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A EROSPACE E NGINEERING AND M ECHANICS Finite Horizon Robustness Analysis of LTV Systems Using Integral Quadratic Constraints Peter Seiler University of Minnesota M. Moore, C. Meissen, M. Arcak, and A. Packard University of California, Berkeley International Workshop on Robust LPV Control Techniques and Anti-Windup Design April 17, 2018

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Page 1: Finite Horizon Robustness Analysis of LTV Systems Using ...SeilerControl/Papers/Slides/2018/... · Finite-Horizon LTV System G defined on [0,T] Induced L 2 Gain L 2-to-Euclidean Gain

AEROSPACE ENGINEERING AND MECHANICS

Finite Horizon Robustness Analysis of LTV SystemsUsing Integral Quadratic Constraints

Peter SeilerUniversity of Minnesota

M. Moore, C. Meissen, M. Arcak, and A. PackardUniversity of California, Berkeley

International Workshop on Robust LPV Control Techniques and Anti-Windup Design

April 17, 2018

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AEROSPACE ENGINEERING AND MECHANICS

Performance Adaptive Aeroelastic Wing (PAAW)

• Goal: Suppress flutter, control wing shape and alter shape to optimize performance

• Funding: NASA NRA NNX14AL36A

• Technical Monitor: Dr. Jeffrey Ouellette

• Two years of testing at UMN followed by two years of testing on NASA’s X-56 Aircraft

2

Schmidt &Associates

LM/NASA X-56UMN Mini-Mutt

LM BFF

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AEROSPACE ENGINEERING AND MECHANICS

The FlexOp Project

3

Flutter Free FLight Envelope eXpansion for ecOnomicalPerformance improvementBalint Vanek ([email protected]), coordinator

Institute for Computer Science and Control, HAS

Approach

*Move towards methods and

tools enabling multidisciplinary

design analysis and optimization

in the aeroservoelastic domain

*Validate the developed tools

with the demonstrator

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AEROSPACE ENGINEERING AND MECHANICS

Aeroservoelasticity (ASE)

Efficient aircraft design

• Lightweight structures

• High aspect ratios

4

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AEROSPACE ENGINEERING AND MECHANICS

Flutter

5

Source: NASA Dryden Flight Research

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AEROSPACE ENGINEERING AND MECHANICS

Classical Approach

6

Frequency

AeroelasticModes

Rigid BodyModes

0

Frequency

Separation

Controller Bandwidth

Flutter AnalysisFlight Dynamics,

Classical Flight Control

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AEROSPACE ENGINEERING AND MECHANICS

Flexible Aircraft Challenges

7

Frequency

AeroelasticModes

Rigid BodyModes

0

Increasing

wing flexibility

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AEROSPACE ENGINEERING AND MECHANICS

Flexible Aircraft Challenges

8

Frequency

Rigid BodyModes

0

Integrated Control Design

Coupled Rigid Body and

Aeroelastic Modes

AeroelasticModes

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AEROSPACE ENGINEERING AND MECHANICS

Modeling and Control for Flex Aircraft

1. Parameter Dependent Dynamics

• Models depend on airspeed due to structural/aero interactions

• LPV is a natural framework.

2. Model Reduction

• High fidelity CFD/CSD models have many (millions) of states.

3. Model Uncertainty

• Use of simplified low order models OR reduced high fidelity models

• Unsteady aero, mass/inertia & structural parameters

9

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AEROSPACE ENGINEERING AND MECHANICS

Current PAAW Aircraft

10

mAEWing1

10 foot wingspan

~14 pounds

Laser-scan replica of BFF

4 aircraft, >50 flights

mAEWing2

14 foot wingspan

~42 pounds

Half-scale X-56

Currently ground testing

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AEROSPACE ENGINEERING AND MECHANICS

mAEWing1 and 2

11

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AEROSPACE ENGINEERING AND MECHANICS

Open-Loop Flutter

12

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AEROSPACE ENGINEERING AND MECHANICS

Animated Mode Shape

The BFF mode (genesis at SWB1) at a velocity near the flutter point.

The coupling of SWB1 and short period is apparent

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AEROSPACE ENGINEERING AND MECHANICS

In Flight Mode Shape

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AEROSPACE ENGINEERING AND MECHANICS

Pole Map for H-Inf Controller

15

Hinf Design procedure due to Julian Theis (’16 AIAA, ‘18 Phd) with re-

tuning by Kotikalpudi, et al (‘18 Aviation).

