仿星器形状优化及灵敏度分析的伴随方法

E. Paul
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引用次数: 3

摘要

设计具有可接受约束特性的仿星器需要在描述其几何形状的非凸高维空间中对磁场进行优化。仿星器计划面临的另一个主要挑战是电磁线圈形状对约束特性的敏感依赖,因此需要在严格的公差下构建线圈。在本论文中,我们通过伴随方法和形状灵敏度分析来解决这些挑战。伴随方法能够有效地计算依赖于方程组(如线性或非线性偏微分方程)解的函数的梯度。这使得基于梯度的高维空间优化和高效的灵敏度分析成为可能。本文首次提出伴随方法在仿星器形状优化中的应用。我们讨论的第一个例子是基于连续电流电位模型的泛化优化线圈形状。了解线圈指标对绕组表面扰动的敏感性,使我们能够理解使线圈更简单的配置特征。接下来我们考虑漂移动力学方程的解。基于Fokker-Planck碰撞算子的自伴随性,导出了伴随漂移动力学方程,从而计算了新经典量对磁场强度扰动的敏感性。最后,我们考虑依赖于MHD平衡方程解的函数。我们推广了MHD力算子的自伴随性质,使其包含了旋转变换的微扰和约束区外的电流。利用这一自伴随性发展了一种伴随方法来计算这些函数对线圈形状或等离子体边界的扰动的导数。
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Adjoint methods for stellarator shape optimization and sensitivity analysis
The design of a stellarator with acceptable confinement properties requires optimization of the magnetic field in the non-convex, high-dimensional spaces describing their geometry. Another major challenge facing the stellarator program is the sensitive dependence of confinement properties on electro-magnetic coil shapes, necessitating the construction of the coils under tight tolerances. In this Thesis, we address these challenges with the application of adjoint methods and shape sensitivity analysis. Adjoint methods enable the efficient computation of the gradient of a function that depends on the solution to a system of equations, such as linear or nonlinear PDEs. This enables gradient-based optimization in high-dimensional spaces and efficient sensitivity analysis. We present the first applications of adjoint methods for stellarator shape optimization. The first example we discuss is the optimization of coil shapes based on the generalization of a continuous current potential model. Understanding the sensitivity of coil metrics to perturbations of the winding surface allows us to understand features of configurations that enable simpler coils. We next consider solutions of the drift-kinetic equation. An adjoint drift-kinetic equation is derived based on the self-adjointness property of the Fokker-Planck collision operator, allowing us to compute the sensitivity of neoclassical quantities to perturbations of the magnetic field strength. Finally, we consider functions that depend on solutions of the MHD equilibrium equations. We generalize the self-adjointness property of the MHD force operator to include perturbations of the rotational transform and the currents outside the confinement region. This self-adjointness property is applied to develop an adjoint method for computing the derivatives of such functions with respect to perturbations of coil shapes or the plasma boundary.
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