1.5 Ordinary differential equations
1.5.1 Existence and uniqueness theorems
(I) Notion of the solution of a differential equation
Let I be an interval of
ℝ
with non-empty interior
I
∘
, Ω a non-empty open subset of
E
=
ℝ
n
and f a mapping from I × Ω into E. We say that a mapping φ : I → E is a solution (or integral) of the differential equation
x . = f t x
[1.22]
if the conditions (ODE
1,2,3) below are satisfied:
-
(ODE
1) φ (t) ∈ Ω for all t ∈ I;
-
(ODE
2) φ is locally absolutely continuous in I (i.e. each of its components with respect to the canonical basis of
ℝ
n
is locally absolutely continuous: see [P2], section 4.1.7(III));
-
(ODE
3)
φ
.
t
=
f
t
φ
t
λ-almost everywhere in I, where λ is the Lebesgue measure on
ℝ
([P2], section 4.1.1(II)).
A Cauchy problem involves determining a function φ that is a solution of [1.22] and that satisfies the Cauchy condition:
φ t 0 = x 0 t 0 ∈ I ∘ x 0 ∈ Ω .
[1.23]
If φ satisfies the conditions (ODE
1,2,3) and [1.23], then, for all t ∈ I,
φ t = x 0 + ∫ t 0 t f τ φ τ dτ .
[1.24]
Conversely, suppose that [1.24] holds, (ODE
1) is satisfied and t ↦ f (t, φ (t)) is locally λ-integrable. Then, [1.23] holds; furthermore, Lusin’s measurability criterion ([P2], section 4.1.6(II)) implies that the function t ↦ f (t, φ (t)) is λ-measurable for every locally absolutely continuous function φ : I → E if the conditions (Cat
1,2) below are satisfied:
-
(Cat
1) the function x ↦ f (t, x) from Ω into E is continuous for every t ∈ I;
-
(Cat
2) the function t ↦ f (t, x) from I into E is λ-measurable for every x ∈ Ω.
Suppose further that:
(Cat
3) For all x
0 ∈ Ω and every r > 0 such that B
r
(x
0) ⊂ Ω, where B
r
(x
0) is the open ball of center x
0 and radius r in E, there exists a locally λ-integrable function m from I into
ℝ
+
such that | f (t, x)| ≤ m (t) for all (t, x) ∈ I × B
r
(x
0).
Then, for every locally absolutely continuous function φ : I → E satisfying φ (I) ⊂ B
r
(x
0), the mapping t ↦ | f (t, φ (t))| is locally λ-integrable in I, so t ↦ f (t, φ (t)) is locally λ-integrable in I ([P2], section 4.1.2(I)).
Definition 1.66
The conditions (Cat
1,2,3
) are known as the Carathéodory conditions.
(II) Existence theorem
Theorem 1.67
(Carathéodory) Suppose that the Carathéodory conditions (Cat
1,2,3
) are satisfied. Then, for all (t
0, x
0) ∈ I × Ω, there exists an interval J ⊂ I with some point t
0 in its interior and a mapping φ : J → E such that φ (J) ⊂ B
r
(x
o
), φ is a solution of
[1.22]
and this solution satisfies the Cauchy condition
[1.23]
.
Proof
We will show that there exist an interval J
β
= [t
0, t
0 + β] ⊂ I (β > 0) and an absolutely continuous mapping φ : J
β
→ E such that φ (J
β
) ⊂ B
r
(x
0) and φ satisfies [1.24]. The same argument works on an interval J′α = [t
0 − α, t
0] (α > 0). Let
M
:
[
t
0
,
+
∞
[
∩
I
→
ℝ
+
be the mapping:
M t = 0 t < t 0 , M t = ∫ t 0 t m τ dτ t ∈ t 0 , + ∞ ∩ I .
Since M is continuous and non-decreasing, there exists an interval J
β
as specified above satisfying the property that, for all t ∈ J
β
,
0 ≤ M t < r .
[1.25]
We can now inductively define a sequence of absolutely continuous mappings φ
i
: J
β
→ E using the conditions:
φ i t = x 0 t 0 ≤ t ≤ β / i , φ i t = x 0 + ∫ t 0 t − β / i f τ φ i τ dτ t 0 + β / i < t ≤ t 0 + β .
