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Chapter 15: Problem 37

Question: A solid cylinder is attached to a horizontal massless spring so that it can roll without slipping along a horizontal surface, as in Fig. 32. The force constant k , of the spring is tex2html_wrap_inline311. If the system is released from rest at a position in which the spring is stretched by tex2html_wrap_inline313, find

  1. The translational kinetic energy of the cylinder as it passes through the equilibrium position.
  2. The rotational kinetic energy of the cylinder as it passes through the equilibrium position.
  3. Show that under these conditions the center of mass of the cylinder executes simple harmonic motion with a period tex2html_wrap_inline315, where M is the mass of the cylinder.

Solution:

We will start by converting everything to units we understand, tex2html_wrap_inline317 and tex2html_wrap_inline319. Initially the cylinder is at rest and therefore the total mechanical energy of the system is equal to the potential energy stored in the spring, tex2html_wrap_inline321. When the cylinder passes through its equilibrium position, the potential energy stored in the spring vanishes, and therefore this total mechanical energy is all in the form of kinetic energy, both translational and rotational. In terms of the speed of the cylinder v, its mass, and its moment of inertia, I, and angular speed tex2html_wrap_inline267, we have that tex2html_wrap_inline327. For a solid cylinder, we have that tex2html_wrap_inline329, where R is the radius of the cylinder, we also have that the angular speed is tex2html_wrap_inline333 (no slipping). Therefore, we have that tex2html_wrap_inline335. This leads to tex2html_wrap_inline337. Hence we have that as the cylinder passes through its equilibrium position, its translational kinetic energy is tex2html_wrap_inline339 and its rotational energy is tex2html_wrap_inline341.

To find the period, lets consider the forces acting on the cylinder. The spring provides a force acting through the center of mass, tex2html_wrap_inline343, while the contact with the surface provides a force tex2html_wrap_inline345 at the surface of the cylinder, and in the opposite direction to tex2html_wrap_inline343. Newton's law tells us that the acceleration tex2html_wrap_inline349 is related to the net force by tex2html_wrap_inline351, while the angular acceleration is related to the torque about the center of the cylinder tex2html_wrap_inline353, from which it follows that tex2html_wrap_inline355. Inserting this into Newton's law, we have that tex2html_wrap_inline351 gives tex2html_wrap_inline359 and hence tex2html_wrap_inline361. We recognize this as an equation describing simple harmonic motion, tex2html_wrap_inline363, with tex2html_wrap_inline365, from with we find a period of tex2html_wrap_inline367.


next up previous
Next: Chapter 19: Problem 2 Up: Waves and OpticsSolutions Previous: Chapter 15: Problem 31

Martin Savage
Tue Jan 12 17:39:44 PST 1999