Rotation de Wick | EPFL Graph Search

En physique, la rotation de Wick est une méthode pour trouver une solution à un problème mathématique dans un espace de Minkowski à partir d'un problème relatif à un espace euclidien, à l’aide d’une transformation qui substitue une variable imaginaire pure à une variable réelle. La est la transformation complexe t\longrightarrow-\mathrm{i}\tau où \mathrm{i} est l'unité imaginaire et \tau est le temps euclidien. Son éponyme est le physicien théoricien italien Gian-Carlo Wick (-) qui l'a proposée en . La transformation est dite rotation car la multiplication par le nombre \mathrm{i} est équivalente à une rotation d'angle -\frac{\pi}{2} du temps dans le plan complexe. La est la transformation \tau\longrightarrow\mathrm{i}t. Cette transformation est aussi utilisée pour résoudre des problèmes en mécanique quantique (notamment en théorie quantique des champs) et dans d'autres domaines (équation de la chaleu

Hysteresis modelling of high temperature superconductors

Marten Sjöström

The present dissertation considers the capabilities, limitations and possible extensions of modelling the hysteresis that is exhibited by type-II superconductors, especially those with high critical temperature. Superconductors of type-II, including high temperature superconductors, are partially penetrated by magnetic flux. The tubes, through which the flux passes the superconductor, are 'pinned' to certain locations due to impurities in the crystal structure of the material, and they must be forced by an external magnetic field or a transport current in order to move. Thus, the pinning of flux tubes constitutes a memory that gives rise to a hysteresis with corresponding losses. The critical state model is a well-known, macroscopic model that describes well this partial flux penetration. Furthermore, the flux tubes can start to flow due to the Lorenz-force when a large transport current flows in the superconductor. This produces an additional resistive voltage. The concept of hysteresis and its main properties are discussed, and a number of various models describing this phenomenon are presented. An emphasis is made on the classical Preisach model of hysteresis, which is a weighted superposition of relay operators. A hysteretic system produces higher harmonics, just as most nonlinear systems. An investigation reveals under what conditions the Preisach model generates only odd harmonics, and also when all odd harmonics are present, as well as how this knowledge can be utilised. A parameterised Preisach model is proposed, which always applies when the critical state model is an acceptable approximation of the superconductor hysteresis. Its capabilities and limitations as a hysteresis model for superconductors are investigated. It is demonstrated how the parameters can be estimated from different electric measurements on high temperature superconductors and that the output and the losses can quickly and accurately be computed for an arbitrary signal, once the parameter identification is made. Moreover, the structure of the parameterised model is such that an inverse model can easily be obtained. It is also shown that the hysteresis saturation, which occurs when the flux flow starts, can be modelled by introducing limiting functions in the model. A generalised equivalent circuit has been proposed that takes into account both the hysteretic and resistive behaviour, the latter being due to flux flow. This extended model describes the global electric behaviour of a superconducting device, which can be applied either when the superconductor is part of a larger system or when it stands alone. A few examples of its application are given.

EPFL2001

Hysteresis modelling of high temperature superconductors

Marten Sjöström

EPFL2001