Bourbaki

§ 1. Existence theorems

1. The concept of a differential equation

Let I be an interval contained in R\mathbf{R}, not reducing to a single point, E a topological vector space over R\mathbf{R}, and A and B two open subsets of E. Let (x,y,t)↦g(x,y,t)(x, y, t) \mapsto g(x, y, t) be a continuous map of A×B×IA \times B \times I into E; to every differentiable map u of I into A whose derivative takes its values in B we associate the map t↦g(u(t),u′(t),t)t \mapsto g(u(t), u'(t), t) of I into E, and denote it by g~(u)\tilde{g}(u); so g~\tilde{g} is defined on the set D(A,B)\mathscr{D}(A, B) of differentiable functions of I into B whose derivatives have their values in B. We shall say that the equation g~(u)=0\tilde{g}(u) = 0 is a differential equation in u (relative to the real variable t); a solution of this equation is also called an integral of the differential equation (on the interval I); it is a differentiable map of I into A, whose derivative takes values in B, such that g(u(t),u′(t),t)=0g(u(t), u'(t), t) = 0 for every t∈It \in I. By abuse of language we shall write the differential equation g~(u)=0\tilde{g}(u) = 0 in the form

g(x,x′,t)=0, g(x, x', t) = 0,

on the understanding that x belongs to the set D(A,B)\mathscr{D}(A, B).

For example, for I=E=RI = E = \mathbf{R} the relations

x′=2t,tx′−2x=0,x′2−4x=0,x−t2=0 x' = 2t, \qquad tx' - 2x = 0, \qquad {x'}^2 - 4x = 0, \qquad x - t^2 = 0

are differential equations, all four of which admit the function x(t)=t2x(t) = t^2 as a solution

In this chapter we consider in principle only the case where E is a complete normed space over R\mathbf{R}, and where the differential equations are of the specific form

x′=f(t,x) x' = f(t, x)

("explicit equations in x′x'"), where f denotes a function defined on I×HI \times H with values in E, and H is an open nonempty subset of E. We shall, moreover, widen a little the concept of a solution (or integral) of such an equation (on the interval I): we shall say that a function u, defined and continuous on I, with values in H, is a solution (or integral) of the equation (I) if there exists a countable subset A of I such that at every point t of the complement of A in I the function u admits a derivative u′(t)u'(t) such that u′(t)=f(t,u(t))u'(t) = f(t, u(t)). If uu is differentiable and satisfies the relation above for every point t∈It \in I we shall say that it is a strict solution of the equation (1) on I.

In the particular case of a differential equation of the form x′=f(t)x' = f(t), where ff is a map of I into E, the solutions in the above sense are the primitives of the function ff (II, p. 51), and the strict solutions are the strict primitives.

When E is a product of complete normed spaces EiE_i (1≤i≤n1 \leq i \leq n), one can write x=(xi)1≤i≤nx = (x_i)_{1 \leq i \leq n} and f=(fi)1≤i≤nf = (f_i)_{1 \leq i \leq n}, where xix_i is a map from I into EiE_i and fif_i is a map from I×HI \times H into EiE_i; the equation (1) is then equivalent to the system of differential equations

xi′=fi(t,x1,x2,…,xn)(1≤i≤n). x'_i = f_i(t, x_1, x_2, \ldots, x_n) \qquad (1 \leq i \leq n).
(2)

The most important case is that where the EiE_i are equal to R\mathbf{R} or to C\mathbf{C}; one then says that (2) is a system of scalar differential equations.

One may reduce the study of relations of the form

x(n)=f(t,x,x′,…,x(n−1)) x^{(n)} = f(t, x, x', \ldots, x^{(n-1)})
to that of the system (2), where xx is an nn times differentiable vector function on I; for on putting x1=xx_1 = x, and xp=x(p−1)x_p = x^{(p-1)} for 2≤p≤n2 \leq p \leq n, the relation (3) is equivalent to the system
{xi′=xi+1(1≤i≤n−1)xn′=f(t,x1,x2,…,xn). \begin{cases} x'_i = x_{i+1} & (1 \leq i \leq n-1) \\ x'_n = f(t, x_1, x_2, \ldots, x_n). \end{cases}
(4)

A relation of the form (3) is called a differential equation of order nn (explicitly resolved for x(n)x^{(n)}); in contrast, equations of the form (1) are called differential equations of first order.

Similarly one may reduce any "system of differential equations" of the form

Dnixi=fi(t,x1,Dx1,…,Dn1x1,…,xp,Dxp,…,Dnp−1xp) D^{n_i} x_i = f_i(t, x_1, Dx_1, \ldots, D^{n_1} x_1, \ldots, x_p, Dx_p, \ldots, D^{n_p-1} x_p)
(1≤i≤p)(1 \leq i \leq p) to a system of the form (2), where xix_i is function on I which is nin_i times differentiable on I (for 1≤i≤p1 \leq i \leq p).

2. Differential equations admitting solutions that are primitives of regulated functions

Recall (II, p. 54, def. 3) that a vector function uu defined on an interval I⊂RI \subset \mathbf{R} is said to be regulated if it is the uniform limit of step functions on every compact subset of I; an equivalent condition is that at every interior point of I the function uu has a right and a left limit, and also a right limit at the left-hand end point of I and a left limit at the right-hand endpoint of I, when these two points belong to I (II, p. 54, th. 3). In this chapter we shall restrict ourselves to differential equations (1) for which every solution is a primitive of a regulated function on I. This condition is clearly satisfied if, for every continuous map uu of I into H, the function f(t,u(t))f(t, u(t)) is regulated on I; the following lemma gives a sufficient condition for this:

Lemma 1

Let ff be a map from I×HI \times H into EE such that, on writing fxf_x (for every x∈Hx \in H) for the map t↦f(t,x)t \mapsto f(t, x) of II into EE, the following conditions are satisfied: 1° fxf_x is regulated on II for every x∈Hx \in H; 2° the map x↦fxx \mapsto f_x of HH into the set F(I,E)\mathscr{F}(I, E) of maps from II into EE is continuous when one endows F(I,E)\mathscr{F}(I, E) with the topology of compact convergence (Gen. Top., X, p. 278). Under these conditions:

1° For every continuous map uu of II into HH the function t↦f(t,u(t))t \mapsto f(t, u(t)) is regulated on II; more precisely, the right (resp. left) limit of this function at a point t0∈It_0 \in I is equal to the right (resp. left) limit of the function t↦f(t,u(t0))t \mapsto f(t, u(t_0)) at the point t0t_0.

2° If (un)(u_n) is a sequence of maps of II into HH which converges uniformly to a continuous function uu of II into HH on every compact subset of II, then the sequence of functions t↦f(t,un(t))t \mapsto f(t, u_n(t)) converges uniformly to f(t,u(t))f(t, u(t)) on every compact subset of II.