Marker descriptions

(X): theoretical (from models)

(◊): system I.D. (from flight tests)

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AEROSPACE ENGINEERING AND MECHANICS

Flight Test Summary

16

Successful flight beyond flutter with 2 controllers!

Indicated Airspeed

(IAS, m/s)

Estimated True

Airspeed (m/s)

20 21.9

23 25.8

25 28.4

27 30.9

29 33.5

31 36.1

Vfl

utt

er,

OL

Vfl

utt

er,

CL

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AEROSPACE ENGINEERING AND MECHANICS

Outline

• Motivation for LTV Analysis

• Nominal LTV Performance

• Robust LTV Performance

• Examples

• Conclusions

17

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AEROSPACE ENGINEERING AND MECHANICS

Outline

• Motivation for LTV Analysis

• Nominal LTV Performance

• Robust LTV Performance

• Examples

• Conclusions

18

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AEROSPACE ENGINEERING AND MECHANICS

Analysis Objective

Goal: Assess the robustness of linear time-varying (LTV) systems on finite horizons.

Approach: Classical Gain/Phase Margins focus on (infinite horizon) stability and frequency domain concepts.

19

Instead focus on:

• Finite horizon metrics, e.g. induced gains and reachable sets.

• Effect of disturbances and model uncertainty (D-scales, IQCs, etc).

• Time-domain analysis conditions.

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AEROSPACE ENGINEERING AND MECHANICS

Two-Link Robot Arm

20

Nonlinear dynamics [MZS]:ሶ𝜂 = 𝑓(𝜂, 𝜏, 𝑑)

where

𝜂 = 𝜃1, ሶ𝜃1, 𝜃2, ሶ𝜃2𝑇

𝜏 = 𝜏1, 𝜏2𝑇

𝑑 = 𝑑1, 𝑑2𝑇

t and d are control torques and disturbances at the link joints.

[MZS] R. Murray, Z. Li, and S. Sastry. A Mathematical Introduction to Robot Manipulation, 1994.

Two-Link Diagram [MZS]

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AEROSPACE ENGINEERING AND MECHANICS

Overview of Analysis Approach

21

Nonlinear dynamics:ሶ𝜂 = 𝑓(𝜂, 𝜏, 𝑑)

Linearize along a (finite –horizon) trajectory ҧ𝜂, ҧ𝜏, 𝑑 = 0ሶ𝑥 = 𝐴 𝑡 𝑥 + 𝐵 𝑡 𝑢 + 𝐵 𝑡 𝑑

Compute bounds on the terminal state x(T) or other quantity e(T) = C x(T) accounting for disturbances and uncertainty.

Comments:

• The analysis can be for open or closed-loop.

• LTV analysis complements the use of Monte Carlo simulations.

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AEROSPACE ENGINEERING AND MECHANICS

Nominal Trajectory (Cartesian Coords.)

22

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AEROSPACE ENGINEERING AND MECHANICS

Effect of Disturbances / Uncertainty

23

Cartesian Coords. Joint Angles

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AEROSPACE ENGINEERING AND MECHANICS

Outline

• Motivation for LTV Analysis

• Nominal LTV Performance

• Robust LTV Performance

• Examples

• Conclusions

24

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AEROSPACE ENGINEERING AND MECHANICS

Finite-Horizon LTV Performance

25

Finite-Horizon LTV System G defined on [0,T]

Induced L2 Gain

L2-to-Euclidean Gain

The L2-to-Euclidean gain requires D(T)=0 to be well-posed.

The definition can be generalized to estimate ellipsoidal bounds on the reachable set of states at T.

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AEROSPACE ENGINEERING AND MECHANICS

General (Q,S,R,F) Cost

Cost function J defined by (Q,S,R,F)

Example: Induced L2 Gain

26

Subject to: LTV Dynamics with x(0)=0

Select (Q,S,R,F) as:

Cost Function J is:

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AEROSPACE ENGINEERING AND MECHANICS

General (Q,S,R,F) Cost

Cost function J defined by (Q,S,R,F)

Example: L2-to-Euclidean Gain

27

Subject to: LTV Dynamics with x(0)=0

Select (Q,S,R,F) as:

Cost Function J is:

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AEROSPACE ENGINEERING AND MECHANICS

Strict Bounded Real Lemma

28

This is a generalization of results contained in:*Tadmor, Worst-case design in the time domain. MCSS, 1990 .

