law into DeepONet ensures semi-global practical exponential stability (SG-PES). The DeepONet operator speeds up the computation of the controller gains by multiple orders of magnitude. Its theoretically proven stabilizing capability is demonstrated through simulations.
Paper Structure (15 sections, 9 theorems, 111 equations, 14 figures)

This paper contains 15 sections, 9 theorems, 111 equations, 14 figures.

Key Result

Lemma 1

For every $\lambda, \mu \in C^1([0, 1]),\ \sigma, \omega, \theta \in C^0([0, 1])$, and $q\in \mathbbm R$, the gain kernels $k_i(x,\xi), \textcolor{black}{m_i(x,\xi),}\ i=1,2$ satisfying the PDE systems eq:k_1--eq:k_BC_2and eq:m_1--eq:m_BC_2, respectively, has a unique $C^1(\mathcal{T})$ solution where $N_i>0,\ M_i>0,\ i=1,2$ are constants.

Figures (14)

  • Figure 1: Learning of the kernel functions via DeepONet and through the operator described by the mapping $(\lambda,\mu,\omega,\sigma,\theta,q)\to (k_1,k_2,m_1,m_2)$. Computing multiple solutions of kernel PDEs \ref{['eq:k_1']}--\ref{['eq:k_BC_2']} in the Goursat form for different functions $\lambda(x),\ \mu(x),\ \omega(x),\ \sigma(x),\ \theta(x)$ and parameters $q$, completes the training procedure of the Neural Operator $\hat{\mathcal{K}}$.
  • Figure 2: The PDE backstepping observer \ref{['eq:sys_u-obs']}--\ref{['eq:sys_BC_2-obs']} uses boundary measurement of the flux $v(0,t)$. The gains $\hat{k}_i$ and $\hat{m}_i$, $i=1,2$ are produced with the DeepONet $\hat{\mathcal{K}}$.
  • Figure 3: The learning architecture of the observer-based control law in three steps.
  • Figure 4: Instability of the uncontrolled plant of $u(x,t)$ and $v(x,t)$ for given coefficients $\lambda(x) = \Gamma x+1$, $\mu(x)=e^{\Gamma x}+2$, $\delta(x)=\Gamma (x+1)$, $\theta(x)=\Gamma (x + 1)$, $\omega(x)=\Gamma(\cosh(x) + 1)$, $q=\Gamma/3$, $\Gamma=2,\ 5$.
  • Figure 5: The kernel of $k_1(x,\xi)$, $\hat{k}_1(x,\xi)$ and $k_1(x,\xi)-\hat{k}_1(x,\xi)$.
  • ...and 9 more figures

Theorems & Definitions (10)

  • Lemma 1
  • Theorem 1
  • Proposition 1
  • Proposition 2
  • Theorem 2
  • Remark 1
  • Theorem 3
  • Proposition 3
  • Proposition 4
  • Theorem 4