Abstract
Let H be a Hilbert space and \(\nu \in \mathbb {R}\). We saw in the previous chapter how initial value problems can be formulated within the framework of evolutionary equations. More precisely, we have studied problems of the form
for U 0 ∈ H, M 0, M 1 ∈ L(H) and \(A\colon \operatorname {dom}(A)\subseteq H\to H\) skew-selfadjoint; that is, we have considered material laws of the form
You have full access to this open access chapter, Download chapter PDF
Let H be a Hilbert space and \(\nu \in \mathbb {R}\). We saw in the previous chapter how initial value problems can be formulated within the framework of evolutionary equations. More precisely, we have studied problems of the form
for U 0 ∈ H, M 0, M 1 ∈ L(H) and \(A\colon \operatorname {dom}(A)\subseteq H\to H\) skew-selfadjoint; that is, we have considered material laws of the form
Here, the initial value is attained in a weak sense as an equality in the extrapolation space H −1(A). The first line is also meant in a weak sense since the left-hand side turned out to be a functional in \(H_{\nu }^{-1}(\mathbb {R};H)\cap L_{2,\nu }(\mathbb {R};H^{-1}(A))\). In Theorem 9.4.3 it was shown that the latter problem can be rewritten as
In this chapter we aim to inspect initial value problems a little closer but in the particularly simple case when A = 0. However, we want to impose the initial condition for U and not just M 0 U. Thus, we want to deal with the problem
for two bounded operators M 0, M 1 and an initial value U 0 ∈ H. This class of differential equations is known as differential algebraic equations since the operator M 0 is allowed to have a non-trivial kernel. Thus, (10.2) is a coupled problem of a differential equation (on \((\operatorname {ker} M_{0})^{\bot }\)) and an algebraic equation (on \(\operatorname {ker} M_{0}\)). We begin by treating these equations in the finite-dimensional case; that is, \(H=\mathbb {C}^{n}\) and \(M_{0},M_{1}\in \mathbb {C}^{n\times n}\) for some \(n\in \mathbb {N}\).
10.1 The Finite-Dimensional Case
Throughout this section let \(n\in \mathbb {N}\) and \(M_{0},M_{1}\in \mathbb {C}^{n\times n}\).
Definition
We define the spectrum of the matrix pair (M 0, M 1) by
and the resolvent set of the matrix pair (M 0, M 1) by
Remark 10.1.1
-
(a)
It is immediate that σ(M 0, M 1) is closed since the mapping \(z\mapsto \det (zM_{0}+M_{1})\) is continuous.
-
(b)
Note in particular that the spectrum (the set of eigenvalues) of a matrix A corresponds in this setting to the spectrum of the matrix pair (1, −A).
In contrast to the case of the spectrum of one matrix, it may happen that \(\sigma (M_{0},M_{1})=\mathbb {C}\) (for example we can choose M 0 = 0 and M 1 singular). More precisely, we have the following result.
Lemma 10.1.2
The set σ(M 0, M 1) is either finite or equals the whole complex plane \(\mathbb {C}\) . If σ(M 0, M 1) is finite then \(\operatorname {card}(\sigma (M_{0},M_{1}))\leqslant n.\)
Proof
The function \(z\mapsto \det (zM_{0}+M_{1})\) is a polynomial of order less than or equal to n. If it is constantly zero, then \(\sigma (M_{0},M_{1})=\mathbb {C}\) and otherwise \(\operatorname {card}(\sigma (M_{0},M_{1}))\leqslant n\). □
Definition
The matrix pair (M 0, M 1) is called regular if \(\sigma (M_{0},M_{1})\ne \mathbb {C}\).
The main problem in solving an initial value problem of the form (10.2) is that one cannot expect a solution for each initial value \(U_{0}\in \mathbb {C}^n\) as the following simple example shows.