By (Cat
3), the second equation implies that, for all t ∈ J
β
,
φ i t − x 0 ≤ ∫ t 0 t − β / i f ( τ φ i τ ) dτ ≤ ∫ t 0 t 0 + β m τ dτ < r ,
so φ
i
(t) ∈ B
r
(x
0) for all t ∈ J
β
. If t
1, t
2 ∈ J
β
, then
φ i t 2 − φ i t 1 ≤ M t 2 − β / i − M t 1 − β / i ,
and M is uniformly continuous in the compact set J
β
by Heine’s theorem ([P2], section 2.4.5, Theorem 2.86), so | M (t
2 − β/i) − M (t
1 − β/i)| → 0 uniformly in i if t
2 − t
1 → 0, and the set
H
≔
φ
i
:
i
∈
ℕ
×
is equicontinuous ([P2], section 2.7.3). Since
H
t
≔
φ
i
t
:
i
∈
ℕ
×
is contained in B
r
(x
0) for all t ∈ J
β
, the third Ascoli–Arzelà theorem (ibid.) implies that H is relatively compact in
φ
∈
C
J
β
E
equipped with the uniform structure of uniform convergence. Hence, there exists a subsequence (φ
i
k
) that converges uniformly to some mapping
φ
∈
C
J
β
E
. Moreover, | f(t, φ
i
k
(t))| ≤ m(t)(t
0 ≤ t ≤ t
0 + β) and f(t, φ
i
k
(t)) → f(t, φ(t)) for i
k
→ ∞ by (Cat
1); furthermore, as we saw earlier, (Cat
2) implies that t ↦ f (t, φ (t)) is measurable. The Lebesgue dominated convergence theorem ([P2], section 4.1.2(II), Theorem 4.9) therefore implies that, for all t ∈ J
β
,
∫ t 0 t f τ φ i k τ dτ → ∫ t 0 t f τ φ τ dτ i k → ∞ .
But, for all t ∈ J
β
,
φ i k t = x 0 + ∫ t 0 t f τ φ i k τ dτ − ∫ t − β / i t f τ φ i k τ dτ ,
and the second integral tends to 0 as i
k
→ ∞, so the equality [1.24] is satisfied for all t ∈ J
β
. Finally, φ
i
k
→ φ in the Banach space AC (J
β
; E) of absolutely continuous mappings from J
β
into E ([P2], section 4.1.7(III)), so φ is absolutely continuous.
Corollary 1.68
(Peano’s theorem) Suppose that f is continuous in I × Ω. Let J be a compact interval that is a neighborhood of t
0 in I and let
m
=
sup
t
∈
J
,
x
∈
B
r
x
0
f
t
x
. For every compact interval [t
0, t
0 + β] contained in J satisfying β < r/m, there exists a solution of
[1.24]
that takes values in B
r
(x
0).
Proof
We have M = mβ, so the inequality [1.25] is satisfied if and only if β < r/m.
Remark 1.69
Corollary 1.68 (and hence
Theorem 1.67
) fails if E is replaced by an arbitrary Banach space ([BOU 76],
Chapter 4
, section 1, Exercise 18). We can define an absolutely continuous mapping φ : J
β
→ E as we did in ([P2], section 4.1.7(I)), but it is not true in general that
φ
t
−
φ
t
0
=
∫
t
0
t
φ
.
τ
dτ
for all t ∈ J
β
(however, this property does hold if E is assumed to be reflexive). Furthermore, since the ball B
r
(x
0) is not relatively compact when E is infinite-dimensional, the proof of
Theorem 1.67
no longer works.
(III) Uniqueness theorem
The fourth Carathéodory condition can be stated as follows (reusing some of the notation of Cat
3):
(Cat
4) For all x
0 ∈ E and every real number r > 0 such that B
r
(x
0) ⊂ Ω, there exists a locally λ-integrable function k from I into
ℝ
+
such that
f t x ′ − f ( t x ″ ) ≤ k t . x ′ − x ″ , ∀ t x ′ , t x ″ ∈ I × B r x 0 .
