Volume 2011, Article ID 123403,13pages doi:10.1155/2011/123403
Research Article
The Boundary Crossing Theorem and the Maximal Stability Interval
Jorge-Antonio L ´opez-Renteria,
1Baltazar Aguirre-Hern ´andez,
1and Fernando Verduzco
21Divisi´on de Ciencias B´asicas e Ingenier´ıa, Departamento de Matem´aticas, Universidad Aut´onoma Metropolitana-Iztapalapa, Avenida San Rafael Atlixco no. 186, Col. Vicentina, 09340 M´exico, DF, Mexico
2Divisi´on de Ciencias Exactas y Naturales, Departamento de Matem´aticas, Universidad de Sonora, Boulevard Rosales y Luis Encinas s/n, Col. Centro, 83000, Hermosillo, Son, Mexico
Correspondence should be addressed to Baltazar Aguirre-Hern´andez,[email protected] Received 9 October 2010; Accepted 11 March 2011
Academic Editor: J. Jiang
Copyrightq2011 Jorge-Antonio L ´opez-Renteria et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
The boundary crossing theorem and the zero exclusion principle are very useful tools in the study of the stability of family of polynomials. Although both of these theorem seem intuitively obvious, they can be used for proving important results. In this paper, we give generalizations of these two theorems and we apply such generalizations for finding the maximal stability interval.
1. Introduction
Consider the linear system
x˙Ax, 1.1
where Ais an n×n matrix with constant coefficients andx ∈ n. It is known that if the characteristic polynomial,pAtis a Hurwitz polynomial, that is, all of its roots have negative real part, then the origin is an asymptoticly stable equilibrium. Great amount of information has been published about these polynomials since Maxwell proposed the problem of finding conditions for verifying if a given polynomial has all of its roots with negative real part 1. At first the researchers focused in the problem proposed for Maxwell and the Routh- Hurwitz criterion, the Hermite-Biehler theorem and other criteria were obtained. For reading the proofs of these results the books2–4can be consulted. After the scientists began to study other related problems, for instance, the problem of giving conditions for a given family
of polynomials consist of Hurwitz polynomials alone. This problem has its motivation in the applications because when a physical phenomenon is modeled, families of polynomials must be considered due the presence of uncertainties. Maybe the most famous results about families of Hurwitz polynomials are the Kharitonov’s theorem5and the Edge theorem6 which consider interval polynomials and polytopes of polynomials, respectively. However, other families have been studied also, for example, the cones and rays of polynomails see 7, 8 or the segments of polynomails 9–11. Besides in the study of Hurwitz polynomials, topological approaches have been used recentlysee12,13. Good references about Hurwitz polynomilas which were reported during 1987–1991 can be found in 14.
The books2,15,16are very recommendable works for consulting questions about families of stable polynomilas. Many proofs of results about the stability of families of polynomials are based in the boundary crossing theorem17and in the zero exclusion principlesee2 for a proof. In this way the importance of these two results has been appreciated. Now, in this paper we give generalizations as the boundary crossing theorem as the zero exclusion principle and we apply these generalizations for giving an alternative method to calculate the maximal interval for robust stability, which was studied by Białas. We will explain the differences between both methods.
2. Main Results
We have divided this section in two parts: in the first subsection we present generalizations of the mentioned theorems and in the second subsection we apply such generalizations for calculating the maximal stability interval for robust stability.
2.1. Generalizations of the Boundary Crossing Theorem and Zero Exclusion Principle
First, we give the known boundary crossing theorem. Consider a family of polynomials Pλ, tsatisfying the following assumption.
Assumption 2.1. Pλ, tis a family of polynomials of 1fixed degreen,
2coefficients are continuous respectλin a fixed intervalI a, b.
Also let us to consider the complex plane and letS ⊂ be any given open set and denote the boundary ofSby∂Sand the complement asU − S. The following results are presented in2, page 34.
Theorem 2.2boundary crossing theorem. Under Assumption2.1, ifPa, thas all its roots in SwhereasPb, thas at least one root inU. Then there exists at least oneρina, bsuch that
iPρ, thas all its roots inS ∪∂S, iiPρ, thas at least one root in∂S.
Now suppose thatδt, pdenotes a polynomial whose coefficients depend continu- ously on the parameter vectorp ∈ l which varies in a setΩ ⊂ l and thus generates the family of polynomials
Δt: δ
t, p
|p∈Ω
. 2.1
Theorem 2.3zero exclusion principle. Assume that the polynomial family2.1 has constant degree, contains at least one stable polynomial, andΩis pathwise connected. Then the entire family is stable if and only if
0∈/Δt∗, ∀t∗∈∂S. 2.2
Now we present our generalizations. In them we will considerS−.