Example 10.1.3
Let \(M_{0}=\begin {pmatrix} 1 & 1\\ 0 & 0 \end {pmatrix}, \,M_{1}=\begin {pmatrix} 1 & 0\\ 0 & 1 \end {pmatrix}\) and let \(U_{0}\in \mathbb {C}^{2}\). We assume that there exists a solution \(U\colon \mathbb {R}_{\geqslant 0}\to \mathbb {C}^{2}\) satisfying (10.2); that is,
The second and third equation yield that the second coordinate of U 0 has to be zero. Then, for \(U_{0}=(x,0)\in \mathbb {C}^{2}\) the unique solution of the above problem is given by
Definition
We call an initial value \(U_{0}\in \mathbb {C}^{n}\) consistent for (10.2) if there exists ν > 0 and \(U\in C(\mathbb {R}_{\geqslant 0};\mathbb {C}^{n})\cap L_{2,\nu }(\mathbb {R}_{\geqslant 0};\mathbb {C}^{n})\) such that (10.2) holds. We denote the set of all consistent initial values for (10.2) by
Remark 10.1.4
It is obvious that \(\operatorname {IV}(M_{0},M_{1})\) is a subspace of \(\mathbb {C}^{n}\). In particular, \(0\in \operatorname {IV}(M_{0},M_{1})\).
It is now our goal to determine the space \(\operatorname {IV}(M_{0},M_{1})\). One possibility for doing so uses the so-called quasi-Weierstraß normal form.
Proposition 10.1.5 (Quasi-Weierstraß Normal Form )
Assume that (M 0, M 1) is regular. Then there exist invertible matrices \(P,Q\in \mathbb {C}^{n\times n}\) such that
where \(C\in \mathbb {C}^{k\times k}\) and \(N\in \mathbb {C}^{(n-k)\times (n-k)}\) for some k ∈{0, …, n}. Moreover, the matrix N is nilpotent; that is, there exists \(\ell \in \mathbb {N}\) such that N ℓ = 0.
Proof
Since (M 0, M 1) is regular we find \(\lambda \in \mathbb {C}\) such that λM 0 + M 1 is invertible. We set and obtain
Let now \(P_{2}\in \mathbb {C}^{n\times n}\) such that
for some invertible matrix \(J\in \mathbb {C}^{k\times k}\) and a nilpotent matrix \(\widetilde {N}\in \mathbb {C}^{(n-k)\times (n-k)}\) (use the Jordan normal form of M 0,1 here). Then
Now, by the nilpotency of \(\widetilde {N}\), the matrix \((1-\lambda \widetilde {N})\) is invertible by the Neumann series. We set
and obtain
Note that \((1-\lambda \widetilde {N})^{-1}\widetilde {N}\) is nilpotent, since the matrices commute and \(\widetilde {N}\) is nilpotent. Thus, the assertion follows with , , P = P 3 P 2 P 1, and \(Q=P_{2}^{-1}\). □
It is clear that the matrices P, Q, C and N in the previous proposition are not uniquely determined by M 0 and M 1. However, the size of N and C as well as the degree of nilpotency of N are determined by M 0 and M 1 as the following proposition shows.
Proposition 10.1.6
Let \(P,Q\in \mathbb {C}^{n\times n}\) be invertible such that
where \(C\in \mathbb {C}^{k\times k}\), \(N\in \mathbb {C}^{(n-k)\times (n-k)}\) for some k ∈{0, …, n}, and N is nilpotent. Then (M 0, M 1) is regular and
-
(a)
k is the degree of the polynomial \(z\mapsto \det (zM_{0}+M_{1})\).
-
(b)
N ℓ = 0 if and only if
$$\displaystyle \begin{aligned} \sup_{|z|\geqslant r}\left\Vert z^{-\ell+1}(zM_{0}+M_{1})^{-1} \right\Vert <\infty \end{aligned}$$for one (or equivalently all) r > 0 such that \(B\left (0,r\right )\supseteq \sigma (M_{0},M_{1})\).