1 Let cc be the right limit of f(t,u(t0))f(t, u(t_0)) at the point t0t_0; for every ε>0\varepsilon > 0 there is a compact neighbourhood VV of t0t_0 in II such that ∥f(t,u(t0))−c∥≤ε\|f(t, u(t_0)) - c\| \leq \varepsilon for t∈Vt \in V and t>t0t > t_0. On the other hand, there exists δ>0\delta > 0 such that the relations

x∈H,∥x−u(t0)∥≤δ x \in H, \quad \|x - u(t_0)\| \leq \delta

imply ∥f(s,x)−f(s,u(t0))∥≤ε\|f(s, x) - f(s, u(t_0))\| \leq \varepsilon for all s∈Vs \in V; if W⊂VW \subset V is a neighbourhood of t0t_0 in II such that ∥u(t)−u(t0)∥≤δ\|u(t) - u(t_0)\| \leq \delta for every t∈Wt \in W, then ∥f(t,u(t))−c∥≤2ε\|f(t, u(t)) - c\| \leq 2\varepsilon for t∈Wt \in W and t>t0t > t_0, which proves that cc is the right limit of f(t,u(t))f(t, u(t)) at the point t0t_0.

2 Let KK be a compact subset of II; since uu is continuous on II, u(K)u(K) is a compact subset of HH; for every ε>0\varepsilon > 0 and x∈u(K)x \in u(K) there exists a number δx\delta_x such that, for every y∈H,∥y−x∥≤δxy \in H, \|y - x\| \leq \delta_x and every t∈Kt \in K, one has ∥f(t,y)−f(t,x)∥≤ε\|f(t, y) - f(t, x)\| \leq \varepsilon. There is a finite number of points xi∈u(K)x_i \in u(K) such that the closed balls with centre xix_i and radius 12δxi\frac{1}{2}\delta_{x_i} form a cover of u(K)u(K); let δ=Min⁡(δxi)\delta = \operatorname{Min}(\delta_{x_i}). By hypothesis there exists an integer n0n_0 such that for n≥n0n \geq n_0 one has ∥un(t)−u(t)∥≤12δ\|u_n(t) - u(t)\| \leq \frac{1}{2}\delta for every t∈Kt \in K. Now, for every t∈Kt \in K there exists an index ii such that

∥u(t)−xi∥≤12δxi; \|u(t) - x_i\| \leq \frac{1}{2}\delta_{x_i};

consequently one has ∥un(t)−xi∥≤δx\|u_n(t) - x_i\| \leq \delta_x, whence ∥f(t,un(t))−f(t,u(t))∥≤2ε\|f(t, u_n(t)) - f(t, u(t))\| \leq 2\varepsilon for every t∈Kt \in K and every n≥n0n \geq n_0

For the rest of this section I will denote an interval contained in R\mathbf{R}, not reducing to a single point, HH an open nonempty set contained in the normed space EE, and ff a map from I×HI \times H into EE satisfying the hypotheses of lemma 1.

Proposition 1

Let t0t_0 be a point of II and x0x_0 a point of HH; for a continuous function uu to be a solution of the equation (1) on II and take the value x0x_0 at the point t0t_0, it is necessary and sufficient that it satisfies the relation

u(t)=x0+∫t0tf(s,u(s)) ds u(t) = x_0 + \int_{t_0}^t f(s, u(s))\, ds

for every t∈It \in I.

Indeed, by lemma 1, if uu is a solution of (1) on II, then f(t,u(t))f(t, u(t)) is regulated, so the right-hand side of (6) is defined and equal to u(t)u(t) for every t∈It \in I. Conversely, if uu is a continuous function that satisfies (6) then f(t,u(t))f(t, u(t)) is regulated, by lemma 1, so uu has derivative equal to f(t,u(t))f(t, u(t)) except at the points of a countable subset of II.

Corollary

At every point of I distinct from the left (resp. right) endpoint of this interval, every solution u of (1) on I admits a left (resp. right) derivative equal to the left (right) limit of f(t,u(t))f(t, u(t)) at this point.

Proposition 2

If f is a continuous map from I×HI \times H into E, then every solution of (1) on I is a strict solution.

Indeed, such a solution uu is a primitive of the continuous function f(t,u(t))f(t, u(t)) (II, p. 66, prop. 3).

Furthermore, we note that a continuous function ff on I×HI \times H satisfies the conditions of lemma 1 (Gen. Top., X, p. 286, cor. 3).

In the sequel we shall choose t0∈It_0 \in I and x0∈Hx_0 \in H arbitrarily and investigate whether there exist solutions of (1) on II (or on a neighbourhood of t0t_0 in II) taking the value x0x_0 at the point t0t_0 (or, what comes to the same, solutions of (6)).

3. Existence of approximate solutions

Given a number ε>0\varepsilon > 0 we shall say that a continuous map uu of II into HH is an approximate solution to within ε\varepsilon of the differential equation

x′=f(t,x) x' = f(t, x)

if, at all the points of the complement of a countable subset of II, the function uu admits a derivative which satisfies the condition

∥u′(t)−f(t,u(t))∥≤ε. \|u'(t) - f(t, u(t))\| \leq \varepsilon.

Let (t0,x0)(t_0, x_0) be a point of I×HI \times H; since ff satisfies the hypotheses of lemma 1 (IV, p. 165) there exist a compact neighbourhood JJ of t0t_0 in II such that f(t,x0)f(t, x_0) is bounded on JJ, and an open ball SS with centre x0x_0 contained in HH, such that f(t,x)−f(t,x0)f(t, x) - f(t, x_0) is bounded on J×SJ \times S; it follows that f(t,x)f(t, x) is bounded on J×SJ \times S. Throughout this subsection J will denote a compact interval which is a neighbourhood of t0 in I, S will be an open ball with centre x_0 and radius r contained in H, with J and S such that f is bounded on J × S; and M will denote the supremum of \|f(t, x)\| over J × S.*

Proposition 3

On every compact interval with left (or right) endpoint t_0 contained in J, with length less than r/(M + ε), there exists an approximate solution to within ε of equation (1), with values in S, and equal to x_0 at t_0.

We suppose that t0t_0 is not the right-hand endpoint of J, and prove the proposition for intervals with left-hand endpoint t0t_0. Let M\mathscr{M} be the set of solutions of (1) to within ε\varepsilon, each of which takes values in S, is equal to x0x_0 at t0t_0, and is defined on a half open interval [t0,b[[t_0, b[ contained in J (the interval depending on the approximate solution under consideration). First we show that M\mathscr{M} is not empty. Let c be right limit of f(t,x0)f(t, x_0) at t0t_0; by lemma 1 (IV, p. 165) the function f(t,x0+c(t−t0))f(t, x_0 + c(t - t_0)) has a right limit equal to c at t0t_0, so the restriction of the function x0+c(t−t0)x_0 + c(t - t_0) to a sufficiently small half open interval [t0,b[[t_0, b[ will belong to M\mathscr{M}.

We order the set M\mathscr{M} by the relation "u is a restriction of v", and show that M\mathscr{M} is inductive (Set Theory, III, p. 154). Let (uα)(u_\alpha) be a totally ordered subset of M\mathscr{M} and [t0,bα[[t_0, b_\alpha[ the interval where uαu_\alpha is defined: for bα≤bβb_\alpha \leq b_\beta the function uβu_\beta is thus an extension of uαu_\alpha. The union of the intervals [t0,bα[[t_0, b_\alpha[ is an interval [t0,b[[t_0, b[ contained in J, and there exists one and only one function u defined on [t0,b[[t_0, b[ that coincides with uαu_\alpha on [t0,bα[[t_0, b_\alpha[ for each α\alpha; among the bαb_\alpha there is an increasing sequence (bαn)(b_{\alpha_n}) tending to b; since u agrees with uαnu_{\alpha_n} on [t0,bαn[[t_0, b_{\alpha_n}[ the function u admits a derivative satisfying (7) at all the points of the complement of a countable subset of [t0,b[[t_0, b[, and so is the supremum of the set (uα)(u_\alpha) in M\mathscr{M}.

