PHY 711 Classical Mechanics and Mathematical Methods

MWF 9 AM-9:50 AM OPL 107 http://www.wfu.edu/~natalie/f17phy711/

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


Course schedule

(Preliminary schedule -- subject to frequent adjustment.)
DateF&W ReadingTopic AssignmentDue
1 Mon, 8/28/2017Chap. 1 Introduction #19/6/2017
2 Wed, 8/30/2017Chap. 1 Scattering theory #29/6/2017
3 Fri, 9/01/2017Chap. 1 Scattering theory
4 Mon, 9/04/2017Chap. 1 Scattering theory #39/6/2017
5 Wed, 9/06/2017Chap. 2 Physics in an non-inertial reference frame #49/8/2017
6 Fri, 9/08/2017Chap. 3 Calculus of variations #59/11/2017
7 Mon, 9/11/2017Chap.3 Calculus of variations #69/13/2017
8 Wed, 9/13/2017Chap. 3 Lagrangian Mechanics #79/15/2017
9 Fri, 9/15/2017Chap. 3 and 6 Lagrangian mechanics and constraints #89/20/2017
10 Mon, 9/18/2017Chap. 3 and 6 Constants of the motion
11 Wed, 9/20/2017Chap. 3 and 6 Hamiltonian formalism #99/27/2017
12 Fri, 9/22/2017Chap. 3 and 6 Liouville equation
13 Mon, 9/25/2017Chap. 6 Canonical transformations
14 Wed, 9/27/2017Chap. 4 Motion from Small oscillations about equilibrium
15 Fri, 9/29/2017Chap. 1-4,6 Review
Mon, 10/02/2017 Take-home exam -- No class
Wed, 10/04/2017 Take-home exam -- No class
16 Fri, 10/06/2017Chap. 4 Vibrational modes
17 Mon, 10/09/2017Chap. 5 Rigid body motion #1010/16/2017
18 Wed, 10/11/2017Chap. 5 Rigid body motion
Fri, 10/13/2017 Fall break -- No class
19 Mon, 10/16/2017 Discuss exam questions and topics for presentations Topic 10/18/2017
20 Wed, 10/18/2017Chap. 7 Wave equation in one dimension #1110/20/2017
21 Fri, 10/20/2017Chap. 7 Solutions of Sturm-Liouville equations #1210/27/2017
22 Mon, 10/23/2017Chap. 7 Solutions of Sturm-Liouville equations
23 Wed, 10/25/2017Chap. 7 Solutions of Sturm-Liouville equations
24 Fri, 10/27/2017App. A Laplace transforms and contour integrals #1311/01/2017
25 Mon, 10/30/2017App. A Contour integrals
26 Wed, 11/01/2017Chap. 8 Mechanics of Elastic Membranes #1411/06/2017
27 Fri, 11/03/2017Chap. 9 Introduction to hydrodynamics
28 Mon, 11/06/2017Chap. 9 Introduction to hydrodynamics #1511/10/2017
29 Wed, 11/08/2017Chap. 9 Sound waves
30 Fri, 11/10/2017Chap. 9 Sound waves #1611/17/2017
Mon, 11/13/2017 Class cancelled
31 Wed, 11/15/2017Chap. 9 Sound waves -- including non-linearities
32 Fri, 11/17/2017Chap. 10 Surface waves in fluids #1711/27/2017
33 Mon, 11/20/2017Chap. 10 Surface waves in fluids
Wed, 11/22/2017 Thanksgiving Holiday -- No class
Fri, 11/24/2017 Thanksgiving Holiday -- No class
34 Mon, 11/27/2017Chap. 11 Heat conductivity
35 Wed, 11/29/2017Chap. 12 Viscous fluids
36 Fri, 12/01/2017Chap. 12 Viscous fluids
Mon, 12/04/2017 Presentations I
Wed, 12/06/2017 Presentations II
Fri, 12/08/2017 Presentations III

No Title
PHY 711 - Assignment #1
PDF VERSION
08/28/2017
  1. Use maple or mathematica to plot the functions
    f(x)=e−x2        and        h(x)=
    x

    0 
    f(t)  dt.
    and to numerically evaluate f(5) and h(5).



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On 27 Aug 2017, 10:53.

PHY 711 -- Assignment #2

Aug. 30, 2017

Read Chapter 1 in Fetter & Walecka.


PHY 711 -- Assignment #3

Sept. 4, 2017

Continue reading Chapter 1 in Fetter & Walecka.


PHY 711 -- Assignment #4

Sept. 6, 2017

Read Chapter 2 in Fetter & Walecka.


PHY 711 -- Assignment #5

Sept. 8, 2017

Start reading Chapter 3, especially Section 17, in Fetter & Walecka.


