The ends of a stretched wire of length L are fixed at x = 0 and x = L. In one experiment the displacement of the wire is y1 = A sin (πxL) sinωt and energy is E1 and in another experiment its displacement is y2 = A sin(2πxL)sin 2 ωt and energy is E2. Then
E2 = 4E1
Energy E ∝ (amplitude)2(frequency)2
Amplitude (A) is same in both the cases, but frequency in the second case is two times the frequency in the first case.
Therefore,E2 = 4E1