A small particle of mass m and charge −q is placed at point P on the axis of uniformly charged ring and released, if R>>x, the particle will undergo oscillations along the axis of symmetry with an angular frequency that is equal to :
The electric field at point P due to the charged ring is E=Q4πϵ0x√(x2+R2)3
when R>>x,E∼Q4πϵ0xR3
Now the equation of motion of charge -q is md2xdt2=−qE=−qQ4πϵ0xR3
or,d2xdt2=−qQ4πϵ0mR3x
therefore, angular frequency ,ω=√qQ4πϵ0mR3