Some results related to modeling systems with uncertainty Neskolko - - PowerPoint PPT Presentation
Some results related to modeling systems with uncertainty Neskolko - - PowerPoint PPT Presentation
Some results related to modeling systems with uncertainty Neskolko rezultatov ob modelirovanie sistem s neopredel ennostmi Dimitri PEAUCELLE - Dmitri i anoviq Posel LAAS-CNRS - Universit de Toulouse - FRANCE Sankt-Peterburg
Introduction ■ Outline ❶ Motivations for uncertain descriptor modeling ❷ Affine polytopic models ❸ LFT models - frequency dependent models ❹ Augmented descriptor models and conservatism reduction
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❶ Motivations for uncertain descriptor modeling
■ Models issued from physics are naturally in descriptor form E ˙ x = Ax + Bu
- Example: mechanical system
M ¨ θ + C ˙ θ + Kθ = u M: inertia ; C: friction ; K: stiffness ; u external forces M O O I ¨ θ ˙ θ = −C −K I O ˙ θ θ + I O u
- Example: robotic systems with Lagrange formulations [MG89]
E may not be invertible
- Example: networks of systems with algebraic constraints describing links
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❶ Motivations for uncertain descriptor modeling
■ Descriptor models can be converted to usual models
- Example: mechanical system
¨ θ + M −1C ˙ θ + M −1Kθ = M −1u
- Assumes that M −1 is well-conditioned and known
- If some parameters are unknown: M(∆), C(∆), K(∆)
¨ θ + M −1(∆)C(∆) ˙ θ + M −1(∆)K(∆)θ = M −1(∆)u
- Increased complexity of the model
■ Descriptor models are preferable for describing systems with uncertainty
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❶ Motivations for uncertain descriptor modeling
■ Example: DC motor I ˙ ω = bu regulated in speed u = −ω
- Parameters are assumed uncertain I = 1 + δ1, b = 1 + δ2
(1 + δ1) ˙ ω = −(1 + δ2)ω ⇒ ˙ ω = −1 + δ2 1 + δ1 ω
- Model is rational w.r.t. uncertainties: exists an LFT representation
z∆ w
∆
∆
Σ
−1 + δ2 1 + δ1 = A + B∆∆(I − D∆∆)−1C∆ = A B∆ C∆ D∆ ⋆ ∆ ▲ Can be build with Robust Control toolbox of Matlab or LFRT [Mag05]
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❶ Motivations for uncertain descriptor modeling
- Building the LFT for ˙
ω = − 1+δ2
1+δ1ω
▲ 1st step: descriptor form with no denominators ˙ ω + δ1 ˙ ω = −ω − δ2ω ▲ 2nd step: all multiplications correspond to a feedback ˙ ω + w1 = −ω − w2 : w1 = δ1z1 z1 = ˙ ω , w1 = δ2z2 z2 = ω ▲ 3rd step: descriptor LFT: ∆ =
- δ1
δ2
- , z∆ =
- z1
z2
- , w∆ =
- w1
w2
- ,
1 −1 1 1
- ˙
ω z∆
- =
−1 −1 −1 1
- ω
w∆
- , w∆ = ∆z∆
▲ last step: invert the left-hand side matrix
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❶ Motivations for uncertain descriptor modeling
- LFT for ˙
ω = − 1+δ2
1+δ1ω − 1+δ2
1+δ1 =
1 −1 1 1
−1
−1 −1 −1 1 ⋆ δ1 δ2 = −1 −1 −1 −1 −1 −1 1 ⋆ δ1 δ2 = −1 +
- −1
−1
-
δ1 δ2 I − −1 −1 δ1 δ2
−1
−1 1 = −1 −
- δ1
δ2
-
1 + δ1 δ2 1
−1
−1 1 = −1 −
- δ1
δ2
-
− 1+δ2
1+δ1
1 = −1 + δ1−δ2
1+δ1 = − 1+δ2 1+δ1
■ The example shows the interest of descriptor models,
even if only for technical manipulations