By Zorn's lemma (Set Theory, III, p. 154, th. 2), M\mathscr{M} admits a maximal element u0u_0; we shall show that if [t0,t1[[t_0, t_1[ is the interval where u0u_0 is defined, then either t1t_1 is the right-hand endpoint of J, or else t1−t0≥r/(M+ε)t_1 - t_0 \geq r/(M + \varepsilon). We argue by contradiction, supposing that neither of these conditions holds; first we show that one can extend u0u_0 by continuity at the point t1t_1; in fact, for any s and t in [t0,t1[[t_0, t_1[,

∥u0(s)−u0(t)∥≤(M+ε)∣s−t∣ \|u_0(s) - u_0(t)\| \leq (M + \varepsilon)|s - t|

by the mean value theorem; Cauchy's criterion shows that u0u_0 admits a left limit x1∈Sx_1 \in S at the point t1t_1. Now let c1c_1 be the right limit at t1t_1 of the function f(t,x1)f(t, x_1); one has ∥c1∥≤M\|c_1\| \leq M; the same argument as that at the beginning of the proof shows that one can extend u0u_0 to a half open interval with left-hand endpoint t1t_1 by the function x1+c1(t−t1)x_1 + c_1(t - t_1), so that the extended function belongs to M\mathscr{M}, which is absurd. This proves the proposition.

When f is uniformly continuous on J×SJ \times S one can prove prop. 3 without using Zorn's lemma (IV, p. 199, exerc. 1a)).

Proposition 4

The set of approximate solutions of (1) to within ε\varepsilon, defined on the same interval K⊂JK \subset J and taking values in S, is uniformly equicontinuous.

Indeed, if u is any function in this set and s and t are two points of K, then by the mean value theorem

∥u(s)−u(t)∥≤(M+ε)∣s−t∣. \|u(s) - u(t)\| \leq (M + \varepsilon)|s - t|.

Corollary (Peano's theorem)

If E is of finite dimension over R\mathbf{R} then there exists a solution of (1) with values in S and equal to x0x_0 at t0t_0, on every compact interval K with left (or right) endpoint t0t_0 contained in J and having length <r/M< r/M.

Indeed, by prop. 3, once nn is large enough there is an approximate solution unu_n of (1) to within 1/n1/n, defined on KK, with values in SS, and equal to x0x_0 at t0t_0. Further, from some value of nn on, un(K)u_n(K) is contained in a closed ball with centre x0x_0 and radius <r< r, independent of nn. The set of unu_n is equicontinuous (prop. 4), and since EE is finite dimensional the set SS is relatively compact in EE; so for every t∈Kt \in K the set of un(t)u_n(t) is relatively compact in EE. By Ascoli’s theorem (Gen. Top., X, p. 290, th. 2) the set of unu_n is relatively compact in the space F(K;E)\mathscr{F}(K; E) of maps from KK into EE endowed with the uniform norm. Thus there is a sequence extracted from (unk)(u_{n_k}) of (un)(u_n) which converges uniformly on KK to a continuous function uu. One has u(K)⊂Su(K) \subset S, so t↦f(t,u(t))t \mapsto f(t, u(t)) is defined on KK; by lemma 1 (IV, p. 165), f(t,unk(t))f(t, u_{n_k}(t)) converges uniformly to f(t,u(t))f(t, u(t)) on KK; by (IV, p. 4, formula (7)), unku_{n_k} is a primitive of a function which tends uniformly to f(t,u(t))f(t, u(t)) on KK, so (II, p. 52, th. 1) uu is a solution of (1) on KK, and equal to x0x_0 at the point t0t_0.

Remark 1

There can be infinitely many integrals of a differential equation (1) taking the same value at a given point. For example, the scalar differential equation x′=2∣x∣x' = 2\sqrt{|x|} has all the functions defined by

u(t)=0for −β≤t≤αu(t)=−(t+β)2for t≤−βu(t)=(t−α)2for t≥α \begin{array}{ll} u(t) = 0 & \text{for } -\beta \leq t \leq \alpha \\ u(t) = -(t + \beta)^2 & \text{for } t \leq -\beta \\ u(t) = (t - \alpha)^2 & \text{for } t \geq \alpha \end{array}

as integrals taking the value 0 at the point t=0t = 0, for any positive numbers α\alpha and β\beta.

Remark 2

Peano’s theorem no longer holds when EE is an arbitrary complete normed space of infinite dimension (IV, p. 204, exerc. 18).

4. Comparison of approximate solutions

In what follows, I and HH denote, as above, an interval contained in R\mathbf{R} and an open set in the normed space EE, respectively; t0t_0 is a point of I.

Definition 1

Given a positive real function* t↦k(t)t \mapsto k(t) defined on II, one says that a map ff from I×HI \times H into EE is Lipschitz with respect to the function k(t)k(t) if, for every x∈Hx \in H, the function t↦f(t,x)t \mapsto f(t, x) is regulated on II, and if, for every t∈It \in I and every pair of points x1,x2x_1, x_2 of HH, *one has (the "Lipschitz condition")

∥f(t,x1)−f(t,x2)∥≤k(t)∥x1−x2∥. \| f(t, x_1) - f(t, x_2) \| \leq k(t) \| x_1 - x_2 \|.

(8)

We shall say that ff is Lipschitz (without being more specific) on I×HI \times H if it is Lipschitz on this set for some constant k≥0k \geq 0. It is immediate that a Lipschitz function on I×HI \times H satisfies the hypotheses of lemma 1 of IV, p. 165 (the converse being false); when ff is Lipschitz (on I×HI \times H) one says that the differential equation

x′=f(t,x) x' = f(t, x)

(1)

is Lipschitz (on I×HI \times H).

Example

When E=RE = \mathbf{R} and HH is an interval in R\mathbf{R}, if the function f(t,x)f(t, x) admits a partial derivative fx′f'_x (II, p. 74) at every point (t,x)(t, x) of I×HI \times H, such that ∣fx′(t,x)∣≤k(t)|f'_x(t, x)| \leq k(t) on I×HI \times H, then condition (8) is satisfied, by the mean value theorem; we shall see later how this example generalizes to the case where EE is an arbitrary normed space.