Theorem 2.4generalization 1 of Theorem2.2. Under Assumption2.1, suppose thatPa, thas n1roots in−andn−n1roots in, andPb, thas at mostn1−1 roots in− and at leastn−n11 roots in. Then there exists at least oneρina, bsuch that
iPρ, thas at leastn1roots in−∪i , iiPρ, thas at least one root ini .
Theorem 2.5generalization 2 of Theorem2.2. Under Assumption2.1, suppose thatPa, thas n1 roots in− andn−n1 roots in, andPb, thasm1 roots in− and n−m1 roots in. If n1/m1, Then there exists at least oneρina, bsuch that
iPρ, thas at leastn1roots in−∪i , iiPρ, thas at leastn−n1roots in ∪i , iiiPρ, thas at least one root ini .
Theorem 2.6 generalization of Theorem 2.3. Consider the polynomial family Pλ, t with constant degree, where λ ∈ Ω and Ω ⊂ l is a pathwise connected set. Suppose there exists an element of the family withn1 roots in− andn−n1roots in. Then the entire family still having n1roots in− andn−n1roots in if and only if
Pλ, iω/0 ∀λ∈Ω,∀ω∈ . 2.3
2.2. Application: An Alternative Method for Calculating the Maximal Stability Interval
We begin this subsection with three important definitions that can be seen in pages 50 to 51 of16.
Definition 2.7. Consider the uncertain polynomialPt, k p0t kp1twithp0tassumed Hurwitz stable and the uncertainty bounding setK k−, kwithk− ≤ 0 andk ≥ 0. We define the subfamilies
Pk
p·, k|0≤k≤k , P
k−
p·, k|k− ≤k≤0
. 2.4
Definition 2.8maximal stability interval. Associated with the subfamilyPkis the right- sided robustness margin
kmax sup
k:Pkis robustly stable
, 2.5
and asociated with the subfamilyPk−is the left-sided robustness margin kmin− inf
k−:P k−
is robustly stable
. 2.6
Subsequently we callKmax k−min, kmax the maximal interval for robust stability.
Definition 2.9. Given ann×nmatrixM, we defineλmaxMto be the maximum positive real eigenvalue ofM. WhenMdoes not have any positive real eigenvalue, we takeλmaxM 0. Similarly, we defineλ−minMto be the minimum negative real eigenvalue ofM. When M does no have any negative real eigenvalue, we takeλ−minM 0−.
Białas10proved the following theorem.
Theorem 2.10eigenvalue criterion. Consider the uncertain polynomialPt, k p0t kp1t withPt,0 p0tHurwitz stable and having positive coefficients and degp0t>degp1t. Then the maximal interval for robust stability is described by
kmax 1
λmax
−H−1 p0
H p1
,
kmin− 1
λ−min
−H−1 p0
H p1
,
2.7
whereHp0andHp1are the corresponding matrices of Hurwitz ofp0tandp1t, respectively, and for purpose of conformability of matrix multiplication, Hp1 is an n×nmatrix obtained by treatingp1tas ann-degree polynomial.
Now we will explain our approach for calculating the maximal stability interval. Let p0tbe ann-degree polynomial andp1ta polynomial such thatn >degp1t. Consider the family of polynomialspct p0t kp1t. By evaluatingp0−tandpctiniωwe get
p0−iω P ω2
−iωQ ω2
, pciω P
ω2 kp
ω2 iω
Q ω2
kq
ω2 , 2.8
wherep, q, P, Qare polynomials. Then pciωp0−iω P2
ω2
ω2Q2 ω2 k
p ω2
P ω2
ω2q ω2
Q ω2 ikω
q ω2
P ω2
−p ω2
Q ω2 .
2.9
Define the polynomials
Fω p ω2
P ω2
ω2q ω2
Q ω2
, Gω P2
ω2
ω2Q2 ω2
, Hω q
ω2 P
ω2
−p ω2
Q ω2
.
2.10
Therefore, we can rewritepciωp0−iωaspciωp0−iω Gω kFω ikωHω.
Definition 2.11. For an arbitrary polynomialftwe define the set of its roots as R
f
ζ∈ |fζ 0
. 2.11
LetRfÊdenote the set of positive real elements ofRf. It is clear thatRfÊcould be an empty set.
Now letFω, Gω, andHωbe the polynomials defined above. Define the sets K{Fωl|ωl∈RHÊ∪ {0}, Fωl>0},
K−{Fωl|ωl∈RHÊ∪ {0}, Fωl<0}. 2.12
If there is no elements inRHÊ∪ {0}such thatFωl> 0 then we will defineK {0}.
