Second order differential equations arise naturally as a result of applying Newton's second law of motion. If no external forces act then the equation may take the form
![]()
where
is a drag or resistance term and
is a restoring force.
If there is no resistance term then the equation becomes
- the equation of simple harmonic motion - and this equation has the solution![]()
If there is no restoring force the the equation becomes![]()
We can write this equations as![]()
Integration gives
We can solve this equation by separation of variables
![]()
Integration gives
and solving for x gives
If there are both resistance and restoring terms then there are three possibilities.
We can substitute
so that
and
The equation becomes
![]()
We can divide by
(since an exponential is never zero) to obtain
![]()
This is a quadratic equation with roots![]()
If
then there are two distinct real roots
and
and![]()
If
then there is one root
and![]()
In both of these cases,
may increase without limit if
is positive, and the motion is non – oscillatory.
If
then there are two distinct complex roots![]()
and
and![]()
This last solution for
represents oscillatory motion. If
the oscillations decay and if
the oscillations increase in size.