To solve this problem, we need to analyze the Laplace transform of the step function \( u(t) \) and its Region of Convergence (ROC).
- Laplace Transform of \( u(t) \): The step function \( u(t) \) is defined as:
\[ u(t) = \begin{cases} 0 & t < 0 \\ 1 & t \geq 0 \end{cases} \]
The Laplace transform of \( u(t) \) is given by:
\[ \mathcal{L}\{u(t)\} = \frac{1}{s} \]
- Region of Convergence (ROC): The ROC for the Laplace transform of a function is the range of values for which the Laplace transform converges. For \( u(t) \), the Laplace transform \( \frac{1}{s} \) converges when the real part of \( s \) is greater than 0, i.e., \( \sigma > 0 \), where \( s = \sigma + j\omega \) and \( \sigma \) is the real part.
The Laplace transform of \( u(t) \) is:
\[ \mathcal{L}\{u(t)\} = \frac{1}{s} \]
The ROC for this Laplace transform is \( \sigma > 0 \), as the integral converges for positive real parts of \( s \). This is because \( u(t) \) is a causal function that starts at \( t = 0 \) and its Laplace transform converges for \( \sigma > 0 \).
The Laplace transform of \( u(t) \) and its ROC is \( \frac{1}{s}, \, \sigma > 0 \).
Signals and their Fourier Transforms are given in the table below. Match LIST-I with LIST-II and choose the correct answer.
| LIST-I | LIST-II |
|---|---|
| A. \( e^{-at}u(t), a>0 \) | I. \( \pi[\delta(\omega - \omega_0) + \delta(\omega + \omega_0)] \) |
| B. \( \cos \omega_0 t \) | II. \( \frac{1}{j\omega + a} \) |
| C. \( \sin \omega_0 t \) | III. \( \frac{1}{(j\omega + a)^2} \) |
| D. \( te^{-at}u(t), a>0 \) | IV. \( -j\pi[\delta(\omega - \omega_0) - \delta(\omega + \omega_0)] \) |