Consider the function $f\left(\frac{t - b}{a}\right)$. We want want to calculate its Laplace transform. There are two approaches:
Firstly,
- let $g(t) = f\left(\frac ta\right)$.
- Then $\mathcal{L}\left\{f\left(\frac{t-b}{a}\right)\right\} = \mathcal{L}\left\{g(t - b)\right\} = e^{-bs}G(s)$ and $G(s) = \mathcal{L}\{g(t)\} = \mathcal{L}\left\{f\left(\frac ta\right)\right\} = |a|F(as)$.
- Therefore $\mathcal{L}\left\{f\left(\frac{t - b}{a}\right)\right\} = |a|e^{-bs}F(as).$
Secondly,
- let $h(t) = f\left(\frac{t - b}{a}\right)$.
- Then $\mathcal{L}\left\{f\left(\frac{t-b}{a}\right)\right\} = \mathcal{L}\left\{h\left(\frac ta\right)\right\} = |a|H(as)$ and $H(s) = \mathcal{L}\{h(t)\} = \mathcal{L}\left\{f\left(\frac{t - b}{a}\right)\right\} = e^{-\left(\frac ba\right) s}F(s)$.
- Therefore $\mathcal{L}\left\{f\left(\frac{t - b}{a}\right)\right\} = |a|e^{-bs}F(as).$
So far so good. However, let $f(t) = e^t$. Then $$F(s) = \frac{1}{s - 1}$$ and $$\mathcal{L}\left\{f\left(\frac{t - b}{a}\right)\right\} = \frac{ae^{-\left(\frac ba\right)s}}{as - 1}$$ from Wolfram Alpha.
The problem comes from the fact that we introduce new data by shifting, i.e., the function is not zero for $t < 0$. What can we do then? Can we not use the time delay property?
What about the Fourier transform? The arguments above are valid for the Fourier transform for $s = j\omega$ and you do not have the requirement of $f(t < 0) = 0$ when applying the shift property. But when you set $f(t) = \cos(t)$ you get: $$\mathcal{F}\left\{f\left(\frac{t - b}{a}\right)\right\}\bigg\vert_{\omega \ge 0,\ a > 0} = \frac{1}{2}e^{\left(\frac ba\right)j\omega}\delta(\omega - 1/a)$$ So it looks like it should be $e^{-\left(\frac ba\right)s}$ instead of $e^{-bs}$. But where have I made a mistake?