Proof
First, note that
for all \((z\in \mathbb {C})\). Hence, (M 0, M 1) is regular and
which shows (a). Moreover, we have ρ(M 0, M 1) = ρ(−C) and
and hence, for r > 0 with \(B\left (0,r\right )\supseteq \sigma (M_{0},M_{1})\) we have
for some K 1⩾0, since \(\sup _{|z|\geqslant r}\left \Vert (z+C)^{-1} \right \Vert <\infty \). Now let \(\ell \in \mathbb {N}\) such that N ℓ = 0. Then
for some constant K 2⩾0 and thus,
Assume on the other hand that
for some \(\ell \in \mathbb {N}\) and r > 0 with \(\sigma (M_{0},M_{1})\subseteq B\left (0,r\right )\). Then there exist \(\widetilde {K}_{1},\widetilde {K}_{2}\geqslant 0\) such that
for all \(z\in \mathbb {C}\) with \(\left \vert z \right \vert \geqslant r\). Now, let \(p\in \mathbb {N}\) be minimal such that N p = 0. We show that \(p\leqslant \ell \) by contradiction. Assume p > ℓ. Then we compute
which contradicts the minimality of p. □
Theorem 10.1.7
Let (M 0, M 1) be regular and \(P,Q\in \mathbb {C}^{n\times n}\) be chosen according to Proposition 10.1.5 . Let \(k=\deg \det ((\cdot )M_{0}+M_{1})\) . Then
Moreover, for each \(U_{0}\in \operatorname {IV}(M_{0},M_{1})\) the solution U of (10.2) is unique and satisfies \(U\in C(\mathbb {R}_{\geqslant 0};\mathbb {C}^{n})\cap C^{1}(\mathbb {R}_{>0};\mathbb {C}^{n})\) as well as
Proof
Let \(C\in \mathbb {C}^{k\times k}\) and \(N\in \mathbb {C}^{(n-k)\times (n-k)}\) be nilpotent as in Proposition 10.1.5. Obviously U is a solution of (10.2) if and only if both is continuous on \(\mathbb {R}_{\geqslant 0}\) and solves
Clearly, if \(Q^{-1}U_{0}=(x,0)\in \mathbb {C}^{k}\times \{0\}\) then V given by for t⩾0 is a solution of (10.3) for ν > 0 large enough. On the other hand, if V given by \(V(t)=(V_{1}(t),V_{2}(t))\in \mathbb {C}^{k}\times \mathbb {C}^{n-k}\) (\(t\geqslant 0\)) is a solution of (10.3) then we have
Since N is nilpotent, there exists \(\ell \in \mathbb {N}\) with N ℓ = 0. Hence,
which in turn implies ∂ t,ν N ℓ−1 V 2 = 0 on \(\left (0,\infty \right )\). Using again the differential equation, we infer N ℓ−2 V 2(t) = 0 for t > 0. Inductively, we deduce V 2(t) = 0 for t > 0 and by continuity , which yields \(V_{0}=Q^{-1}U_{0}\in \mathbb {C}^{k}\times \{0\}\). The uniqueness follows from Proposition 10.2.7 below. □
10.2 The Infinite-Dimensional Case
Let now M 0, M 1 ∈ L(H). Again, it is our aim to determine the space of consistent initial values for the problem
Here, consistent initial values are defined as in the finite-dimensional setting:
Definition
We call an initial value U 0 ∈ H consistent for (10.4) if there exist ν > 0 and \(U\in C(\mathbb {R}_{\geqslant 0};H)\cap L_{2,\nu }(\mathbb {R}_{\geqslant 0};H)\) such that (10.4) holds. We denote the set of all consistent initial values for (10.4) by
Before we try to determine \(\operatorname {IV}(M_{0},M_{1})\) we prove a regularity result for solutions of (10.4).
Proposition 10.2.1
Let ν > 0, U 0 ∈ H and \(U\in C(\mathbb {R}_{\geqslant 0};H)\cap L_{2,\nu }(\mathbb {R}_{\geqslant 0};H)\) be a solution of (10.4). Then and
Proof
We extend U to \(\mathbb {R}\) by 0. First, observe that is continuous, since U is continuous and . By Lemma 9.4.2 (with A = 0), we obtain
Since ∂ t,ν is closed and M 0 is bounded, ∂ t,ν M 0 is closed as well. Since M 1 is bounded, therefore also ∂ t,ν M 0 + M 1 is closed. Thus, and therefore , and
□
We now come back to the space \(\operatorname {IV}(M_{0},M_{1})\). Since we are now dealing with an infinite-dimensional setting, we cannot use normal forms to determine \(\operatorname {IV}(M_{0},M_{1})\) without dramatically restricting the class of operators. Thus, we follow a different approach using so-called Wong sequences.
Definition
We set
and for \(k\in \mathbb {N}_0\) we set
The sequence \((\operatorname {IV}_{k})_{k\in \mathbb {N}_0}\) is called the Wong sequence associated with (M 0, M 1).
Remark 10.2.2
By induction, we infer \(\operatorname {IV}_{k+1}\subseteq \operatorname {IV}_{k}\) for each \(k\in \mathbb {N}_0\).
As in the matrix case, we denote by
the resolvent set of (M 0, M 1) .
Lemma 10.2.3
Let \(k\in \mathbb {N}_0\) . Then:
-
(a)
M 1(zM 0 + M 1)−1 M 0 = M 0(zM 0 + M 1)−1 M 1 for each z ∈ ρ(M 0, M 1).
