$\lambda_{1} \propto$ velocity $\left(v_{1}\right)=\sqrt{\frac{T_{1}}{\mu}}$
Similarly, $\lambda_{2} \propto v_{2}=\sqrt{\frac{T_{2}}{\mu}}$
$\therefore \quad \frac{\lambda_{2}}{\lambda_{1}}=\sqrt{\frac{T_{2}}{T_{1}}}=\sqrt{\frac{\left(m_{1}+m_{2}\right) g}{m_{2} g}}$
$=\sqrt{\frac{m_{1}+m_{2}}{m_{2}}}$
$(A)$ $y(t)=A \sin \frac{\pi x}{6} \cos \frac{50 \pi t}{3}$
$(B)$ $y(t)=A \sin \frac{\pi x}{3} \cos \frac{100 \pi t}{3}$
$(C)$ $y(t)=A \sin \frac{5 \pi x}{6} \cos \frac{250 \pi t}{3}$
$(D)$ $y(t)=A \sin \frac{5 \pi x}{2} \cos 250 \pi t$