$$ \text { Match List - I with List - II. } $$
| $$ \text { List - I } $$ |
$$ \text { List - II } $$ |
||
|---|---|---|---|
| A. | $$ \sin ^2 \omega t $$ |
I. | Periodic with time period $T=\frac{\pi}{\omega}$ but not simple harmonic motion (SHM) |
| B. | $$ \sin ^3(2 \omega t) $$ |
II. | Periodic with time period $T=\frac{2 \pi}{\omega}$ but Not SHM |
| C. | $$ \sin (\omega t)+\cos (\pi \omega t) $$ |
III. | Periodic with time period $T=\frac{\pi}{\omega}$ and SHM |
| D. | $$ \cos \omega t+\cos 2 \omega t $$ |
IV. | Non-periodic |
Choose the correct answer from the options given below :
A metal rod of length $L$ rotates about one end at origin with a uniform angular velocity $\omega$. The magnetic field radially falls off as $B(\mathrm{r})=B_{\mathrm{o}} \mathrm{e}^{-\lambda r} ; \lambda$ being a positive constant. The emf induced (neglecting the centripetal force on electrons in the rod) is :
Under steady state condition the potential difference across the capacitor in the circuit is $\_\_\_\_$ V.
A particle of charge $q$ and mass $m$ is projected from origin with an initial velocity $\vec{v}=\left(\frac{v_0}{\sqrt{2}} \hat{x}+\frac{v_0}{\sqrt{2}} \hat{y}\right)$. There exists a uniform magnetic field $\vec{B}=B_0 \hat{z}$ and a space varying electric field $\vec{E}=E_{\mathrm{o}} \mathrm{e}^{-\lambda x} \hat{x}$ within the region $0 \leqslant x \leqslant L$. After travelling a distance such that $x$-coordinate has changed from $x=0$ to $x=L$, the change in the kinetic energy is $\_\_\_\_$ .
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