Theorem 1.70
(Carathéodory) Suppose that the Carathéodory conditions
Cat
1,2,3,4 are satisfied. Then, for all
t
0
x
0
∈
I
∘
×
Ω
, there exists an interval J ⊂ I with interior point t
0 and a unique mapping φ : J → Ω that is a solution of
[1.22]
and which satisfies the Cauchy condition
[1.23]
.
Proof
Let
K t = ∫ t 0 t 0 + t k τ dτ 0 ≤ t ≤ b
and choose the real number β > 0 in the proof of Theorem 1.67 to satisfy the additional condition K (β) < 1. Furthermore, let
X = ψ ∈ C 0 β E : ψ 0 = 0 & ψ t ∈ B r c 0 ∀ t ∈ 0 β
and, for every function
ψ
∈
X
, set
T . ψ t ≔ ∫ t 0 t 0 + t f τ ψ τ − t 0 + x 0 dτ 0 ≤ t ≤ β .
Clearly,
T
X
⊂
X
. The set
X
is a closed subset of the space
C
0
β
E
equipped with the uniform structure of uniform convergence; the norm of
C
0
β
E
is ‖ψ‖∞ ≔ sup
t ∈ [0, β]| ψ(t)|. The space
C
0
β
E
is complete ([P2], section 2.7.2, Corollary 2.115), so
X
is complete ([P2], section 2.4.4(II), Lemma 2.77). Furthermore,
ψ
∈
C
0
β
E
is a fixed point of T if and only if the function
φ
∈
C
t
0
t
0
+
β
E
defined by
φ t ≔ ψ t − t 0 + x 0 0 ≤ t ≤ β
satisfies [1.24]; finally, ψ (t – t
0) ∈ B
r
(0) if and only if φ (t) ∈ B
r
(x
0). If
ψ
1
,
ψ
2
∈
X
for all t ∈ [0, β], then
T . ψ 1 t − T . ψ 2 t ≤ ∫ t 0 t 0 + t k τ . ψ 1 τ − t 0 − ψ 2 τ − t 0 dτ ≤ K b ψ 1 − ψ 2 ∞
and hence ‖T. ψ
1 − T. ψ
2‖∞ ≤ K(b)‖ψ
1 − ψ
2‖∞. Therefore, T has a unique fixed point by Theorem 1.27.
Definition 1.71
-
1)
We say that f : I × Ω → E is locally Lipschitz in the second variable in I × Ω if, for every (t, x) ∈ I × Ω, there exists a neighborhood V of t, a neighborhood S of x and a constant k
V,S
> 0 such that f (., x) is regulated on V (
[DIE 93]
, Volume 1, section 7.6) and f satisfies the Lipschitz condition:
f
t
x
′
−
f
(
t
x
″
)
≤
k
V
,
S
.
x
′
−
x
″
,
∀
t
∈
V
,
∀
x
′
,
x
″
∈
S
.
- 2)
We say that f is Lipschitz with constant k > 0 in the second variable if the above statement is satisfied when V = I, S = Ω and k
V,S
= k.
Any locally Lipschitz function in the second variable clearly satisfies the conditions Cat
1,2,3,4, and we may therefore apply Theorem 1.70 to this function. We also have the following result:
Corollary 1.72
(Cauchy–Lipschitz theorem) If f is Lipschitz with constant k in the second variable in I × Ω, let J be a compact interval contained in I with non-empty interior, t
0 a point of
I
∘
, x
0 a point of E, r > 0 a real number such that B
r
(x
0) ⊂ Ω,
m
=
sup
t
∈
J
,
x
∈
B
r
x
0
f
t
x
and ρ = min {r/m, 1/k}. For every compact interval K contained in J ∩ ]t
0 − ρ, t
0 + ρ[, there exists a unique mapping φ that is a solution of
[1.22]
and which satisfies the
Cauchy condition
[1.23]
.