Similarly, if there is no elements inRHÊ∪ {0}such thatFωl<0 then defineK− {0−}.
Note that only can happen eitherK− {0−}orK {0}but both at the same time never since we can always evaluate inω0. That is, we always have an extreme.
Therefore we have the following alternative method for calculating the maximal stability interval.
Theorem 2.12. Consider the polynomial familypct p0t kp1twithp0tHurwitz stable and having positive coefficients, and letFω, Gω, andHωbe the polynomials defined above. Then the maximal interval of stability forpctis described by
k−minmax
−Gωl
Fωl |Fωl∈K
,
kmaxmin
−Gωl
Fωl |Fωl∈K−
.
2.13
Remark 2.13. A difference with the Białas method is that in our approach it is not necessary to calculate the inverse of any matrix. Other difference is that in the Białas method the roots of ann-degree polynomial must be found while in our approach we have that if degree of both nandm, resp., n > mp0tandp1tis either even or odd then degHω nm−2 and in the other cases degHω nm−1. Therefore, by symmetry ofHωwe have to find the roots of a polynomial with degreenm−2/2 ornm−1/2 both less than or equal to n−1.
Example 2.14. Consider the polynomialp0t t36t212t6 andp1t t2−2t1, for the polynomial familypt, k p0t kp1t. We will verify the maximal stability interval by Białas method. First we have
H p0t
⎛
⎜⎜
⎝ 6 6 0 1 12 0 0 6 6
⎞
⎟⎟
⎠, H p1t
⎛
⎜⎜
⎝ 1 1 0 0 −2 0 0 1 1
⎞
⎟⎟
⎠. 2.14
Next,
−H p0t−1
H p1t
−
⎛
⎜⎜
⎜⎜
⎜⎝ 2 11 −1
11 0
− 1 66
1 11 0 1
66 −1 11
1 6
⎞
⎟⎟
⎟⎟
⎟⎠
⎛
⎜⎜
⎝ 1 1 0 0 −2 0 0 1 1
⎞
⎟⎟
⎠
⎛
⎜⎜
⎜⎜
⎜⎝
− 2 11 −4
11 0 1
66 13 66 0
− 1 66 −4
11 −1 6
⎞
⎟⎟
⎟⎟
⎟⎠,
2.15
whose characteristic polynomial is λ3 −2/11λ2−1/36λ 1/198 which is a 3-degree polynomial and has as roots λ1 λ2 −1/6 andλ3 2/11. Thus λmaxHp0−1Hp1
2/11 and λ−minHp0−1Hp1 −1/6. Then pt, k p0t kp1t is robustly stable in k−min, kmax −6,11/2.
Now with our proposed method. We see
p0iω
6−6ω2 iω
12−ω2 P
ω2
iωQ ω2
, p1iω
1−ω2
iω−2 p
ω2 iωq
ω2 .
2.16
Thus,
Fω 8ω4−36ω26, Gω ω612ω472ω236, Hω −ω425ω2−24.
2.17
ThusRHÊ{1,√
24}. Now,
F1 −22<0, F√
24
3750>0, F0 6>0, G1 121, G√
24
22527, G0 36.
2.18
Therefore
kmax−G1 F1 11
2 , k−minmax
⎧⎨
⎩−G√ 24 F√
24
,−G0 F0
⎫⎬
⎭−6.
2.19
Note that we just only need to compute a 2-degree polynomial root in our method, while in Białas one it is a 3-degree polynomial.
