Basically the Taylor Series is a function represented as an infinite sum of terms that are ordered like an infinite polynomial.

## Background

Introduced in 1715 by Brook Taylor

- Brook Taylor:
- Born 18 August 1685
- Edmonton, Middlesex, England

- Death 30 November 1731 (aged 46)
- London, England

- English mathematician
- best known for Taylor’s theorem and Taylor series
- attended St. John’s College

- Born 18 August 1685
- Colin Maclaurin:
- Born February, 1698
- Kilmodan, Cowall, Argyll, Scotland

- Death 14 June 1746
- Edinburgh, Scotland

- Scottish mathematician
- Maclaurin Series
- special case of Taylor Series

- Born February, 1698

## The Idea

or for fans of the sigma notation:

The core idea here is to be able to write all functions in one common, differientiable and generic way.

## The Concept

Using the Power Series (or the more specific Taylor Series) one can represent complex function as a simple chain of powers, just like in a polynomial. This can drastically improve the way we handle certain functions.

### Power Series

A power series is a simple infinite polynomial:

The power series is very simple. Every term in the function has some arbitrary coefficient in front that could be anything.

### Taylor Series

Brook Taylor furthermore said that most(every?) functions could be represented as such an power series.

Lets make two assumptions.

- f(x) does in fact have a power representation about x = a
- f(x) has derivatives of every order and we can find them all

At this point we need to find the coefficients ```
\(
a_0, a_1, a_2, a_3, …, a_{\infty}
\)
```

Looking back at the original function (`\(a_0+a_1 (x-a)+a_2 (x-a)^2+a_3 (x-a)^3 \cdots\)`

) we can try evaluating it at: `\(a\)`

Every term will end up going to zero except for the first coefficient.

We can reapply the same idea to the derivatives of the power series.

Therefore when plugging in a again: `\(f'(a)=a_1\)`

For the second derivative: ```
\(
\ddot{f}(x) = 0+0+2a_2+a_3 6(x-a) \cdots\
\)
```

A pattern is starting to form here:

```
\(
f^{n}(x) = n!a_n \rightarrow a_n = \frac{f^{(n)}(a)}{n!}
\)
```

**Taylor Series for** `\(f\(x\)\)`

**about** `\(x=a\)`

### Maclaurin Series

If we use `\(a = 0\)`

, so we are talking about the Taylor Series about x = 0, we call the series a **Maclaurin Series** for f(x):

### Examples

**__PLACEHOLDER__**

## Sources

- http://en.wikipedia.org/wiki/Brook_Taylor
- http://en.wikipedia.org/wiki/Colin_Maclaurin
- http://en.wikipedia.org/wiki/Taylor_series