In a coil of resistance 10 Ω, the induced current developed by changing magnetic flux through it is shown in the figure as a function of time. The magnitude of change in flux through the coil in Weber is:
1. 2
2. 6
3. 4
4. 8
A coil of resistance 400 Ω is placed in a magnetic field. The magnetic flux ϕ (Wb) linked with the coil varies with time t (s) as ϕ=50t2+4. The current in the coil at t=2 s is:
1. 0.5 A
2. 0.1 A
3. 2 A
4. 1 A
1. | increases continuously. |
2. | decreases continuously. |
3. | first increases and then decreases. |
4. | remains constant throughout. |
1. | 5 V | 2. | 0.5 V |
3. | 0.05 V | 4. | 5×10−4 V |
The figure shows planar loops of different shapes moving out of or into a region of a magnetic field which is directed normally to the plane of the loop away from the reader. Then:
1. | for the rectangular loop abcd, the induced current is clockwise. |
2. | for the triangular loop abc, the induced current is clockwise. |
3. | for the irregularly shaped loop abcd, the induced current is anti-clockwise. |
4. | none of these. |
A conducting circular loop is placed in a uniform magnetic field, B=0.025 T with its plane perpendicular to the loop. The radius of the loop is made to shrink at a constant rate of 1 mm s−1. The induced emf, when the radius is 2 cm, is:
1. 2π μV
2. π μV
3. π2 μV
4. 2 μV
1. | twice per revolution. |
2. | four times per revolution. |
3. | six times per revolution. |
4. | once per revolution. |