Figure shows three circular arcs, each of radius R and total charge as indicated. The net electric potential at the centre of curvature is –

1. $\frac{\mathrm{Q}}{2{\mathrm{\pi \epsilon }}_0\mathrm{R}}$                               

2. $\frac{\mathrm{Q}}{4{\mathrm{\pi \epsilon }}_0\mathrm{R}}$

3. $\frac{2\mathrm{Q}}{{\mathrm{\pi \epsilon }}_0\mathrm{R}}$                                 

4. $\frac{\mathrm{Q}}{{\mathrm{\pi \epsilon }}_0\mathrm{R}}$

Two metallic bodies separated by a distance of 20 cm, are given equal and opposite charges of the magnitude of 0.88$\mu$C. The component of the electric field along the line AB, between the plates, varies as, ${\mathrm{E}}_{\mathrm{x}}=(3{\mathrm{x}}^2 + 0.4) \mathrm{N}/\mathrm{C}$ where x (in meters) is the distance from one body towards the other body as shown.

1. The capacitance of the system is 10F 

2. The capacitance of the system is 20F 

3. The potential difference between A and C is 0.088 volt 

4. The potential difference between A and C is cannot be determined from the given data 

Two concentric, thin metallic spheres of radii ${\mathrm{R}}_1$ and ${\mathrm{R}}_2$ $\left({\mathrm{R}}_1 > {\mathrm{R}}_2\right)$ bear changes ${\mathrm{Q}}_1$ and ${\mathrm{Q}}_2$ respectively. Then the potential at distance r between ${\mathrm{R}}_1$ and ${\mathrm{R}}_2$ will be $\left(\mathrm{k}=\frac{1}{4{\mathrm{\pi \epsilon }}_0}\right)$

1.  $\mathrm{k} \left(\frac{{\mathrm{Q}}_1+{\mathrm{Q}}_2}{\mathrm{r}}\right)$                       

2.  $\mathrm{k} \left(\frac{{\mathrm{Q}}_1}{\mathrm{r}}+\frac{{\mathrm{Q}}_2}{{\mathrm{R}}_2}\right)$

3.  $\mathrm{k} \left(\frac{{\mathrm{Q}}_2}{\mathrm{r}}+\frac{{\mathrm{Q}}_1}{{\mathrm{R}}_1}\right)$                     

4.  $\mathrm{k} \left(\frac{{\mathrm{Q}}_1}{{\mathrm{R}}_1}+\frac{{\mathrm{Q}}_1}{{\mathrm{R}}_2}\right)$

Figure shows an electric line of force which curves along a circular arc.

The magnitude of electric field intensity is same at all points on this curve and is equal to E. If the potential at A is V, then the potential at B is –

1. $\mathrm{V}-\mathrm{ER\theta }$                             

2. $\mathrm{V}-\mathrm{E}2\mathrm{R} \sin \frac{\mathrm{\theta }}{2}$

3. $\mathrm{V}+\mathrm{ER\theta }$                             

4. $\mathrm{V}+2\mathrm{ER} \sin \frac{\mathrm{\theta }}{2}$

In the figure, two conducting concentric spherical shells are shown.

If the electric potential at the centre is 20V and the electric potential at the surface of outer shell is 5V, then the potential at the surface of inner shell is –

1.  5V                   

2.  15V 

3.  20V                 

3.  cannot be determined as radii are not given

At the mid point of a line joining an electron and a proton, the values of E and V will be.

1. $\mathrm{E}=0, \mathrm{V}\ne 0$                   

2. $\mathrm{E}\ne 0, \mathrm{V}=0$

3. $\mathrm{E}\ne 0, \mathrm{V}\ne 0$                   

4. $\mathrm{E}=0, \mathrm{V}=0$

Two point charge of $8 \mathrm{\mu C}$ and $12 \mathrm{\mu C}$ are kept in air at a distance of 10 cm from each other. The work required to change the distance between them to 6 cm will be.

1.  $5.8 \mathrm{J}$                       

2.  $4.8 \mathrm{J}$

3.  $3.8 \mathrm{J}$                       

4.  $2.8 \mathrm{J}$

Maximum charge stored on a metal sphere of radius $15$ cm may be $7.5 \mu \mathrm{C}$. The potential energy of the sphere in this case is :

1.  $9.67 \mathrm{J}$                   

2.  $0.25 \mathrm{J}$ 

3.  $3.25 \mathrm{J}$                    

4.  $1.69 \mathrm{J}$

Four identical particles each of mass m and charge q are kept at the four corners of a square of length L. The final velocity of these particles after setting them free will be.

1. ${\left[\frac{{\mathrm{Kq}}^2}{\mathrm{mL}}\left(5.4\right)\right]}^{1/2}$                           

2. ${\left[\frac{{\mathrm{Kq}}^2}{\mathrm{mL}}\left(1.35\right)\right]}^{1/2}$

3. ${\left[\frac{{\mathrm{Kq}}^2}{\mathrm{mL}}\left(2.7\right)\right]}^{1/2}$                           

4. Zero

A charge $+\mathrm{Q}$ is uniformly distributed over a thin ring of radius $\mathrm{R}$, velocity of an electron at the moment it passes through the centre $\mathrm{O}$ of the ring, if the electron was initially at rest at a point $\mathrm{A}$ which is very far away from the centre and on the axis of the ring is

1. $\sqrt{\frac{2\mathrm{kQe}}{\mathrm{mR}}}$                     

2. $\sqrt{\frac{\mathrm{kQe}}{\mathrm{m}}}$

3. $\sqrt{\frac{\mathrm{kme}}{\mathrm{QR}}}$                       

4. $\sqrt{\frac{\mathrm{kQe}}{\mathrm{mR}}}$