A charged particle with charge $q$ and mass $m$ starts with an initial kinetic energy $K$ at the centre of a uniformly charged spherical region of total charge $Q$ and radius $R$. Charges $q$ and $Q$ have opposite signs. The spherically charged region is not free to move and kinetic energy $K$ is just sufficient for the charge particle to reach boundary of the spherical charge. How much time does it take the particle to reach the boundary of the region?
$\sqrt[\pi ]{{\frac{{4\pi {\varepsilon _o}m{R^3}}}{{qQ}}}}$
$\sqrt[{\frac{\pi }{2}}]{{\frac{{4\pi {\varepsilon _o}m{R^3}}}{{qQ}}}}$
$\sqrt[{\frac{\pi }{4}}]{{\frac{{4\pi {\varepsilon _o}m{R^3}}}{{qQ}}}}$
None of the above.
In the circuit, shown in the figure, the effective capacitance between $A$ and $B$ is......$\mu F$
A capacitor $C = 100$ $ \mu F$ is connected to three resistors each of resistance $1$ $kW$ and a battery of emf $9$ $V$. The switch $S $ has been closed for long time so as to charge the capacitor. When switch $S $ is opened, the capacitor discharges with time constant.....$ms$
The force on a charge situated on the axis of a dipole is $F$. If the charge is shifted to double the distance, the new force will be
Four point $+ve$ charges of same magnitude $(Q)$ are placed at four corners of a rigid square frame in $xy$ plane as shown in figure. The plane of the frame is perpendicular to $z-$ axis. If a $-ve$ point charges is placed at a distance $z$ away from the above frame $(z << L)$ then
A parallel plate capacitor has a uniform electric field $E$ in the space between the plates. If the distance between the plates is $d$ and area of each plate is $A$ , the energy stored in the capacitor is