If ff is Lipschitz on I×HI \times H then ff is bounded on J×SJ \times S for every compact subinterval J⊂IJ \subset I and every open ball S⊂HS \subset H. Thus prop. 3 (IV, p. 166) can be applied, and demonstrates the existence of approximate solutions of equation (1). But we also have the following proposition, which allows us to compare two approximate solutions:

Proposition 5

Let k(t)k(t) be a real regulated function and >0> 0 on II, and let f(t,x)f(t, x) be a function that is defined and Lipschitz with respect to k(t)k(t) on I×HI \times H. If uu and vv are two approximate solutions of (1), to within ε1\varepsilon_1 and ε2\varepsilon_2 respectively, defined on II with values in HH, then, for all t∈It \in I such that t≥t0t \geq t_0,

∥u(t)−v(t)∥≤∥u(t0)−v(t0)∥Φ(t)+(ε1+ε2)Ψ(t) \|u(t) - v(t)\| \leq \|u(t_0) - v(t_0)\| \Phi(t) + (\varepsilon_1 + \varepsilon_2)\Psi(t)

where

{Φ(t)=1+∫t0tk(s)exp⁡(∫stk(τ)dτ)dsΨ(t)=t−t0+∫t0t(s−t0)k(s)exp⁡(∫stk(τ)dτ)ds. \begin{cases} \Phi(t) = 1 + \int_{t_0}^t k(s) \exp \left( \int_s^t k(\tau) d\tau \right) ds \\ \Psi(t) = t - t_0 + \int_{t_0}^t (s - t_0)k(s) \exp \left( \int_s^t k(\tau) d\tau \right) ds. \end{cases}

From the relation ∥u′(t)−f(t,u(t))∥≤ε1\|u'(t) - f(t, u(t))\| \leq \varepsilon_1, valid on the complement of a countable set, one deduces, from the mean value theorem, that

∥u(t)−u(t0)−∫t0tf(s,u(s)) ds∥≤ε1(t−t0) \left\| u(t) - u(t_0) - \int_{t_0}^t f(s, u(s))\, ds \right\| \leq \varepsilon_1 (t - t_0)

and similarly

∥v(t)−v(t0)−∫t0tf(s,v(s)) ds∥≤ε2(t−t0) \left\| v(t) - v(t_0) - \int_{t_0}^t f(s, v(s))\, ds \right\| \leq \varepsilon_2 (t - t_0)

whence

∥u(t)−v(t)∥≤∥u(t0)−v(t0)∥ \|u(t) - v(t)\| \leq \|u(t_0) - v(t_0)\|
+∥∫t0t(f(s,u(s))−f(s,v(s))) ds∥+(ε1+ε2)(t−t0). + \left\| \int_{t_0}^t (f(s, u(s)) - f(s, v(s)))\, ds \right\| + (\varepsilon_1 + \varepsilon_2)(t - t_0).

By the Lipschitz condition (8) one has

∥∫t0t(f(s,u(s))−f(s,v(s))) ds∥≤∫t0t∥f(s,u(s))−f(s,v(s))∥ ds \left\| \int_{t_0}^t (f(s, u(s)) - f(s, v(s)))\, ds \right\| \leq \int_{t_0}^t \|f(s, u(s)) - f(s, v(s))\|\, ds
≤∫t0tk(s)∥u(s)−v(s)∥ ds \leq \int_{t_0}^t k(s) \|u(s) - v(s)\|\, ds

whence, putting w(t)=∥u(t)−v(t)∥w(t) = \|u(t) - v(t)\|,

w(t)≤w(t0)+(ε1+ε2)(t−t0)+∫t0tk(s)w(s) ds. w(t) \leq w(t_0) + (\varepsilon_1 + \varepsilon_2)(t - t_0) + \int_{t_0}^t k(s)w(s)\, ds.

The proposition is thus a consequence of the following lemma:

Lemma 2

If w is a continuous real function on the interval [t_0, t_1] and satisfies the inequality

w(t)≤φ(t)+∫t0tk(s)w(s) ds w(t) \leq \varphi(t) + \int_{t_0}^{t} k(s) w(s) \, ds
(12)

where φ\varphi is a regulated function ≥0\geq 0 on [t0,t1][t_0, t_1], then, for t0≤t≤t1t_0 \leq t \leq t_1,

w(t)≤φ(t)+∫t0tφ(s)k(s)exp⁡(∫stk(τ) dτ) ds. w(t) \leq \varphi(t) + \int_{t_0}^{t} \varphi(s) k(s) \exp \left( \int_s^t k(\tau) \, d\tau \right) \, ds.
(13)

Put y(t)=∫t0tk(s)w(s) dsy(t) = \int_{t_0}^t k(s) w(s) \, ds; the relation (12) implies that

y′(t)−k(t)y(t)≤φ(t)k(t) y'(t) - k(t) y(t) \leq \varphi(t) k(t)
(14)

on the complement of a countable set.

Put z(t)=y(t)exp⁡(−∫t0tk(s) ds)z(t) = y(t) \exp \left( - \int_{t_0}^t k(s) \, ds \right); then (14) is equivalent to

z′(t)≤φ(t)k(t)exp⁡(−∫t0tk(s) ds). z'(t) \leq \varphi(t) k(t) \exp \left( - \int_{t_0}^t k(s) \, ds \right).

On applying the mean value theorem (I, p. 15, th. 2) to this inequality, and noting that z(t0)=0z(t_0) = 0, we obtain

z(t)≤∫t0tφ(s)k(s)exp⁡(−∫t0sk(τ) dτ) ds z(t) \leq \int_{t_0}^t \varphi(s) k(s) \exp \left( - \int_{t_0}^s k(\tau) \, d\tau \right) \, ds

whence

y(t)≤∫t0tφ(s)k(s)exp⁡(∫stk(τ) dτ) ds y(t) \leq \int_{t_0}^t \varphi(s) k(s) \exp \left( \int_s^t k(\tau) \, d\tau \right) \, ds

and since w(t)≤φ(t)+y(t)w(t) \leq \varphi(t) + y(t) one thus obtains (13).

Corollary

Let f\mathbf{f} be a Lipschitz function for the constant k>0k > 0, defined on I×H\mathbf{I} \times \mathbf{H}. If u\mathbf{u} and v\mathbf{v} are two approximate solutions of (1) to within ε1\varepsilon_1 and ε2\varepsilon_2 respectively, defined on I\mathbf{I} and taking their values in H\mathbf{H}, then, for all t∈It \in \mathbf{I},

∥u(t)−v(t)∥≤∥u(t0)−v(t0)∥ek∣t−t0∣+(ε1+ε2)ek∣t−t0∣−1k. \| \mathbf{u}(t) - \mathbf{v}(t) \| \leq \| \mathbf{u}(t_0) - \mathbf{v}(t_0) \| e^{k |t - t_0|} + (\varepsilon_1 + \varepsilon_2) \frac{e^{k |t - t_0|} - 1}{k}.
(15)

This inequality is in fact an immediate consequence of (9) when t≥t0t \geq t_0; to prove it for t≤t0t \leq t_0 it suffices to apply it to the equation

dxds=−f(−s,x) \frac{d \mathbf{x}}{ds} = -\mathbf{f}(-s, \mathbf{x})

obtained from (1) by the change of variable t=−st = -s.

Remark 1

When k=0k = 0 the inequality (15) is replaced by the inequality

∥u(t)−v(t)∥≤∥u(t0)−v(t0)∥+(ε1+ε2)∣t−t0∣ \| \mathbf{u}(t) - \mathbf{v}(t) \| \leq \| \mathbf{u}(t_0) - \mathbf{v}(t_0) \| + (\varepsilon_1 + \varepsilon_2) |t - t_0|
whose proof is immediate.

Remark 2

When E is of finite dimension, and f\mathbf{f} is Lipschitz on I×HI \times H, one can show the existence of approximate solutions of (1) (IV, p. 166, prop. 3) without using the axiom of choice (IV, p. 199, exerc. 1 b)).

