Question
The potential energy function for a particle executing linear simple harmonic motion is given by $\text{V(x)} = \frac{\text{kx}^2}{2},$ where k is the force constant of the oscillator. For $k = 0.5Nm^{-1}$, the graph of V(x) versus x is shown in Show that a particle of total energy $1J$ moving under this potential must ‘turn back’ when it reaches $\text{x} =\pm 2\text{m}.$


