The first part of your question.
Total energy of a particle is kinetic energy plus potential energy The force field is conservative so the potential energy depends only on the position of a particle. Total energy of a particle has the same value for any because of energy conservation law.
a) at the potential energy is as we see from the graph. The kinetic energy is so the full energy is
b) a particle escapes a force field if its can be arbitrary large. Denote the total particle's energy as and consider the equation
From it we obtain From the graph we see that as Also recall that the displacement is the integral of the velocity (the velocity is the derivative of the displacement with respect to time).
b1) if then cannot be arbitrary large ( will become negative which is impossible), and a particle won't escape.
b2) if then Therefore
So a particle will escape.
b3) if then the answer may be different for different
The second part of the question:
If the total energy of the particle is , then the potential energy of the particle E(x) is either less or equal to 150 J, as follows from the equation
This corresponds to the region on the potential energy curve which lies below the horizontal line corresponding to E(x) = 150 J. This region on the interval where x is greater than 1.3 m and less than 3.4 m: . So, if the total energy of the particle is 150 J, the particle will be "trapped" by the force field in between these two values of x.
The velocity of the particle will be zero when , which happens at x = 1.3 m and x = 3.4 m.
The velocity will be maximum at the point where E(x) is minimum, which is at the point x = 2.6 m. At this point, the particle is in equilibrium.