Proposition 6

Let f\mathbf{f} and g\mathbf{g} be two functions defined on I×HI \times H, satisfying the hypotheses of lemma 1 of IV, p. 165, and such that, on I×HI \times H,

∥f(t,x)−g(t,x)∥≤α. \| \mathbf{f}(t, \mathbf{x}) - \mathbf{g}(t, \mathbf{x}) \| \leq \alpha.
(16)

Suppose further that g\mathbf{g} is Lipschitz for the constant k>0k > 0 on I×HI \times H. In these circumstances, if u\mathbf{u} is an approximate solution of x′=f(t,x)\mathbf{x}' = \mathbf{f}(t, \mathbf{x}) to within ε1\varepsilon_1, defined on II, with values in HH, and v\mathbf{v} is an approximate solution of x′=g(t,x)\mathbf{x}' = \mathbf{g}(t, \mathbf{x}) to within ε2\varepsilon_2, defined on II, with values in HH, then, for all t∈It \in I

∥u(t)−v(t)∥≤∥u(t0)−v(t0)∥ek∣t−t0∣+(α+ε1+ε2)ek∣t−t0∣−1k. \| \mathbf{u}(t) - \mathbf{v}(t) \| \leq \| \mathbf{u}(t_0) - \mathbf{v}(t_0) \| e^{k|t-t_0|} + (\alpha + \varepsilon_1 + \varepsilon_2) \frac{e^{k|t-t_0|} - 1}{k}.
(17)

Indeed

∥u′(t)−g(t,u(t))∥≤α+ε1 \left\| \mathbf{u}'(t) - \mathbf{g}(t, \mathbf{u}(t)) \right\| \leq \alpha + \varepsilon_1
for all tt in the complement in II of a countable subset of II; in other words, u\mathbf{u} is an approximate solution of x′=g(t,x)\mathbf{x}' = \mathbf{g}(t, \mathbf{x}) to within α+ε1\alpha + \varepsilon_1, so the inequality (17) follows on applying prop. 5 of IV, p. 169.

5. Existence and uniqueness of solutions of lipschitz and locally lipschitz equations

Theorem 1 (Cauchy)

Let f\mathbf{f} be a Lipschitz function on I×HI \times H, let J be a compact subinterval of II, not reducing to a single point, t0t_0 a point of J, S an open ball with centre x0\mathbf{x}_0 and radius r, contained in H, and M the least upper bound of ∥f(t,x)∥\| \mathbf{f}(t, \mathbf{x}) \| on J×SJ \times S. In these circumstances, for every compact interval K that does not reduce to a single point and is contained in the intersection of J with ]t0−r/M,t0+r/M[]t_0 - r/M, t_0 + r/M[, and contains t0t_0, there exists one and only one solution of the differential equation x′=f(t,x)\mathbf{x}' = \mathbf{f}(t, \mathbf{x}) defined on K, with values in S, and equal to x0\mathbf{x}_0 at the point t0t_0.

Indeed, for ε>0\varepsilon > 0 sufficiently small, the set FεF_\varepsilon of approximate solutions of (1) to within ε\varepsilon, defined on K, with values in S, and equal to x0\mathbf{x}_0 at the point t0t_0, is not empty (IV, p. 166, prop. 3); further, if u\mathbf{u} and v\mathbf{v} belong to FεF_\varepsilon then, by (15) (IV. p. 170)

∥u(t)−v(t)∥≤2εek∣t−t0∣−1k \| \mathbf{u}(t) - \mathbf{v}(t) \| \leq 2\varepsilon \frac{e^{k|t-t_0|} - 1}{k}

for all t∈Kt \in K, so the sets FεF_\varepsilon form a filter base G\mathscr{G} which converges uniformly on KK to a continuous function ww, equal to x0x_0 at t0t_0; also ww takes values in SS, since, for ε\varepsilon small enough, the functions u∈Fεu \in F_\varepsilon take their values in a closed ball contained in SS. Since f(t,u(t))f(t, u(t)) tends uniformly on KK to f(t,w(t))f(t, w(t)) along G\mathscr{G}, ww satisfies equation (6) of IV, p. 165, so is a solution of (1). The uniqueness of the solution follows immediately from inequality (15) of IV, p. 170 where one takes ε1=ε2=0\varepsilon_1 = \varepsilon_2 = 0 and u(t0)=v(t0)u(t_0) = v(t_0).

We shall say that a function ff defined on I×HI \times H is locally Lipschitz if, for every point (t,x)(t, x) of I×HI \times H, there exists a neighbourhood VV of tt (with respect to II) and a neighbourhood SS of xx such that ff is Lipschitz on V×SV \times S (for a constant kk depending on VV and SS). By the Borel-Lebesgue theorem, for every compact interval J⊂IJ \subset I and every point x0∈Hx_0 \in H there exists an open ball SS with centre x0x_0, contained in HH, such that ff is Lipschitz on J×SJ \times S; thus ff satisfies the hypotheses of lemma 1 of IV, p. 3. When ff is locally Lipschitz on I×HI \times H we shall say that the equation x′=f(t,x)x' = f(t, x) is locally Lipschitz on I×HI \times H.

We shall generalize and clarify th. 1 of IV, p. 10 for locally Lipschitz equations; we restrict ourselves to the case where t0t_0 is the left endpoint of the interval II; one can pass easily to the case where t0t_0 is an arbitrary point of II (cf. IV, §IV ??, p. 9, corollary).

Theorem 2

Let I⊂RI \subset \mathbf{R} be an interval (not reducing to a single point) with left-hand endpoint t0∈It_0 \in I, let HH be a nonempty open set in EE, and ff a locally Lipschitz function on I×HI \times H.

1∘1^\circ For x0∈Hx_0 \in H there exists a largest interval J⊂IJ \subset I, with left-hand endpoint t0∈Jt_0 \in J, on which there exists an integral uu of the equation x′=f(t,x)x' = f(t, x) taking values in HH and equal to x0x_0 at the point t0t_0; this integral is unique.

2∘2^\circ If J≠IJ \neq I then JJ is a half-open interval [t0,β[[t_0, \beta[ of finite length; further, for every compact subset K⊂HK \subset H the set u‾(K)\overline{u}(K) is a compact subset of R\mathbf{R}.

3∘3^\circ If JJ is bounded, and if f(t,u(t))f(t, u(t)) is bounded on JJ, then u(t)u(t) has a left limit cc at the right-hand endpoint of JJ; further, if J≠IJ \neq I then cc is a boundary point of HH in EE.

1∘1^\circ Let M\mathfrak{M} be the set of intervals LL (not reducing to a single point) with left-hand endpoint t0∈Lt_0 \in L which are contained in II and are such that on LL there is a solution of (1) (IV, p. 163) with values in HH and equal to x0x_0 at t0t_0; by th. 1 (IV, p. 171) the set M\mathfrak{M} is not empty. Let LL and L′L' be two intervals belonging to M\mathfrak{M}, and suppose, for example, that L⊂L′L \subset L'; if uu and vv are two integrals of (1) defined respectively on LL and L′L', with values in HH, and equal to x0x_0 at t0t_0, we shall see that vv is an extension of uu. Indeed, let t1t_1 be the supremum of the set of t∈Lt \in L such that u(s)=v(s)u(s) = v(s) for t0≤s≤tt_0 \leq s \leq t; we shall show that t1t_1 is the right-hand endpoint of LL. If this were not so, we would have u(t1)=v(t1)u(t_1) = v(t_1) by continuity, and x1=u(t1)x_1 = u(t_1) would belong to HH; since ff is locally Lipschitz, th. 1 shows that there can exist only one integral of (1) defined on a neighbourhood of t1t_1 with values in HH and equal to x1x_1 at t1t_1; it is therefore a contradiction to suppose that t1t_1 is not the right-hand endpoint of LL. We now see that if JJ is the union of the intervals L∈ML \in \mathfrak{M} there exists one and only one integral uu of (1), defined on JJ, with values in HH and equal to x0x_0 at t0t_0.

