1. | \(9~\mathrm{\mu F}\) | 2. | \(2~\mathrm{\mu F}\) |
3. | \(3~\mathrm{\mu F}\) | 4. | \(6~\mathrm{\mu F}\) |
1. | \(30\) \(\mu\)F | 2. | \(15\) \(\mu\)F |
3. | \(25\) \(\mu\)F | 4. | \(20\) \(\mu\)F |
1. | \(\frac{rV}{R^2}\) | 2. | \(\frac{R^2V}{r^3}\) |
3. | \(\frac{RV}{r^2}\) | 4. | \(\frac{V}{r}\) |
1. | dependent on the material property of the sphere |
2. | more on bigger sphere |
3. | more on smaller sphere |
4. | equal on both the spheres |
1. | \(180^\circ\) | 2. | \(0^\circ\) |
3. | \(45^\circ\) | 4. | \(90^\circ\) |
1. | \(1.5\times 10^{-6}~\text{J}\) | 2. | \(4.5\times 10^{-6}~\text{J}\) |
3. | \(3.25\times 10^{-6}~\text{J}\) | 4. | \(2.25\times 10^{-6}~\text{J}\) |
A hollow metal sphere of radius \(R\) is given \(+Q\) charges to its outer surface. The electric potential at a distance \(\frac{R}{3}\) from the centre of the sphere will be:
1. | \(\frac{1}{4\pi \varepsilon_0}\frac{Q}{9R}\) | 2. | \(\frac{3}{4\pi \varepsilon_0}\frac{Q}{R}\) |
3. | \(\frac{1}{4\pi \varepsilon_0}\frac{Q}{3R}\) | 4. | \(\frac{1}{4\pi \varepsilon_0}\frac{Q}{R}\) |
Three capacitors, each of capacitance \(0.3~\mu \text{F}\) are connected in parallel. This combination is connected with another capacitor of capacitance \(0.1~\mu \text{F}\) in series. Then the equivalent capacitance of the combination is:
1. | \(0.9~\mu\text{F}\) | 2. | \(0.09~\mu\text{F}\) |
3. | \(0.1~\mu\text{F}\) | 4. | \(0.01~\mu\text{F}\) |
When a particle with charge \(+q\) is thrown with an initial velocity \(v\) towards another stationary change \(+Q,\) it is repelled back after reaching the nearest distance \(r\) from \(+Q.\) The closest distance that it can reach if it is thrown with initial velocity \(2v,\) is:
1. | \(\frac{r}{4}\) | 2. | \(\frac{r}{2}\) |
3. | \(\frac{r}{16}\) | 4. | \(\frac{r}{8}\) |