Laplace transforms of two time-scaled rectangular pulses
Find the Laplace transforms of x(t) = u(t) − u(t − a) and x(2t) = u(2t) − u(2t − a).
We have already found the Laplace transform of u(t), which is 1/s, σ > 0. Using the linearity and time-shifting properties,
u(t)-u(t-a) \stackrel{\mathcal{L}}{\longleftrightarrow} \frac{1-e^{-a s}}{s} , all σ.
Now, using the time scaling property,
\mathrm{u}(2 t)-\mathrm{u}(2 t-a) \stackrel{\mathcal{L}}{\longleftrightarrow} \frac{1}{2} \frac{1-e^{-a s / 2}}{s / 2}=\frac{1-e^{-a s / 2}}{s}, all σ.
This result is sensible when we consider that u(2t) = u(t) and u(2t − a) = u(2(t − a/2)) = u(t − a/2).