Step 1: Inverse Fourier transform.
The signal \(x(t)\) is obtained from the given \(X(\omega)\):
\[
x(t) = \frac{1}{2\pi} \int_{-W_0}^{W_0} e^{j\omega t} d\omega.
\]
Step 2: Evaluate integral.
\[
x(t) = \frac{1}{2\pi} \left[\frac{e^{j\omega t}}{jt}\right]_{-W_0}^{W_0}
= \frac{1}{2\pi jt} \left( e^{jW_0 t} - e^{-jW_0 t} \right).
\]
\[
x(t) = \frac{1}{\pi t} \sin(W_0 t).
\]
Step 3: Value at \(t=0\).
By L'Hospital's rule:
\[
x(0) = \lim_{t \to 0} \frac{\sin(W_0 t)}{\pi t} = \frac{W_0}{\pi}.
\]
Thus, as \(W_0\) increases, \(x(0)\) increases, not decreases. Hence option (B) is false.
Step 4: Asymptotic behavior.
As \(W_0 \to \infty\):
\[
x(t) = \frac{\sin(W_0 t)}{\pi t} \to \delta(t),
\]
since the sinc pulse becomes narrower and taller, converging to the delta function.
This matches option (A).
Step 5: Check at \(t=\tfrac{\pi}{2W_0}\).
\[
x\left(\tfrac{\pi}{2W_0}\right) = \frac{\sin(\pi/2)}{\pi \cdot (\pi/(2W_0))}
= \frac{2W_0}{\pi^2},
\]
which is not equal to \(\pm \tfrac{1}{\pi}\). So both options (C) and (D) are incorrect.
Final Answer: \[ \boxed{x(t) \to \delta(t) \;\; \text{as} \;\; W_0 \to \infty} \]
Let \( X(\omega) \) be the Fourier transform of the signal
\( x(t) = e^{-4t}\cos(t), \; -\infty < t < \infty \).
The value of the derivative of \( X(\omega) \) at \( \omega = 0 \) is _____________
(rounded off to 1 decimal place).
Given an open-loop transfer function \(GH = \frac{100}{s}(s+100)\) for a unity feedback system with a unit step input \(r(t)=u(t)\), determine the rise time \(t_r\).
Consider a linear time-invariant system represented by the state-space equation: \[ \dot{x} = \begin{bmatrix} a & b -a & 0 \end{bmatrix} x + \begin{bmatrix} 1 0 \end{bmatrix} u \] The closed-loop poles of the system are located at \(-2 \pm j3\). The value of the parameter \(b\) is: