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) $ |
The figure shows an opamp circuit with a 5.1 V Zener diode in the feedback loop. The opamp runs from \( \pm 15 \, {V} \) supplies. If a \( +1 \, {V} \) signal is applied at the input, the output voltage (rounded off to one decimal place) is:

A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is:
