2021
DOI: 10.1016/j.procs.2021.04.167
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Tokamak plasma models development for plasma magnetic control systems design by first principle equations and identification approach

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Cited by 2 publications
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“…where x i (t) is the state vector, u i (t) is the control action vector, y i (t) is the output vector, A (i) (t), B (i) (t), and C (i) (t) are time-varying matrices of the model, f i (t) and w i (t) are additive disturbance vectors at state and output equations, respectively, index i denotes a characteristic plasma discharge, t ∈ t 0i , T (i) , T (i) is the duration of the discharge, and t 0i is the initial time of discharges when the plasma control system begins to operate. The evolution of plasma position and currents in the Tokamak is described by Faraday's law [35]:…”
mentioning
confidence: 99%
“…where x i (t) is the state vector, u i (t) is the control action vector, y i (t) is the output vector, A (i) (t), B (i) (t), and C (i) (t) are time-varying matrices of the model, f i (t) and w i (t) are additive disturbance vectors at state and output equations, respectively, index i denotes a characteristic plasma discharge, t ∈ t 0i , T (i) , T (i) is the duration of the discharge, and t 0i is the initial time of discharges when the plasma control system begins to operate. The evolution of plasma position and currents in the Tokamak is described by Faraday's law [35]:…”
mentioning
confidence: 99%