Remark 1.73
-
i)
Theorem 1.70
fails if E is replaced by an arbitrary Banach space. However,
Corollary 1.72
remains valid, with an identical proof. Furthermore, ρ = r/m (
[BOU 76]
,
Chapter 4
,
section 1.5
, Theorem 1)
12
. Interested readers can find additional existence and uniqueness results for the solutions of
[1.22]
in infinite dimensions in
[DEI 77]
, section 8, and
[SCH 89]
. Note, however, that “infinite-dimensional systems” are not governed by a functional differential equation of the form [1.22], where E is a Banach space: see [HAL 77]
.
-
ii)
By the mean value theorem (
Theorem 1.13
), in order for f to be locally Lipschitz, it is sufficient for it to be of class C
1
.
Theorem 1.74
Let E be the space
ℝ
n
(respectively any Banach space),
I
⊂
ℝ
an interval with some interior point t
0, Ω a non-empty open subset of E and f : I × Ω → E a mapping satisfying the conditions
Cat
1,2,3,4 (respectively a locally Lipschitz function in the second variable). For all x
0 ∈ Ω, there exists a maximal interval J (t
0, x
0) ⊂ I with interior point t
0 in which
[1.22]
has a solution φ satisfying the Cauchy condition
[1.23]
and such that φ (J (t
0, x
0)) ⊂ Ω. This solution φ (.; t
0, x
0) is unique.
Definition 1.75
The solution φ (.; t
0, x
0) defined in J is called the maximal integral of
[1.22]
satisfying
[1.23]
.
Remark 1.76
Suppose that f is locally Lipschitz in the second variable.
-
1)
Let t
f
:= sup (J (t
0, x
0)) ≤ +∞ (the argument below also works when t
i
:= inf (J (t
0, x
0)) ≥ −∞, mutatis mutandis). If f (t, φ (.;t
0, x
0)) is bounded in J (t
0, x
0), then ψ (t; t
0, x
0) admits a limit c := φ (t
f
− 0; t
0, x
0); furthermore, c is a frontier point of Ω if J(t
0, x
0) ∩ [t
0, + ∞ [ ≠ I ∩ [t
0, + ∞ [. This inequality, together with the condition Ω = E, implies that lim
t → t
f
| φ(t; t
0, x
0)| = + ∞; by contrast, if t
f
∈ I and Ω = E, then J(t
0, x
0) ∩ [t
0, + ∞ [ = I ∩ [t
0, + ∞ [ (
[BOU 76]
,
Chapter 4
,
section 1.5
, Theorems 2 and Corollaries 1 and 2). In addition to this remark, see
Theorem 5.67
in
section 5.7.1
.
-
2)
Let (τ, ξ) be an arbitrary point of I × Ω. There exists an interval K ⊂ I, a neighborhood of τ in I and a neighborhood S of ξ in Ω, such that, for every point (t
0, x
0) ∈ K × S, there is a unique solution φ (., t
0, x
0) of
[1.22]
satisfying
[1.23]
, definedin K (i.e. J(t
0, x
0) ⊃ K). The mapping (t, t
0, x
0) ↦ φ(t; t
0, x
0) from K × K × S into Ω is uniformly continuous ([BOU 76]
,
Chapter 4
,section 1.7, Theorem 4).
(IV) Differential equations in implicit form
Let I be an open interval of
ℝ
, t
0 a point of I, F a Banach space and Ω a non-empty open subset of F
n + 1, where n is a natural integer. Let g : I × Ω → F be a mapping of class C
1 and consider the differential equation:
g t y y . … y n − 1 y n = 0 .
[1.26]
Let η
0 = (η
0
0, η
0
1,…, η
0
n − 1) ∈ F
n
and ξ
0 ∈ F such that (η
0, ξ
0) ∈ Ω, g (t
0, η
0, ξ
0) = 0, and suppose that the following condition (Inv) is satisfied:
(Inv)
∂
g
∂
ξ
t
0
η
0
ξ
0
is invertible in
ℒ
F
.
By the implicit function theorem (Theorem 1.30), there exists an open neighborhood J × U of (t
0, η
0) in I × F
n
, an open neighborhood V of ξ
0 in F, where U × V ⊂ Ω, and a mapping h : J × U → V of class C
1, such that, for all (t, η, ξ) ∈ J × U × V,
g t η ξ = 0 ⇔ ξ = h t η .
