By Cornelius T. Leondes
This can be a 4 quantity series dedicated to the numerous subject of advances in electrical strength platforms research and keep watch over strategies. The large components concerned contain tranmission line and transformer modelling. The 4 quantity series will concentrate on advances in components together with strength circulate research, fiscal operation of strength platforms, generator modelling, strength approach balance, voltage and gear regulate suggestions, and approach defense
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Extra info for Analysis and Control System Techniques for Electric Power Systems
S. interconnected power grid. The need to operate the system in a more dynamic mode than in the past is assessed from the viewpoint of making new FACTS devices truly useful in meeting this need. The role of adequate modeling and control is emphasized. Although advances in communications are not discussed in this chapter, their importance should not be underestimated, in particular their impact through fiber optics technology on implementing more information-exchange-intensive control schemes. l.
Any effect of the rest of the system is conveyed only via coupling variables φ_·, which are also locally measurable. The coupling equations associated with subsystem /, on the other hand, only involve variables directly connected to this subsystem, since by definition coefficient Cg(t) = 0 for any other subsystem. This structure should greatly facilitate both system analysis and control. Zaborzsky more than a decade ago . 2. In order to make a clear distinction between the unique equilibrium following system change (secondary control) and the instability due to dynamic problems associated with the transition from one equilibrium to the next, we recall: Definition 1.
Then the model of the interconnected system consists of (1) A set of differential equations describing the local dynamics of each subsystem i, for all subsystems i = 1 , . . ,N (13) where ï l i Z±, ffiR t ^ieR k i l IfiR P i , u^R , niiixii (2) Nondynamic coupling equations, typically nonlinear, involving variables at all nodes adjacent to each subsystem. The general form of these equations is Ν Σ c±j(t) f^ix^^ x j t ^ j r r i r u i t t) - 0 , i - i , . . , # ( 1 4 ) i t J-l ki where cn ij KU} ,.