-
(b)
\((zM_{0}+M_{1})^{-1}M_{0}[\operatorname {IV}_{k}]\subseteq \operatorname {IV}_{k+1}\) for each z ∈ ρ(M 0, M 1).
-
(c)
If \(x\in \operatorname {IV}_{k}\) we find x 1, …, x k+1 ∈ H such that for each z ∈ ρ(M 0, M 1) ∖{0}
$$\displaystyle \begin{aligned} (zM_{0}+M_{1})^{-1}M_{0}x=\frac{1}{z}x+\sum_{\ell=1}^{k}\frac{1}{z^{\ell+1}}x_{\ell}+\frac{1}{z^{k+1}}(zM_{0}+M_{1})^{-1}x_{k+1}. \end{aligned}$$ -
(d)
If \(\rho (M_{0},M_{1})\ne \varnothing \) then \(M_{1}^{-1}[M_{0}[\overline {\operatorname {IV}_{k}}]]\in \overline {\operatorname {IV}_{k+1}}\).
Proof
The proofs of the statements (a) to (c) are left as Exercise 10.6. We now prove (d). If k = 0 there is nothing to show. So assume that the statement holds for some \(k\in \mathbb {N}_0\) and let \(x\in M_{1}^{-1}\left [M_{0}\left [\overline {\operatorname {IV}_{k+1}}\right ]\right ]\). Since \(\overline {\operatorname {IV}_{k+1}}\subseteq \overline {\operatorname {IV}_{k}}\), we infer \(x\in M_{1}^{-1}\left [M_{0}\left [\overline {\operatorname {IV}_{k}}\right ]\right ]\subseteq \overline {\operatorname {IV}_{k+1}}\) by induction hypothesis. Hence, we find a sequence \((w_{n})_{n\in \mathbb {N}}\) in \(\operatorname {IV}_{k+1}\) with w n → x. Let now z ∈ ρ(M 0, M 1). Then, by (b), we have \((zM_{0}+M_{1})^{-1}M_{0}w_{n}\in \operatorname {IV}_{k+2}\) for each \(n\in \mathbb {N}\) and hence, \((zM_{0}+M_{1})^{-1}M_{0}x\in \overline {\operatorname {IV}_{k+2}}\). Moreover, since \(M_{1}x\in M_{0}\left [\overline {\operatorname {IV}_{k+1}}\right ]\), we find a sequence \((y_{n})_{n\in \mathbb {N}}\) in \(\operatorname {IV}_{k+1}\) with M 0 y n → M 1 x. Setting now
(where, again, we have used (b)) for \(n\in \mathbb {N}\), we derive
as n →∞ and thus, \(x\in \overline {\operatorname {IV}_{k+2}}\). □
The importance of the Wong sequence becomes apparent if we consider solutions of (10.4).
Lemma 10.2.4
Assume that \(\rho (M_{0},M_{1})\ne \varnothing \) . Let ν > 0 and \(U\in L_{2,\nu }(\mathbb {R}_{\geqslant 0};H)\cap C(\mathbb {R}_{\geqslant 0};H)\) be a solution of (10.4). Then \(U(t)\in \bigcap _{k\in \mathbb {N}_0}\overline {\operatorname {IV}_{k}}\) for each t⩾0.
Proof
We prove the claim, \(U(t)\in \overline {\operatorname {IV}_k}\) for all \(t\geqslant 0\) and \(k\in \mathbb {N}_0\), by induction. For k = 0 there is nothing to show. Assume now that \(U(t)\in \overline {\operatorname {IV}_{k}}\) for each t⩾0 and some \(k\in \mathbb {N}_0\). By Proposition 10.2.1 we know that
and thus, in particular,
Let now t⩾0 and h > 0. Then we infer
and hence,
by Lemma 10.2.3 (d). Since U is continuous, the fundamental theorem of calculus implies \(U(t)\in \overline {\operatorname {IV}_{k+1}}\), which yields the assertion. □
In particular, the space of consistent initial values has to be a subspace of \(\bigcap _{k\in \mathbb {N}_0}\overline {\operatorname {IV}_{k}}\). We now impose an additional constraint on the operator pair (M 0, M 1), which is equivalent to being regular in the finite-dimensional setting (cf. Proposition 10.1.6).
