A pendulum consists of a mass, \(m,\) swinging on the end of a string of length
\(l .\) With the angle between the string and the vertical represented by
\(\theta,\) the motion satisfies the differential equation $$\theta^{\prime
\prime}+\frac{g}{l} g \sin \theta=0$$. (a) For small swings, we can replace
sin \(\theta\) by its lowest nonzero Taylor approximation. What does the
differential equation become? (b) If the amplitude of the oscillation is
\(\theta_{0},\) the solutions to the original differential equation are
oscillations with \(^{7}\) $$\text { Period }=2 \pi
\sqrt{\frac{l}{g}}\left(1+\frac{1}{16} \theta_{0}^{2}+\cdots\right)$$. The
solutions to the approximate differential equation are oscillations with
$$\text { Period }=2 \pi \sqrt{\frac{l}{g}}$$. If \(\theta_{0}=20^{\circ},\) by
what percentage is the more accurate estimate of the period obtained using the
solution to the original equation up to the \(\theta_{0}^{2}\) -term different
to the approximate estimate using the solution of the approximate equation?