The ends of a stretched wire of length L are fixed at x=0 and x=L. If in an experiment, the displacement of the wire is y1=Asin(πxL)sinωt and energy is E1 and in another experiment, its displacement is y2=Asin(2πxL)sin2ωt and energy is E2, then
[Assume, there is no energy loss at the ends of the stretched wire]