«new paradigms for control theory» romeo ortega lss-cnrs-supelec gif-sur-yvette, france

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«NEW PARADIGMS «NEW PARADIGMS FOR CONTROL THEORY» FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

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Page 1: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

«NEW PARADIGMS«NEW PARADIGMS FOR CONTROL FOR CONTROL THEORY»THEORY»

«NEW PARADIGMS«NEW PARADIGMS FOR CONTROL FOR CONTROL THEORY»THEORY»

Romeo OrtegaLSS-CNRS-SUPELEC

Gif-sur-Yvette, France

Page 2: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

ContentContentContentContent

BackgroundProposalExamples

Page 3: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

FactsFactsFactsFactsModern (model-based) control theory is not providing solutions to new practical control problems

Prevailing trend in applications: data-based « solutions »

Neural networks, fuzzy controllers, etc They might work but we will not understand why/when

New applications are truly multidomain

There is some structure hidden in «complex systems »

Revealed through physical laws Pattern of interconnection is more important than detail

Page 4: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Why?Why?Why?Why?Signal processing viewpoint is not adequate:

= Input-Output-Reference-Disturbance.

Classical assumptions not valid: linear + «small » nonlinearities interconnections with large impedances time-scale separations lumped effects

Methods focus on stability (of a set of given ODEs)

no consideration of the physical nature of the model.

Page 5: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

ProposalProposalProposalProposalReconcile modelling with, and incorporate energy information into, control design.

How?How?Propose models that capture main physical ingredients:

energy, dissipation, interconnection

Attain classical control objectives (stability, performance) as by-products of:

Energy-shaping, interconnection and damping assignment.

Confront, via experimentation, the proposal with current practice.

Page 6: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Prevailing paradigmPrevailing paradigmPrevailing paradigmPrevailing paradigm

• Models

• Control objectives

• Controller design

Signal procesing viewpoint

Models

C

Pd

u

z

yzd

r s

P

r

du

s

zy

:

Uncertainty

Known structure,

• •

RHd D L

Page 7: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Control objectives z-zd « small »

effect of d on z « small »

Controller

y

zu:C

d

Class of admissible systems TOO LARGE !!

Conservativeness (min max designs)

High gain (sliding modes, backstepping…)

Complexity

Practically useless

Intrinsic to signal-processing viewpoint

Drawbacks!!!Drawbacks!!!

Page 8: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

C I

Unmodelled

environment

i i i

x

c

ec

e

v v v

(Energy-based) Control by interconnection

Proposed alternativeProposed alternativeProposed alternativeProposed alternative

Page 9: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Models

PLANT:

• H(x) energy function, x state,

• (v,i) conjugated port variables,

• Geometric (Dirac) structure capturing energy exchange

• Dissipation

ENVIRONMENT:

• Passive port

• Flexibility and dissipation effects

• Parasitic dynamics

Control objectives

• Focus on energy and dissipation

• Shape and exchange pattern

Controller

C

I

• controller, Hc(z) energy

• power preserving

Page 10: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

IDA-PBC of mechanical IDA-PBC of mechanical systemssystemsIDA-PBC of mechanical IDA-PBC of mechanical systemssystems

To stabilize some underactuated mechanical devices it is necessary to modify the total energy function. In open loop

Where qRn, pRn are the generalized position and momenta, respectively, M(q)=MT(q)>0 is the inertia matrix, and V(q) is the potential energy

MODELMODEL

Control uRm, and assume rank(G)=m < nConvenient to decompose u=ues(q,p)+udi(q,p)

Page 11: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

TARGET TARGET DYNAMICSDYNAMICS

Desired (closed loop) energy function

where Md=MdT>0 and Vd(q)

with port controlled Hamiltonian dynamics

where

Page 12: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

All assignable energy All assignable energy functions are characterized by a functions are characterized by a PDE!!PDE!!

All assignable energy All assignable energy functions are characterized by a functions are characterized by a PDE!!PDE!!

The PDE is parameterized by The PDE is parameterized by two free matrices (related to two free matrices (related to physics)physics)

Page 13: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

ExamplesExamplesExamplesExamples

BALL AND BEAMBALL AND BEAM

Page 14: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Ball and BeamBall and BeamBall and BeamBall and Beam

Page 15: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Ball and BeamBall and BeamBall and BeamBall and Beam

Page 16: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Vertical take-off and landing Vertical take-off and landing aircraftaircraftVertical take-off and landing Vertical take-off and landing aircraftaircraft

Page 17: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Cart with inverted pendulumCart with inverted pendulumCart with inverted pendulumCart with inverted pendulum

Page 18: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

ExamplesExamplesExamplesExamples(PASSIVE) (PASSIVE) WALKING WALKING

• Plant: double pendulum

• Environement:

elastic (stiff)

Model

Page 19: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

(Passive) walking(Passive) walking(Passive) walking(Passive) walking

Control objetive:

Shape energy

Page 20: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

(Passive) walking(Passive) walking(Passive) walking(Passive) walking

Page 21: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

(Passive) walking(Passive) walking(Passive) walking(Passive) walking

other other mechatronic mechatronic systems: systems:

teleoperators, robots in interaction (with environement)

Page 22: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

• Plant: (controlled) wave eq.

• Environment: passive mech. contact

• model

• control objective: shape energy

Piezoelectric actuatorsPiezoelectric actuatorsPiezoelectric actuatorsPiezoelectric actuators

Page 23: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Control through long cablesControl through long cablesControl through long cablesControl through long cablesE.g., overvoltage in drivesE.g., overvoltage in drives

• model

• control objective: change interconnection to suppress waves

Page 24: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France
Page 25: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France
Page 26: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France
Page 27: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Dual to teleoperators

Many examples in power electronics and power systems

Page 28: «NEW PARADIGMS FOR CONTROL THEORY» Romeo Ortega LSS-CNRS-SUPELEC Gif-sur-Yvette, France

Thank Thank you!!you!!Thank Thank you!!you!!