Total charge –Q is uniformly spread along length of a ring of radius R. A small test charge +q of mass m is kept at the centre of the ring and is given a gentle push along the axis of the ring.
(a) Show that the particle executes a simple harmonic oscillation.
(b) Obtain its time period.
a)

Due to a small element of the ring on the z-axis the effective field will be
.cosθeq .1
In triangle AOC,
 ( By Pythagoras Theorem)
Now,
 eq .2
Equating 1 and 2
=
 eq.3
=![]()
Integrating above equation we get,
=![]()
Since, -Q charge is uniformly distributed over the ring,

According to question +q is displaced by z distance along the centre of the ring at the axis of ring. So,
Force on +q charge will be,
F=
 eq.4
But as z<<r ,
<<1 and 
<<<1
F= ![]()
Using binomial expansion,
,where x<<1
So,
F=
 eq.5
Since 
 is very small the term in the bracket can be taken as 1. Therefore equation 5 becomes,
F=
 eq.6
From simple harmonic motion(SHM) we know that a particle to follow a simple harmonic motion it should follow the relation
a 
 –x
where x=displacement from mean position and
a=-
 eq.7
and
 =![]()
so comparing the force equation as we obtained in the equation 6 with equation 7 we get,
=![]()
∴![]()
b) As we know ![]()
∴T=![]()