Example 2.15. Consider the linear control system
x˙
⎛
⎜⎜
⎜⎜
⎜⎝
0 1 0 0
0 0 1 0
0 0 0 1
−1 −7 −2 −3
⎞
⎟⎟
⎟⎟
⎟⎠x
⎛
⎜⎜
⎜⎜
⎜⎝ 0 0 0 1
⎞
⎟⎟
⎟⎟
⎟⎠−3k,−2k,−k,0x. 2.20
From this system we have thatp0t t4t37t22t3 andp1t t22t3 and their Hurwitz matrices are
H p0t
⎛
⎜⎜
⎜⎜
⎜⎝
1 2 0 0 1 7 3 0 0 1 2 0 0 1 7 3
⎞
⎟⎟
⎟⎟
⎟⎠, H p1t
⎛
⎜⎜
⎜⎜
⎜⎝
0 2 0 0 0 1 3 0 0 0 2 0 0 0 1 3
⎞
⎟⎟
⎟⎟
⎟⎠, 2.21
where the inverse ofHp0is
H p0t−1
⎛
⎜⎜
⎜⎜
⎜⎜
⎜⎜
⎜⎝ 11
2 −4 7
6
7 0
−2 7
2 7 −3
7 0 1
7 −1 7
5
7 0
− 5 21
5 21 −32
21 1 3
⎞
⎟⎟
⎟⎟
⎟⎟
⎟⎟
⎟⎠
. 2.22
Hence, the 4-degree characteristic polynomial of the matrix
−H p0t−1
H p1t
−
⎛
⎜⎜
⎜⎜
⎜⎜
⎜⎜
⎜⎝ 11
2 −4 7
6
7 0
−2 7
2 7 −3
7 0 1
7 −1 7
5
7 0
−5 21
5 21 −32
21 1 3
⎞
⎟⎟
⎟⎟
⎟⎟
⎟⎟
⎟⎠
⎛
⎜⎜
⎜⎜
⎜⎝
0 2 0 0 0 1 3 0 0 0 2 0 0 0 1 3
⎞
⎟⎟
⎟⎟
⎟⎠
⎛
⎜⎜
⎜⎜
⎜⎜
⎜⎜
⎜⎝ 0 −18
7 −24 7 0 0 2
7 12
7 0 0 −1
7 −13 7 0 0 5
21 24
7 1
⎞
⎟⎟
⎟⎟
⎟⎟
⎟⎟
⎟⎠
2.23
ist4 12/7t3 3/7t2 −2/7t and has as rootsλ1 0, λ2 2/7 and λ3,4 −1. Then λmaxHp0−1Hp1 2/7 andλ−minHp0−1Hp1 −1. Therefore, system2.20is robustly stable in−1,7/2.
Now with our method. By evaluatingp0tandp1tiniωwe have p0iω
ω4−7ω23 iω
−ω22 P
ω2
iωQ ω2
, p1iω
−ω23
iω2 p
ω2 iωq
ω2 .
2.24
Thus,
Fω −ω68ω4−20ω29, Gω ω8−13ω651ω4−38ω29, Hω ω2
−9ω2 .
2.25
It is not hard to see thatRHÊ {0,3}. Next,F0 9 >0,F3 −252<0, andG0 9, G3 882. Therefore,
kmax −G3 F3 7
2 k−min−G0
F0 −1.
2.26
Note the easiness of roots finding for our polynomialHω.
As we see, in our method computations are easier operatively speaking since matrices inverse and roots of bigger degree polynomials have been found in Białas method.
3. Proofs of the Theorems
Before start with the proofs of the theorems we present the following lemma wich can be found in3.
Lemma 3.1 continuous root dependence. Consider the family of polynomials P described by Pλ, t n
i0aiλtiandλ∈Ωunder Assumption2.1. Then the roots ofPλ, tvary continuously with respect toλ∈Ω. That is, there exist continuously mappingsti :Ω → fori1,2, . . . , nsuch thatt1λ, . . . , tnλare the roots ofPλ, t.
3.1. Proof of Theorem
2.4SincePλ, tsatisfies Assumption2.1, by Lemma3.1there existncontinuous function roots ofPλ, t, sayt1λ, . . . , tnλ,λ ∈ a, b. Let us denote αjλ Êtjλas the real parts of the roots. Without loss of generality we can suppose that forj 1, . . . , n1,αja ∈ − and
for j n1 1, . . . , n,αja ∈ , while forλ bat most n1−1 αjb’s belong to − and at leastn−n11 belong to . Then there exists at least onetjλsuch thatαja < 0 and αjb > 0. Letαj1λ, . . . , αjmλbe such functions. Then by continuity and the intermediate value theorem we have that for each 1≤r ≤mthere existsρr ∈a, bsuch thatαjrρr 0.
Defineρmin{ρr |r1, . . . , m}. Therefore, forλρat least oneαjrρ 0. ThusPρ, thas n1roots in−∪i with at least one root ini , as we claim.
The proof of Theorem2.5is similar.
3.2. Proof of Theorem
2.6⇒If all of the elements of the family haven1roots in− andn−n1roots in the it is clear thatPλ, iω/0 for allω∈ and for allλ∈Ω.
⇐Suppose thatPλ, iω/0 for allω ∈ and for allλ ∈ Ω. If there isλ0 ∈Ωsuch that the polynomialPλ0, thasm1roots in− andn−m1roots in withn1/m1, the from Theorem2.5there exsistsρsuch thatPρ, iω 0 for someω∈ , which is a contradiction.
