L'Hôpital's rule evaluates indeterminate limits of the form $\frac{0}{0}$ or $\frac{\infty}{\infty}$ by differentiating numerator and denominator separately.
If $\displaystyle\lim_{x\to a} f(x) = \lim_{x\to a} g(x) = 0$ (or $\pm\infty$), and $g'(x) \ne 0$ near $a$, then:
$$\lim_{x\to a} \frac{f(x)}{g(x)} = \lim_{x\to a} \frac{f'(x)}{g'(x)}$$
The rule may be applied repeatedly if the result remains indeterminate.
The Maclaurin series is a Taylor series expanded about $x=0$. It expresses a function as an infinite polynomial.
$e^x = 1 + x + \dfrac{x^2}{2!} + \dfrac{x^3}{3!} + \cdots$
$\sin x = x - \dfrac{x^3}{3!} + \dfrac{x^5}{5!} - \cdots$
$\cos x = 1 - \dfrac{x^2}{2!} + \dfrac{x^4}{4!} - \cdots$
$\ln(1+x) = x - \dfrac{x^2}{2} + \dfrac{x^3}{3} - \dfrac{x^4}{4} + \cdots$ ($|x| \le 1$, $x\ne -1$)
$(1+x)^n = 1 + nx + \dfrac{n(n-1)}{2!}x^2 + \dfrac{n(n-1)(n-2)}{3!}x^3 + \cdots$
A differential equation (DE) relates a function to its derivatives. The general solution contains an arbitrary constant $C$; a particular solution uses an initial condition to fix $C$.
A DE of the form $\dfrac{dy}{dx} = f(x)g(y)$ is separable: rearrange to $\dfrac{1}{g(y)}dy = f(x)dx$ and integrate both sides.
For $\dfrac{dy}{dx} + P(x)y = Q(x)$, the integrating factor is $\mu(x) = e^{\int P(x)\,dx}$. Multiply both sides by $\mu$; the LHS becomes $\dfrac{d}{dx}[\mu y]$, then integrate.
$$\int u\,\frac{dv}{dx}\,dx = uv - \int v\,\frac{du}{dx}\,dx$$
LIATE rule for choosing $u$: Logarithm, Inverse trig, Algebraic, Trigonometric, Exponential (choose $u$ from the earlier category).
$\frac{0}{0}$ form. Apply once: $\displaystyle\lim_{x\to 0}\frac{e^x-1}{2x}$ — still $\frac{0}{0}$. Apply again: $\displaystyle\lim_{x\to 0}\frac{e^x}{2} = \frac{1}{2}$.
Let $u = x$, $dv = e^x dx$. Then $du = dx$, $v = e^x$.
$\displaystyle\int xe^x\,dx = xe^x - \int e^x\,dx = xe^x - e^x + C = e^x(x-1) + C$
Integrating factor: $\mu = e^{\int 1/x\,dx} = e^{\ln x} = x$.
Multiply: $\dfrac{d}{dx}(xy) = x^3$. Integrate: $xy = \dfrac{x^4}{4} + C$. So $y = \dfrac{x^3}{4} + \dfrac{C}{x}$.