Math Notes

Maclaurin Series

Representing a function as a power series centered at x = 0

analysis series

What is the Maclaurin Series?

The Maclaurin series is a power series expansion of a function f(x)f(x) centered at x=0x = 0. It is a special case of the Taylor series with a=0a = 0.

Definition (Maclaurin Series)

If f(x)f(x) is infinitely differentiable at x=0x = 0:

f(x)=n=0f(n)(0)n!xn=f(0)+f(0)x+f(0)2!x2+f(0)3!x3+f(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f'''(0)}{3!}x^3 + \cdots

Common Expansions

exe^x

Since f(n)(x)=exf^{(n)}(x) = e^x, we have f(n)(0)=1f^{(n)}(0) = 1 for all nn:

ex=n=0xnn!=1+x+x22!+x33!+e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!} = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \cdots

sinx\sin x

Only odd-degree terms survive:

sinx=n=0(1)n(2n+1)!x2n+1=xx33!+x55!\sin x = \sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} x^{2n+1} = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \cdots

cosx\cos x

Only even-degree terms survive:

cosx=n=0(1)n(2n)!x2n=1x22!+x44!\cos x = \sum_{n=0}^{\infty} \frac{(-1)^n}{(2n)!} x^{2n} = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \cdots

11x\frac{1}{1-x} (Geometric series)

11x=n=0xn=1+x+x2+x3+(x<1)\frac{1}{1-x} = \sum_{n=0}^{\infty} x^n = 1 + x + x^2 + x^3 + \cdots \quad (|x| < 1)

Connection to Euler’s Formula

Substituting x=iθx = i\theta into the expansions of exe^x, sinx\sin x, and cosx\cos x yields:

eiθ=cosθ+isinθe^{i\theta} = \cos\theta + i\sin\theta

This is Euler’s formula.

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