Two simple harmonic motions,
\( y _{1}= a \sin \omega t \) and
\( y _{2}=2 a \sin \left(\omega t +\frac{2 \pi}{3}\right) \) are
superimposed on a particle of mass \( m \). The maximum kinetic energy of the particle is:
1. \( \frac{1}{2} m \omega^{2} a^{2} \)
2. \( \frac{5 m \omega^{2} a ^{2}}{4} \)
3. \( \frac{3}{2} m \omega^{2} a^{2} \)
4. Zero