Taylor series operator commutes with differentiation: Difference between revisions
No edit summary |
|||
| Line 8: | Line 8: | ||
* [[Taylor series operator is linear]] | * [[Taylor series operator is linear]] | ||
* [[Taylor series operator is multiplicative]] | * [[Taylor series operator is multiplicative]] | ||
==Proof== | |||
'''Given''': <math>f</math> is a function defined on a subset of the reals and it is infinitely differentiable at a point <math>x_0</math> in its domain. | |||
'''To prove''': The derivative <math>f'</math> is defined and infinitely differentiable at <math>x_0</math> and the Taylor series for <math>f'</math> is the derivative of the Taylor series for <math>f</math>. | |||
'''Proof''': We have the following relation between the derivatives of <math>f</math> and <math>f'</math>: | |||
<math>(f')^{(k)}(x_0) = f^{(k+1)}(x_0) \ \forall \ k \in \{ 0,1,2,\dots,\} \qquad (\dagger)</math> | |||
In particular, this means that, since <math>f</math> is infinitely differentiable at <math>x_0</math>, so is <math>f'</math>, with the derivatives given by the above relationship. Thus, it makes sense to take the Taylor series of <math>f'</math>. | |||
===Derivative of the Taylor series=== | |||
We note that: | |||
<math>\mbox{Taylor series for } f \mbox{ at } x_0 = \sum_{k=0}^\infty \frac{f^{(k)}(x_0)}{k!}(x - x_0)^k</math> | |||
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: | |||
<math>\frac{d}{dx}\left[\frac{f^{(k)}(x_0)}{k!}(x - x_0)^k\right]</math> | |||
The expression <math>\frac{f^{(k)}(x_0)}{k!}</math> is constant, so we use the [[differentiation rule for power functions]] on <math>(x - x_0)^k</math> (with the chain rule) and obtain: | |||
<math>>\frac{d}{dx}\left[\frac{f^{(k)}(x_0)}{k!}(x - x_0)^k\right] = \frac{kf^{(k)}(x_0)}{k!}(x - x_0)^{k-1}</math> | |||
For <math>k = 0</math>, this becomes 0. For <math>k \ge 1</math>, set <math>l= k - 1</math> (note that <math>l \ge 0</math> now) and this becomes: | |||
<math>\frac{f^{(l + 1)}(x_0)}{l!}(x - x_0)^l</math> | |||
Now adding together all the terms, we get: | |||
<math>\mbox{Derivative of Taylor series for } f \mbox{ at } x_0 = \sum_{l=0}^\infty \frac{f^{(l + 1)}(x_0)}{l!}(x - x_0)^l</math> | |||
Since <math>l</math> is a dummy variable, we can use the dummy variable <math>k</math> instead, and get: | |||
<math>\mbox{Derivative of Taylor series for } f \mbox{ at } x_0 = \sum_{k=0}^\infty \frac{f^{(k + 1)}(x_0)}{k!}(x - x_0)^k</math> | |||
===Taylor series of the derivative=== | |||
We note that: | |||
<math>\mbox{Taylor series for } f' \mbox{ at } x_0 = \sum_{k=0}^\infty \frac{(f')^{(k)}(x_0)}{k!}(x - x_0)^k</math> | |||
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> | |||
===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>. | |||
Revision as of 15:35, 30 June 2012
Statement
Suppose if a function defined on a subset of the reals that is infinitely differentiable at a point in its domain. Then, the derivative is also defined and infinitely differentiable at , and the Taylor series for is the derivative (in the sense of derivative of power series) of the Taylor series for .
Related facts
- Differentiation theorem for power series
- Taylor series operator is linear
- Taylor series operator is multiplicative
Proof
Given: is a function defined on a subset of the reals and it is infinitely differentiable at a point in its domain.
To prove: The derivative is defined and infinitely differentiable at and the Taylor series for is the derivative of the Taylor series for .
Proof: We have the following relation between the derivatives of and :
In particular, this means that, since is infinitely differentiable at , so is , with the derivatives given by the above relationship. Thus, it makes sense to take the Taylor series of .
Derivative of the Taylor series
We note that:
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:
The expression is constant, so we use the differentiation rule for power functions on (with the chain rule) and obtain:
For , this becomes 0. For , set (note that now) and this becomes:
Now adding together all the terms, we get:
Since is a dummy variable, we can use the dummy variable instead, and get:
Taylor series of the derivative
We note that:
By , we can rewrite on the right side as , and get:
Failed to parse (syntax error): {\displaystyle \mbox{Taylor series for } f' \mbox{ at } x_0 = \sum_{k=0}^\infty \frac{f^{(k+1)}}(x_0)}{k!}(x - x_0)^k}
Checking equality
It is now easy to verify that we have precisely the same expressions for the derivative of the Taylor series of and the Taylor series of .