Definition
We call the operator pair (M 0, M 1) regular if there exists ν 0⩾0 such that
-
(a)
\(\mathbb {C}_{\operatorname {Re}>\nu _{0}}\subseteq \rho (M_{0},M_{1})\), and
-
(b)
there exist C⩾0 and \(\ell \in \mathbb {N}\) such that for all \(z\in \mathbb {C}_{\operatorname {Re}>\nu _{0}}\) we have \(\left \Vert (zM_{0}+M_{1})^{-1} \right \Vert \leqslant C\left \vert z \right \vert ^{\ell -1}\).
Moreover, we call the smallest \(\ell \in \mathbb {N}\) satisfying (b) the index of (M 0, M 1) , which is denoted by \(\operatorname {ind}(M_{0},M_{1})\).
Remark 10.2.5
Note that for matrices M 0 and M 1 the index equals the degree of nilpotency of N in the quasi-Weierstraß normal form by Proposition 10.1.6.
From now on, we will require that (M 0, M 1) is regular. First, we prove an important result on the Wong sequence in this case.
Proposition 10.2.6
Let (M 0, M 1) be regular, \(k\in \mathbb {N}_0\) , and \(k\geqslant \operatorname {ind}(M_{0},M_{1})\) . Then
Proof
We show that \(\overline {\operatorname {IV}_{k}}=\overline {\operatorname {IV}_{k+1}}\) for each \(k\geqslant \operatorname {ind}(M_{0},M_{1}).\) Since the inclusion “⊇” holds trivially, it suffices to show \(\operatorname {IV}_{k}\subseteq \overline {\operatorname {IV}_{k+1}}\). For doing so, let \(k\geqslant \operatorname {ind}(M_{0},M_{1})\) and \(x\in \operatorname {IV}_{k}\). By Lemma 10.2.3 (c) we find x 1, …, x k+1 ∈ H such that
for each \(z\in \mathbb {C}_{\operatorname {Re}>\nu _{0}}\). Since \(k\geqslant \operatorname {ind}(M_{0},M_{1}),\) we derive
and since the elements on the left-hand side belong to \(\operatorname {IV}_{k+1}\), by Lemma 10.2.3 (b), the assertion immediately follows. □
We now prove that in case of a regular operator pair (M 0, M 1) the solution of (10.4) for a consistent initial value U 0 is uniquely determined.
Proposition 10.2.7
Let (M 0, M 1) be regular, \(U_{0}\in \operatorname {IV}(M_{0},M_{1})\) , and ν > 0 such that a solution \(U\in C(\mathbb {R}_{\geqslant 0};H)\cap L_{2,\nu }(\mathbb {R}_{\geqslant 0};H)\) of (10.4) exists. Then this solution is unique. In particular
for each \(\rho >\max \{\nu ,\nu _{0}\}\).
Proof
By Proposition 10.2.1 we have and
Applying the Fourier–Laplace transformation, \(\mathcal {L}_{\rho }\), for \(\rho >\max \{\nu ,\nu _{0}\}\) we deduce
which in turn yields
and, in particular, proves the uniqueness of the solution. □
Remark 10.2.8
Let U be a solution of (10.4) for a consistent initial value U 0. Then the formula in Proposition 10.2.7 shows that \(U\in \bigcap _{\rho >\nu _0}L_{2,\rho }(\mathbb {R};H)\) and hence, we also have . If ν 0 > 0 then we even obtain \(U\in L_{2,\nu _0}(\mathbb {R};H)\) since \(\sup _{\rho >\nu _0}\left \Vert U \right \Vert { }_{L_{2,\rho }(\mathbb {R};H)}=\sup _{\rho >\nu _0} \left \Vert \mathcal {L}_{\rho }U \right \Vert { }_{L_2(\mathbb {R};H)} < \infty \) (cp. Lemma 8.1.1), and therefore also .
One interesting consequence of the latter proposition is the following.
Corollary 10.2.9
Let (M 0, M 1) be regular. Then the operator \(M_{0}\colon \operatorname {IV}(M_{0},M_{1})\to H\) is injective.
Proof
Let \(U_{0}\in \operatorname {IV}(M_{0},M_{1})\) with M 0 U 0 = 0. By Proposition 10.2.7, the solution U of (10.4) with satisfies
and hence, U = 0, which in turn implies . □
We now want to determine the space \(\operatorname {IV}(M_{0},M_{1})\) in terms of the Wong sequence.
