A magnetic dipole is suspended in a region where two uniform magnetic fields are inclined at \(75^\circ\) with each other. In stable equilibrium, if the dipole makes an angle of \(30^\circ\) with the direction of field of \(10\sqrt2\,\text{mT}\), then the value of the second magnetic field is
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For two magnetic fields making an angle \(\theta\),
\[
\boxed{
\tan\alpha=
\frac{B_2\sin\theta}
{B_1+B_2\cos\theta},
}
\]
where \(\alpha\) is the angle made by the resultant field with \(B_1\).
A freely suspended magnetic dipole always aligns along the resultant magnetic field.