• Nem Talált Eredményt

92 CHAPTER 7 Connected cruise controllers andV(h)is a range policy function (e.g. constant time-gap spacing policy). The derivative ofV(h) at the uniform equilibrium flow(h, v)equals toV0(h) =κ+ ˜κ(where1/V0(h)is the time-gap).

The parameters of the linearized system areκ,α, βandτ, where the additive uncertainty of these parameters (˜κ,α,˜ β,˜ τ) denote the static uncertainty of the parameters of the human-driven vehicle.˜ The transfer function between the velocity fluctuations of the follower and leader vehicles is written as

T(s) =

(κ+ ˜κ)(α+ ˜α) + (β+ ˜β)s

e1−sϑ(s)˜ 1 +sϑ(s)˜ s2+ (κ+ ˜κ)(α+ ˜α) + (α+ ˜α+β+ ˜β)s

e−sτ1−sϑ(s)˜ 1 +sϑ(s)˜ ,

where the uncertainty of the time delay is modeled by the Rekasius substitution with restriction to s = iω, moreover ω is the frequency and ϑ(iω) =˜ ω−1tan(0.5ω˜τ) is a frequency-dependent real parameter. The follower vehicle is robust string stable if|T(iω)| <1, ω > 0for all allowed uncertainties. Robust string stability with respect to uncertain parameters in the follower’s model can be analyzed by constructing the M-∆uncertain interconnection structure and analyzing the structured singular values, where (s= iωand in case of the Rekasius substitution0≤ω < π/|τ˜|)

M(s) =

M1,1(s) M1,2(s) M2,1(s) M2,2(s)

,

∆(s) = diag[˜κ,α,˜ β,˜ ϑ(s), δ˜ c], δc ∈C,|δc|<1, moreover

M1,1(s) = 1

D(s)



−αe−sτ −e−sτ −e−sτ −2 s2+βse −(κ+s)e −(κ+s)e 2(κ+s)

−αse −se −se 2s

αs3e s3e s3e −s3+s κα+s(α+β) e



,

M1,2(s) = 1 D(s)



s+αe−sτ κs−βse s2+αse (καs2+βs3)e−sτ



,

M2,1(s) = 1 D(s)

αse−sτ se−sτ se−sτ −2s (κα+βs)e−sτ , M2,2(s) = (κα+βs)e

D(s) , D(s) = s2+ κα+s(α+β)

e. Related publications: [179], [180].

APPENDIX A

Computation of the structured singular value

The structured singular value was originally introduced for complex diagonal perturbations in [30], and more detailed mathematical investigations were provided in [181, 134]. Real structured perturbations and mixed perturbation problems were investigated more in details in [182, 135, 175].

It is important to mention that a very similar approach (based on geometric considerations) to calculate the stability margins was introduced in [183, 184].

The definition ofµdepends upon the underlying block structureXK of allowed uncertainties

∆. Here, we follow the notations and definition provided by [175]. Let us consider a matrix M ∈ Cn×n, and three non-negative integers mr,mcandmC withm = mr+mc+mC ≤ n, the block structure is anm-tuple of positive integerski ∈Z+is written as

K={k1, . . . , kmr, kmr+1, . . . , kmr+mc, kmr+mc+1, . . . , kmr+mc+mC}, Σmi=1ki =n, (A.1) and define the set of all allowed perturbation matrices as

XK={∆= diag δr1Ik1, . . . , δmrrIkmr, δ1cIkmr+1, . . . , δcmcIkmr+mc,∆C1, . . . ,∆CmC :

δri ∈R, δci ∈C,∆Ci ∈Ckmr+mc+i×kmr+mc+i}. (A.2) This block structure is able to represent repeated real scalar (δir), repeated complex scalar (δic) and full block complex perturbations (∆Ci ).

Letσ(¯ ·) denote the largest singular value of(·). Then theµ-value ofM is the inverse of the smallestσ(∆)¯ ,∆∈ XK, such that1is an element of the spectrum of the matrix product∆M(see [21, 185]). An equivalent definition says that theµ-value of matrixMis the inverse of the smallest perturbation such thatdet(I−∆M) = 0, i.e.,

µ(M) :=





min∈XK

¯

σ(∆) : det (I−M∆) = 0 1

0, if no∆∈ XKmakesI−M∆singular.

(A.3)

Note that the larger theµ-value, the less robust the system. Also, it can be shown from the definition that for anyα∈ C,µ(αM) =|α|µ(M). However,µ:Cn×n →Ris not a norm, since it does not satisfy the triangle inequality [134].