2) Suppose that J ≠ I and let β be the right endpoint of J; if β is the right-hand endpoint of I then β ∈ I (so β is finite) and J = [t_0, β[ by hypothesis. Suppose then that β is not the right-hand endpoint of I; if β ∈ J then u(β) = c belongs to H; by th. 1 there exists an integral of (1) with values in H, defined on an interval

[β,β1[⊂I [\beta, \beta_1[ \subset I

and equal to c at β; then J would not be the largest of the intervals in M\mathfrak{M}, which is absurd; so J = [t_0, β[.

If K is a compact subset of H then uˉ−1(K)\bar{u}^{-1}(K) is closed in J; we shall see that there exists a γ ∈ J such that uˉ−1(K)\bar{u}^{-1}(K) is contained in [t_0, γ ], which will prove that uˉ−1(K)\bar{u}^{-1}(K) is compact. If not, there would be a point c ∈ K such that (β, c) is a cluster point of the set of points (t, u(t)) such that t < β and u(t) ∈ K. Since β ∈ I and c ∈ H there exists a neighbourhood V of β in I, and an open ball S with centre c and radius r contained in H, such that f is Lipschitz and bounded on V × S; let M be the supremum of ∥f(t,x)∥\|f(t, x)\| over this set. By hypothesis there exists a t_1 ∈ J such that β−t1<r/2M\beta - t_1 < r/2M, t1∈Vt_1 \in V and ∥u(t1)−c∥≤r/2\|u(t_1) - c\| \leq r/2; th. 1 shows that there exists one and only one integral of (1), with values in H, defined on an interval [t_1, t_2] containing β, and equal to u(t_1) at t_1; since this interval coincides with u on the interval [t_1, β[ it follows that J = [t_0, β[ is not the largest interval in M\mathfrak{M}, which is absurd.

3 Suppose that J is bounded and that ∥f(t,u(t))∥≤M\|f(t, u(t))\| \leq M on J; then ∥u′(t)∥≤M\|u'(t)\| \leq M on the complement of a countable subset of J; then, by the mean value theorem, ∥u(s)−u(t)∥≤M∣s−t∣\|u(s) - u(t)\| \leq M |s - t| for any s and t in J; by the Cauchy criterion, u has a left limit c at the right endpoint β of J. If J ≠ I then c cannot belong to H, for on extending u by continuity at β, u would be an integral of (1) with values in H, defined on an interval [t_0, β] and equal to x_0 at t_0; then one would have J = [t_0, β], contradicting what we have seen in 2 .

Corollary 1

If H = E and J ≠ I then f(t, u(t)) is not bounded on J, if, further, E is finite dimensional, then ∥u(t)∥\|u(t)\| has left limit +∞+\infty at the right-hand endpoint of J.

The first part is an immediate consequence of the third part of th. 2 If E is finite dimensional then every closed ball S ⊂ E is compact, so the second part of th. 2 shows that there exists a γ ∈ J such that u(t) ∉ S for t > γ.

If E is finite dimensional it can happen that J ≠ I but that ∥u(t)∥\|u(t)\| remains bounded as t tends to the right-hand endpoint of J (IV, p. 200, exerc. 5).

Corollary 2

If, on I × H, the function f is Lipschitz with respect to a regulated function k(t), and if the right-hand endpoint β of J belongs to I, then u has a left limit at β; if H = E and if f is Lipschitz with respect to a regulated function k(t) on I × E, then J = I.

Indeed, if β ∈ I, there exists a compact neighbourhood V of β in I, such that f(t, x_0) and k(t) are bounded on V; then ∥f(t,x)∥≤m∥x∥+h\|f(t, x)\| \leq m \|x\| + h (m and h constant) on V×HV \times H, whence ∥u′(t)∥≤m∥u(t)∥+h\|u'(t)\| \leq m \|u(t)\| + h on the complement of a countable subset of V∩JV \cap J, so that ∥u(t)∥≤m∫t0t∥u(s)∥ ds+q\|u(t)\| \leq m \int_{t_0}^t \|u(s)\|\ ds + q (qq constant) on V∩JV \cap J; lemma 2 (IV, p. 170) shows that ∥u(t)∥≤c emt+d\|u(t)\| \leq c\ e^{mt} + d (cc and dd constant) on V∩JV \cap J, and thus f(t,u(t))f(t, u(t)) remains bounded on JJ, and the corollary results from th. 2 of IV, p. 172.

Example 1

For a differential equation of the form x′=g(t)x' = g(t), where gg is regulated on II, every integral uu is clearly defined on all of II. One should note that uu can be bounded on II without g(t)g(t) being so.

Example 2

For the scalar equation x′=1−x2x' = \sqrt{1 - x^2} one has I=R, H=]−1,+1[I = \mathbf{R},\ H = ] - 1, +1[. If one takes t0=x0=0t_0 = x_0 = 0 the corresponding integral is sin⁡t\sin t on the largest interval containing 0 where the derivative of sin⁡t\sin t is positive, that is to say, on ]−π/2,+π/2[] - \pi/2, +\pi/2[; at the endpoints of this interval the integral tends to an endpoint of HH.

Example 3

For the scalar equation x′=1+x2x' = 1 + x^2 one has I=H=RI = H = \mathbf{R}: the integral that vanishes at t=0t = 0 is tan⁡t\tan t, and the largest interval containing 0 where this function is continuous is J=]−π/2,+π/2[J = ] - \pi/2, +\pi/2[; and ∣tan⁡t∣|\tan t| tends to +∞+\infty at the endpoints of JJ (cf. IV, p. 173, cor. 1).

Example 4

For the scalar equation x′=sin⁡txx' = \sin tx one has I=H=RI = H = \mathbf{R} and the right-hand side is bounded on I×HI \times H, so (IV, p. 173, cor. 1) every integral is defined on all of R\mathbf{R}.

6. Continuity of integrals as functions of a parameter

Prop. 6 (IV, p. 171) shows that when a differential equation

x′=f(t,x) x' = f(t, x)

is "close" to a Lipschitz equation x′=g(t,x)x' = g(t, x) and when one supposes that both equations have an approximate solution on the same interval, then these approximate solutions are "close"; we shall clarify this result by showing that the existence of solutions of the Lipschitz equation x′=g(t,x)x' = g(t, x) on an interval implies that of approximate solutions of x′=f(t,x)x' = f(t, x) on the same interval, so long as, on the latter, the values of the solution of x′=g(t,x)x' = g(t, x) are not "too close" to the boundary of HH.