Therefore, any mapping ψ : J → F such that
ψ
t
ψ
.
t
…
ψ
n
−
1
t
∈
U
and ψ
(n) (t) ∈ V for all t ∈ J is a solution of [1.26] in J if and only if ψ is a solution of the following differential equation on J, said to be in explicit form:
y n = h t y y . … y n − 1 .
[1.27]
Let x
i
= y
(i − 1) (i = 1,…, n) and x =(x
0, …, x
n
). For (t, x) ∈ J × U × V, the differential equation [1.27] is equivalent to [1.22], where f = (f
1,…, f
n
) and
f 1 t x = x 2 , … , f n − 1 t x = x n , f n t x = h t x .
The mapping f : J × U → F
n
is of class C
1 and hence locally Lipschitz in x by the mean value theorem (Theorem 1.13(i)). We can therefore apply Theorem 1.72 according to Remark 1.73. Let x
0 = (η
0
1, …, η
0
n − 1); any solution φ = (φ
0, …, φ
n
) of [1.22] of class C
1 in J satisfies the Cauchy condition [1.23] if and only if φ = φ
1 is a solution of [1.26], of class C
n
in J and ψ (t
0) = η
0
1, …, ψ
(n − 1) (t
0) = η
0
n − 1.
Remark 1.77
If the condition (Inv) is not satisfied, the differential equation
[1.26]
is singular. We already encountered this situation in the linear case ([P2], section 5.4.6), where it was necessary to introduce solutions in the form of hyperfunctions. The nonlinear case does not have an equivalent general theory.
1.5.2 Linear differential equations
(I) Let I be an interval of
ℝ
with non-empty interior
I
∘
and let
E
=
ℝ
n
. Consider the linear differential equation
x . = A t . x + b t ,
[1.28]
where
A
:
I
→
ℒ
E
and b : I → E are locally λ-integrable. The Carathéodory conditions Cat
1,2,3,4 are all satisfied. (In particular, setting f (t, x) = A (t).x + b (t), we have
f t x ′ − f ( t x ″ ) ≤ A t . x ′ − x ″ ) ,
which shows that Cat
4 is satisfied.) Hence, for all
t
0
∈
I
∘
and every x
0 ∈ E, there exists a unique solution φ (.; t
0, x
0) of [1.28] in I satisfying [1.23].
The linear equation [1.28] is said to be homogeneous if b = 0, in which case
x . = A t . x .
[1.29]
(II) The set of solutions of [1.29] (where A is locally λ-integrable) is an
ℝ
-vector space. Let φ
0 (.; t
0, x
0) be a solution of [1.29] in I satisfying [1.23]. The mapping x
0 ↦ φ
0 (t; t
0, x
0) is a bijective linear mapping Φ (t, t
0) from E onto E, and Φ(., t
0) is identical to the solution of the differential equation
dU dt = A t U
[1.30]
for U (t
0) = 1
E
. For all t
1, t
2, t
3 ∈ I, we have Φ(t
3, t
1) = Φ (t
3, t
2) ∘ Φ(t
2, t
1) and Φ(t
1, t
2) = Φ(t
2, t
1)− 1.
Definition 1.78
The mapping Φ is called the resolvent of the equation
[1.29]
. The matrix representing this resolvent with respect to the canonical basis of E is called the transition matrix.
Theorem 1.79
We have
det
Φ
t
t
0
=
exp
∫
t
0
t
Tr
A
τ
.
dτ
.
Proof
Set Φ(t, t
0) = U (t), Δ(t) = det (U (t)) and write U (t + h) = U (t) + h.V + o (h), where
V
=
U
.
t
. Then, Δ(t + h) = Δ (t).det (I + h.V.U
− 1 (t) + o (h)). But
det
I
+
h
.
V
.
U
−
1
t
+
o
h
=
h
n
det
h
−
1
.
I
+
V
.
U
−
1
t
+
o
1
.
Furthermore, by [P1], section 2.3.11
(VII),
det
h
−
1
.
I
+
V
.
