Esta lección aún no está traducida. Por ahora se muestra en inglés; la versión en español está en camino.
Not every function is a geometric series in disguise. Taylor series give a recipe for any function you can differentiate again and again: the coefficients come from its higher derivatives at the center, using term-by-term differentiation.
💡 Por qué funciona
Suppose $$\begin{aligned} f(x) = c_0 &+ c_1(x - a) + c_2(x - a)^{2} \\ &+ c_3(x - a)^{3} + \cdots. \end{aligned}$$ At $x = a$ every term but the first vanishes, so $c_0 = f(a)$. Differentiate once: $$\begin{aligned} f'(x) = c_1 &+ 2c_2(x - a) \\ &+ 3c_3(x - a)^{2} + \cdots, \end{aligned}$$ so $c_1 = f'(a)$. Again: $f''(x) = 2c_2 + 3\cdot 2\,c_3(x - a) + \cdots$, so $c_2 = \frac{f''(a)}{2}$. After $n$ differentiations the term $c_n(x - a)^{n}$ has become $n!\,c_n$, so
$$c_n = \frac{f^{(n)}(a)}{n!}.$$
🔑 Idea clave
The Taylor series of $f$ at $a$ is $\sum_{n=0}^{\infty}\frac{f^{(n)}(a)}{n!}(x - a)^{n}$; at $a = 0$ it is called a Maclaurin series. The partial sum $T_n(x)$ is the Taylor polynomial of degree $n$: the polynomial that matches $f$ and its first $n$ derivatives at $a$.
✏️ Ejemplo resuelto: The exponential
Find the Maclaurin series of $e^{x}$.
Every derivative of $e^{x}$ is $e^{x}$, and $e^{0} = 1$.
So $c_n = \frac{1}{n!}$: $e^{x} = 1 + x + \frac{x^{2}}{2!} + \frac{x^{3}}{3!} + \cdots = \sum\frac{x^{n}}{n!}$.
The ratio test gives $R = \infty$, and (see the next topic) the series equals $e^{x}$ for every $x$.
Respuesta: $\sum\frac{x^{n}}{n!}$
⚠️ Error común
Forgetting the $n!$. Writing $e^{x} \approx 1 + x + x^{2} + x^{3}$ uses $f^{(n)}(0)$ as the coefficient. At $x = 1$ that gives 4 instead of about $2.67$ (and $e \approx 2.718$). The factorial undoes the $n!$ that appears when you differentiate $(x - a)^{n}$ $n$ times. Check by differentiating your polynomial at the center: you should get back $f^{(n)}(a)$.
Taylor polynomials of $\sin x$ at 0. Each new term bends the polynomial to follow the sine wave farther from the center. Move the probe point to see the error shrink.
✏️ Ejemplo resuelto: Away from 0
Find the Taylor polynomial $T_2$ of $\sqrt{x}$ centered at 4.
$f(4) = 2$; $f'(x) = \frac{1}{2\sqrt{x}}$, so $f'(4) = \frac{1}{4}$; $f''(x) = -\frac{1}{4x^{3/2}}$, so $f''(4) = -\frac{1}{32}$.