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 (πx/L) sin ωt and energy is E1 and in another experiment its displacement is y2 = A sin (2πx/L) sin 2 ωt and energy is E2. Then
1
E2 = E1
2
E2 = 2E1
3
E2 = 4E1
4
E2 = 16E1
5
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