U
−
1
t
+
o
1
=
h
−
n
I
+
h
−
n
+
1
Tr
V
.
U
−
1
t
+
o
h
−
n
+
1
,
so det (I + h.V.U
− 1 (t) + o(h)) = 1 + h.Tr (V.U
− 1 (t)) + o (h). Hence, Δ(t + h) = Δ (t).(1 + h.Tr (V.U
− 1 (t
0)) + o (h)), so
Δ
.
t
=
Tr
U
.
t
.
U
−
1
t
.
Δ
t
.
We now simply apply the relation
U
.
t
U
−
1
t
=
A
t
, which follows from [1.30].
(III) The above shows that the general solution of [1.29] is of the form t ↦ Φ(t, t
0)ξ. The “variation of constants” method (exercise) allows us to obtain the following solution (defined in I) of [1.28] and the Cauchy condition [1.23]:
φ t t 0 x 0 = Φ t t 0 . x 0 + ∫ t 0 t Φ τ t 0 . b τ . dτ .
(IV) The integration of linear differential equations with constant coefficients is a classical problem and is performed using the Jordan normal form ([P1], section 3.4.3
(IV)): see, for example, [BOU 10], section 12.5.2.
1.5.3 Parameter dependence of solutions
Let I be an interval of
ℝ
with non-empty interior, E a Banach space (see Remark 1.73), Ω a non-empty open subset of E, Λ a topological space and f a mapping from I × Ω × Λ into E. Write f
λ
(t, x) for the value of f at the point (t, x, λ) ∈ I × Ω × Λ. It is possible to show the following result ([BOU 76], Chapter 4, section 1.6, Theorem 3):
Theorem 1.80
(parameter dependence of solutions) Suppose that, for all λ ∈ Λ, (t, x) ↦ f
λ (t, x) is Lipschitz in the second variable x in I × Ω and that f
λ
(t, x) → f
λ
0
(t, x) uniformly in I × Ω as λ → λ
0. Let φ
λ
0
be a solution of
x
.
=
f
λ
0
t
x
satisfying the Cauchy condition
φ
λ
0
t
0
=
x
0
t
0
∈
I
∘
x
0
∈
Ω
, defined on an interval J = [t
0, t
0 + β[ ⊂ I and taking values in Ω. For every compact interval [t
0, t
1] ⊂ J, there exists a neighborhood V of λ
0 in Λ such that, for all λ ∈ V, the differential equation
x
.
=
f
λ
t
x
[1.31]
admits a unique solution φ
λ
defined in [t
0, t
1] satisfying the Cauchy condition φ
λ
(t
0) = x
0 and taking values in Ω; furthermore, as λ → λ
0, φ
λ
→ φ
λ
0
uniformly in [t
0, t
1].
Suppose now that Λ is an open subset of a normed vector space F and that the mapping (t, x, λ) ↦ f
λ (t, x) is continuous with continuous partial differentials
13
t
x
λ
↦
∂
f
λ
∂
x
t
x
and
t
x
λ
↦
∂
f
λ
∂
λ
t
x
. Then, f
λ
is locally Lipschitz in the second variable x (see section 1.5.1
(V)). Suppose further that the mappings x
0 : Λ → Ω: λ → x
0 (λ) and t
0 : Λ → I : λ ↦ t
0 (λ) are of class C
1 in Λ. For all λ
ο ∈ Λ, Theorem 1.80 implies that there exist an open neighborhood V of λ
0 in Λ and an open interval J ⊂ I such that t
0 (λ
0) ∈ J, where the sets V and J satisfy the following condition: for all λ ∈ V, t
0 (λ) ∈ J and there exists a solution φ
λ
= φ (.,t
0 (λ), x
0 (λ)) of [1.31] in J taking the value x
0 (λ) ∈ Ω at the point t
0 (λ). Then, we have the following result:
Theorem 1.81
For every t ∈ J, the mapping λ ↦ φ
λ
(t) from V into Ω has a differential
h
t
∈
ℒ
F
E
at the point λ
0 of V ; h is of class C
1 in J and is the unique solution of the linear equation:
y
.
