PHY 711 Classical Mechanics

MWF 11-11:50 AM OPL 107 http://www.wfu.edu/~natalie/f99phy711/

Instructor: Natalie Holzwarth Phone:758-5510Office:300 OPL e-mail:natalie@wfu.edu


Homework Assignments



PHY 711 -- Assignment #1

August 25, 1999

Read Chapter 1 in Fetter & Walecka and make note of useful appendices.

  1. Work problem #1.15

PHY 711 -- Assignment #2

August 27 1999

Complete Chapter 1 in Fetter & Walecka

  1. Work problem #1.16

PHY 711 -- Assignment #3

August 30, 1999

Complete Chap 1 in Fetter & Walecka

  1. Write a general expression for Rutherford scattering in the laboratory frame of reference, assuming that the incident particle has a mass m and the target particle has a mass M.
  2. Extra Credit -- Plot the differential cross section as a function the scattering angle in the laboratory frame of reference assuming that the incident a particle has an energy of 10 MeV when
    1. The target is He (Z=2).
    2. The target is Cu (Z=29).

PHY 711 -- Assignment #4

September 1, 1999

Read Chapter 2 in Fetter & Walecka

  1. Analyze the motion of a Foucault pendulum in Winston-Salem, NC and compare the results with the that which would be observed in another location of your choice. Assume that the length of the pendulum is l=10 m.

Sep 7, 1999

PHY 711 -- Problem Set PHY 711 - Problem Set # 5

Start reading Chapter 3 of Fetter & Walecka.

  1. Suppose you want to extremize an integral of the form:
    I º ó
    õ
    x2

    x1 
    f(y,y¢,y¢¢;x)   dx,
    where y = y(x), y¢ º [dy/ dx], and y¢¢ º [(d2y)/( d2x)], and where f is a given function. Find the generalization of the Euler-Lagrange equation (Eq. 17.34 in your text) for this function f. In order to solve this problem, you should assume that the end point values and slopes are all fixed (not varying). That is, y(x1) = A, y(x2) = B, y¢(x1) = C, and y¢(x2) = D, where A, B, and C, and D are all fixed values.

  2. Extra Credit

    Consider an integral of the form:

    E = ó
    õ
     d3r  F[r(r),g(r)],
    where r(r) is a function of position in three dimensions, and g(r) º |Ñr(r)|. Show that the functional variation of E with respect to r(r) is given by:
    dE = ó
    õ
     d3r   ì
    í
    î
    F
    r
    - F
    g
    æ
    ç
    è
    Ñ2r
    g
    - Ñ r·Ñg
    g2
    ö
    ÷
    ø
    - 2 F
    rg
    g - 2 F
    2 g
    Ñ r·Ñ g
    g
    ü
    ý
    þ
    dr(r).


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PHY 711 -- Assignment #6

September 8, 1999

Continue reading Chapter 3 in Fetter & Walecka

  1. Work problem #3.10

Sep 14, 1999

PHY 711 -- Problem Set PHY 711 - Problem Set # 7

Consider a particle of mass m and charge q moving in a constant magnetic file B = B0 [^(z)].

  1. Show that this magnetic field can be described by the vector potential
    A = 1
    2
    B0 ( x ^
    y
     
    -y ^
    x
     
    ).
  2. From Newton's second law in cartesian coordinates, the equations of motion of the particle.
  3. Form the Lagrangian and determine the equations of motion, comparing your results with part (2).


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Sep 14, 1999

PHY 711 -- Problem Set PHY 711 - Problem Set # 8

Read Chapter 6 in Fetter and Walecka.

  1. Consider the Lagrangian for the motion of a symmetric top under the acceleration of gravity:
    L(q,f,y, .
    q
     
    , .
    f
     
    , .
    y
     
    ) = 1
    2
    A æ
    è
    .
    f
     
    2
     
    sin2(q) + .
    q
     
    2
     
    ö
    ø
    + 1
    2
    B æ
    è
    .
    f
     
    cos(q) + .
    y
     
    ö
    ø
    2
     
    -Mgh cos(q),

    where A, B, M, g, and h are parameters related to the moments of inertia, the mass, the acceleration of gravity, and the location of the center of mass. The angles q, f, and y are called the ``Euler angles" and are the generalized coordinates for this system. Identify the constants of the motion and find the Hamiltonian (in canonical form) for this system.

  2. Consider a particle of mass m and charge q moving in a constant magnetic file B = B0 [^(z)] as in Problem Set #7. Starting from the Lagrangian for this system, find the Hamiltonian (in canonical form).


