A current \(i\) ampere flows in a circular arc of wire whose radius is \(R,\) which subtend an angle radian at its centre. The magnetic induction \(B\) at the centre is:
1. \(\frac{\mu_0i}{R}\)
2. \(\frac{\mu_0i}{2R}\)
3. \(\frac{2\mu_0i}{R}\)
4. \(\frac{3\mu_0i}{8R}\)
A straight section PQ of a circuit lies along the X-axis from x= to x= and carries a steady current i. The magnetic field due to the section PQ at a point X = + a will be:
1. Proportional to a 2. Proportional to
3. Proportional to 4. Zero
1. | \(3.33\times 10^{-9}\) Tesla |
2. | \(1.11\times 10^{-4}\) Tesla |
3. | \(3\times 10^{-3}\) Tesla |
4. | \(9\times 10^{-2}\) Tesla |
1. | At a distance \(\frac{d}{2}\) from any of the wires in any plane. |
2. | At a distance \(\frac{d}{3}\) 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.
2.
3.
4.
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. \( B =\frac{\mu_0}{4 \pi} \frac{2 i}{r} \)
2. \(B =\frac{\mu_0}{4 \pi} \frac{r}{2 i} \)
3. \(B =\frac{4 \pi}{\mu_0} \frac{2 i}{r} \)
4. \(B =\frac{4 \pi}{\mu_0} \frac{r}{2 i}\)
The magnetic induction at the centre O in the figure shown is:
1. 2.
3. 4.
In the figure shown, the magnetic induction at the centre of the arc due to the current in portion AB will be
(a) (c)
(b) (d) 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 at the centre is :
(a) (b)
(c) (d)
In the figure shown below there are two semicircles of radius \(r_1\) and \(r_2\) in which a current \(i\) is flowing. The magnetic induction at the centre of \(O\) will be:
1. | \(\dfrac{\mu_{0} i}{r} \left(r_{1} + r_{2}\right)\) | 2. | \(\dfrac{\mu_{0} i}{4} \left[\frac{r_{1} + r_{2}}{r_{1} r_{2}}\right]\) |
3. | \(\dfrac{\mu_{0} i}{4} \left(r_{1} - r_{2}\right)\) | 4. | \(\dfrac{\mu_{0} i}{4} \left[\frac{r_{2} - r_{1}}{r_{1} r_{2}}\right]\) |