The general form of the Taylor series representation with base point of a function is given by the following

In class we have derived the following four important Taylor series,

where the last series is really the formula for the sum of a geometric series in disguise.

Once you have a Taylor series representation for a function, it can be used in several ways to generate Taylor series representations of related functions. This is because of the following theorem.

for all in some interval around . Then,

Thus a function cannot have more than one power series in that represents it.

The rest of the Background describes several different techniques for generating Taylor series of functions that are related to Taylor series that are already known. The four techniques are substitution, multiplication and division, integration, and differentiation. We have already seen examples of all of these techniques in class.

Writing out the first few terms gives

By the uniqueness theorem, this must be the Taylor series for .

The most commonly useful Taylor series have base point and that
is what we will focus on in this lab. The technique of substitution is
most useful if the substitution is of the form where is a
constant and is a positive integer. For example, the series for
is easy to obtain as

but it is not clear at all if the following substitution

produces a useful result. This is because you would have to do a lot of work expanding powers of and collecting terms to recover a power series in .

Even if you use a substitution of the form , you have to be
careful if the series is only valid for a finite interval about the
base point. For example, suppose you wanted to find the Taylor series
with base point for the function

You can obtain the desired series by substitution as

but you have to be careful because this formula is not valid for all values of . In fact this formula is only valid if . The reason for this is that the series for is only valid if and when we substitute for , the formula only makes sense if .

then the derivative of has the Taylor series representation

obtained by differentiating each term in the series for , and the series

obtained by integrating each term in the Taylor series for , is an antiderivative of .

2006-04-10