11.9: Power Series
( \newcommand{\kernel}{\mathrm{null}\,}\)
Recall that we were able to analyze all geometric series "simultaneously'' to discover that ∞∑n=0kxn=k1−x, if |x|<1, and that the series diverges when |x|≥1. At the time, we thought of x as an unspecified constant, but we could just as well think of it as a variable, in which case the series ∞∑n=0kxn is a function, namely, the function k/(1−x), as long as |x|<1. While k/(1−x) is a reasonably easy function to deal with, the more complicated ∑kxn does have its attractions: it appears to be an infinite version of one of the simplest function types---a polynomial. This leads naturally to the questions: Do other functions have representations as series? Is there an advantage to viewing them in this way?
The geometric series has a special feature that makes it unlike a typical polynomial---the coefficients of the powers of x are the same, namely k. We will need to allow more general coefficients if we are to get anything other than the geometric series.
A power series has the form ∑∞n=0anxn, with the understanding that an may depend on n but not on x.
∑∞n=1xnn is a power series. We can investigate convergence using the ratio test:
limn→∞|x|n+1n+1n|x|n=limn→∞|x|nn+1=|x|.
Thus when |x|<1 the series converges and when |x|>1 it diverges, leaving only two values in doubt. When x=1 the series is the harmonic series and diverges; when x=−1 it is the alternating harmonic series (actually the negative of the usual alternating harmonic series) and converges. Thus, we may think of
∞∑n=1xnn
as a function from the interval [−1,1]) to the real numbers.
A bit of thought reveals that the ratio test applied to a power series will always have the same nice form. In general, we will compute
limn→∞|an+1||x|n+1|an||x|n=limn→∞|x||an+1||an|=|x|limn→∞|an+1||an|=L|x|,
assuming that lim|an+1|/|an| exists. Then the series converges if L|x|<1, that is, if |x|<1/L, and diverges if |x|>1/L. Only the two values x=±1/L require further investigation. Thus the series will definitely define a function on the interval (−1/L,1/L), and perhaps will extend to one or both endpoints as well. Two special cases deserve mention: if L=0 the limit is 0 no matter what value x takes, so the series converges for all x and the function is defined for all real numbers. If L=∞, then no matter what value x takes the limit is infinite and the series converges only when x=0. The value 1/L is called the radius of convergence of the series, and the interval on which the series converges is the interval of convergence.
Consider again the geometric series, ∑∞n=0xn=11−x. Whatever benefits there might be in using the series form of this function are only available to us when x is between −1 and 1. Frequently we can address this shortcoming by modifying the power series slightly. Consider this series:
∞∑n=0(x+2)n3n=∞∑n=0(x+23)n=11−x+23=31−x,
because this is just a geometric series with x replaced by (x+2)/3. Multiplying both sides by 1/3 gives
∞∑n=0(x+2)n3n+1=11−x,
the same function as before. For what values of x does this series converge? Since it is a geometric series, we know that it converges when
|x+2|/3<1|x+2|<3−3<x+2<3−5<x<1.
So we have a series representation for 1/(1−x) that works on a larger interval than before, at the expense of a somewhat more complicated series. The endpoints of the interval of convergence now are −5 and 1, but note that they can be more compactly described as −2±3. We say that 3 is the radius of convergence, and we now say that the series is centered at −2.
A power series centered at a has the form ∑∞n=0an(x−a)n, with the understanding that an may depend on n but not on x.