PDF (Thesis) - Nottingham eTheses - University of Nottingham
PDF (Thesis) - Nottingham eTheses - University of Nottingham
PDF (Thesis) - Nottingham eTheses - University of Nottingham
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CHAPTER 1: INTRODUCTION<br />
the filters individually, and the parametrization is described with the guideline they<br />
have been using for the selection <strong>of</strong> the resonance frequency and the value <strong>of</strong> the com-<br />
ponents. There is also a description <strong>of</strong> the key role the parasitic components play at<br />
high frequency, hindering a good attenuation. Their proposed circuit is shown in Fig.<br />
1.12, however there is no indication on which materials have been used for the induc-<br />
tors, nor is there an indication on how the filter has been realized or its dimensions.<br />
In addition the standard they are referring to is the CISPR-11[23], that has different<br />
requirements respect to the case <strong>of</strong> an airspace related application. Therefore the indi-<br />
cations they provide can be used only for a general idea, they are not sufficient for an<br />
extensive study needed for this thesis.<br />
1.6 Existing HF models<br />
A good approach for a proper filter design implies first an accurate HF modelling and<br />
simulation for the whole system, to perform an initial decision on the filter required and<br />
afterwards an initial tuning <strong>of</strong> it, without the need <strong>of</strong> any practical work that is time<br />
and resource consuming. For this application, the HF parametrization started focus-<br />
ing on the motor, that is the device to be controlled. In the scientific literature various<br />
HF models for AC Induction Motors are present, with a range <strong>of</strong> analytical approaches<br />
[24, 25] and more practical approaches, as in [26], where a model has been developed<br />
(Fig. 1.13a) and then tuned to match existing measurements. Different models with<br />
more detailed information and guidelines for the tuning are provided in [4, 27, 28]. In<br />
particular this last model provides good accuracy in a wide frequency range. It consists<br />
<strong>of</strong> two coil-like networks in series to represent the part <strong>of</strong> the winding embedded in<br />
the stator’s slots and the end windings respectively, together with the mutual coupling<br />
(Fig. 1.13b). To tune the model parameters values, a trial and error method has been<br />
used by the authors. The models in [26] and in [4] have been chosen as a starting point<br />
for the HF motor modelling; however, using this model, the matching <strong>of</strong> the experi-<br />
mental impedance measurements <strong>of</strong> the motor under test was not satisfying, despite<br />
the large number <strong>of</strong> attempts tried with the GA algorithms. Hence further investiga-<br />
tion was necessary to find a suitable HF model for the motor <strong>of</strong> the experimental setup.<br />
Together with the motor HF model, cables and converter need a model too. For the<br />
cables the model will be created as in [29], starting from its geometrical dimensions.<br />
Regarding the converter model, no literature has so far appeared on HF modelling <strong>of</strong><br />
Matrix converter, showing therefore the need <strong>of</strong> investigations in this direction. The<br />
converter model will be here derived starting from the impedance measurements too;<br />
since its power side consists only <strong>of</strong> IGBTs, its main characteristic is expected to be<br />
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