=
A
t
∘
y
+
b
t
[1.32]
where
A
t
≔
∂
f
λ
∂
x
(
t
φ
λ
t
)
λ
=
λ
0
,
b
t
≔
∂
f
λ
∂
λ
(
t
φ
λ
t
)
λ
=
λ
0
.
This differential h satisfies the Cauchy condition:
h
t
0
λ
0
=
Dx
0
λ
0
−
f
λ
(
t
0
λ
x
0
λ
)
λ
=
λ
0
∘
Dt
λ
0
.
Proof
For all t ∈ J,
φ
λ
t
=
x
0
λ
+
∫
t
0
λ
t
f
λ
τ
φ
λ
τ
dτ
.
Hence, by [DIE 93], Volume 1, section 8.11, (8.11.2) and Problem 1,
h
t
=
∫
t
0
λ
0
t
∂
f
λ
∂
x
(
τ
φ
λ
τ
)
h
τ
+
∂
f
λ
∂
λ
(
τ
φ
λ
τ
)
λ
=
λ
0
dτ
+
Dx
0
λ
0
−
f
λ
(
τ
φ
λ
τ
)
λ
=
λ
0
∘
Dt
λ
0
.
Therefore,
h
is of class C
1 in J and
h
.
t
=
∂
f
λ
∂
x
(
t
φ
λ
t
)
λ
=
λ
0
h
t
+
∂
f
λ
∂
λ
(
τ
φ
λ
τ
)
λ
=
λ
0
,
h
t
0
λ
0
=
Dx
0
λ
0
−
f
λ
(
τ
φ
λ
τ
)
λ
=
λ
0
∘
Dt
λ
0
Note that, in the linear equation [1.32],
A
t
∈
ℒ
F
E
; moreover,
y
, A(t) ∘
y
, and
b
(t) belong to
ℒ
F
E
. In the Cauchy condition, f
λ
(t
0
λ),
x
0
λ
)
λ
=
λ
0
∈
E
≅
ℒ
ℝ
E
,
Dx
0
λ
0
∈
ℒ
F
E
,
Dt
λ
0
∈
ℒ
F
ℝ
=
F
∨
, and f
λ (t
0 (λ),
x
0
λ
)
λ
=
λ
0
∘
Dt
λ
0
∈
ℒ
F
E
.
Corollary 1.82
(differentiability of the solution with respect to x
0) Suppose that F = E, Λ = Ω, and λ = x
0, and adopt the same hypotheses as
Theorem 1.81
(mutatis mutandis). Write f and φ for f
λ and φ
λ respectively. Then:
∂
φ
∂
x
0
t
t
0
x
0
=
Φ
t
t
0
where Φ is the resolvent (
Definition 1.78
) of the linear differential equation
y
.
=
A
t
∘
y
,
A
t
≔
∂
f
∂
x
t
φ
t
t
0
x
0
.
[1.33]
Corollary 1.83
(differentiability with respect to the initial time) Suppose that
F
=
ℝ
, Λ = I, and λ = t
0
. With the notation of
Corollary 1.82
and the same hypotheses (exercise):
∂
φ
∂
t
0
t
t
0
x
0
=
−
Φ
t
t
0
f
t
0
x
0
.
Remark 1.84
Let E be finite-dimensional. The statement of
Corollary 1.82
still holds under the weaker condition (
[ALE 87]
,
Chapter 2
,section 2.5.6) that f satisfies the Carathéodory conditions (
Cat
1,2,3
) and Lusin’s condition
(L) holds:
(L): For all t ∈ I, the mapping x ↦ f (t, x) is continuously differentiable on Ω and, for every compact set K ⊂ Ω, there exists a locally λ-integrable function
k
:
I
→
ℝ
+
such that
∂
f
∂
x
t
x
≤
k
t
,
∀
t
x
∈
I
×
K
.
It is clear that condition (L) implies (Cat
4
) by the mean value theorem. This condition does not require f to be continuous in t, which is very important in optimal control theory (Pontryagin maximum principle): see op. cit. and
[PON 62]
. We can further weaken (L) by considering generalized gradients and differential inclusions (
[CLA 90]
,Theorem 7.4.1), but this exceeds the scope of the present book.