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 7: FILTER DESIGN AND REALIZATION<br />
Type Sigle Stage Double stage<br />
π<br />
T<br />
L<br />
C<br />
2<br />
L<br />
C<br />
2<br />
Attenuation = 60 dB/dec Attenuation = 100 dB/dec<br />
L<br />
2<br />
L<br />
2<br />
C<br />
Attenuation = 60 dB/dec Attenuation = 100 dB/dec<br />
L<br />
C<br />
Attenuation = 40 dB/dec Attenuation = 80 dB/dec<br />
C<br />
2<br />
L<br />
2<br />
L<br />
L<br />
L<br />
C<br />
C<br />
C<br />
Table 7.1: Type <strong>of</strong> filters for EMI applications [9]<br />
an iterative one: it starts identifying crucial points on the emission experimental mea-<br />
surements, i.e. those with higher emissions or the emissions at the lowest frequency.<br />
The relative attenuations Att and frequencies fa are then collected. For each pair <strong>of</strong><br />
points, for a given filter topology, it is possible to extrapolate the filter’s cut-<strong>of</strong>f fre-<br />
quency that will provide the required attenuation with the formula:<br />
f0 = fa<br />
10 Ad<br />
Att<br />
where Ad is the nominal attenuation for that particular filter.<br />
L<br />
L<br />
L<br />
2<br />
C<br />
C<br />
C<br />
2<br />
(7.2.1)<br />
The first step consists in designing the DM filter. Adding it to the system will attenuate<br />
part <strong>of</strong> the CM emissions too because it will intrinsically add some inductance on the<br />
common mode path; therefore the design <strong>of</strong> the CM filter needs to consider the induc-<br />
tors already present, in order to obtain the desired attenuation, thus saving size and<br />
weight.<br />
Table 7.2 reports a list <strong>of</strong> frequencies chosen on the measured EM emission graph,<br />
with the relative attenuation to bring the emissions below the limits imposed by the<br />
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