The computation of the structured singular value is not straightforward, and in general only upper and lower bounds can be determined. It can be shown, that very conservative bounds for complex perturbations can be calculated as

ρ(M)≤µ(M)≤σ(M),¯ (A.4)

where ρ(·)is the spectral radius. Lower bound is exact if ∆ = δc1I, δ1c ∈ Cis a repeated scalar perturbation, and upper bound is exact if∆∈ Cn×nis a full block perturbation. A review on the complex structured singular values and their computation is given by [134].

93

94 Appendix A Computation of the structured singular value The bounds provided by the formulas (A.4) are easily computable, however, rarely sufficient when accurate calculations are required, since the gap between upper and lower bounds can be arbitrarily large [181]. Tighter bounds can be calculated by introducing transformations that affect ρandσ, but does not affect¯ µ. These bounds in case of complex perturbations are reformulated as

max

U∈UK

ρ(UM)≤µ(M)≤ inf

D∈DK

¯

σ(DMD1) =νC(M), (A.5) where

UK={U∈ XK : UU=I}, (A.6)

DK={0<D=D :D∆=∆D, for all∆∈ XK}, (A.7) for details see [30, 181]. The upper bound can be reformulated as a mathematically convex optimization problem that makes the computation of the upper bound feasible. The reformulated bound as a linear matrix inequality (LMI) is written as

νC(M) = inf

ν>0 D∈DK

{ν :MDM< ν2D}. (A.8) In comparison, the lower bound can be found by maximizing the spectral radius of a scaled matrix, however, the problem is not convex and global maximum is not guaranteed to be found.

The computation of real structured singular values is more time consuming, similarly to the complex case, the upper bound can be computed by

νR(M) = inf

ν>0 D∈DK

G∈GK

{ν:MDM+ i(GM−MG)< ν2D}, (A.9)

where

GK ={G=G :G∆=∆G, for all∆∈ XK}, (A.10) andGis block-diagonal with zero block for complex uncertainties. For the detailed structures, see [175].

In the present work the computation of the structured singular value is carried out in Matlab environment, using the built-inmussvfunction included in theµ-Analysis and Synthesis Toolbox developed by [137].

APPENDIX B

Structured singular value and weighted maximum norm

The calculation of the structured singular values is time consuming, even if the upper bound is reformulated into a mathematically convex problem, see Appendix A. Computational effort can be reduced if simpler, but more conservative upper bounds are calculated. Following the results of [21], we give an upper approximation ofµfor complex perturbation structures.

Let us consider a matrix M ∈ Cn×n and the set of perturbations X = {∆ ∈ Cn×n : ∆ = diag(∆C1, . . . ,∆Cl )}, then theµ-value ofMis defined as

µ(M) :=





min∈X

¯

σ(∆) : det (I−M∆) = 0 −1

0, if no∆∈ X makesI−M∆singular. (B.1) Another alternative expression follows from the definition

µ(M) = max

∈X

¯ σ(∆)1

ρ M∆

, (B.2)

where the proof uses the property that for anyα∈C,µ(αM) =|α|µ(M).

The computation of the complex structured singular value requires the solution of a convex optimization problem (see Appendix A) that can be time-consuming for large-scale matrices. In order to speed up the calculation, [21] provided an alternative approach for complex perturbations in order to bound the structured singular value from above. Let us replace the perturbation measure

¯

σin definition (B.1), and introduce a weighted maximum norm instead as k∆kmax:= max

j,k R−1jk|∆jk|, (B.3)

where Rjk ≥ 0 are the elements of the non-negative weight matrixR ∈ Rn×n. In this case the following equivalence holds for∆

k∆kmax≤1 ⇔ |∆jk| ≤Rjk, for all j, k. (B.4) Then an upper bound ofµ-values can be given by the relations [21]

µ(M) = max

∈X kkmax≤1

ρ(M∆)≤ρ MR

, (B.5)

whereMis a non-negative matrix with elementsMjk =|Mjk|. Using this approach the structured singular value can be bounded from above using the spectral radius. To prove the inequality, the

95

96 Appendix B Structured singular value and weighted maximum norm following properties can be used

P1:|[M∆]jk|=| Xn

i=1

Mjiik| ≤ Xn

i=1

|Mji||∆ik|= [M ∆]jk, (B.6) P2:if A1,A2 ∈Rn×n, and0≤[A1]jk ≤[A2]jk, thenρ(A1)≤ρ(A2), (B.7) P3:ρ





A11 · · · A1n ... ... ...

An1 · · · Ann



≤ρ





|A11| · · · |A1n| ... ... ...

|An1| · · · |Ann|



. (B.8)

Detailed derivations, theorems and proofs related to the topic can be found in [21]. An important note is that the inequality in (B.5) is actually an equality ifMis a diagonal matrix.

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