1. | 3.33×10−9 Tesla |
2. | 1.11×10−4 Tesla |
3. | 3×10−3 Tesla |
4. | 9×10−2 Tesla |
1. | At a distance d2 from any of the wires in any plane. |
2. | At a distance d3 from any of the wires in the horizontal plane. |
3. | Anywhere on the circumference of a vertical circle of radius d and centre halfway between the wires. |
4. | At points halfway between the wires in the horizontal plane. |
A circular coil of radius R carries an electric current. The magnetic field due to the coil at a point on the axis of the coil located at a distance r from the centre of the coil, such that r >> R, varies as
1. 1r
2. 1r3/2
3. 1r2
4. 1r3
The magnetic induction due to an infinitely long straight wire carrying a current i at a distance r from the wire is given by:
1. B=μ04π2ir
2. B=μ04πr2i
3. B=4πμ02ir
4. B=4πμ0r2i
The magnetic induction at the centre O in the figure shown is:
1. μ0i4(1R1-1R2) 2. μ0i4(1R1+1R2)
3. μ0i 4(R1-R2) 4. μ0i4(R1+R2)
In the figure shown, the magnetic induction at the centre of the arc due to the current in portion AB will be
1. μ0ir 3. μ0i4r
2. μ0i2r 4. Zero
Two concentric circular coils of ten turns each are situated in the same plane. Their radii are 20 and 40 cm and they carry respectively 0.2 and 0.3 ampere current in opposite direction. The magnetic field in weber/m2 at the centre is :
1. 354μ0
2. μ080
3. 780μ0
4. 54μ0
In the figure shown below there are two semicircles of radius r1 and r2 in which a current i is flowing. The magnetic induction at the centre of O will be:
1. | μ0ir(r1+r2) | 2. | μ0i4[r1+r2r1r2] |
3. | μ0i4(r1−r2) | 4. | μ0i4[r2−r1r1r2] |
The direction of magnetic lines of forces close to a straight conductor carrying current will be:
1. along the length of the conductor.
2. radially outward.
3. circular in a plane perpendicular to the conductor.
4. helical.
A vertical wire kept in Z-X plane carries a current from Q to P (see figure). The magnetic field due to current-carrying wire will have the direction at the origin O along :
1. OX
2. OX'
3. OY
4. OY'