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Taylor's theorem

Statement

If ff is n+1n+1 times differentiable on an interval containing aa and xx, then f(x)=∑k=0nf(k)(a)k!(x−a)k+Rn(x)f(x) = \sum_{k=0}^n \frac{f^{(k)}(a)}{k!}(x-a)^k + R_n(x), where the Lagrange remainder is Rn(x)=f(n+1)(ξ)(n+1)!(x−a)n+1R_n(x) = \frac{f^{(n+1)}(\xi)}{(n+1)!}(x-a)^{n+1} for some ξ\xi strictly between aa and xx.

Why is it true?

A smooth function near a point is well approximated by a polynomial that matches its value and all its derivatives up to some order at that point; the remainder term measures exactly how good the approximation is and typically shrinks very fast as you add more terms.

Proof sketch

Fix xx and define g(t)=f(x)−∑k=0nf(k)(t)k!(x−t)kg(t)=f(x)-\sum_{k=0}^n\frac{f^{(k)}(t)}{k!}(x-t)^k and h(t)=(x−t)n+1h(t)=(x-t)^{n+1}. Then g(x)=h(x)=0g(x)=h(x)=0 and, after telescoping, g′(t)=−f(n+1)(t)n!(x−t)ng'(t)=-\frac{f^{(n+1)}(t)}{n!}(x-t)^n, while h′(t)=−(n+1)(x−t)nh'(t)=-(n+1)(x-t)^n. Applying the Cauchy mean value theorem to g,hg,h on the interval between aa and xx gives g(a)−g(x)h(a)−h(x)=g′(ξ)h′(ξ)\frac{g(a)-g(x)}{h(a)-h(x)}=\frac{g'(\xi)}{h'(\xi)} for some ξ\xi between aa and xx, which simplifies exactly to Rn(x)=f(n+1)(ξ)(n+1)!(x−a)n+1R_n(x)=\frac{f^{(n+1)}(\xi)}{(n+1)!}(x-a)^{n+1}.

Proved by

Topics that use this theorem

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Step-by-step proofs

No step-by-step proof yet for this theorem.

References

  1. Brook Taylor (1715). Methodus Incrementorum Directa et Inversa
  2. Joseph-Louis Lagrange (1797). Théorie des fonctions analytiques