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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Application and Verification 161<br />
TABLE 70, PERFORMANCE OF THE INDIVIDUAL NP CONTROL SCHEMES AT ACTIVE POWER OPERATION<br />
AND LOW MODULATION DEPTH (m = 0.1)<br />
Unconstrained DC<br />
CM injection<br />
- m = 0.1<br />
CH1 (yellow):<br />
CH2 (cyan):<br />
U out1<br />
U out2<br />
CH3 (mag<strong>en</strong>ta): U NP<br />
CH4 (gre<strong>en</strong>):<br />
MATH (red):<br />
Time/div:<br />
I out2<br />
U out1-2<br />
100ms<br />
Modified and<br />
virtual vectors<br />
- m = 0.1<br />
CH1 (yellow):<br />
CH2 (cyan):<br />
U out1<br />
U out2<br />
CH3 (mag<strong>en</strong>ta): U NP<br />
CH4 (gre<strong>en</strong>):<br />
MATH (red):<br />
Time/div:<br />
I out2<br />
U out1-2<br />
100ms<br />
The operating point of very high modulation <strong>de</strong>pth is ev<strong>en</strong> more critical than the operation at<br />
low modulation <strong>de</strong>pth. At high modulation <strong>de</strong>pth, typically load curr<strong>en</strong>ts are higher and distortion<br />
my produce significant NP bias curr<strong>en</strong>ts that need to be comp<strong>en</strong>sated. This is especially true for<br />
line connected applications, where exceptional line conditions may be very <strong>de</strong>manding. TABLE 71<br />
shows experim<strong>en</strong>tal results for very high modulation <strong>de</strong>pth and differ<strong>en</strong>t NP control schemes.<br />
Unconstrained DC CM injection is capable of controlling the NP voltage up to maximum<br />
sinusoidal line to line voltage. However, ev<strong>en</strong> without line distortion or any other source of NP bias<br />
curr<strong>en</strong>t, there is a low frequ<strong>en</strong>cy ripple appar<strong>en</strong>t on the NP voltage, indicating that the controller is<br />
operating at its limits and cannot comp<strong>en</strong>sate the full NP curr<strong>en</strong>t. The transi<strong>en</strong>t has a duration of<br />
~80ms corresponding with an average dv/dt of 250V/s. The corresponding NP curr<strong>en</strong>t is 1A or<br />
8.5% of 11.5A peak phase curr<strong>en</strong>t. With the modified and virtual vector scheme, the NP voltage is<br />
significantly more stable and the transi<strong>en</strong>t has a duration of 50ms (400V/s). This corresponds with<br />
1.6A NP curr<strong>en</strong>t or 14% of the peak phase curr<strong>en</strong>t. The differ<strong>en</strong>ce is significant, but it may not<br />
justify the use of the more complicated scheme, introducing distortion in the line to line voltage<br />
(nicely visible in TABLE 71 b, red waveform during transi<strong>en</strong>t). However, the unconstrained DC CM<br />
injection does not work anymore for maximum over modulation (NP voltage diverging in<br />
experim<strong>en</strong>tal verification), whereas the modified and virtual vector scheme keeps its properties also<br />
in this operating mo<strong>de</strong>. TABLE 71 I shows maximum trapezoidal operation still yielding a NP<br />
voltage dv/dt of 250V/s or 1A NP curr<strong>en</strong>t (8% of peak phase curr<strong>en</strong>t). A hysteresis controller as<br />
introduced in the previous paragraph can make best use of that control power and the good<br />
performance regarding switching losses and output harmonics of the other modulators.