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 at the centre is :
(a) (b)
(c) (d)
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.
2.
3.
4.
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'
The magnetic field at the centre of a coil of n turns, bent in the form of a square of side 2 l, carrying current i, is :
(a) (b)
(c) (d)
In a current-carrying long solenoid, the field produced does not depend upon:
1. | Number of turns per unit length | 2. | Current flowing |
3. | Radius of the solenoid | 4. | All of the above |
A circular coil A has a radius \(R\) and the current flowing through it is \(I.\) Another circular coil B has a radius \(2R\) and if \(2I\) is the current flowing through it, then the magnetic fields at the centre of the circular coil are in the ratio of (i.e. to ):
1. \(4:1\)
2. \(2:1\)
3. \(3:1\)
4. \(1:1\)
A straight wire of diameter 0.5 mm carrying a current of 1 A is replaced by another wire of 1 mm diameter carrying the same current. The strength of the magnetic field far away is :
(1) Twice the earlier value
(2) Half of the earlier value
(3) Quarter of its earlier value
(4) Unchanged
Which one of the following gives the value of the magnetic field according to Biot-Savart’s law?
1. | \(\frac{\mathrm{i} \Delta \mathrm{l} \sin (\theta)}{\mathrm{r}^2} \) | 2. | \(\frac{\mu_0}{4 \pi} \frac{\mathrm{i} \Delta \mathrm{l} \sin (\theta)}{\mathrm{r}} \) |
3. | \(\frac{\mu_0}{4 \pi} \frac{\mathrm{i} \Delta \mathrm{l} \sin (\theta)}{\mathrm{r}^2} \) | 4. | \(\frac{\mu_0}{4 \pi} \mathrm{i} \Delta \mathrm{l} \sin (\theta)\) |
A neutral point is obtained at the centre of a vertical circular coil carrying current. The angle between the plane of the coil and the magnetic meridian is :
a) 0 (b) 45°
(c) 60° (d) 90°