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Christoph Haederli - Les thèses en ligne de l'INP - Institut National ...

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98 NP Control with Carrier based PWM<br />

For low modulation <strong>de</strong>pth and cos(ϕ) not equal to zero, both outer sections of the piecewise<br />

linear function have the same absolute value but opposite signs. Maximum and minimum curr<strong>en</strong>t<br />

functions (with lowest absolute value CM) are clearly <strong>de</strong>fined. These maximum and minimum<br />

curr<strong>en</strong>t functions have singularities with CM jumps as can be se<strong>en</strong> from TABLE 34. Nevertheless,<br />

continuous CM voltage operation is possible with suitable 3 rd harmonic injection, as proposed in<br />

TABLE 34. The third harmonic required has significantly differ<strong>en</strong>t amplitu<strong>de</strong> and phase angle than<br />

the one use in TABLE 32. Of course, other strategies of CM injection staying within the minimum<br />

and maximum boundaries are possible, but a strategy leading to continuous CM injection function<br />

is preferable for commutation reasons; any jump in the CM function will g<strong>en</strong>erate multiple<br />

commutations simultaneously and lead to higher overall switching losses.<br />

Note that minimum and maximum NP curr<strong>en</strong>t CM values do not cross each other in this case<br />

(as opposed to the approach in TABLE 32). Consequ<strong>en</strong>tly, no AC CM needs to be injected to<br />

g<strong>en</strong>erate a DC NP curr<strong>en</strong>t, but a pure DC CM voltage injection can be used both for minimum and<br />

maximum DC NP curr<strong>en</strong>t. This is shown in the third column TABLE 34. Note that there is a<br />

smooth transition possible from active to reactive power with this control scheme. The 3 rd<br />

harmonic amplitu<strong>de</strong> and phase can be <strong>de</strong>fined as a continuous function of amplitu<strong>de</strong> of the<br />

fundam<strong>en</strong>tal and the angle ϕ betwe<strong>en</strong> voltage and curr<strong>en</strong>t.<br />

The 6 th harmonic injection scheme can still be applied at low modulation <strong>de</strong>pth and non zero<br />

cos(ϕ) if the CM function for minimum and maximum NP curr<strong>en</strong>t are adapted accordingly,<br />

conforming with the constraints above. In fact the examples in TABLE 32 use a phase angle of 1.56,<br />

which leads to small but noticeable differ<strong>en</strong>ce of NP curr<strong>en</strong>ts in the two outer sections of the NP<br />

curr<strong>en</strong>t functions. The performance impact is very low. Both schemes have very similar<br />

performance. The 6 th harmonic injection scheme will have slightly reduced maximum and minimum<br />

NP curr<strong>en</strong>ts but it has a higher <strong>de</strong>gree of freedom regarding 3 rd harmonic injection and it requires<br />

no DC CM injection for the NP control.<br />

We can conclu<strong>de</strong> that there are two almost equival<strong>en</strong>t concepts for NP curr<strong>en</strong>t control for<br />

reactive power operation at low modulation <strong>de</strong>pth. This is not true for high modulation <strong>de</strong>pth,<br />

because the outer sections of the piecewise linear CM curr<strong>en</strong>t function cannot physically be<br />

reached. Consequ<strong>en</strong>tly, the minimum and maximum NP curr<strong>en</strong>t functions are clearly <strong>de</strong>fined. Only<br />

6 th harmonic injection is possible as shown in TABLE 33.

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