1. | μ0i4R[1−2π] pointed into the page |
2. | μ0i4R pointed into the page |
3. | μ0i4R pointed away from the page |
4. | μ0i4R[1−2π] pointed away from the page |
1. | will turn towards right of direction of motion |
2. | will turn towards left of direction of motion |
3. | speed will decrease |
4. | speed will increase |
1. | 6.28×10−4 T | 2. | 6.28×10−2 T |
3. | 12.56×10−2 T | 4. | 12.56×10−4 T |
Statement I: | Biot-Savart's law gives us the expression for the magnetic field strength of an infinitesimal current element (Idl) of a current-carrying conductor only. |
Statement II: | Biot-Savart's law is analogous to Coulomb's inverse square law of charge q, with the former being related to the field produced by a scalar source, (Idl) while the latter being produced by a vector source, q. |
1. | Statement I is incorrect but Statement II is correct. |
2. | Both Statement I and Statement II are correct. |
3. | Both Statement I and Statement II are incorrect. |
4. | Statement I is correct but Statement II is incorrect. |
1. | A linearly decreasing function of distance upto the boundary of the wire and then a linearly increasing one for the outside region. |
2. | Uniform and remains constant for both regions. |
3. | A linearly increasing function of distance upto the boundary of the wire and then a linearly decreasing one for the outside region. |
4. | A linearly increasing function of distance r upto the boundary of the wire and then decreasing one with 1/r dependence for the outside region. |
The ratio of the radii of two circular coils is 1:2. The ratio of currents in the respective coils such that the same magnetic moment is produced at the centre of each coil is:
1. | 4:1 | 2. | 2:1 |
3. | 1:2 | 4. | 1:4 |
1. | a parabolic path |
2. | the original path |
3. | a helical path |
4. | a circular path |