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❶ Motivations for uncertain descriptor modeling
■ All fractional models have affine descriptor representations [MAS03] ▲ Proof: All fractional models can be converted to an LFT ˙ x z∆ = A B∆ C∆ D∆ x w∆ , w∆ = ∆z∆ ▲ the LFT gives the affine descriptor form: I −B∆∆ O I − D∆∆ ˙ x z∆ = A C∆ x
- Can give representations of smaller dimensions
▲ Example
1 δ1 δ2 1 + δ1 δ2 1
˙ ω z1 z2
=
−1 −1 1
ω ⇔ (1 + δ1) ˙ ω = −(1 + δ2)ω
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❶ Motivations for uncertain descriptor modeling
■ General descriptor models Exx ˙ x + Exππ = Ax + Bu y + Exy ˙ x + Eyππ = Cx + Du
- x: state ; u: inputs
- π: linearly constrained signals
- Exx and A may not be square
▲ Can be converted to ˆ E ˙ ˆ x = ˆ Aˆ x+ ˆ Bu with ˆ E and ˆ A square and ˙ ˆ x =
˙ x π λ
▲ Not recommend: increased size of the model
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Outline ❶ Motivations for uncertain descriptor modeling ❷ Affine polytopic models ❸ LFT models - frequency dependent models ❹ Augmented descriptor models and conservatism reduction
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❷ Affine polytopic models
■ All fractional models have affine descriptor representations Exx(∆) ˙ x + Exπ(∆)π = A(∆)x + B(∆)u y + Exy(∆) ˙ x + Eyπ(∆)π = C(∆)x + D(∆)u
- Models also used for polynomial non-linear models [CTF02]
■ General affine descriptor data −Exx(∆) −Exπ(∆) A(∆) B(∆) −Eyx(∆) −Eyπ(∆) C(∆) D(∆) = M(∆)
- Different classes of affine models
▲ intervals: M M(∆) M
(element-wise mij ≤ mij(∆) ≤ mij)
▲ parallelotopes: M(∆) = M |0| + ¯
p p=1 δpM |p|
: |δp| ≤ 1 ▲ polytopes: M(∆) ∈ co
- M [v=1...¯
v]
- intervals ⊂ parallelotopes ⊂ polytopes
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❷ Affine polytopic models
■ Example: two mass spring system
M1 M2 x1 u k f x2eq w1 w2
M1¨ x1 + f( ˙ x1 − ˙ x2) + k(x1 − x2) = u + w1 M2¨ x2 + f( ˙ x2 − ˙ x1) + k(x2 − x1) = w2
- General affine data model
M1 f −f k −k M2 −f f −k k
- =M(∆)
¨ x1 ¨ x2 ˙ x1 ˙ x2 x1 x2
=
- u + w1
w2
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❷ Affine polytopic models
■ Example: two mass spring system - continued
- 4 uncertain parameters Mi ≤ Mi ≤ M i,
f ≤ f ≤ f, k ≤ k ≤ k M(∆) =
- M1
f −f k −k M2 −f f −k k
- Interval model generates conservatism (elements assumed independent)
M1 f −f k −k M2 −f f −k k
-
M1 f −f k −k M2 −f f −k k
-
M1 f −f k −k M2 −f f −k k
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❷ Affine polytopic models
■ Example: two mass spring system - continued M(∆) =
- M1
f −f k −k M2 −f f −k k
- Parallelotopic model
▲ Nominal model: M |0| (center of the intervals)
M(∆) = M|0| + δM1
1 2(M1 − M1)
1
. . .
+δk 1 2(k − k) 0 1 −1 −1 1
- M|k|
▲ M |k| "axis" of variations along δk.
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❷ Affine polytopic models
■ Example: two mass spring system - continued M(∆) =
- M1
f −f k −k M2 −f f −k k
- Polytopic model: 24 = 16 vertices (δi = ±1 in parallelotopic model)
M [1] =
- M1
f −f k −k M2 −f f −k k
- M [2] =
- M1
f −f k −k M2 −f f −k k
- .
. .
