01

(a)


(b)

02

(a) Notice the matching powers. Collect powers and then observe the geometric series pattern:


(b)

03

Notice that .

We have this series for :

Therefore:

Now we use the “Next Term Bound” rule. Calculate terms until we find a term less than :

So we take the following partial sum approximation:

04

(a)


(b)

05

Calculate derivatives. Use .

0
1
2
3
4
5
6

Each new derivative takes down the next power as a factor, and switches the sign. The accumulation of powers follows a factorial pattern, and these factorials cancel those added to the denominator to make .

So we have:


Alternate method:

We can derive this Taylor series using some algebraic tricks with the standard geometric series:

06

(a)


(b)


(c)

07

(a)


(b)


(c)


(d)

08

Use the formula :

Therefore:

09

(a)

Recall the series for :

This matches our series if we set . So the total sum is:


(b)

10

The Coefficient-Derivative Identity says that where is the coefficient of the power .

Solve:

So, for the coefficient :

11

Write the alternating series for :

This is an alternating series, so we can apply the “Next Term Bound” rule. Calculate some terms:

(Without a calculator, we can see that . Dividing by will only decrease this value.)

So we add up the prior terms:

12

Write the series of the integrand:

Integrate:

Now apply the “Next Term Bound” and look for the first term below :

So we simply add the first two terms: