To finish a Laplace problem you must go back from $F(s)$ to $f(t)$. There is no new integral to learn: you rewrite $F$ as a sum of table entries, usually with partial fractions, and read the table backwards.
Idea clave
Por qué funciona
Ejemplo resuelto: Distinct linear factors
- Write $\frac{A}{s + 1} + \frac{B}{s + 3}$.
- Cover-up at $s = -1$: $A = \frac{-3 + 7}{-1 + 3} = 2$. At $s = -3$: $B = \frac{-9 + 7}{-3 + 1} = 1$.
- Invert each piece.
Respuesta: $2e^{-t} + e^{-3t}$
Ejemplo resuelto: Completing the square
- $s^{2} + 4s + 13 = (s + 2)^{2} + 9$.
- Rewrite the numerator around $s + 2$: $2s + 7 = 2(s + 2) + 3$.
- $F$ $= 2\cdot\frac{s + 2}{(s + 2)^{2} + 9}$ $+ \frac{3}{(s + 2)^{2} + 9}$, and the second piece is exactly $\mathcal{L}\{e^{-2t}\sin 3t\}$.
Respuesta: $e^{-2t}(2\cos 3t + \sin 3t)$
Ejemplo resuelto: A repeated factor
- $\mathcal{L}\{t^{2}e^{2t}\} = \frac{2!}{(s - 2)^{3}}$.
- So $\frac{5}{(s - 2)^{3}} = \frac{5}{2}\cdot\frac{2}{(s - 2)^{3}}$.
Respuesta: $\frac{5}{2}t^{2}e^{2t}$
Error común