355135 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 \(y_{1}=A \sin \left(\dfrac{\pi x}{L}\right) \sin\) \((\omega t)\) and energy is \(E_{1}\) and in another experiment its displacement is \({y_2} = A\sin \left( {\frac{{2\pi x}}{L}} \right)\sin (2\omega t)\) and energy is \(E_{2}\). Then
355135 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 \(y_{1}=A \sin \left(\dfrac{\pi x}{L}\right) \sin\) \((\omega t)\) and energy is \(E_{1}\) and in another experiment its displacement is \({y_2} = A\sin \left( {\frac{{2\pi x}}{L}} \right)\sin (2\omega t)\) and energy is \(E_{2}\). Then
355135 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 \(y_{1}=A \sin \left(\dfrac{\pi x}{L}\right) \sin\) \((\omega t)\) and energy is \(E_{1}\) and in another experiment its displacement is \({y_2} = A\sin \left( {\frac{{2\pi x}}{L}} \right)\sin (2\omega t)\) and energy is \(E_{2}\). Then
355135 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 \(y_{1}=A \sin \left(\dfrac{\pi x}{L}\right) \sin\) \((\omega t)\) and energy is \(E_{1}\) and in another experiment its displacement is \({y_2} = A\sin \left( {\frac{{2\pi x}}{L}} \right)\sin (2\omega t)\) and energy is \(E_{2}\). Then