Proposition 7

Let ff and gg be two functions defined on I×HI \times H, satisfying the hypotheses of lemma 1 of IV. p. 165, and such that, on I×HI \times H

∥f(t,x)−g(t,x)∥≤α. \|f(t, x) - g(t, x)\| \leq \alpha .
(16)

Suppose further that gg is Lipschitz with respect to a constant k>0k > 0 on I×HI \times H and that ff is locally Lipschitz on I×HI \times H, or that EE is finite dimensional. Let (t0,x0)(t_0, x_0) be a point of I×HI \times H, μ\mu a number >0> 0, and

φ(t)=μ ek(t−t0)+α ek(t−t0)−1k. \varphi(t) = \mu\ e^{k(t-t_0)} + \alpha\ \frac{e^{k(t-t_0)} - 1}{k} .

Let uu be an integral of the equation x′=g(t,x)x' = g(t, x) defined on an interval K=[t0,b[K = [t_0, b[ contained in II, equal to x0x_0 at the point t0t_0, and such that for all t∈Kt \in K the closed ball with centre u(t)u(t) and radius φ(t)\varphi(t) is contained in HH. Under these conditions, for every y∈Hy \in H such that ∥y−x0∥≤μ\|y - x_0\| \leq \mu there exists an integral vv of x′=f(t,x)x' = f(t, x), defined on KK, with values in HH, and equal to yy at the point t0t_0; moreover, ∥u(t)−v(t)∥≤φ(t)\|u(t) - v(t)\| \leq \varphi(t) on KK.

Let M\mathscr{M} be the family of integrals of x′=f(t,x)x' = f(t, x) each of which takes its values in HH, is equal to yy at t0t_0, and is defined on a half-open interval [t0,τ[[t_0, \tau[ contained in II (depending on the interval considered). By th. 1 of IV, p. 171 (when ff is locally Lipschitz) or IV, p. 167 corollary (when EE is finite dimensional), M\mathscr{M} is not empty, and the same reasoning as in prop. 3 of IV, p. 166 shows that M\mathscr{M} is inductive for the order "v is a restriction of w". Let v0v_0 be a maximal element of M\mathscr{M} and [t0,t1[[t_0, t_1[ the interval of definition of v0v_0; by prop. 6 of IV, p. 171, it all comes down to proving that t1≥bt_1 \geq b. If not, one would have

∥u(t)−v0(t)∥≤φ(t) \| u(t) - v_0(t) \| \leq \varphi(t)

on the interval [t0,t1[[t_0, t_1[ by prop. 6; now on the compact interval [t0,t1][t_0, t_1] the regulated function g(t,u(t))g(t, u(t)) is bounded, so the function g(t,v0(t))g(t, v_0(t)) is bounded on the interval [t0,t1[[t_0, t_1[, for ∥g(t,v0(t))∥≤∥g(t,u(t))∥+kφ(t)\| g(t, v_0(t)) \| \leq \| g(t, u(t)) \| + k \varphi(t) on this interval. Since v0v_0 is an approximate solution of x′=g(t,x)x' = g(t, x) to within α\alpha on [t0,t1[[t_0, t_1[ there exists a number M>0M > 0 such that ∥v0′(t)∥≤M\| v_0'(t) \| \leq M on this interval, except at the points of a countable set; the mean value theorem now shows that ∥v0(s)−v0(t)∥≤M∣s−t∣\| v_0(s) - v_0(t) \| \leq M |s - t| for every pair of points s,ts, t of [t0,t1[[t_0, t_1[, so (by Cauchy's criterion) v0(t)v_0(t) has a left limit cc at the point t1t_1, and, by continuity, one has ∥c−u(t1)∥≤φ(t1)\| c - u(t_1) \| \leq \varphi(t_1), and so c∈Hc \in H. Now one sees, from IV, p. 171, th. 1 or IV, p. 167, corollary, that there exists an integral of x′=f(t,x)x' = f(t, x) defined on an interval [t1,t2[[t_1, t_2[ and equal to cc at t1t_1, which contradicts the definition of v0v_0.

Theorem 3

Let F be a topological space and let f be a map from I × H × F into E such that, for every ξ∈F\xi \in F, the function (t,x)↦f(t,x,ξ)(t, x) \mapsto f(t, x, \xi) is Lipschitz on I × H, and such that, when ξ\xi tends to ξ0\xi_0, f(t,x,ξ)f(t, x, \xi) tends uniformly to f(t,x,ξ0)f(t, x, \xi_0) on I × H. Let u0(t)u_0(t) be an integral of x′=f(t,x,ξ0)x' = f(t, x, \xi_0) defined on an interval J=[t0,b[J = [t_0, b[ contained in I, with values in H, and equal to x0x_0 at t0t_0. For every compact interval [t0,t1][t_0, t_1] contained in J there exists a neighbourhood V of ξ0\xi_0 in F such that, for every ξ∈V\xi \in V, the equation x′=f(t,x,ξ)x' = f(t, x, \xi) has an integral (and only one) u(t,ξ)u(t, \xi) defined on [t0,t1][t_0, t_1], with values in H and equal to x0x_0 at t0t_0; moreover, when ξ\xi tends to ξ0\xi_0 the solution u(t,ξ)u(t, \xi) tends uniformly to u0(t)u_0(t) on [t0,t1][t_0, t_1].

Indeed, let r>0r > 0 be such that for t0≤t≤t1t_0 \leq t \leq t_1 the closed ball with centre u0(t)u_0(t) and radius rr is contained in HH; if f(t,x,ξ)f(t, x, \xi) is Lipschitz with respect to the constant k>0k > 0 on I×HI \times H we take α\alpha small enough that αek(t1−t0)−1k<r\alpha \frac{e^{k(t_1-t_0)} - 1}{k} < r; taking VV such that, for every ξ∈V\xi \in V, one has ∥f(t,x,ξ)−f(t,x,ξ0)∥≤α\| f(t, x, \xi) - f(t, x, \xi_0) \| \leq \alpha on I×HI \times H, one can apply prop. 7 of IV, p. 174; moreover,

∥u(t,ξ)−u0(t)∥≤αek(t1−t0)−1k \| u(t, \xi) - u_0(t) \| \leq \alpha \frac{e^{k(t_1-t_0)} - 1}{k}

on [t0,t1][t_0, t_1], which completes the proof of the theorem.

Remark

When H=EH = E and the condition (16) of IV, p. 174 is satisfied on I×EI \times E, prop. 7 of IV, p. 174 applies to every solution uu of x′=g(t,x)x' = g(t, x) on any interval where this solution is defined; one may even assume that g(t,x)g(t, x) is Lipschitz with respect to a regulated function k(t)k(t) though not necessarily bounded on this interval.

7. Dependence on initial conditions

Let x′=f(t,x)x' = f(t, x) be a locally Lipschitz equation on I×HI \times H; by th. 2 (IV, p. 172), for every point (t0,x0)(t_0, x_0) of I×HI \times H there exists a largest interval J(t0,x0)⊂IJ(t_0, x_0) \subset I, not reducing to a single point, containing t0t_0, and on which there exists an integral (and only one) of this equation, equal to x0x_0 at t0t_0; we shall clarify the manner in which this integral, and the interval J(t0,x0)J(t_0, x_0) where it is defined, depend on the point (t0,x0)(t_0, x_0).

Theorem 4

Let ff be a locally Lipschitz function on I×HI \times H and (a,b)(a, b) an arbitrary point of I×HI \times H.

