A particle of charge \( '-q '\) and mass \(' m' \) moves in a circle of radius \( 'r '\) around an infinitely long line charge of linear charge density \(' +\lambda' \). Then time period will be given as:(Consider \( k \) as Coulomb’s constant)
\( T=\dfrac{1}{2\pi}\sqrt{\dfrac{2k\lambda q}{m}} \)
\( T=2\pi r\sqrt{\dfrac{m}{2k\lambda q}} \)
\( T=\dfrac{1}{2\pi r}\sqrt{\dfrac{m}{2k\lambda q}} \)
\( T^{2}=\dfrac{4\pi^{2}m}{2k\lambda q}\,r^{3} \)