M [16] =
- M1
f −f k −k M2 −f f −k k
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❷ Affine polytopic models
■ Some techniques to deal with affine uncertain models
- General type of analysis criteria
ηTΘ(∆)η < 0 , ∀η = 0 : M(∆)η = 0 ▲ Example: negative definite derivative of Lyapunov function V = xTP(∆)x ˙ V = ηT
- O
P(∆) P(∆) O
- η < 0, ∀η =
- ˙
x x
- = 0 :
- −I
A(∆)
- η = 0
- Usual LMI type result
(M ⊥(∆) matrix generating the null-space of M(∆))
M ⊥T(∆)Θ(∆)M ⊥(∆) < O ▲ Problem: M ⊥(∆) is a rational function of ∆ ▲ Solutions: SOS [HG05, Sch06], Polyá [CGTV09, OdOP08]
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❷ Affine polytopic models
■ Some techniques to deal with affine uncertain models
- General type of analysis criteria
ηTΘ(∆)η < 0 , ∀η = 0 : M(∆)η = 0
- Usual LMI type result
(M ⊥(∆) matrix generating the null-space of M(∆))
M ⊥T(∆)Θ(∆)M ⊥(∆) < O
- Slack variables results
(variables issued from the "creation" Finsler lemma)
∃F : Θ(∆) < FM(∆) + M T(∆)F T ▲ Conservative, but sufficient to test at the vertices ▲ Θ(∆) affine (parameter-dependent Lyapunov function) ▲ [OBG99, PABB00, EH04, PDSV09]
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Outline ❶ Motivations for uncertain descriptor modeling ❷ Affine polytopic models ❸ LFT models - frequency dependent models ❹ Augmented descriptor models and conservatism reduction
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❸ LFT models
■ Affine polytopic models well adapted for scalar parametric uncertainty ■ LFT suitable for other types of uncertainties:
- Frequency dependent uncertainties
- Linear / non-linear operators
- Time-varying parameters
- ...
z∆ w
∆
∆
Σ
■ Linear combination of repeated uncertainties [Sch06] ∆ =
- Jj(Irj ⊗ ∆j)Kj ,
[J1 · · · J¯
] orthonormal
▲ Example: bloc-diagonal uncertainties ∆ =
∆1 δ2 δ2
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❸ LFT models
■ Dissipative structured parametric uncertainties
- An uncertain matrix ∆ is said to be {Ψ1, Ψ2, Ψ3}-dissipative if
- I
∆∗
-
Ψ1 Ψ2 Ψ∗
2
Ψ3 I ∆ ≤ O .
- An uncertain matrix ∆ is said to be {Φ1, Φ2, Φ3}-structured if
- I
∆∗
-
Φ1 Φ2 Φ∗
2
Φ3 I ∆ = O .
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❸ LFT models
- Examples of {Ψ1, Ψ2, Ψ3}-dissipative uncertainties
▲ Norm-bounded uncertainties are {−γ2I, O, I}-dissipative
- I
∆∗ −γ2I O O I I ∆
- = −γ2I + ∆∗∆ ≤ O .
w∆ = ∆z∆ ⇒ w∆ ≤ γz∆ ▲ Positive real uncertainties are {O, −I, O}-dissipative
- I
∆∗ O −I −I O I ∆
- = −(∆∗ + ∆) ≤ O .
w∆ = ∆z∆ ⇒ < w∆|z∆ > ≥ 0
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❸ LFT models
- Examples of {Ψ1, Ψ2, Ψ3}-dissipative uncertainties - continued
▲ Uncertainties in an "ellipsoid" are {∆∗
0Z∆0 − R, −∆∗ 0Z, Z}-dissipative
- I
∆∗ ∆∗
0Z∆0 − R
−∆∗
0Z
−Z∆0 Z I ∆
- = (∆ − ∆0)∗Z(∆ − ∆0) − R ≤ O .
(discs of the complex plane for scalar ∆ = δ)
▲ Uncertainties in a "half space" {−∆∗
0N + N∆0, N ∗, O}-dissipative
- I
∆∗ −∆∗
0N + N∆0
N∗ N O I ∆
- = (∆ − ∆0)∗N + N ∗(∆ − ∆0) ≤ O .