Proposition 10.2.10
Let (M 0, M 1) be regular. Then
Proof
The second inclusion follows from Lemma 10.2.4 and Proposition 10.2.6. Let now \(U_{0}\in \operatorname {IV}_{\operatorname {ind}(M_{0},M_{1})}\) and set
Let . By Lemma 10.2.3 (c) we find x 1, …, x k+1 ∈ H such that
In particular, we read off that \(V\in \mathcal {H}_2(\mathbb {C}_{\operatorname {Re}>\nu };H)\) for all ν > ν 0. Now, let ν > ν 0. By the Theorem of Paley–Wiener (more precisely by Corollary 8.1.3) there exists \(U\in L_{2,\nu }(\mathbb {R}_{\geqslant 0};H)\) such that
Moreover,
and hence \(\left (z\mapsto zV(z)-\frac {1}{\sqrt {2\pi }}U_{0}\right )\in \mathcal {H}_2(\mathbb {C}_{\operatorname {Re}>\nu };H)\) as well. Since
we infer and, thus, is continuous by Theorem 4.1.2. Hence, \(U\in C(\mathbb {R}_{\geqslant 0};H)\) and since \( \operatorname {\mathrm {spt}} U\subseteq \mathbb {R}_{\geqslant 0}\) we derive . Finally, by the definition of V ,
for all \(z\in \mathbb {C}_{\operatorname {Re}>\nu }.\) Hence,
from which we see that U solves (10.4). □
Finally, we treat the case when \(\operatorname {IV}(M_{0},M_{1})\) is closed.
Theorem 10.2.11
Let (M 0, M 1) be regular and \(\operatorname {IV}(M_{0},M_{1})\) closed. Then the operator \(S\colon \operatorname {IV}(M_{0},M_{1})\to C(\mathbb {R}_{\geqslant 0};H)\) , which assigns to each initial state, \(U_0\in \operatorname {IV}(M_{0},M_{1})\) , its corresponding solution, \(U\in C(\mathbb {R}_{\geqslant 0};H)\) , of (10.4) is bounded in the sense that
is bounded for each \(n\in \mathbb {N}\).
Proof
By Proposition 10.2.10 we infer that \(\operatorname {IV}(M_{0},M_{1})=\overline {\operatorname {IV}_{k}}\) with . Let ν > ν 0⩾0. By Proposition 10.2.7 and Corollary 8.1.3, there exists C⩾0 such that
for each \(U_{0}\in \operatorname {IV}(M_{0},M_{1})\), where we have used the regularity of (M 0, M 1) and
In particular, \(S\colon \operatorname {IV}(M_{0},M_{1})\to H^{-1}(\partial _{t,\nu }^k)\) is bounded. Since \(L_{2,\nu _{0}}(\mathbb {R}_{\geqslant 0};H)\hookrightarrow H^{-1}(\partial _{t,\nu }^k)\) continuously, we infer that \(S\colon \operatorname {IV}(M_{0},M_{1})\to L_{2,\nu _{0}}(\mathbb {R}_{\geqslant 0};H)\) is bounded by the closed graph theorem. Hence, also
is bounded for each \(n\in \mathbb {N}\) and since C([0, n];H)↪L 2([0, n];H) continuously, we infer that S n is bounded with values in C([0, n];H) again by the closed graph theorem. □
Remark 10.2.12
The variant of the closed graph theorem used in the proof above is the following: Let X, Y be Banach spaces and Z a Hausdorff topological vector space (e.g. a Banach space) such that Y ↪Z continuously. Let T : X → Z be linear and continuous with T[X] ⊆ Y . Then T ∈ L(X, Y ). Indeed, by the closed graph theorem it suffices to show that T : X → Y is closed. For doing so, let (x n)n be a sequence in X with x n → x and Tx n → y for some x ∈ X, y ∈ Y . Then Tx n → Tx in Z by the continuity of T and Tx n → y in Z by the continuous embedding. Hence, y = Tx and thus, T is closed.
10.3 Comments
The theory of differential algebraic equations in finite dimensions is a very active field. The main motivation for studying these equations comes from the modelling of electrical circuits and from control theory (see e.g. [28] and Exercise 10.5). The main reference for the statements presented in the first part of this chapter is the book by Kunkel and Mehrmann [57]. Of course, also in the finite-dimensional case Wong sequences can be used to determine the consistent initial values, see Exercise 10.1. For instance, in [13] the connection between Wong sequences and the quasi-Weierstraß normal form for matrix pairs is studied. Of course, the theory is not restricted to linear and homogeneous problems. Indeed, in the non-homogeneous case it turns out that the set of consistent initial values also depends on the given right-hand side.