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PHY 711 -- Assignment #9

September 17, 1999

Continue reading Chapter 6 in Fetter & Walecka

  1. Work problem #6.11

PHY 711 -- Assignment #10

September 20, 1999

Continue reading Chapter 6 in Fetter & Walecka

  1. Work problem #6.17 or #6.18. (Extra credit for working both.)

PHY 711 -- Assignment #11

September 29, 1999

Read Chapter 4 in Fetter & Walecka

  1. Work problem #4.2
  2. Work problem #4.9

PHY 711 -- Assignment #12

October 1, 1999

Complete Chapter 4 in Fetter & Walecka

  1. Work problem #4.14

Oct 5, 1999

PHY 711 -- Problem Set PHY 711 - Problem Set # 13

Consider the above retangular solid composed of a uniform material of density r.

    1. Find the moment of inertia tensor about the corner.
    2. Find the center of mass of the solid
    3. Find the moment of inertia tensor about the center of mass.


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PHY 711 -- Assignment #14

October 8, 1999

Continue reading Chapter 5 in Fetter & Walecka

  1. Work problem #5.6

PHY 711 -- Assignment #15

October 11, 1999

Continue reading Chapter 5 in Fetter & Walecka

  1. Consider the Euler angles as defined in Section 29 of your text. In most classical mechanics texts (such as Marion or Goldstein or Symon), the Euler angles { q,f,y} are defined slightly differently. In that convention the directions of q and y are the same as a and g respectively, but the direction of f is measured relative to the body-fixed 1 direction (instead of the 2 direction). Derive the equations equivalent to 29.7 for this convention.

PHY 711 -- Assignment #16

October 18, 1999

Read Chapter 7 in Fetter & Walecka

    Work problem #7.1 in Fetter & Walecka

PHY 711 -- Assignment #17

October 20, 1999

Continue reading Chapter 7 in Fetter & Walecka

    Work problem #7.11 in Fetter & Walecka

PHY 711 -- Assignment #18

October 29, 1999

Read Chapter 8 of Fetter & Walecka

    Work problem #8.5 in Fetter & Walecka

PHY 711 -- Assignment #19

November 1, 1999

Read Chapter 9 of Fetter & Walecka

  1. "Prove" Thomson's theorem; Eq. 48.61 in F & W.

PHY 711 -- Assignment #20

November 1, 1999

Continue reading Chapter 9 of Fetter & Walecka

  1. Assuming the ideal gas law, calculate the speed of sound for normal air and for He at atmospheric pressure and T=25 degrees Celcius.

PHY 711 -- Assignment #21

November 5, 1999

Continue reading Chapter 9 of Fetter & Walecka

  1. Problem 9.3 in Fetter & Walecka

PHY 711 -- Assignment #22

November 8, 1999

Continue reading Chapter 9 of Fetter & Walecka

  1. Problem 9.16 in Fetter & Walecka

PHY 711 -- Assignment #23

November 15, 1999

Finish reading Chapter 9 of Fetter & Walecka

  1. Derive the effective velocity function u(r) for an ideal gas (Eq. 52.33b in Fetter & Walecka. Plot u as a function of r for a gas of your choice.

Nov 17, 1999

PHY 711 -- Problem Set PHY 711 - Problem Set # 24

  1. Consider the density r(x,t) a one dimensional fluid described by an equation of the form:
    r
    t
    + u(r) r
    x
    = 0.
    Here, the effective velocity function is given by
    u(r) º d m(r)
    d r
    = 3 r
    for this particular system.

    1. Suppose that at time t = 0 the density function has the shape:
      r(x,0) = ì
      í
      î
      1
      for x < 0
      2
      for x > 0.
      Find the form of r(x,t) for t > 0.
    2. Suppose that at time t = 0 the density function has the shape:
      r(x,0) = ì
      í
      î
      2
      for x < 0
      1
      for x > 0.
      Find the form of r(x,t) for t > 0. In particular, find the velocity of the shock front for this system.


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PHY 711 -- Assignment #25

November 19, 1999

Continue reading Chapter 10 of Fetter & Walecka

  1. Work Problem #10.3 in Fetter & Walecka.

PHY 711 -- Assignment #26

November 29, 1999

Continue reading Chapter 10 of Fetter & Walecka

  1. Work Problem #10.9 or #10.12 in Fetter & Walecka (extra credit for both).

PHY 711 -- Assignment #27

December 1, 1999

Continue reading Chapter 10 of Fetter & Walecka

  1. Work throught the derivation of the solitary wave solution of the non-linear surface wave equations discussed in section 56 of your text or in the soliton lecture notes (pdf) (html). Taking the final solitary wave form, evaluate some of the discarded terms to check that the approximations are self-consistent. Extra credit will be awarded for finding errors in the lecture notes.


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