Taylor Series

Taylor Series

Arun Ram
Department of Mathematics and Statistics
University of Melbourne
Parkville, VIC 3010 Australia
aram@unimelb.edu.au
and

Department of Mathematics
University of Wisconsin, Madison
Madison, WI 53706 USA
ram@math.wisc.edu

Last updates: 1 December 2009

Taylor series

Taylor's theorem.

  1. If f x = a 0 + a 1 x + a 2 x 2 + ⋯ then a l = 1 l ! d l f d x l | x = 0 .
  2. If f : a b → ℝ and N ∈ ℤ > 0 and f N : a b → ℝ is continuous and f N + 1 : a b → ℝ exists then there exists c ∈ a b such that f b = f a + f ′ a b - a + 1 2 ! f ″ a b - a 2 + ⋯ + 1 N ! f N a b - a N + 1 N + 1 ! f N + 1 c b - a N + 1 .

Remark. The following results follow from (a) after a tiny bit of algebra. If f a + x = a 0 + a 1 x + a 2 x 2 + ⋯ then a l = 1 l ! d l f d x l | x = 0 . If f z = a 0 + a 1 z - a + a 2 z - a 2 + ⋯ then a l = 1 l ! d l f d z l | z = a .

Remark. The special case N = 1 is the mean value theorem. The special case N = 1 and f a = f b is Rolle's theorem. The last term in f a + f ′ a b - a + 1 2 ! f ″ a b - a 2 + ⋯ + 1 N ! f N a b - a N + 1 N + 1 ! f N + 1 c b - a N + 1 is Lagrange's form of the remainder.

Proof of Taylor's theorem, part (a).
  1. Assume f x = a 0 + a 1 x + a 2 x 2 + ⋯ = ∑ i = 0 ∞ a i x i
  2. To show: a l = d l f d x l | x = 0 for l ∈ ℤ > 0 .
  3. We have d l f d x l = d l d x l ∑ i = 0 ∞ a i x i = ∑ i = l ∞ i - l - 1 i - l - 2 ⋯ i - 1 i a i x i - l = ∑ i = l ∞ ∏ j = 1 l i - l - j a i x i - l , by repeated differentiation.
  4. So d l f d x l | x = 0 = ∑ i = l ∞ ∏ j = 1 l i - l - j a i x i - l | x = 0 = ∏ j = 1 l l - l - j a l = l ! a l .
  5. Solving for a l givs the required result.proof changed

Proof of the mean value theorem.
  1. To show: there exists c ∈ a b such that f b = f a + f ′ c b - a .
  2. First do the case: f a = f b .
    1. Then, since a b is compact and connected and f : a b → ℝ is continuous, f a b is compact and connected.
    2. So f a b is a closed interval.
    3. So f a b = min max for some min max ∈ ℝ .
    4. So there exists c ∈ a b such that f c = max .
    5. Then, if ε ∈ ℝ > 0 is small enough f c + ε ≤ f c and f c - ε ≤ f c .
    6. So f ′ c ≥ 0 and f ′ c ≤ 0 .
    7. So f ′ c = 0 .
  3. Next do the case f a ≠ f b .
    1. Let g x = - f b - f a b - a x - a + f x .
    2. So g a = f a and g b = f a and g ′ x = - f b - f a b - a + f ′ x .
    3. So by the first case, there exists c ∈ a b with g ′ c = 0 .
    4. So f ′ c - f b - f a b - a = 0 .
    5. So f ′ c = f b - f a b - a and f b = f a + f ′ c b - a .

References [PLACEHOLDER]

[BG] A. Braverman and D. Gaitsgory, Crystals via the affine Grassmanian, Duke Math. J. 107 no. 3, (2001), 561-575; arXiv:math/9909077v2, MR1828302 (2002e:20083)