The electric potential at the centre of two concentric half rings of radii \( R_1 \) and \( R_2 \), having same linear charge density \( \lambda \), is:
\( \dfrac{2\lambda}{\varepsilon_0} \)
\( \dfrac{\lambda}{2\varepsilon_0} \)
\( \dfrac{\lambda}{4\varepsilon_0} \)
\( \dfrac{\lambda}{\varepsilon_0} \)