Dulranga's Notes
Semester 3MathematicsDifferential EquationsLaplace TransformLaplace Derivations

Laplace Time scaling Property

Scaling the time variable compresses or expands the frequency spectrum:

Note
L{f(at)}=1aF(sa)for a>0\mathcal{L}\{f(at)\} = \frac{1}{a} F\left(\frac{s}{a}\right) \quad \text{for } a > 0

Derivation:

L{f(t)}=∫0∞e−stf(t) dt=F(s)L{f(at)}=∫0∞e−stf(at) dttake, u=atua=t(t→0,u→0)(t→∞,u→∞ if a>0)1a⋅du=dtL{f(at)}=∫0∞e−suaf(u)1a⋅duL{f(at)}=1a∫0∞e−(sa)⋅uf(u) duL{f(at)}=1a⋅F(sa)\begin{align*} \mathcal{L}\{f(t)\} &= \int_{0}^{\infty} e^{-st}f(t)\, dt = F(s)\\ \mathcal{L}\{f(at)\} &= \int_{0}^{\infty} e^{-st}f(at)\, dt \\ \text{take,}\, u &= at \\ \frac{u}{a} &= t \\ ({t \to 0, u \to 0}) \\ ({t \to \infty, u \to \infty \, \text{if a>0}}) \\ \frac{1}{a}\cdot du &= dt \\ \\ \mathcal{L}\{f(at)\} &= \int_{0}^{\infty} e^{-s\frac{u}{a}}f(u)\frac{1}{a}\cdot du \\ \mathcal{L}\{f(at)\} &= \frac{1}{a}\int_{0}^{\infty} e^{-\left(\frac{s}{a}\right)\cdot u}f(u)\, du \\ \mathcal{L}\{f(at)\} &= \frac{1}{a} \cdot F\left(\frac{s}{a}\right) \end{align*}
  • a>0a > 0 criteria is for the bounds to be preserved from 00 to ∞\infty
  • In real world, tt must be positive since time cannot be reversed.