1 There exist an interval K⊂IK \subset I, a neighbourhood of aa in II, and a neighbourhood VV of bb in HH such that, for every point (t0,x0)(t_0, x_0) of K×VK \times V, there exists an integral (and only one) u(t,t0,x0)u(t, t_0, x_0) defined on KK, with values in HH and equal to x0x_0 at the point t0t_0 (in other words, J(t0,x0)⊃KJ(t_0, x_0) \supset K for all (t0,x0)∈K×V(t_0, x_0) \in K \times V).

2 The map (t,t0,x0)↦u(t,t0,x0)(t, t_0, x_0) \mapsto u(t, t_0, x_0) of K×K×VK \times K \times V into HH is uniformly continuous.

3 There exists a neighbourhood W⊂VW \subset V of bb in HH such that, for every point

(t,t0,x0)∈K×K×W, (t, t_0, x_0) \in K \times K \times W,
the equation x0=u(t0,t,x)x_0 = u(t_0, t, x) has a unique solution xx on VV equal to u(t,t0,x0)u(t, t_0, x_0) ("resolution of the integral with respect to the constant of integration").

1 Let SS be a ball with centre bb and radius rr contained in HH, and J0J_0 an interval contained in II, a neighbourhood of aa in II, such that ff is bounded and Lipschitz (with respect to some constant kk) on J0×SJ_0 \times S; denote by MM the supremum of ∥f(t,x)∥\|f(t, x)\| on J0×SJ_0 \times S. Then there exist (IV, p. 171, th. 1) an interval J⊂J0J \subset J_0, a neighbourhood of aa in II, and an integral vv of x′=f(t,x)x' = f(t, x) defined on JJ, with values in SS and equal to bb at aa. We shall see that the open ball VV with centre bb and radius r/2r/2, and the intersection KK of JJ with an interval ]a−l,a+l[]a - l, a + l[, where ll is small enough, are as required. Indeed, prop. 7 of IV, p. 174 (applied to the set J0×SJ_0 \times S and the case where α=0\alpha = 0) shows that there exists an integral of x′=f(t,x)x' = f(t, x) defined on KK, with values in SS, and equal to x0x_0 at a point t0∈Kt_0 \in K, provided that

∥v(t)−b∥+∥v(t0)−x0∥ek∣t−t0∣<r \|v(t) - b\| + \|v(t_0) - x_0\| e^{k|t-t_0|} < r
for every t∈Kt \in K. Now, by the mean value theorem, one has
∥v(t)−b∥≤M∣t−a∣≤Ml \|v(t) - b\| \leq M |t - a| \leq Ml
for every t∈Kt \in K; since ∥x0−b∥<r/2\|x_0 - b\| < r/2 one sees that it suffices to take ll such that
Ml+(Ml+r/2)e2kl<r Ml + (Ml + r/2)e^{2kl} < r
or the relation (18) to be satisfied for every (t,t0,x0)(t, t_0, x_0) of K×K×VK \times K \times V.

2) By the mean value theorem we have

∥u(t1,t0,x0)−u(t2,t0,x0)∥≤M∣t2−t1∣ \| \mathbf{u}(t_1, t_0, \mathbf{x}_0) - \mathbf{u}(t_2, t_0, \mathbf{x}_0) \| \leq M |t_2 - t_1|

(20)

for all t0,t1,t2t_0, t_1, t_2 in K and x0\mathbf{x}_0 in V. Now prop. 5 (IV, p. 169) shows that

∥u(t,t0,x1)−u(t,t0,x2)∥≤e2kt ∥x2−x1∥ \| \mathbf{u}(t, t_0, \mathbf{x}_1) - \mathbf{u}(t, t_0, \mathbf{x}_2) \| \leq e^{2kt} \ \| \mathbf{x}_2 - \mathbf{x}_1 \|

(21)

for every tt and t0t_0 in K, and x1\mathbf{x}_1 and x2\mathbf{x}_2 in V. Finally, if t1t_1 and t2t_2 are any two points in K,

∥u(t1,t2,x0)−u(t2,t2,x0)∥≤M∣t2−t1∣ \| \mathbf{u}(t_1, t_2, \mathbf{x}_0) - \mathbf{u}(t_2, t_2, \mathbf{x}_0) \| \leq M |t_2 - t_1|

by the mean value theorem, that is to say

∥u(t1,t2,x0)−x0∥≤M∣t2−t1∣; \| \mathbf{u}(t_1, t_2, \mathbf{x}_0) - \mathbf{x}_0 \| \leq M |t_2 - t_1| ;

since u(t,t2,x0)\mathbf{u}(t, t_2, \mathbf{x}_0) is identical to the integral which takes the value u(t1,t2,x0)\mathbf{u}(t_1, t_2, \mathbf{x}_0) at the point t1t_1, prop. 5 (IV, p. 169) shows that

∥u(t,t1,x0)−u(t,t2,x0)∥≤Me2kl∣t2−t1∣ \| \mathbf{u}(t, t_1, \mathbf{x}_0) - \mathbf{u}(t, t_2, \mathbf{x}_0) \| \leq Me^{2kl} |t_2 - t_1|

(22)

for all t,t1,t2t, t_1, t_2 in K and x0\mathbf{x}_0 in V. The three inequalities (20), (21) and (22) thus prove the uniform continuity of the map (t,t0,x0)↦u(t,t0,x0)(t, t_0, \mathbf{x}_0) \mapsto \mathbf{u}(t, t_0, \mathbf{x}_0) on K×K×VK \times K \times V.

3 By (20), we have ∥u(t,t0,x0)−x0∥≤M∣t−t0∣≤2Ml\| \mathbf{u}(t, t_0, \mathbf{x}_0) - \mathbf{x}_0 \| \leq M |t - t_0| \leq 2Ml on

K×K×V. K \times K \times V.

If ll is taken small enough, so that 2Ml<r/42Ml < r/4, one then sees that if x0\mathbf{x}_0 is any point of the open ball W with centre b\mathbf{b} and radius r/4r/4, that u(t,t0,x0)∈V\mathbf{u}(t, t_0, \mathbf{x}_0) \in V for any tt and t0t_0 in K. If x=u(t,t0,x0)\mathbf{x} = \mathbf{u}(t, t_0, \mathbf{x}_0), the function s↦u(s,t,x)s \mapsto \mathbf{u}(s, t, \mathbf{x}) is then defined on K and is equal to the integral of (1) which takes the value x\mathbf{x} at the point tt, that is, to u(s,t0,x0)\mathbf{u}(s, t_0, \mathbf{x}_0); in particular

x0=u(t0,t0,x0)=u(t0,t,x). \mathbf{x}_0 = \mathbf{u}(t_0, t_0, \mathbf{x}_0) = \mathbf{u}(t_0, t, \mathbf{x}).

Moreover, if y∈Vy \in V is such that x0=u(t0,t,y)\mathbf{x}_0 = \mathbf{u}(t_0, t, y), then the integral s↦u(s,t,y)s \mapsto \mathbf{u}(s, t, y) takes the value x0\mathbf{x}_0 at t0t_0 so is identical to s↦u(s,t0,x0)s \mapsto \mathbf{u}(s, t_0, \mathbf{x}_0), which consequently takes the value x\mathbf{x} at tt, which shows that y=xy = \mathbf{x} and concludes the proof.

Exercises

See the exercises for § 1.

Transcribed from the printed volume. Not translated.