3.3. Proof of Theorem
2.12By generalization of zero exclusion principle, the polynomialpctp0−thasnroots in − andnroots in if and only if
pciωp0−iω/0 3.1
for allω∈ . Thus, ifksatisfies
pciωp0−iω 0 3.2
for someω∈ , then
Gω kFω ikωHω 0 3.3
for someω∈ . Consequently
ωHω 0,
Gω kFω 0. 3.4
And this system is satisfied ifk−Gωl/Fωl, whereωl 0 orωl∈RH. SinceGω>0 for allω∈ and we want to know the minimumk >0 and the maximumk <0 where it does not happen, then
k−minmax
−Gωl
Fωl |Fωl>0, ωl0 orωl∈RH
,
kmaxmin
−Gωl
Fωl |Fωl<0, ωl0 or ωl∈RH
.
3.5
Now by symmetry ofFωandHωwe will just consider real positive roots ofHω. Thus
k−minmax
−Gωl
Fωl |Fωl∈K
,
kmaxmin
−Gωl
Fωl |Fωl∈K−
.
3.6
This ends the proof.
Remark 3.2. In the proof it is not necessary to consider cases whenFωl 0, since in other case in the system3.4we would haveGωl 0, but
Gωl p0iωl2 p0iωlp0−iωl 0,
3.7
which is impossible sincep0tis Hurwitz. However, if occurs eitherK{0}orK−{0−}, then we evaluate inω0 and depending on sign ofF0we will get either
k−min lim
r→0−G0
r −∞ 3.8
or
kmax lim
r→0−−G0
r ∞. 3.9
The following example illustrates the second part of Remark3.2.
Example 3.3. Consider the linear control system
x˙
⎛
⎜⎜
⎝
0 1 0
0 0 1
−6 −11 −6
⎞
⎟⎟
⎠x
⎛
⎜⎜
⎝ 0 0 1
⎞
⎟⎟
⎠
−13
2 k,−11k,−5k
x. 3.10
Then we have thatp0t t36t211t6 andp1t 5t211t 13/2. First, for Białas’s method we have that the Hurwitz matrices ofp0tandp1tare
H p0t
⎛
⎜⎜
⎝ 6 6 0 1 11 0 0 6 6
⎞
⎟⎟
⎠, H p1t
⎛
⎜⎜
⎜⎜
⎝ 5 13
2 0
0 11 0 0 5 13
2
⎞
⎟⎟
⎟⎟
⎠. 3.11
Hence,
−H p0t−1
H p1t
⎛
⎜⎜
⎜⎜
⎜⎝ 11 60 −1
10 0
− 1 60
1 10 0 1
60 −1 10
1 6
⎞
⎟⎟
⎟⎟
⎟⎠
⎛
⎜⎜
⎜⎜
⎝ 5 13
2 0
0 11 0 0 5 13
2
⎞
⎟⎟
⎟⎟
⎠
⎛
⎜⎜
⎜⎜
⎜⎝
−11 12 −11
120 0 1
12 −119 120 0
− 1 12
19 120 −13
12
⎞
⎟⎟
⎟⎟
⎟⎠,
3.12
whose characteristic polynomial isλ3−359/120λ2 4297/1140λ−143/144which is a 3-degree polynomial and its roots areλ1,2 −229±i√
359/240 and λ3 −13/12. Hence λmax−Hp0−1Hp1 0−andλ−min−Hp0−1Hp1 −13/12. Thenpt, k p0t kp1t is robustly stable forkin−12/13,∞.
With our proposed method we can see that p0iω
6−6ω2 iω
11−ω2 P
ω2
iωQ ω2
, p1iω
13 2 −5ω2
11iω p
ω2 iωq
ω2 .
3.13
Thus,
Fω 19ω4112ω239, Gω ω6−94ω449ω236, Hω −5ω4−9ω2−11.
3.14
Note that Fω > 0 for all ω ∈ and by a single test for second-order equations, Hω have no real roots. Therefore by Remark3.2kmax ∞andkmin −G0/F0 −12/13.
Consequently,p0t kp1tis stable for allk∈−12/13,∞.
4. Conclusions
In this paper, first we obtain generalizations of the Boundary Crossing Theorem and the Zero Exclusion Principle, which are results that allow to obtain important results about stability of families of polynomials. Next we use such generalizations for calculating the maximal
interval of stability, which is a different approach to the Białas method. Since in Białas method we have to find the inverse of the matrixHp0and the roots of then-degree characteristic polynomial of−Hp0−1Hp1, we have found that in our approach easier computations have arisen due if degree of bothp0tandp1tis either even or odd then degHω nm−2 and in the other cases degHω nm−1 and by symmetry ofHωwe must to find the roots of a polynomial with degreenm−2/2 ornm−1/2 both less than or equal to n−1, respectively.
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