“…In the aforementioned equation, is the spectator gain matrix, and is the output feedback matrix. The modules and J may be combined, and the resulting module has the form [6].…”
Section: Youla Parameterized Adaptive Control Algorithm For Upper Coilsmentioning
confidence: 99%
“…Where π£(π) = π 12 (q β1 )π»(q β1 )π(π) , π The signal πΜ (π) = [π 12 (π β1 )π Μ π β π Μ π π 12 (π β1 )]π»(π β1 )π(π) and the correction error πΜ0(π) = β (π) β πΜ (π) are defined. From reference [6], the corresponding posterior errors are π(π + 1) = π π (π + 1)π Μ(π + 1) + β 0 (π + 1). RLS with a time-varying forgetting factor is then used to change the system parameters Q. π Μ(π + 1) = π Μ(π) + π(π)π(π + 1)π(π + 1)/(1 + π π (π + 1)π(π)π(π + 1))…”
Section: Youla Parameterized Adaptive Control Algorithm For Upper Coilsmentioning
To increase the correction effectiveness of full-order aberration, a control system based on a magnetic fluid flexible mirror with dual-layer actuators is presented. The combined magnetic field created by the Maxwell coil and the double-layer driving coils controls the geometry of the magnetic fluid surface. A model-based optical sensorless control approach for lower layer coils is developed and aimed to enable high magnitude restoration of lower-order aberrations. An adaptive important factor that causes on Youla parameterization, on the other hand, is developed for the upper coils to rectify higher-order residual aberrations. Matlab is used to simulate the algorithm in order to test its performance in full-order aberration correction, and the results reveal that the approach has good correction performance.
“…In the aforementioned equation, is the spectator gain matrix, and is the output feedback matrix. The modules and J may be combined, and the resulting module has the form [6].…”
Section: Youla Parameterized Adaptive Control Algorithm For Upper Coilsmentioning
confidence: 99%
“…Where π£(π) = π 12 (q β1 )π»(q β1 )π(π) , π The signal πΜ (π) = [π 12 (π β1 )π Μ π β π Μ π π 12 (π β1 )]π»(π β1 )π(π) and the correction error πΜ0(π) = β (π) β πΜ (π) are defined. From reference [6], the corresponding posterior errors are π(π + 1) = π π (π + 1)π Μ(π + 1) + β 0 (π + 1). RLS with a time-varying forgetting factor is then used to change the system parameters Q. π Μ(π + 1) = π Μ(π) + π(π)π(π + 1)π(π + 1)/(1 + π π (π + 1)π(π)π(π + 1))…”
Section: Youla Parameterized Adaptive Control Algorithm For Upper Coilsmentioning
To increase the correction effectiveness of full-order aberration, a control system based on a magnetic fluid flexible mirror with dual-layer actuators is presented. The combined magnetic field created by the Maxwell coil and the double-layer driving coils controls the geometry of the magnetic fluid surface. A model-based optical sensorless control approach for lower layer coils is developed and aimed to enable high magnitude restoration of lower-order aberrations. An adaptive important factor that causes on Youla parameterization, on the other hand, is developed for the upper coils to rectify higher-order residual aberrations. Matlab is used to simulate the algorithm in order to test its performance in full-order aberration correction, and the results reveal that the approach has good correction performance.
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