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: \[ \boxed{x(t) \to \delta(t) \;\; \text{as} \;\; W_0 \to \infty} \]
List I (Signal) | List II (Fourier Transform) | ||
---|---|---|---|
A | $ x(t-t_0)$ | I | $ \frac{dx(\omega)}{{d\omega}}$ |
B | $ e^{j \omega_0 t} x(t) $ | II | $ e^{j \omega t_0} X(\omega) $ |
C | $ \frac{dx(t)}{{dt}}$ | III | $ x(\omega-\omega_0)$ |
D | $(-jt)x(t) $ | IV | $j\omega X(\omega) $ |
In the Wheatstone bridge shown below, the sensitivity of the bridge in terms of change in balancing voltage \( E \) for unit change in the resistance \( R \), in V/Ω, is __________ (round off to two decimal places).
The relationship between two variables \( x \) and \( y \) is given by \( x + py + q = 0 \) and is shown in the figure. Find the values of \( p \) and \( q \). Note: The figure shown is representative.