The theory of differential algebraic equations in infinite dimensions is less well studied than the finite-dimensional case. We refer to [114], where the theory of C 0-semigroups is used to deal with such equations. Moreover, we refer to [97, 98], where sequences of projectors are used to decouple the system. Moreover, there exist several references in the Russian literature, where the equations are called Sobolev type equations (see e.g. [111]). The results on infinite-dimensional problems presented here are based on [121, 124, 125]. In [124] the focus was on systems with index 0 with an emphasis on exponential stability and dichotomy.
We also add the following remark concerning the result in Theorem 10.2.11. By Corollary 10.2.9 we know that \(M_{0}\colon \operatorname {IV}(M_{0},M_{1})\to H\) is injective. If \(\operatorname {IV}(M_{0},M_{1})\) is closed, it follows that the operator \(C\colon \operatorname {dom}(C)\subseteq \operatorname {IV}(M_{0},M_{1})\to \operatorname {IV}(M_{0},M_{1})\) given by
is well-defined and closed. Using this operator, C, Theorem 10.2.11 states that if \(\operatorname {IV}(M_{0},M_{1})\) is closed then − C generates a C 0-semigroup on \(\operatorname {IV}(M_{0},M_{1})\). The precise statement can be found in [121, Theorem 5.7]. Moreover, C is bounded if \(\operatorname {IV}_{\operatorname {ind}(M_{0},M_{1})}\) is closed (cf. Exercise 10.7).
Exercises
Exercise 10.1
Let \(M_{0},M_{1}\in \mathbb {C}^{n\times n}\) such that (M 0, M 1) is regular and define the Wong sequence \((\operatorname {IV}_{j})_{j\in \mathbb {N}_0}\) associated with (M 0, M 1). Moreover, let \(P,Q\in \mathbb {C}^{n\times n}\), \(C\in \mathbb {C}^{k\times k},\) and \(N\in \mathbb {C}^{(n-k)\times (n-k)}\) be as in the quasi-Weierstraß normal form for (M 0, M 1) with N nilpotent (cf. Proposition 10.1.5). We decompose a vector \(x\in \mathbb {C}^{n}\) into and \(\widehat {x}\in \mathbb {C}^{n-k}\) such that . Prove that
Moreover, show that for each z ∈ ρ(M 0, M 1) we have
Exercise 10.2
Let \(E\in \mathbb {C}^{n\times n}\). We set , where 1 denotes the identity matrix in \(\mathbb {C}^{n\times n}\). A matrix \(X\in \mathbb {C}^{n\times n}\) is called a Drazin inverse of E if the following properties hold:
-
EX = XE,
-
XEX = X,
-
XE k+1 = E k.
Prove that each matrix \(E\in \mathbb {C}^{n\times n}\) has a unique Drazin inverse.
Hint: For the existence consider the quasi-Weierstraß form for (E, 1).
Exercise 10.3
Let \(M_{0},M_{1}\in \mathbb {C}^{n\times n}\) with (M 0, M 1) regular and M 0 M 1 = M 1 M 0. Denote by \(M_{0}^{\mathrm {D}}\) the Drazin inverse of M 0 (see Exercise 10.2). Prove:
-
(a)
\(M_{0}^{\mathrm {D}}M_{1}=M_{1}M_{0}^{\mathrm {D}}\),
-
(b)
\(\operatorname {ran} M_{0}^{\mathrm {D}}M_{0}=\operatorname {IV}(M_{0},M_{1})\),
-
(c)
For all \(U_{0}\in \operatorname {IV}(M_{0},M_{1})\) the solution U of (10.2) is given by
$$\displaystyle \begin{aligned} U(t)=\mathrm{e}^{-tM_{0}^{\mathrm{D}}M_{1}}U_{0}\quad (t\geqslant0). \end{aligned}$$
Exercise 10.4
Let \(M_{0},M_{1}\in \mathbb {C}^{n\times n}\) with (M 0, M 1) regular. Prove that there exist two matrices \(E,A\in \mathbb {C}^{n\times n}\) with (E, A) regular and EA = AE such that
-
\(\operatorname {IV}(E,A)=\operatorname {IV}(M_{0},M_{1})\),
-
U solves the initial value problem (10.2) for the matrices M 0, M 1 if and only if U solves the initial value problem (10.2) for the matrices E, A with the same initial value \(U_{0}\in \operatorname {IV}(M_{0},M_{1})\).
