A long cylindrical volume contains a uniformly distributed charge of density \( \rho \). The radius of cylindrical volume is \( R \). A charge particle (\( q \)) revolves around the cylinder in a circular path. The kinetic energy of the particle is:
\( \dfrac{\rho q R^{2}}{4\varepsilon_{0}} \)
\( \dfrac{\rho q R^{2}}{2\varepsilon_{0}} \)
\( \dfrac{q\rho}{4\varepsilon_{0}R^{2}} \)
\( \dfrac{4\varepsilon_{0}R^{2}}{\rho q} \)