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Optimal Control of H-Mode Tokamak Plasma Temperature based on Pontryagin's Principle

Slim Jmal, Matteo Tacchi-Bénard, Emmanuel Witrant

TL;DR

This work develops a forward-looking, adjoint-based optimal control framework for Tokamak plasma temperature, casting the problem as a PDE-constrained optimization with a continuum of receding horizons. By coupling a nonlinear diffusion model for $T_e(x,t)$ with an extended Bohm/gyro-Bohm diffusivity and a receding-horizon Pontryagin principle, the authors derive a forward-in-time feedback controller via a state–costate system and an adaptive regularization parameter $α(t)$. They establish regularity and convergence properties, and validate the approach on Tore Supra data, showing exponential error decay and bounded control energy while achieving near-perfect tracking of the target profile. The methodology bridges PMP theory and model-predictive control in infinite-dimensional settings, offering a scalable, real-time capable tool for achieving robust, energy-efficient high-confinement operation in current and future fusion devices.

Abstract

This paper studies the decay of an objective functional using a new control technique within Pontryagin's framework. Convergence analysis is carried out on the infinite-dimensional space of Tokamak plasma dynamical state as described by weakly decoupled nonlinear partial differential equations. An adjoint-based optimal control is derived to minimize the deviation from a predefined dynamical trajectory leading to the desired target state at stationary regime, by turning Pontryagin's transversality conditions into a continuum of horizons. A feedback controller is proposed to steer the system efficiently in real time, as opposed to an open-loop controller resulting from the classical Pontryagin's setting. An algorithm synthesizing the constraint-free optimal controller is used for profile tracking based on experimental data.

Optimal Control of H-Mode Tokamak Plasma Temperature based on Pontryagin's Principle

TL;DR

This work develops a forward-looking, adjoint-based optimal control framework for Tokamak plasma temperature, casting the problem as a PDE-constrained optimization with a continuum of receding horizons. By coupling a nonlinear diffusion model for with an extended Bohm/gyro-Bohm diffusivity and a receding-horizon Pontryagin principle, the authors derive a forward-in-time feedback controller via a state–costate system and an adaptive regularization parameter . They establish regularity and convergence properties, and validate the approach on Tore Supra data, showing exponential error decay and bounded control energy while achieving near-perfect tracking of the target profile. The methodology bridges PMP theory and model-predictive control in infinite-dimensional settings, offering a scalable, real-time capable tool for achieving robust, energy-efficient high-confinement operation in current and future fusion devices.

Abstract

This paper studies the decay of an objective functional using a new control technique within Pontryagin's framework. Convergence analysis is carried out on the infinite-dimensional space of Tokamak plasma dynamical state as described by weakly decoupled nonlinear partial differential equations. An adjoint-based optimal control is derived to minimize the deviation from a predefined dynamical trajectory leading to the desired target state at stationary regime, by turning Pontryagin's transversality conditions into a continuum of horizons. A feedback controller is proposed to steer the system efficiently in real time, as opposed to an open-loop controller resulting from the classical Pontryagin's setting. An algorithm synthesizing the constraint-free optimal controller is used for profile tracking based on experimental data.

Paper Structure

This paper contains 14 sections, 2 theorems, 47 equations, 6 figures, 1 algorithm.

Key Result

Theorem 1

Let $w \in L^\infty(\Omega)$ be a nonnegative function such that $w(x) > 0$ a.e.. Then there exists a constant $C > 0$ such that for all $v \in H^1_w(\Omega)$ The optimal Poincaré constant is $C = \lambda_{1,w}(\Omega)^{-1}$, where $\lambda_{1,w}$ is the first Dirichlet-Laplacian eigenvalue of $\Omega$ as the infimum of the weighted Rayleigh quotient $\mathcal{R}_w$ over $H^1_w(\Omega)$ and $\| \c

Figures (6)

  • Figure 1: Boundedness of the Optimal Power Input
  • Figure 2: Controlled Plasma Temperature Evolution
  • Figure 3: Controlled Plasma Temperature at Final Time
  • Figure 4: Optimal Power Input Control Law
  • Figure 5: Convergence of the Objective Functional
  • ...and 1 more figures

Theorems & Definitions (5)

  • Remark 1
  • Theorem 1: Weighted Poincaré Inequality
  • Remark 2
  • Lemma 1.1: Gradient Flow
  • Remark 3