1. Show that the Laplace transform of f is F(s) = r- Fi(s). Hint: Split the domain [0, 0] as [0, T]U [T, ∞0]; for the second integral, do a change of variable to make the integral look like the standard Laplace integral. %3D 1–e-

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**Transcription of Laplace Transform Educational Material**

---

**III. Periodic Function and Laplace Transform**

Let function \( f \) be periodic with period \( T > 0 \), that is, \( f(t) = f(t + T) \), for \( -\infty < t < \infty \). Define 

\[ 
F_1(s) = \int_0^T e^{-st} f(t) dt.
\]

1. **Show that the Laplace Transform of \( f \) is \( F(s) = \frac{1}{1 - e^{-sT}} F_1(s) \).**

   *Hint*: Split the domain \([0, \infty)\) as \([0, T] \cup [T, \infty)\); for the second integral, do a change of variable to make the integral look like the standard Laplace integral.

2. **Use the result to compute the Laplace transform of the half-wave rectified sine signal given by:**

   \[
   f(t) = 
   \begin{cases} 
   \sin \omega t & \text{if } \frac{2n\pi}{\omega} < t < \frac{(2n+1)\pi}{\omega} \\ 
   0 & \text{if } \frac{(2n+1)\pi}{\omega} < t < \frac{(2n+2)\pi}{\omega}, \quad n = 0, 1, 2, \ldots 
   \end{cases}
   \]

   *You may use:*

   \[
   \int e^{\alpha t} \sin(\omega t) dt = \frac{e^{\alpha t}}{\alpha^2 + \omega^2} (-\omega \cos(\omega t) + \alpha \sin(\omega t)).
   \]

---

This transcription outlines the steps to demonstrate and apply the Laplace transform for periodic functions and specifically for a half-wave rectified sine signal. It includes definitions, a mathematical hint for splitting domains, and the integral identities used to perform the calculations.
Transcribed Image Text:**Transcription of Laplace Transform Educational Material** --- **III. Periodic Function and Laplace Transform** Let function \( f \) be periodic with period \( T > 0 \), that is, \( f(t) = f(t + T) \), for \( -\infty < t < \infty \). Define \[ F_1(s) = \int_0^T e^{-st} f(t) dt. \] 1. **Show that the Laplace Transform of \( f \) is \( F(s) = \frac{1}{1 - e^{-sT}} F_1(s) \).** *Hint*: Split the domain \([0, \infty)\) as \([0, T] \cup [T, \infty)\); for the second integral, do a change of variable to make the integral look like the standard Laplace integral. 2. **Use the result to compute the Laplace transform of the half-wave rectified sine signal given by:** \[ f(t) = \begin{cases} \sin \omega t & \text{if } \frac{2n\pi}{\omega} < t < \frac{(2n+1)\pi}{\omega} \\ 0 & \text{if } \frac{(2n+1)\pi}{\omega} < t < \frac{(2n+2)\pi}{\omega}, \quad n = 0, 1, 2, \ldots \end{cases} \] *You may use:* \[ \int e^{\alpha t} \sin(\omega t) dt = \frac{e^{\alpha t}}{\alpha^2 + \omega^2} (-\omega \cos(\omega t) + \alpha \sin(\omega t)). \] --- This transcription outlines the steps to demonstrate and apply the Laplace transform for periodic functions and specifically for a half-wave rectified sine signal. It includes definitions, a mathematical hint for splitting domains, and the integral identities used to perform the calculations.
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