
Magnetic field at $C$ is resultant field due to arcs of radius $R$ and $r$.
$\therefore \quad B =\frac{1}{4}\left(\frac{\mu_{0} I}{2 r}\right) \odot-\frac{1}{4}\left(\frac{\mu_{0} I}{2 R}\right) \otimes$
$=\frac{1}{8} \cdot \mu_0 I\left(\frac{1}{r}-\frac{1}{R}\right) \odot$
Net field is out of the plane of paper.
$1^{st}$ Way : By using spring of smaller torsion constant.
$2^{nd}$ Way : By using a smaller coil
$3^{rd}$ Way : By using a stronger magnet
$4^{th}$ Way : By using a coil having fewer number of turns.

