Philippe BARRADE, Alain BOUSCAYROL, Philippe DELARUE ... · Philippe BARRADE, Alain BOUSCAYROL,...

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EMR’11 Lausanne July 2011 Joint Summer School EMR’11 “Energetic Macroscopic Representation” Philippe BARRADE , Alain BOUSCAYROL, Philippe DELARUE,Walter LHOMME

Transcript of Philippe BARRADE, Alain BOUSCAYROL, Philippe DELARUE ... · Philippe BARRADE, Alain BOUSCAYROL,...

EMR’11 Lausanne July 2011

Joint Summer School EMR’11 “Energetic Macroscopic Representation”

Philippe BARRADE, Alain BOUSCAYROL, Philippe DELARUE,Walter LHOMME

EMR’11, Lausanne, July 2011 2

•  Introduction

•  Input filter oscillations –  Structure and conventional control scheme –  From oscillations rejection to instabilities

•  Merged control –  Objectives and tuning parameters –  Merged control loops –  Modeling and sizing rules –  Input filter stability

•  Experimental validation –  Stability abacus –  Results

•  Conclusion

- Content -

EMR’11, Lausanne, July 2011 3

•  General frame –  DC/DC or 3 phases DC/AC converters –  Feeding from a DC source via a 2nd order low pass filter

•  Depending on the control of the converter –  Some input filter oscillations can occur –  In extreme cases, instabilities can be observed

•  Depending on the operating point – Reference output power, DC feeding voltage

•  Main goal –  Allow the input filter stabilization by the appropriate control of the converter

•  Obtained from an Energetic Macroscopic Representation (EMR)

- Outline -

EMR’11, Lausanne, July 2011 4

•  Structure and conventional control scheme –  Example of a battery charger – Simplified control

•  A resistor R is needed to damp the input filter •  The input filter oscillations impact on the output current if not taken into

account by the control of the converter

- Input filter oscillations -

EMR’11, Lausanne, July 2011 5

•  From oscillations rejection to instabilities (1) –  The control must enable the regulation of the input current, by rejecting the

input filter oscillations •  Use of an Energetic Macroscopic Representation (EMR), leading to an

inversion based control identification

- Input filter oscillations -

EMR’11, Lausanne, July 2011 6

•  From oscillations rejection to instabilities (2) –  The input filter oscillations are now rejected

•  The input filter becomes unstable •  The input filter oscillations still impact on the output current

ripple

0 = IeδUc +UcδIe ⇒ Zd =δUcδIe

= −UcIe

= −Uc

2

Po

Po =Uc Ie

By rejecting the input filter oscillations, the converter absorbs an average constant power:

This makes the converter to behave as a negative impedance which loads the input filter:

Zd versus R defines the unstability conditions of the input filter:

•  function of the operating point Po

- Input filter oscillations -

EMR’11, Lausanne, July 2011 7

•  Objectives and tuning parameters –  2 solutions for the input filter stabilization

•  Adapt the value of the damping resistor •  Stabilization by the correct control of the converter

–  Control for the input filter stabilization

•  Only 1 tuning parameter (D) for two objectives – Regulation of the input current – Stabilization of the input filter

- Merged control -

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•  Merged control loop –  One defines 2 independant control loops (one per objective)

•  2 duty cycles are then defined – Du for the input filter stabilization loop – Di for the output current control

•  The two duty cycles are merged to obtain the required duty cycle D – Weightning factor kw

D = kwDu + 1 − kw( )Di

- Merged control -

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•  Modeling and sizing rules (1) –  Open loop average model

–  Duty cycles definition

CU•c =

1RUe −Uc( ) + Il − DIs

L I•l =Ue −Uc

Ls I•s = DUc −Uso

Du =Ie _ refIs

=1Is

−kp Ue −Uc( ) + Il +1RUe −Uc( )

