The magnetic field on the axis of the magnet at a distance d1 = 14 cm, can be written as:
\(B_1\) = \(\frac{\mu_0 2M}{4\pi (d_1)^3}\)=H ...(1)
Where,
M = Magnetic moment
\(\mu_0\) = Permeability of free space
H = Horizontal component of the magnetic field at d1
If the bar magnet is turned through 180°, then the neutral point will lie on the equatorial line.
Hence, the magnetic field at a distance d2, on the equatorial line of the magnet can be written as:
\(B_2\) = \(\frac{\mu_0 M}{4\pi (d_2)^3}\)=H ...(2)
Equating equations (1) and (2), we get:
\(\frac{2}{(d_1)^3}\)=\(\frac{1}{(d_2)^3}\)
\(\bigg(\frac{d_2}{d_1}\bigg)^3\)=\(\frac{1}{2}\)
∴ d2 = d1 × \(\bigg(\frac{1}{2}\bigg)^{\frac{1}{3}}\)
=14 × 0.794 = 11.1cm
The new null points will be located 11.1 cm on the normal bisector.
A current-carrying coil is placed in an external uniform magnetic field. The coil is free to turn in the magnetic field. What is the net force acting on the coil? Obtain the orientation of the coil in stable equilibrium. Show that in this orientation the flux of the total field (field produced by the loop + external field) through the coil is maximum.


Magnets are used in many devices like electric bells, telephones, radio, loudspeakers, motors, fans, screwdrivers, lifting heavy iron loads, super-fast trains, especially in foreign countries, refrigerators, etc.
Magnetite is the world’s first magnet. This is also called a natural magnet. Though magnets occur naturally, we can also impart magnetic properties to a substance. It would be an artificial magnet in that case.
Read More: Magnetism and Matter