A particle free to move along the x-axis has potential energy given by U(x)=k[1−exp(−x)2] for −∞≤x≤+∞, where k is a positive constant of appropriate dimensions. Then
For small displacements from x = 0, the motion is simple harmonic
Potential energy of the particle U=k(1−e−x2)
Force on particle F=−dUdx=−k[−ex2×(−2x)]
F=−2kxe−x2=−2kx[1−x2+x42!−........]
For small displacement F = -2kx
⇒F ∞ −x i.e. motion is simple harmonic motion.