When a Taylor series really equals its function, how Taylor's inequality proves it, why power series coefficients are unique, and which operations on series are valid where.
A Taylor series can converge and still add up to the wrong function. So two questions are always separate. Does the series converge at x? Does it converge to f(x)? The answer to the second comes from the remainder, and once it is settled for a few basic functions, uniqueness of coefficients lets you get many more series by algebra alone.
Key terms
Equality requires the remainder to tend to zero
Definition Let f have derivatives of all orders on an open interval I containing a, let Tn be its Taylor polynomials at a and Rn(x)=f(x)−Tn(x). For x∈I,
f(x)=n=0∑∞n!f(n)(a)(x−a)nif and only ifn→∞limRn(x)=0.
This holds because the partial sums of the Taylor series are exactly the Tn(x), and Tn(x)→f(x) means Rn(x)→0.
In plain words The series equals the function at x exactly when the error of the Taylor polynomials at x shrinks to zero.
Example For ex at a=0 and x=0 the Lagrange form gives
Rn(x)=(n+1)!ezxn+1
with z between 0 and x, so
∣Rn(x)∣≤e∣x∣(n+1)!∣x∣n+1.
For any fixed x the factorial eventually outgrows the power, so
n→∞lim(n+1)!∣x∣n+1=0.
At x=0 the remainder is 0 anyway. So ex=∑n!xn for every real x.
Taylor’s inequality for series
Definition Let f have derivatives of all orders on [a−d,a+d], where d>0, and suppose there are constants Mn with f(n+1)(t)≤Mn for every n≥0 and every t in that interval. Taylor’s inequality gives
∣Rn(x)∣≤(n+1)!Mn∣x−a∣n+1,∣x−a∣≤d.
If the right side tends to 0 as n→∞, in particular if one constant M bounds every derivative on that interval, then the Taylor series equals f(x) for all ∣x−a∣≤d.
In plain words If you can bound all the derivatives on an interval well enough, the Taylor series is guaranteed to give the right answer there.
Example Every derivative of sinx is ±sinx or ±cosx, so Mn=1 works on every interval. Then
∣Rn(x)∣≤(n+1)!∣x∣n+1→0for every x,
and the Maclaurin series of sinx equals sinx on all of R.
Convergence domain
Definition For a function f with derivatives of all orders at a, three sets can differ. They are the domain of f, the interval of convergence of its Taylor series at a, and the set of x where the series converges to f(x). The third is contained in the second, and both can be much smaller than the first.
In plain words A function can be perfectly fine at a point where its series has already stopped working, and a series can converge to the wrong value.
Example The function f(x)=1+x21 is defined and smooth for every real x. Its Maclaurin series ∑(−1)nx2n has radius 1, so at x=2 the function equals 51 but the series diverges. For e−1/x2 (with value 0 at 0) the series converges everywhere and equals the function only at 0.
Uniqueness of coefficients
Definition If f(x)=∑cn(x−a)n for all x with ∣x−a∣<R, where R>0, then
cn=n!f(n)(a)for every n≥0.
So a function has at most one power series expansion about a given center, and any such expansion is its Taylor series. This follows by differentiating the series term by term n times and setting x=a.
In plain words However you find a power series for f, by substitution, multiplication or any other valid method, it is the Taylor series. You can then read derivatives off the coefficients.
Example From 1+x21=∑(−1)nx2n the coefficient of x10 is (−1)5=−1. So
10!f(10)(0)=−1,f(10)(0)=−10!=−3628800,
with no differentiation needed.
Operations with valid convergence conditions
Definition Let f(x)=∑an(x−a)n for ∣x−a∣<R1 and g(x)=∑bn(x−a)n for ∣x−a∣<R2. Then the following hold.
Sums and Cauchy products give f+g and fg for ∣x−a∣<min(R1,R2).
Term-by-term differentiation and integration give f′ and antiderivatives of f for ∣x−a∣<R1.
For a series centered at 0, substituting u=kxm into ∑anun is valid where ∣kxm∣<R1.
By uniqueness, each resulting series is the Taylor series of the new function. Endpoints must be checked separately each time.
In plain words Combine known series freely, but write down where each result holds. The answer is valid only where every ingredient was valid.
Example Substituting u=−x2 into eu=∑n!un, valid for every u, gives
e−x2=n=0∑∞n!(−1)nx2n=1−x2+2x4−6x6+⋯
for every real x. The coefficient of x4 is 21, so the fourth derivative of e−x2 at 0 is 4!⋅21=12.
Check yourself
Prove that the Maclaurin series of cosx equals cosx for every real x.
Show the answer
Every derivative of cosx is ±sinx or ±cosx, so it is bounded by M=1 everywhere. Taylor’s inequality gives
∣Rn(x)∣≤(n+1)!∣x∣n+1,
which tends to 0 for every x.
Find f(7)(0) for f(x)=x2ex.
Show the answer
Multiply the series for ex by x2 to get
x2ex=n=0∑∞n!xn+2.
The coefficient of x7 comes from n=5 and is 5!1. By uniqueness
f(7)(0)=5!7!=42.
Find the Maclaurin series of ln(1+x2) and the set where it equals the function.
Show the answer
Substitute u=x2 into
ln(1+u)=n=1∑∞n(−1)n−1un,
which is valid for −1<u≤1. This gives
ln(1+x2)=n=1∑∞n(−1)n−1x2n,
valid when x2≤1, that is for −1≤x≤1. For ∣x∣>1 the terms do not tend to 0.
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