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Connection of disturbing loads in micro-grids

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Title: Connection of disturbing loads in micro-grids


1
Connection of disturbing loads in micro-grids
  • National Advanced Polytechnique Institute of
    Yaounde - Cameroon

2
Objectifs du projet
  • Many papers may be found in the literature
    studying the impact of dispersed generation on
    power quality, where the generators are
    considered as disturbing installations (sources
    of flicker, harmonics, or higher-frequency
    components). We report on a study with another
    point of view  what about the connection of
    "classical" disturbing loads in a micro-grid fed
    by renewable energy generators ?

3
Description
  • The system which was modeled is shown in Fig.1.
    It simply consists of a DC Generator connected to
    load by DC/AC converter.
  •  
  • Fig. 1 Electrical System to study

4
The analysis of dynamic behavior of this system
  • Knowing that load power can be explained as a
    function of the short circuit power and the
    relation between positive and negative sequence
    voltages, we can write that

  • (1)
  • The determination of the load power can be done
    using


  • (2)

5
  • After the calculation of the short circuit power
    we can get the short circuit impedance through
    the relation



  • (3)
  • The objective of this calculation is to compare
    the Zcc obtainedby simulation (DC Source-
    Converter- Unbalanced Load) with the Zcc of a
    similar system where the DC Source-Converter can
    be replaced by an AC Source.

6
Results of simulations
  • Fig. 2 Voltages obtained at the phases (a, b,
    c)
  • of the unbalanced load

7
  • Fig. 3 Current at the DC side of the converter
    when
  • AC connected to unbalanced load

8
  • What we were looking for, is the equivalent short
    circuit impedance (given by Scc  Sload x Ud/Ui).
    The value obtained is around 1.083 O.
  • The short circuit impedance obtained from the
    result of the simulation (1.083 O) is not very
    greater than the calculated value from the filter
    (1.0101 O).
  • Thus, with the simple model which was used for
    the PWM AC/DC converter (no active filtering
    function), the "short-circuit" impedance
    (Thevenin equivalent) of the generator is
    practically equal to the impedance of the filter.
    The question is then  how to choose the
    parameters L and C ? (the influence of C being
    low for 50 Hz phenomena, but important at
    harmonic frequencies).

9
Choice of filter parameters
  • It can be shown that the filter parameters L and
    C result from the choice of
  • - zcc (pu) the series 50 Hz impedance of the
    generator, and
  • - um Um/U (pu) the accepted relative
    magnitude of the modulation frequency component
  •  

  • (H)

  • (F) 

10
  • Where
  • - U phase-to-phase 50 Hz voltage of the
    generator (V).
  • - ? 2?f 2?50 (rad/s).
  • - Sn ?3UIn nominal power of the generator
    (VA).
  • - n fm/f ratio between modulation frequency
    and power frequency.
  • If we want to have zcc as low as possible, we
    have to accept if and um as high as possible.
  • If we accept 0.5  for the magnitude of the HF
    voltage component and 10  for the magnitude of
    the no-load current in the filter then 

11
  • zcc 2.2  at 15 kHz
  • zcc 5  at 10 kHz
  • zcc 20  at 5 kHz.
  • It appears that the achievable short-circuit
    power strongly depends on the modulation
    frequency. We know that a classical value for the
    impedance of a MV/LV transformer is 4 . Such a
    low impedance may be obtained with the PWM
    generator if the modulation frequency is higher
    than 10 kHz.
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