No Title
PHY 711 - Assignment #6
PDF VERSION
Sep 9, 2017
This exercise is designed to illustrate the differences between partial and total derivatives.
  1. Consider an arbitrary function of the form f=f(q,· q,t), where it is assumed that q=q(t) and · q ≡ dq/dt.
    1. Evaluate

      ∂q
      df

      dt
      d

      dt
      ∂f

      ∂q
      .
    2. Evaluate


      q
       
      df

      dt
      d

      dt
      ∂f


      q
       
      .
    3. Evaluate
      df

      dt
      .
    4. Now suppose that
      f(q,

      q
       
      ,t) = q

      q
       
      2
       
      t2,       where      q(t)=e−t/τ.
      Here τ is a constant. Evaluate df/dt using the expression you just derived. Now find the expression for f as an explicit function of t ( f(t) ) and take its time derivative directly to check your previous results.



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On 9 Sep 2017, 18:14.

No Title
PHY 711 - Assignment #7
PDF VERSION
Sep 12, 2017
  1. Consider a Lagrangian describing the motion of a particle of mass m and charge q given by
    L(x,y,z,

    x
     
    ,

    y
     
    ,

    z
     
    ) = 1

    2
    m

    x
     
    2
     
    +

    y
     
    2
     
    +

    z
     
    2
     

    + q

    c
    B

    y
     
    x.
    Here c denotes the speed of light and B represents the magnitude of a constant magnetic field along the z-axis. Determine the Euler-Lagrange equations of motion for the particle and discuss how the motion compares with the similar example discussed in class.



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On 12 Sep 2017, 22:30.

No Title
PHY 711 - Assignment #8
PDF VERSION
9/15/2017
Continue reading Chapters 3 and 6 in Fetter and Walecka.
  1. The figure above shows a box of mass m sliding on the frictionless surface of an inclined plane (angle θ). The inclined plane itself has a mass M and is supported on a horizontal frictionless surface. Write down the Lagrangian for this system in terms of the generalized coordinates X and s and the fixed constants of the system (θ, m, M, etc.) and solve for the equations of motion, assuming that the system is initially at rest. (Note that X and s represent components of vectors whose directions are related by the angle θ.)



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On 14 Sep 2017, 20:33.

PHY 711 -- Assignment #9

Sept. 20, 2017

Continue reading Chapters 3 and 6 in Fetter & Walecka.


PHY 711 -- Assignment #10

Oct. 9, 2017

Start Chapter 5 in Fetter & Walecka.

the above figure shows an object with four particles held together with massless bonds at the coordinates shown. The masses of the particles are m1=m2 ≡ 2m and m3=m4 ≡ m.

  1. Evaluate the moment of inertia tensor for this object in the given coordinate system.
  2. Find the principal moments of inertia and the corresponding principal axes. Sketch the location of the axes.

No Title
PHY 711 - Assignment #11
PDF VERSION
10/18/2017
Continue reading Chapter 7 in Fetter and Walecka.
  1. Consider a displacement function u(x,t) representing a one-dimensional traveling wave (either transverse or longitudinal) which is a solution of the one-dimensional wave equation with wave speed c:

    2 u

    ∂x2
    1

    c2
    2 u

    ∂t2
    =0.
    If the initial conditions for the wave displacement u(x,t) are given by

    u(x,0) = U0 e−(x−x0)22,
    and
    ∂u

    ∂t
    (x,0) = V0
    x

    μ

    3

     
    e−(x/μ)4,
    find the form of u(x,t) for t > 0. Express your result in terms of the constants U0, V0, σ, μ, x0, and c.



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On 17 Oct 2017, 17:15.

PHY 711 -- Assignment #12

Oct. 20,, 2017

Continue reading Chapter 7 in Fetter & Walecka.

  1. Work problem 7.1 at the end of Chap. 7 in Fetter & Walecka.

No Title
10/27/2017
PDF VERSION
PHY 711 - Homework # 13
Read Appendix A of Fetter and Walecka.
  1. Assume that a > 0 and use contour integration methods to evaluate the integral:




    0 
    cos(ax)

    4x4+5x2+1
    dx.



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On 26 Oct 2017, 21:42.

PHY 711 -- Assignment #14

Nov. 01, 2017

Read Chapter 8 in Fetter & Walecka.

  1. Work problem 8.5 at the end of Chap. 8 in Fetter & Walecka

PHY 711 -- Assignment #15

Nov. 6, 2017

Continue reading Chapter 9 in Fetter & Walecka.

  1. Determine the form of the velocity potential for a 3-dimensional compressible fluid which flows at uniform velocity in the z direction at large distances from a spherical obstruction of radius a. Find the form of the velocity potential and the velocity field for all r > a. Assume that the velocity in the radial direction is 0 for r = a and assume that the velocity is uniform in the azimuthal direction.

PHY 711 -- Assignment #16

Nov. 10, 2017

Continue reading Chapter 9 in Fetter & Walecka.

  1. Work Problem 9.2 at the end of Chapter 9 in Fetter and Walecka.

PHY 711 -- Assignment #17

Nov. 17, 2017

Start reading Chapter 10 in Fetter & Walecka.

  1. Work Problem 10.3 at the end of Chapter 10 in Fetter and Walecka. If helpful, you may wish to use some of the material presented in Lecture 32.




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Last modfied: Thursday, 16-Nov-2017 20:39:06 EST