*Ravi, Nagpal, and Khargonekar. H∞ control of linear time-varying systems. SIAM JCO, 1991.

*Green and Limebeer. Linear Robust Control, 1995.

*Chen and Tu. The strict bounded real lemma for linear time-varying systems. JMAA, 2000.

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AEROSPACE ENGINEERING AND MECHANICS

Proof: 31

By Schur complements, the RDI is equivalent to:

This is an LMI in P. It is also equivalent to a dissipation inequality with the storage function 𝑉 𝑥, 𝑡 ≔ 𝑥𝑇𝑃 𝑡 𝑥.

Integrate from t=0 to t=T:

Apply x(0)=0 and P(T)≥F:

29

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AEROSPACE ENGINEERING AND MECHANICS

Strict Bounded Real Lemma

30

Comments:

*For nominal analysis, the RDE can be integrated. If the solution exists on [0,T] then nominal performance is achieved. This typically involves bisection, e.g. over g, to find the best bound on a gain.

*For robustness analysis, both the RDI and RDE will be used to construct an efficient numerical algorithm.

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AEROSPACE ENGINEERING AND MECHANICS

Outline

• Motivation for LTV Analysis

• Nominal LTV Performance

• Robust LTV Performance

• Examples

• Conclusions

31

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AEROSPACE ENGINEERING AND MECHANICS

Uncertainty Model

• Standard LFT Model, Fu(G,D), where G is LTV:

D is block structured and used to model parametric / dynamic uncertainty and nonlinear perturbations.

32

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AEROSPACE ENGINEERING AND MECHANICS

Integral Quadratic Constraints (IQCs)

33

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AEROSPACE ENGINEERING AND MECHANICS

Integral Quadratic Constraints (IQCs)

34

Comments:

*A library of IQC for various uncertainties / nonlinearities is given in

[MR]. Many of these are given as frequency domain inequalities.

*Time-domain IQCs that hold over finite horizons are called hard.

*This generalizes D and D/G scales for LTI and parametric uncertainty.

It can be used to model the I/O behavior of nonlinear elements.

[MR] Megretski and Rantzer. System analysis via integral quadratic constraints, TAC, 1997.

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AEROSPACE ENGINEERING AND MECHANICS

Robustness Analysis

The robustness analysis is performed on the extended (LTV) system of (G,Y) using the constraint on z.

35

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AEROSPACE ENGINEERING AND MECHANICS

Robustness Analysis: Induced L2 Gain

36

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AEROSPACE ENGINEERING AND MECHANICS

Proof:

The Differential LMI (DLMI) is equivalent to a dissipation ineq. with storage function 𝑉 𝑥, 𝑡 ≔ 𝑥𝑇𝑃 𝑡 𝑥.

Integrate and apply the IQC + boundary conditions to conclude that the induced L2 gain is ≤g.

Robustness Analysis: Induced L2 Gain

37

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AEROSPACE ENGINEERING AND MECHANICS

Comments:

*A similar result exists for L2-to-Euclidean or, more generally (Q,S,R,F) cost functions.

*The DLMI can be expressed as a Riccati Differential Ineq. (RDI) by Schur Complements.

*The RDI is equivalent to a related Riccati Differential Eq. (RDE) condition by the strict Bounded Real Lemma.

Robustness Analysis: Induced L2 Gain

38

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AEROSPACE ENGINEERING AND MECHANICS

Comments:

*The DLMI is convex in the IQC matrix M but requires gridding on time tand parameterization of P.

*The RDE form directly solves for P by integration (no time gridding) but the IQC matrix M enters in a non-convex fashion.

Robustness Analysis: Induced L2 Gain

39

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AEROSPACE ENGINEERING AND MECHANICS

Numerical Implementation

An efficient numerical algorithm is obtained by mixing the LMI and RDE conditions.

Sketch of algorithm:

1. Initialize: Select a time grid and basis functions for P(t).

2. Solve DLMI: Obtain finite-dimensional optim. by enforcing DLMI on the time grid and using basis functions.

3. Solve RDE: Use IQC matrix M from step 2 and solve RDE. This gives the optimal storage P for this matrix M.

4. Terminate: Stop if the costs from Steps 2 and 3 are similar. Otherwise return to Step 2 using optimal storage P as a basis function.

