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Reading:

Read quantitatively B & O Sections 3.7 and 5.1; KB 361 lecture notes 31 -- 33.
Read qualitatively B & O Sections 5.2 -- 5.3; KB 361 lecture note summaries 34 -- 36.
Problems for Review:
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  1. A spherical pendulum consists of a bob of mass m and a weightless rod of length l. One end of the rod is fixed at the origin, while the other is attached to the bob, so that the bob pivots in any direction about the origin, yet always remains at fixed radius l. The bob thus moves on a spherical surface of radius l, subject to gravity.

    1. Write the Lagrangian for the spherical pendulum in spherical coordinates, eliminating any constraints.
    2. Legendre transform to obtain the Hamiltonian for the spherical pendulum, in terms of tex2html_wrap_inline67 .
    3. Show that tex2html_wrap_inline69 is conserved.
    4. Combine the Hamiltonian term depending on tex2html_wrap_inline69 with the ordinary potential energy term to define an effective potential energy tex2html_wrap_inline73 . Sketch tex2html_wrap_inline73 for varying values of tex2html_wrap_inline69 . What does this tell you about the allowed motions of constant tex2html_wrap_inline79 ? Sketch these allowed motions for varying values of tex2html_wrap_inline69 .

  2. Consider a particle of mass m constrained to move on the surface of a cylinder defined by tex2html_wrap_inline85 . The particle is attracted toward the origin by a radial force tex2html_wrap_inline87 .

    1. Write the Lagrangian in cylindrical coordinates tex2html_wrap_inline89 , eliminating any constraints. Find the Euler-Lagrange equations for tex2html_wrap_inline79 and z.
    2. Legendre transform to obtain the Hamiltonian, in terms of tex2html_wrap_inline95 .
    3. Find Hamilton's equations and show that they reproduce the Euler-Lagrange equations in (a).
    4. Sketch the allowed motions of the particle. Under what conditions are these motions periodic?

  3. (essentially B & O 5-3) A particle is attracted toward a force center at the origin via the central force tex2html_wrap_inline97 .
    1. Find the potential V(r) corresponding to this central force.
    2. Find and sketch the effective potential tex2html_wrap_inline101 . For what values of the energy are there bound orbits? scattering orbits?
    3. At what radius is there a circular orbit? What is its period?
    4. Find the frequency tex2html_wrap_inline103 of small radial oscillations about the circular orbit. Relate it to the angular frequency tex2html_wrap_inline105 . What does this tell you about whether near-circular orbits close?
  4. (essentially B & O 5-2) Find the condition for stable circular orbits for a potential energy of the form

    displaymath107

    where tex2html_wrap_inline109 is nonzero and tex2html_wrap_inline111 is positive. Under what condition on tex2html_wrap_inline113 do perturbed near-circular orbits close? Sketch the orbits for two values of tex2html_wrap_inline113 meeting your criterion.

Problems to Solve:
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  1. B & O 3-14.
  2. In a child's toy, a bead, subject to gravity, moves along a spiraling wire of shape tex2html_wrap_inline117 , tex2html_wrap_inline119 in cylindrical coordinates with k constant.

    1. Write the Lagrangian in terms of z and tex2html_wrap_inline125 only, eliminating constraints. Derive the Euler-Lagrange equation for z.
    2. Legendre transform your Lagrangian of (a) to obtain the Hamiltonian in terms of tex2html_wrap_inline129 .
    3. Find Hamilton's equations and show that they reproduce the Euler-Lagrange equation in (a).
    4. Comment on the sensibility of the equation of motion obtained in (a) and (c), focusing on how tex2html_wrap_inline131 varies with changing spiral slope tex2html_wrap_inline133 .

  3. A particle is attracted toward the origin via the radial potential V= cr.
    1. Find and sketch the effective potential tex2html_wrap_inline101 .
    2. At what radius is there a circular orbit? What is its period?
    3. Find the frequency tex2html_wrap_inline103 of small radial oscillations about the circular orbit. Relate it to the angular frequency tex2html_wrap_inline105 . What does this tell you about whether near-circular orbits close?
  4. A particle is attracted toward the origin via the radial potential tex2html_wrap_inline143 .
    1. Find and sketch the effective potential tex2html_wrap_inline101 .
    2. Show that the only allowed circular orbit has the period expected from simple harmonic motion, tex2html_wrap_inline147 .
    3. Consider a small radial perturbation of the circular orbit. Show that the motions remains periodic, with the same harmonic oscillator period T derived above. Sketch the motion.



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Next: About this document

Katherine Benson
Wed Mar 20 17:08:37 EST 2002