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Control and Design of Microgrid Components - Power Systems ...

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ω<br />

Unit 2 Max<br />

Unit 2<br />

ω<br />

o<br />

Unit 1<br />

ω<br />

1<br />

ω<br />

2<br />

ΔPmax<br />

ΔPmax<br />

Δωmax<br />

P<br />

P = 0<br />

Output <strong>Power</strong><br />

Within Limits<br />

Pmax<br />

Figure 3.16 Effectively Limiting Pmax on Output <strong>Power</strong> <strong>Control</strong>.<br />

Figure 3.16 shows two units in isl<strong>and</strong> mode operating at the frequency ω1 (circles) where unit 2<br />

has:<br />

P1(at ω1) = P1_1<br />

P2(at ω1) = Pmax + ΔPmax<br />

Here, ΔPmax is the amount <strong>of</strong> power that is given in excess <strong>of</strong> Pmax. The main idea is that a<br />

change must be performed so that at the final operating point unit 2 is injecting Pmax (<strong>and</strong> no<br />

more), while unit 1 injects the amount <strong>of</strong> power that it had previously added <strong>of</strong> the excess <strong>of</strong><br />

power (ΔPmax ) <strong>of</strong> unit 1:<br />

P1(at ω2) = P1_1 + ΔPmax<br />

P2(at ω2) = Pmax<br />

Frequency ω2 is also shown on Figure 3.16 <strong>and</strong> the corresponding power outputs are shown with<br />

squares. Notice that the sum <strong>of</strong> power injected does not (<strong>and</strong> must not) change between the two<br />

frequencies, since the overall sum <strong>of</strong> the load dem<strong>and</strong> has not changed. The question now is how<br />

to make sure that unit 1 (that reaches max) will rearrange its frequency as to end up at frequency<br />

ω2 <strong>and</strong> not ω1. The reason why it would reach ω1 in the first place is because <strong>of</strong> the droop<br />

equation, reported here for convenience:<br />

i<br />

= o o , i<br />

( P P )<br />

ω ω − m −<br />

Eq. 3.4<br />

i<br />

33

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