An electric dipole of the moment $\overrightarrow{P}$ is released in a uniform electric field $\overrightarrow{E}$ from the position of maximum torque. The angular speed of the dipole when $\overrightarrow{P}$ becomes parallel to $\overrightarrow{E}$ will be [l = moment of inertia of dipole]

1.  $\sqrt{\frac{2PE}{I}}$

2.  $\sqrt{\frac{PE}{I}}$

3.  $\sqrt{\frac{4PE}{I}}$

4.  $\sqrt{\frac{2I}{PE}}$

A charge Q is given to a conducting sphere of radius R. Now if a charge -Q is placed, as shown, at a distance r from the center, then the magnitude of the force of attraction between charges is

1.  $\frac{1}{4{\mathrm{\pi \epsilon }}_0}\frac{Q^2}{r^2}$

2.  <$\frac{1}{4{\mathrm{\pi \epsilon }}_0}\frac{Q^2}{r^2}$

3.  >$\frac{1}{4{\mathrm{\pi \epsilon }}_0}\frac{Q^2}{r^2}$

4.  $\frac{1}{4{\mathrm{\pi \epsilon }}_0}\frac{Q^2}{{\left(r-R\right)}^2}$

If the electric flux entering and leaving a closed surface are respectively of magnitude ${\varphi }_1<mspace\; width="1em"></mspace>\mathrm{and}<mspace\; width="1em"></mspace>{\varphi }_2$, then the electric charge inside the surface will be

1.  ${\epsilon }_0\left({\varphi }_2-{\varphi }_1\right)$

2.  $\left({\varphi }_1-{\varphi }_2\right){\mathrm{/2\epsilon }}_0$

3.  ${\epsilon }_0\left({\varphi }_2+{\varphi }_1\right)$

4.  $\frac{{\varphi }_2-{\varphi }_1}{{\epsilon }_0}$

Electric field at an axial point of short dipole is  $\overrightarrow{E_1}$. If the electric field at the equatorial point of same dipole is $\overrightarrow{E_2}$, then which of the following is correct?

1.  $\overrightarrow{E_1}$ . $\overrightarrow{E_2}$ < 0

2.  $\overrightarrow{E_1}$ . $\overrightarrow{E_2}$ > 0

3.  $\overrightarrow{E_1}$ . $\overrightarrow{E_2}$ = 0

4.  $\overrightarrow{E_1}$ . $\overrightarrow{E_2}$ = $\overrightarrow{0}$

A long thin rod is charged such that charge per unit length of the rod is $\lambda$. The rod is inserted into a hollow spherical surface of radius R. Maximum electric flux coming out the surface is

1.  $\frac{\lambda R}{{\epsilon }_0}$

2.  $\frac{2\lambda \pi R^2}{{\epsilon }_0}$

3.  $\frac{2\lambda R}{{\epsilon }_0}$

4.  $\frac{2\lambda R^2}{{\epsilon }_0}$

Two charges q and 4q are separated by a distance r. The neutral point(in between the line joining the charges) is at a distance:

1.  $\frac{r}{3}\mathrm{from}<mspace\; width="1em"></mspace>q$

2.  $\frac{2r}{3}\mathrm{from}<mspace\; width="1em"></mspace>q$

3.  $2r<mspace\; width="1em"></mspace>\mathrm{from}<mspace\; width="1em"></mspace>q$

4.  $r<mspace\; width="1em"></mspace>\mathrm{from}<mspace\; width="1em"></mspace>4q$

A positron and a proton are projected normally into a uniform electric field with equal kinetic energy. The trajectory followed by them are:

The distance between two point charges is increased by 10%. The force of interaction

1.  Increases by 10%

2.  Decreases by 10%

3.  Decreases by 17%

4.  Increases by 17%

Cm is the SI unit of 

1.  Electric flux

2.  Electric potential

3.  Electric dipole moment

4.  Electric field intensity

A solid sphere of radius R has a uniform distribution of electric charge in its volume. At a distance x from its center (x<R), the electric field is directly proportional to

1.  $\frac{1}{x^2}$

2.  $\frac{1}{x}$

3.  x

4.  $x^2$