40

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AEROSPACE ENGINEERING AND MECHANICS

Outline

• Motivation for LTV Analysis

• Nominal LTV Performance

• Robust LTV Performance

• Examples

• Conclusions

41

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AEROSPACE ENGINEERING AND MECHANICS

Example 1: LTI Plant

• Compute the induced L2 gain of Fu(G,D) where D is LTI with Δ ≤ 1 and G is:

• By (standard) mu analysis, the worst-case (infinite horizon) L2 gain is 1.49.

• This example is used to assess the finite-horizon robustness results.

42

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AEROSPACE ENGINEERING AND MECHANICS

Example 1: Finite Horizon Results

Total comp. time is 466 sec to compute worst-case gains on nine finite horizons.

43

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AEROSPACE ENGINEERING AND MECHANICS

Example 2: Two-Link Robot Arm

• Assess the worst-case L2-to-Euclidean gain from disturbances at the arm joints to the joint angles.

• LTI uncertainty with Δ ≤ 0.8 injected at 2nd joint.

• Analysis performed along nominal trajectory in with LQR state feedback.

44

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AEROSPACE ENGINEERING AND MECHANICS

Example 2: Results

Bound on worst-case L2-to-Euclidean gain = 0.0592.

Computation took 102 seconds.

45

Cartesian Coords. Joint Angles

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AEROSPACE ENGINEERING AND MECHANICS

Worst-case Disturbance / Uncertainty

Numerically robust algorithm to construct the worst-case disturbance (work with A. Iannelli and A. Marcos)

46

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Outline

• Motivation for LTV Analysis

• Nominal LTV Performance

• Robust LTV Performance

• Examples

• Conclusions

47

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Extensions: Rational Dependence on Time

48

Ref: Seiler, IQC-Analysis of Uncertain LTV Systems With

Rational Dependence on Time, submitted to the ‘18 CDC.

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Dynamic IQC for Time Operator Dt

Swapping Lemma

IQC for Dt

49

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Example: Nominal Analysis

50

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Example: Robust Analysis

51

Plant, P

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AEROSPACE ENGINEERING AND MECHANICS

Example: Robust Analysis

52

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Conclusions

• Main Result: Bounds on finite-horizon robust performance can be computed using differential equations or inequalities.

• These results complement the use of nonlinear Monte Carlo simulations.

• It would be useful to construct worst-case inputs / uncertainties analogous to m lower bounds.

• An LTVTools toolbox is in development with b-code of the proposed methods.

• References• Moore, Finite Horizon Robustness Analysis Using Integral Quadratic Constraints,

MS Thesis, 2015.

• Seiler, Moore, Meissen, Arcak, Packard, Finite Horizon Robustness Analysis of LTV Systems Using Integral Quadratic Constraints, arXiv + submission to Automatica.

• Related work by Biertümpfel and Pfifer with application to rocket launchers submitted to the 2018 IEEE Conference on Control Technology and Applications.

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AEROSPACE ENGINEERING AND MECHANICS54

Acknowledgements

• US National Science Foundation • Grant No. NSF-CMMI-1254129: “CAREER: Probabilistic Tools for High

Reliability Monitoring and Control of Wind Farms.” Prog. Manager: J. Berg.

• Grant No. NSF/CNS-1329390: “CPS: Breakthrough: Collaborative Research: Managing Uncertainty in the Design of Safety-Critical Aviation Systems”. Prog. Manager: D. Corman.

• NASA• NRA NNX14AL36A: "Lightweight Adaptive Aeroelastic Wing for Enhanced

Performance Across the Flight Envelope," Tech. Monitor: J. Ouelette.

• NRA NNX12AM55A: “Analytical Validation Tools for Safety Critical Systems Under Loss-of-Control Conditions.” Tech. Monitor: C. Belcastro.

• SBIR contract #NNX12CA14C: “Adaptive Linear Parameter-Varying Control for Aeroservoelastic Suppression.” Tech. Monitor. M. Brenner.

• Eolos Consortium and Saint Anthony Falls Laboratory• http://www.eolos.umn.edu/ & http://www.safl.umn.edu/

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