Christoph Haederli - Les thèses en ligne de l'INP - Institut National ...
Christoph Haederli - Les thèses en ligne de l'INP - Institut National ...
Christoph Haederli - Les thèses en ligne de l'INP - Institut National ...
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84 3-L DC Link ML Converter Properties<br />
A similar table as above can be drawn based on the actual switching function s x(t) instead of<br />
abs(s x(t)). However, such a table inclu<strong>de</strong>s much more compon<strong>en</strong>ts, as all the harmonic terms in<br />
abs(s x(t)) can be g<strong>en</strong>erated by multiple terms in s x(t). TABLE 28 inclu<strong>de</strong>s the most important<br />
compon<strong>en</strong>ts only; in reality an infinite number of higher harmonic terms apply to each field, with<br />
<strong>de</strong>creasing importance. All positive and negative sequ<strong>en</strong>ce NP curr<strong>en</strong>ts will cancel out in the neutral<br />
point, if the system is symmetrical and balanced. The remaining harmonics visible in the NP<br />
curr<strong>en</strong>t and consequ<strong>en</strong>tly in the NP voltage are 3 rd , 9 th , 15 th etc. Therefore only zero sequ<strong>en</strong>ce NP<br />
curr<strong>en</strong>ts are shown in TABLE 28. On the line si<strong>de</strong> only positive and negative sequ<strong>en</strong>ce curr<strong>en</strong>ts are<br />
consi<strong>de</strong>red, as zero sequ<strong>en</strong>ce curr<strong>en</strong>ts are not pres<strong>en</strong>t in three wire systems.<br />
TABLE 28, RELATIONSHIP BETWEEN HARMONIC ORDERS OF LINE SIDE CURRENT, THE<br />
SWITCHING FUNCTION S(T) AND THE OVERALL NP CURRENT<br />
I-NP<br />
AC si<strong>de</strong> curr<strong>en</strong>t DC 1 2 3 4 5 6 7 8 9<br />
DC<br />
1 DC / 2 nd / 6 th 1 st / 3 rd 4 th / 6 th 7 th / 9 th<br />
2 1 st / 3 rd DC / 2 nd / 6 th 3 rd / 5 th 6 th / 8 th<br />
3<br />
4 3 rd / 5 th DC / 2 nd / 6 th 1 st / 3 rd 4 th / 6 th<br />
5 4 th / 6 th 1 st / 3 rd DC / 2 nd / 6 th 3 rd / 5 th<br />
6<br />
7 6 th / 8 th 3 rd / 5 th DC / 2 nd / 6 th 1 st / 3 rd<br />
8 7 th / 9 th 4 th / 6 th 1 st / 3 rd DC / 2 nd / 6 th<br />
9<br />
s(t)<br />
This overview helps to un<strong>de</strong>rstand both how the NP can be disturbed and how it can be<br />
controlled. The input i<strong>de</strong>ally only contains a fundam<strong>en</strong>tal and high or<strong>de</strong>r harmonics g<strong>en</strong>erated by<br />
the switching function as it is actively controlled. In reality, the input voltage (line voltage or motor<br />
back EMF) may contain low or<strong>de</strong>r harmonics also g<strong>en</strong>erating input curr<strong>en</strong>t harmonics if not<br />
actively eliminated. These harmonics are typically odd harmonics. The convolution of input curr<strong>en</strong>t<br />
and rectified switching function th<strong>en</strong> leads primarily to odd NP curr<strong>en</strong>t harmonics, as the rectified<br />
switching function contains primarily ev<strong>en</strong> harmonics (see TABLE 27). This is not very significant as<br />
there is no DC and amplitu<strong>de</strong>s are low. If however there are odd harmonics in the rectified<br />
switching function, a DC NP curr<strong>en</strong>t can be g<strong>en</strong>erated. If there are ev<strong>en</strong> harmonics pres<strong>en</strong>t (2 nd , 4 th ,<br />
etc.) in the output curr<strong>en</strong>t, they interact with the fundam<strong>en</strong>tal and the 3 rd of the switching function<br />
and result in a DC NP curr<strong>en</strong>t.<br />
To control the NP, it is best to focus on a scheme using the fundam<strong>en</strong>tal input curr<strong>en</strong>t, as the<br />
pres<strong>en</strong>ce of curr<strong>en</strong>t harmonics is uncertain. This means that mainly a fundam<strong>en</strong>tal in the rectified<br />
switching function can be used to g<strong>en</strong>erate a DC NP curr<strong>en</strong>t. A fundam<strong>en</strong>tal in the rectified<br />
switching function can be obtained by applying a DC offset or an ev<strong>en</strong> harmonic term to the