Taylor series operator commutes with differentiation: Difference between revisions

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By <math>(\dagger)</math>, we can rewrite <math>(f')^{(k)}(x_0)</math> on the right side as <math>f^{(k+1)}(x_0)</math>, and get:
By <math>(\dagger)</math>, we can rewrite <math>(f')^{(k)}(x_0)</math> on the right side as <math>f^{(k+1)}(x_0)</math>, and get:


<math>\mbox{Taylor series for } f' \mbox{ at } x_0 = \sum_{k=0}^\infty \frac{f^{(k+1)}}(x_0)}{k!}(x - x_0)^k</math>
<math>\mbox{Taylor series for } f' \mbox{ at } x_0 = \sum_{k=0}^\infty \frac{f^{(k+1)}(x_0)}{k!}(x - x_0)^k</math>


===Checking equality===
===Checking equality===


It is now easy to verify that we have precisely the same expressions for the derivative of the Taylor series of <math>f</math> and the Taylor series of <math>f'</math>.
It is now easy to verify that we have precisely the same expressions for the derivative of the Taylor series of <math>f</math> and the Taylor series of <math>f'</math>.

Latest revision as of 16:25, 4 July 2012

Statement

Suppose f if a function defined on a subset of the reals that is infinitely differentiable at a point x0 in its domain. Then, the derivative f is also defined and infinitely differentiable at x0, and the Taylor series for f is the derivative (in the sense of derivative of power series) of the Taylor series for f.

Related facts

Proof

Given: f is a function defined on a subset of the reals and it is infinitely differentiable at a point x0 in its domain.

To prove: The derivative f is defined and infinitely differentiable at x0 and the Taylor series for f is the derivative of the Taylor series for f.

Proof: We have the following relation between the derivatives of f and f:

(f)(k)(x0)=f(k+1)(x0)k{0,1,2,,}()

In particular, this means that, since f is infinitely differentiable at x0, so is f, with the derivatives given by the above relationship. Thus, it makes sense to take the Taylor series of f.

Derivative of the Taylor series

We note that:

Taylor series for f at x0=k=0f(k)(x0)k!(xx0)k

Let's try differentiating this. Differentiation of power series is term-wise, so we compute the derivative for each term, i.e., we try to calculate:

ddx[f(k)(x0)k!(xx0)k]

The expression f(k)(x0)k! is constant, so we use the differentiation rule for power functions on (xx0)k (with the chain rule) and obtain:

ddx[f(k)(x0)k!(xx0)k]=kf(k)(x0)k!(xx0)k1

For k=0, this becomes 0. For k1, set l=k1 (note that l0 now) and this becomes:

f(l+1)(x0)l!(xx0)l

Now adding together all the terms, we get:

Derivative of Taylor series for f at x0=l=0f(l+1)(x0)l!(xx0)l

Since l is a dummy variable, we can use the dummy variable k instead, and get:

Derivative of Taylor series for f at x0=k=0f(k+1)(x0)k!(xx0)k

Taylor series of the derivative

We note that:

Taylor series for f at x0=k=0(f)(k)(x0)k!(xx0)k

By (), we can rewrite (f)(k)(x0) on the right side as f(k+1)(x0), and get:

Taylor series for f at x0=k=0f(k+1)(x0)k!(xx0)k

Checking equality

It is now easy to verify that we have precisely the same expressions for the derivative of the Taylor series of f and the Taylor series of f.