Exercise 10.5
We consider the following electrical circuit (see Fig. 10.1) with a resistor with resistance R > 0, an inductor with inductance L > 0 and a capacitor with capacitance C > 0. We denote the respective voltage drops by v R, v L and v C. Moreover, the current is denoted by i. The constitutive relations for resistor, inductor and capacitor are given by
respectively. Moreover, by Kirchhoff’s second law we have
Write these equations as a differential algebraic equation and compute the index and the space of consistent initial values. Moreover, compute the solution for each consistent initial value for R = 2 and C = L = 1.
Exercise 10.6
Prove the assertions (a) to (c) in Lemma 10.2.3.
Exercise 10.7
Let M 0, M 1 ∈ L(H).
-
(a)
Assume that \(\rho (M_{0},M_{1})\ne \varnothing \). Prove that for each \(k\in \mathbb {N}\) the space \(\operatorname {IV}_{k}\) is closed if and only if \(M_{0}\left [\operatorname {IV}_{k-1}\right ]\) is closed.
-
(b)
Assume that (M 0, M 1) is regular with \(\operatorname {ind}(M_{0},M_{1})\geqslant 1\). Prove that if \(\operatorname {IV}_{\operatorname {ind}(M_{0},M_{1})}\) is closed then the operator
$$\displaystyle \begin{aligned} M_{0}|{}_{\operatorname{IV}_{\operatorname{ind}(M_{0},M_{1})}} \colon \operatorname{IV}_{\operatorname{ind}(M_{0},M_{1})}\to M_{0}\left[\operatorname{IV}_{\operatorname{ind}(M_{0},M_{1})-1}\right] \end{aligned}$$is an isomorphism.
References
T. Berger, A. Ilchmann, S. Trenn, The quasi-Weierstrass form for regular matrix pencils. Linear Algebra Appl. 436(10), 4052–4069 (2012)
L. Dai, Singular Control Systems, vol. 118 (Springer, Berlin, 1989)
P. Kunkel, V. Mehrmann, Differential-Algebraic Equations. EMS Textbooks in Mathematics. Analysis and Numerical Solution (European Mathematical Society (EMS), Zürich, 2006)
T. Reis, Consistent initialization and perturbation analysis for abstract differential-algebraic equations. Math. Control Signals Syst. 19(3), 255–281 (2007)
T. Reis, C. Tischendorf, Frequency domain methods and decoupling of linear infinite dimensional differential algebraic systems. J. Evol. Equ. 5(3), 357–385 (2005)
G.A. Sviridyuk, V.E. Fedorov, Linear Sobolev Type Equations and Degenerate Semigroups of Operators. Inverse and Ill-posed Problems Series (VSP, Utrecht, 2003)
B. Thaller, S. Thaller, Factorization of degenerate Cauchy problems: the linear case. J. Oper. Theory 36(1), 121–146 (1996)
S. Trostorff, Semigroups associated with differential-algebraic equations. In: Semi-groups of Operators – Theory and Applications. Selected papers based on the presentations at the conference, SOTA 2018, Kazimierz Dolny, Poland, September 30–October 5, 2018. In honour of Jan Kisyński’s 85th birthday (Springer, Cham, 2020), pp. 79–94
S. Trostorff, M. Waurick, On differential-algebraic equations in infinite dimensions. J. Differ. Equ. 266(1), 526–561 (2019)
S. Trostorff, M. Waurick, On higher index differential-algebraic-equations in infinite dimensions, in The Diversity and Beauty of Applied Operator Theory, vol. 268, ed. by P.S. Albrecht Böttcher, D. Potts, D. Wenzel. Operator Theory: Advances and Applications (Birkhäuser, Basel, 2018), pp. 477–486
Author information
Authors and Affiliations
Rights and permissions
Open Access This chapter is licensed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license and indicate if changes were made.
The images or other third party material in this chapter are included in the chapter's Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the chapter's Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder.
Copyright information
© 2022 The Author(s)
About this chapter
Cite this chapter
Seifert, C., Trostorff, S., Waurick, M. (2022). Differential Algebraic Equations. In: Evolutionary Equations. Operator Theory: Advances and Applications, vol 287. Birkhäuser, Cham. https://doi.org/10.1007/978-3-030-89397-2_10
Download citation
DOI: https://doi.org/10.1007/978-3-030-89397-2_10
Published:
Publisher Name: Birkhäuser, Cham
Print ISBN: 978-3-030-89396-5
Online ISBN: 978-3-030-89397-2
eBook Packages: Mathematics and StatisticsMathematics and Statistics (R0)