Define v:[0,T]βR by v(t)=β«0tβu(s)ds, with v(0)=0 by the stated convention. The hypothesis reads u(t)β€a+bv(t) for 0β€tβ€T.
Case b=0. By item 1 of Basic Properties of the Exponential Function, exp(0)=1, so for every tβ[0,T], u(t)β€a=aexp(bt). Assume from now on b>0.
Step 1: regularity of v. The function u is continuous at every point of [0,T], by hypothesis and Continuity on a Closed Interval. By Fundamental Theorem of Calculus, Part I in One Dimension applied with f=u on [0,T], the integral defining v(t) is well defined for every tβ[0,T] and v is differentiable at every tβ(0,T) with vβ²(t)=u(t) (with the same degenerate-interval convention v(0)=0, so v is the function F of that theorem).
By the extreme value theorem there are xminβ,xmaxββ[0,T] with u(xminβ)β€u(s)β€u(xmaxβ) for all sβ[0,T]; put K=max(β£u(xminβ)β£,β£u(xmaxβ)β£), so β£u(s)β£β€K on [0,T]. Let 0β€t0β<t1ββ€T. By additivity of the Riemann integral on adjacent intervals (Additivity of the Riemann Integral on Adjacent Intervals), together with the convention v(0)=0 in the case t0β=0,
v(t1β)βv(t0β)=β«t0βt1ββu(s)ds,
and by the mean value theorem for integrals there is cββ[t0β,t1β] with β«t0βt1ββu(s)ds=u(cβ)(t1ββt0β). Hence β£v(t1β)βv(t0β)β£β€K(t1ββt0β) for all 0β€t0β<t1ββ€T. Given any tββ[0,T] and Ξ΅>0, taking Ξ΄=Ξ΅/(K+1) in Continuity at a Point shows that v is continuous at tβ; thus v is continuous at every point of [0,T].
Step 2: the auxiliary function decreases. Define Ο:[0,T]βR by
Ο(t)=exp(βbt)(baβ+v(t)).
By the scaled-exponential lemma with c=βb, the function tβ¦exp(βbt) on R is differentiable at every real point with derivative βbexp(βbt) and continuous at every real point. The defining conditions of Derivative at an Interior Point and Continuity at a Point quantify only over points of the domain, so the restriction of this function to [0,T] is continuous at every point of [0,T] and differentiable, with the same derivative, at every interior point of the interval [0,T].
By claim 4 of the one-dimensional rules lemma applied with E=[0,T] (constants are continuous, and sums and products of continuous functions are continuous), together with Step 1, Ο is continuous at every point of [0,T], i.e., continuous on [0,T].
Let tβ(0,T); then t is an interior point of [0,T], since 0<t<T with 0,Tβ[0,T]. By claim 2 of the rules lemma, tβ¦a/b+v(t) is differentiable at t with derivative vβ²(t)=u(t) (Step 1), and by claim 3 (the product rule),
Οβ²(t)=βbexp(βbt)(baβ+v(t))+exp(βbt)u(t)=exp(βbt)(u(t)βaβbv(t)).
By item 2 of Basic Properties of the Exponential Function, exp(βbt)>0, and u(t)βaβbv(t)β€0 by hypothesis; hence Οβ²(t)β€0 for every tβ(0,T).
Step 3: conclusion. Fix tβ(0,T]. The function Ο is continuous at every point of [0,t] and differentiable at every point of (0,t)β(0,T). By the mean value theorem applied to Ο on [0,t] (with the interval I=[0,T]), there is ΞΎβ(0,t) with
Ο(t)βΟ(0)=Οβ²(ΞΎ)(tβ0)β€0.
Since Ο(0)=exp(0)(a/b+v(0))=a/b, using exp(0)=1 and v(0)=0, we obtain, for every tβ[0,T] (the case t=0 holding with equality),
exp(βbt)(baβ+v(t))β€baβ.
By items 1 and 2 of Basic Properties of the Exponential Function, exp(bt)>0 and exp(βbt)exp(bt)=exp(0)=1; multiplying the last display by exp(bt) therefore gives
baβ+v(t)β€baβexp(bt),
hence bv(t)β€aexp(bt)βa, and by the hypothesis,
u(t)β€a+bv(t)β€aexp(bt)(0β€tβ€T).
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