The total number of turns and the cross-sectional area of a solenoid are fixed. However, its length \(L\) is varied by adjusting the separation between the windings. The inductance of the solenoid will be proportional to:
| 1. | \(L\) | 2. | \(L^2\) |
| 3. | \(\dfrac{1}{L^2}\) | 4. | \(\dfrac{1}{L}\) |
| 1. | \(4~\text{J}\) | 2. | \(3~\text{J}\) |
| 3. | \(1~\text{J}\) | 4. | \(6~\text{J}\) |
| I. | The time elapsed before the current acquires half of its steady–state value. |
| II. | The energy stored in the magnetic field associated with the coil at an instant \(15\) ms after the circuit is switched on. |
| 1. | \(1~\text{H}\) | 2. | \(2~\text{H}\) |
| 3. | \(4~\text{H}\) | 4. | \(5~\text{H}\) |
| \(\mathrm{(A)}\) | The self-inductance of the coil depends on its geometry. |
| \(\mathrm{(B)}\) | Self-inductance does not depend on the permeability of the medium. |
| \(\mathrm{(C)}\) | Self-induced \(\mathrm{EMF }\) opposes any change in the current in a circuit. |
| \(\mathrm{(D)}\) | Self-inductance is electromagnetic analogue of mass in mechanics. |
| \(\mathrm{(E)}\) | Work needs to be done against self-induced \(\mathrm{EMF }\) in establishing the current. |
| 1. | \(\mathrm{(A), (B), (C), (E)}\) only |
| 2. | \(\mathrm{(A), (B), (C), (D)}\) only |
| 3. | \(\mathrm{(A), (C), (D), (E)}\) only |
| 4. | \(\mathrm{(B), (C), (D), (E)}\) only |