Final answer:
a) The potential energy function U(x) is U(x) = -kx^2/2 + kx^4/(4α^2). b) Equilibrium points are x = 0, x = ±√(α^2/2), and the stability can be determined by examining the second derivative of the potential energy function. c) The sketch of the potential energy function will show a stable minimum at x = 0 and unstable maxima at x = ±√(α^2/2). d) The maximum total energy E_max occurs at the unstable equilibrium points, where E_max = kα^2/4. e) For bounded motion, the total energy E must be less than or equal to E_max, so E ≤ kα^2/4.
Step-by-step explanation:
a) To find the potential energy function U(x), we integrate the force function with respect to x. Since U(x=0) = 0, the constant of integration is also 0. The potential energy function is given by U(x) = -kx^2/2 + kx^4/(4α^2).
b) Equilibrium points are where the force is zero, so we set F(x) = 0 and solve for x. In this case, there are three equilibrium points: x = 0, x = ±√(α^2/2). To determine stability, we can examine the second derivative of the potential energy function at each equilibrium point. If the second derivative is positive, the equilibrium point is stable; if negative, it is unstable. For this potential energy function, the equilibrium point x = 0 is stable and the points x = ±√(α^2/2) are unstable.
c) The sketch of the potential energy function will show a symmetric curve with a stable minimum at x = 0 and unstable maxima at x = ±√(α^2/2).
d) The maximum total energy E_max occurs at the unstable equilibrium points. At these points, the kinetic energy is equal to the potential energy, so E_max = U(x = ±√(α^2/2)) = kα^4/(4α^2) = kα^2/4.
e) For bounded motion, the total energy E must be less than or equal to E_max, so E ≤ kα^2/4.