(half of the complex plane limited by a line for scalar ∆ = δ)
- {Φ1, Φ2, Φ3}-structured uncertainties: border of "ellipsoids" or of "half spaces"
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❸ LFT models
- {Ψ1, Ψ2, Ψ3}-dissipative {Φ1, Φ2, Φ3}-structured, examples
[IH05]
▲ δ = (jω)−1 with bounded frequencies ω ∈ [ ω ω ]: {2, −j(ω + ω), 2ωω}-dissipative {0, 1, 0}-structured ▲ δ = (jω)−1 with high frequencies ω ≥ ω ≥ 0: {0, −jω, 2ω2}-dissipative {0, 1, 0}-structured ▲ δ = e−jω with bounded frequencies ω ∈ [ ω ω ]: {2 cos ω−ω
2 , −ej ω+ω
2 , 0}-dissipative
{−1, 0, 1}-structured
- −ω
- ω
ω −j / −j / −ω
▲ δ ∈ R bounded δ ∈ [ δ δ ]: {2δδ, −(δ + δ), 2}-dissipative {0, j, 0}-structured
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❸ LFT models
■ System analysis in frequency intervals: s−1 = (jω)−1 , ω ∈ [ ω ω ]
- Allows loop-shaping type specifications
- Have interpretations in time domain [IHF05]
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❸ LFT models
■ Performances?
- Stability: no poles in C+ ⇔ well-posedness w.r.t. s−1 ∈ C+
- L2 perf: z2 ≤ γw2 ⇔ well-posedness w.r.t. w = ∇z : ∇2 ≤ 1
γ
▲ Can be tested for given frequencies or for frequency intervals
- Dissipativity:
∞
- z(t)
w(t)
∗
Ψ1 Ψ2 Ψ∗
2
Ψ3 z(t) w(t)
- dt ≥ 0
⇔ well-posedness w.r.t. w = ∇z : ∇ {Ψ1, Ψ2, Ψ3}-dissipative ■ Performances ⇔ well-posedness w.r.t. uncertain operators
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❸ LFT models
■ Well-posedness [Saf80]
z w w z
- For all bounded external signals ( ¯
w, ¯ z)
the internal signals (w, Ez) are unique and bounded
▲ Example: z = ˙ x, w = ∇ ˙ x = x (i.e. ∇ integrator).
Well posedness ⇔
∀ initial conditions ¯ w = x(0) and bounded disturbances ¯ z x is unique, no impulsive modes, no divergence (stability)
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❸ LFT models
■ Well-posedness [PAHG07]
z w w z
- Integral quadratic separation (IQS) result
▲ Assume E = E1E2 with E1 full column rank and let M =
- −E1
A
- ▲ The loop is well-posed iff there exists Θ such that
ηTΘη < 0 , ∀η = 0 : Mη = 0
(1) and for all “uncertainties"
∞ E2z(t) [∇z](t)
∗
Θ E2z(t) [∇z](t) dt ≥ 0
(2)
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❸ LFT models
- IQS result
▲ (1): LMI-type constraint (M ⊥TΘM ⊥ < O) ▲ (2): Integral quadratic constraint (IQC)
- IQS applies easily to uncertainties defined, or included in IQCs
▲ Example: ∇ = Ir ⊗ ∆, ∆ is {Ψ1, Ψ2, Ψ3}-dissipative {Φ1, Φ2, Φ3}-structured Θ = P ⊗ Ψ1 P ⊗ Ψ2 P ⊗ Ψ∗
2
P ⊗ Ψ3 + R ⊗ Ψ1 R ⊗ Ψ2 R ⊗ Ψ∗
2
R ⊗ Ψ3 P > O R = R∗
(generalized version of D/G-scaling)
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❸ LFT models
■ IQC also defined in the frequency domain (Parseval) ∞ E2z(jω) [∇z](jω)
∗
Θ E2z(jω) [∇z](jω) dω ≥ 0
(3)
- IQC formulas [MR97, JM99] apply for building IQS results
- ∇ can contain
▲ Saturations [FLR06, PTGSB12] ▲ Delays [JS01, GP07, PAHG07] ▲ ... to be continued ■ Parametrizing Θ solutions to the IQC is in general conservative [MSF97, IH05] ▲ Lossless formulas iff ∆ =
¯
- j=1
Jj(Irj⊗∆j)Kj ¯ = 2 , r1 > 1 , r2 = 1 ¯ = 3 , r1 = r2 = r3 = 1