⎝ ⎜

⎠ ⎟

Di =Us _ refUc

- Merged control -

EMR’11, Lausanne, July 2011 10

•  Modeling and sizing rules (2) –  Closed loop average model

•  Linearization along a given operating point

U•c

I•l

I•s

⎢ ⎢ ⎢ ⎢ ⎢

⎥ ⎥ ⎥ ⎥ ⎥

= A.UcIlIs

⎢ ⎢ ⎢

⎥ ⎥ ⎥

+ BUe

Us _ ref

⎣ ⎢

⎦ ⎥

A =

kw −1RC

−kwk pC

+Po 1− kw( )CUe

21− kwC

−Uso 1− kw( )CUe

−1L

0 0

kwLs

UsoUe

+UeIso

k p −1R

⎝ ⎜

⎠ ⎟

⎝ ⎜

⎠ ⎟

UekwLsIso

−UsokwLsIso

⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢

⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥

B =

1C

1R−kwR

+ kwk p⎛

⎝ ⎜

⎠ ⎟ −

Iso 1− kw( )CUe

1L

0

kwUeLsIso

1R− k p

⎝ ⎜

⎠ ⎟ −

UsoLsUe

1− kwLs

⎢ ⎢ ⎢ ⎢ ⎢ ⎢

⎥ ⎥ ⎥ ⎥ ⎥ ⎥

- Merged control -

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•  Modeling and sizing rules (3) –  Stability analysis

•  Considering the transfer function

•  Focusing on its denominator

– The coefficients are functions of » Main parameters (L,C,R, etc…) » Operating point (Ue, Uso, Is_ref=Iso)

– Dominant poles only are considered » Equivalent 2nd order system: oscillation frequency (ωn) and

damping (ζ)

Fs (s) =Uc (s)Iso (s)

D(s) = a0s4 + a1s

3 + a2s2 + a3s + a4

- Merged control -

EMR’11, Lausanne, July 2011 12

•  Input filter stability (1) –  Defined by the weightning factor kw –  Defined by the input filter stabilization control loop

•  Simple proportional controler kp

12

System unstable for kw=0 and kw≥1

Is_ref=Iso=50A

System stable in the zones (I) and (II)

Zone (I) of a great interest: •  Allow the required stabilization •  Enable to set the dynamic behavior

- Merged control -

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•  Input filter stability (2) –  Results for 2 different dynamic properties:

•  ζ=0.1 (kp=1, kw=0.36) •  ζ=0.7 (kp=1, kw=0.89)

- Merged control -

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•  Experimental validation has been performed at L2EP, from calculations made at LEI

•  Topology of theinput filter is an LC filter, taking into account the coil series resistance –  Needs in identifying stability conditions for this new topology (@20A)

- Experimental validation -

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•  Experimental results –  For various values of kw

- Experimental validation -

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•  An new and original method for the stabilization of input filter has been proposed

•  This method has been identified thanks to an energetic macroscopic representation –  Allows the identification of efficients control structures

•  The model of the system and its control has shown: –  The control structure based on an inversion method leads to the

effective input filter stabilization –  One can moreover adjust the dynamic behavior

- Conclusion -

EMR’11, Lausanne, July 2011 17

•  [1] R.D. Middlebrook, S. Cuk, “A general unified approach to modelling switching converters power stages”, IEEE PESC Rec. pp 18-34, 1976.

•  [2] R.D. Middlebrook, “Input filter considerations in design and application of switching regulators”, IEEE Industry Applications annual meeting, 1976

•  [3] P. Barrade, “Comportement dynamique des ensembles filter-convertisseur”, PhD thesism Institut National Polytechnique de Toulouse, France, 1997.

•  [4] F. Barruel, N. Retiere, J. Schanen, A Caisley, “Stability approach for vehicles DC power network: application to aircraft on-board system”, Power Electronics Specialists Conference, PESC’05, pp 1163-1169, june 16th, 2005.

•  [5] X.G. Feng, J.J. Liu, F.C. Lee, “Impedance specifications for stable DC distributed power systems”, IEEE Transactions on Power Electronics, vol. 17, pp. 157-162, 2002.

•  [6] Ph. Delarue, A. Bouscayrol, A. Tounzi, X. Guillaud, G. Lancigu, “Modelling, control and simulation of an overall wind energy conversion system", Renewable Energy, vol. 28, no. 8, pp. 1159-1324, July 2003.

•  [7] K. Chen, A. Bouscayrol, W. Lhomme, "Energetic macroscopic representation and inversion-based control: application to an electric vehicle with an electrical differential", Journal of Asian Electric Vehicles, Vol. 6, N°. 1, pages. 1097-1102, 6-2008.

- References -