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The Preisach model of hysteresis generalizes hysteresis loops as the parallel connection of independent relay ''hysterons''. It was first suggested in 1935 by Ferenc (Franz) Preisach〔Ralph Smith, (''Smart material systems: model development'' ), SIAM, 2005. p. 189.〕 in the German academic journal "''Zeitschrift für Physik''".〔F. Preisach, ''Über die magnetische Nachwirkung''. ''Zeitschrift für Physik'', 94:277-302, 1935〕 Since then, it has become a widely accepted model of hysteresis.〔Augusto Visintin, ''Differential Models of Hysteresis (Applied Mathematical Sciences)'', Springer, 1995〕 The Preisach model is especially accurate in the field of ferromagnetism, as the ferromagnetic material can be described as a network of small domains, each magnetized to a value of either or . A sample of iron, for example, may have evenly distributed magnetic domains, resulting in a net magnetic field of zero. ==Nonideal relay== The relay hysteron is the fundamental building block of the Preisach model. It is described as a two-valued operator denoted by . Its I/O map takes the form of a loop, as shown: Above, a relay of magnitude 1. defines the "switch-off" threshold, and defines the "switch-on" threshold. Graphically, if is less than , the output is "low" or "off." As we increase , the output remains low until reaches —at which point the output switches "on." Further increasing has no change. Decreasing , does not go low until reaches again. It is apparent that the relay operator takes the path of a loop, and its next state depends on its past state. Mathematically, the output of is expressed as: Where if the last time was outside of the boundaries 抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)』 ■ウィキペディアで「Preisach model of hysteresis」の詳細全文を読む スポンサード リンク
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