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Outline ❶ Motivations for uncertain descriptor modeling ❷ Affine polytopic models ❸ LFT models - frequency dependent models ❹ Augmented descriptor models and conservatism reduction
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❹ Augmented descriptor models and conservatism reduction
■ Except in special cases finding Θ solution to the IQCs is conservative
- Existing parameterizations of Θ apply both for constant and time-varying ∆
- But ∆
∆∞ ⊂ ∆ ∆d ⊂ ∆ ∆0 where ▲ ∆ ∆0 set of constant uncertainties such that Σ(∆) is stable ▲ ∆ ∆d set of uncertainties with ˙ ∆ ≤ d such that Σ(∆) is stable ▲ ∆ ∆∞ set of TV uncertainties with switches such that Σ(∆) is stable
- Reducing conservatism: can be achieved by introducing information about ˙
∆
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❹ Augmented descriptor models and conservatism reduction
■ Descriptor augmentation method - example
- Assume system in LFT form
- ˙
x = Ax + Bw∆ z∆ = Cx + Dw∆
⋆
- x = s−1 ˙
x w∆ = ∆z∆
- Add information about derivative of uncertainty:
˙ w∆ = ∆ ˙ z∆
- =w∆1
+ ˙ ∆z∆
- =w∆2
- Define derivative of exogenous signals:
˙ z∆ = C ˙ x + D ˙ w∆ = C ˙ x + Dw∆1 + Dw∆2 , w∆ = s−1 ˙ w∆
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❹ Augmented descriptor models and conservatism reduction
■ Descriptor augmentation method - example - continued
- ˙
x = Ax + Bw∆ z∆ = Cx + Dw∆
⋆
- x = s−1 ˙
x w∆ = ∆z∆
- All equations gathered separating linear constrains and "uncertainties"
˙ x = Ax + Bw∆ z∆ = Cx + Dw∆ ˙ z∆ − C ˙ x = Dw∆1 + Dw∆2 ˙ w∆ = w∆1 + w∆2 0 = w∆ − w∆
⋆
x = s−1 ˙ x w∆ = s−1 ˙ w∆ w∆ = ∆z∆ w∆1 = ∆ ˙ z∆ w∆2 = ˙ ∆z∆
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❹ Augmented descriptor models and conservatism reduction
■ Descriptor augmentation method - example - continued
- Descriptor LFT form of system augmented with information on derivatives
z =
- ˙
x ˙ w∆ z∆ ˙ z∆ T , w =
- x
w∆ w∆ w∆1 w∆2 T
I O O O O O I O −C O O I O I O O O O O O
z =
A B O O O C D O O O O O O D D O O O I I O I −I O O
w ⋆ w =
s−1In+m O O O ∆ O O O ∆ O ˙ ∆ O
z
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❹ Augmented descriptor models and conservatism reduction
■ IQS results applicable to the original & the augmented descriptor model
- LMI formulas for augmented model are less conservative
- IQS formulas implicitly contain Lyapunov certificates
▲ Lyapunov certificate in case of LMI for original model V = xTPx ▲ Parameter-dependent Lyapunov certificate in case of augmented system V = x w∆
T
P x w∆ , w∆ = ∆(I − D∆)−1Cx
- The system augmentation technique is also proved efficient for systems with
delays [PAHG07], with saturations [PTGSB12]...
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Conclusions ■ Some advantages of descriptor models
- Natural models from physics
- More flexibility for system description
- Affine descriptor models are alternatives to LFT models
- Well-posedness of descriptor LFT loops
= general framework for robust analysis problems (includes frequency dependent specifications/uncertainties)
- System augmentation with derivatives = less conservative results
(made possible thanks to descriptor modeling)
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