TheoremBase

The mean value theorem applied to an auxiliary function writes the remainder as half the increment of f'' times h2h^2; this increment is bounded by 2M2 directly and by M3|h| through a second application of the mean value theorem.

Proof

Fix v,h∈Rv,h\in\mathbb{R} and let R=f(v+h)−f(v)−f′(v)h−12f′′(v)h2R=f(v+h)-f(v)-f'(v)h-\tfrac12f''(v)h^{2}. If h=0h=0, then R=0R=0 and there is nothing to prove; let h≠0h\neq0, and put w=v+hw=v+h, so that w−v=h≠0w-v=h\neq0.

The remainder as an increment of f′′f''. Let K=(f(w)−f(v)−f′(v)h)/h2K=\bigl(f(w)-f(v)-f'(v)h\bigr)/h^{2}, so that R=Kh2−12f′′(v)h2R=Kh^{2}-\tfrac12f''(v)h^{2}, and let ψ:R→R\psi:\mathbb{R}\to\mathbb{R} be the function

ψ(s)=f(s)+f′(s)(w−s)+K(w−s)2.\psi(s)=f(s)+f'(s)(w-s)+K(w-s)^{2}.

Then ψ(v)=f(v)+f′(v)h+Kh2=f(w)\psi(v)=f(v)+f'(v)h+Kh^{2}=f(w) by the choice of KK, and ψ(w)=f(w)\psi(w)=f(w). By the sum and product rules, the function ψ\psi is differentiable, with

ψ′(s)=f′(s)+f′′(s)(w−s)−f′(s)−2K(w−s)=(w−s)(f′′(s)−2K)(s∈R)\psi'(s)=f'(s)+f''(s)(w-s)-f'(s)-2K(w-s)=(w-s)\bigl(f''(s)-2K\bigr)\qquad(s\in\mathbb{R})

(Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (i), Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (ii), Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (iv), Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (v), Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (vi)), and hence continuous (The Increment Form of the Derivative, and Differentiability Implies Continuity (ii)). Let x=min⁡{v,w}x=\min\{v,w\} and y=max⁡{v,w}y=\max\{v,w\}, so x<yx<y. By the mean value theorem on the interval R\mathbb{R} (Mean Value Theorem on a Closed Real Interval and on Any Interval (ii)) there is ξ\xi with x<ξ<yx<\xi<y, that is, ξ\xi strictly between vv and ww, and

0=ψ(y)−ψ(x)=ψ′(ξ) (y−x).0=\psi(y)-\psi(x)=\psi'(\xi)\,(y-x).

Since y−x=∣h∣≠0y-x=|h|\neq0 and w−ξ≠0w-\xi\neq0, this gives f′′(ξ)=2Kf''(\xi)=2K, and therefore

f(w)−f(v)−f′(v)h−12f′′(v)h2=R=12(f′′(ξ)−f′′(v))h2.f(w)-f(v)-f'(v)h-\tfrac12f''(v)h^{2}=R=\tfrac12\bigl(f''(\xi)-f''(v)\bigr)h^{2}.

Two bounds on the increment. First, ∣f′′(ξ)−f′′(v)∣≤∣f′′(ξ)∣+∣f′′(v)∣≤2M2|f''(\xi)-f''(v)|\le|f''(\xi)|+|f''(v)|\le2M_{2}. Second, ξ≠v\xi\neq v and f′′f'' is differentiable, hence continuous (The Increment Form of the Derivative, and Differentiability Implies Continuity (ii)), so the mean value theorem (Mean Value Theorem on a Closed Real Interval and on Any Interval (ii)), applied to f′′f'' on the interval R\mathbb{R} between vv and ξ\xi, gives η\eta strictly between vv and ξ\xi with f′′(ξ)−f′′(v)=f′′′(η) (ξ−v)f''(\xi)-f''(v)=f'''(\eta)\,(\xi-v); hence ∣f′′(ξ)−f′′(v)∣≤M3∣ξ−v∣|f''(\xi)-f''(v)|\le M_{3}|\xi-v|. Since ξ\xi lies strictly between vv and ww, ∣ξ−v∣<∣w−v∣=∣h∣|\xi-v|<|w-v|=|h|, and since M3≥∣f′′′(v)∣≥0M_{3}\ge|f'''(v)|\ge0, it follows that M3∣ξ−v∣≤M3∣h∣M_{3}|\xi-v|\le M_{3}|h|. Together,

∣f′′(ξ)−f′′(v)∣≤min⁡{2M2,M3∣ξ−v∣}≤min⁡{2M2,M3∣h∣},|f''(\xi)-f''(v)|\le\min\bigl\{2M_{2},M_{3}|\xi-v|\bigr\}\le\min\bigl\{2M_{2},M_{3}|h|\bigr\},

and so

∣R∣≤12min⁡{2M2,M3∣h∣}h2=min⁡{M2h2,12M3∣h∣3},|R|\le\tfrac12\min\bigl\{2M_{2},M_{3}|h|\bigr\}h^{2}=\min\bigl\{M_{2}h^{2},\tfrac12M_{3}|h|^{3}\bigr\},

which is (i).

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