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The previous exercises introduced some of WAVE's features. They suggest
similarities and differences among the various equations; we will
examine many of these similarities and differences
in the following exercises. We begin by
considering the eigenfunctions or modes for the four linear
PDEs for a uniform medium of length L with fixed boundaries.
Various equations and eigenfunctions can be selected by first choosing
an EquationType
under [Parameters]
followed by
[Init]|[Modes]
and then selecting the eigenfunction
number. Modes 1 through 5 can be selected by checking the appropriate box.
Modes that are not listed can be selected using the two input fields at
the bottom of the screen. Select the Fixed
boundary condition
before you begin the following exercises; eigenfunctions are different
for different boundary conditions.
Table: Eigenfunctions for various PDEs with fixed boundaries on
.
- Fixed-Boundary Eigenfunctions
- a.
- Select [Parameters]|[Electromagnetic]
and set the initial condition
to mode 4. Create a detector by clicking on the blue button (labeled ``d")
in the lower
left corner of the
wave graph and then clicking inside the
wave graph. Create two additional detectors. Run the program. Notice
that all the detectors have the same frequency but different phases.
Measure the frequency of this mode by holding down the mouse inside the
detector graph and reading the time at two different maxima. Measure the
wavelength by holding the mouse down in the wave graph and reading the
separation between two maxima. Calculate the phase velocity,
. Place the system in another mode and repeat. Are the phase
velocities the same?
- b.
- Repeat [a.] for the Schrödinger equation. Since the quantum detectors measure propability current, they cannot be used to measure phase
oscillations. You can, however, follow a phase oscillation in the
bottom graph by looking at the real (or the imaginary) part of the wavefunction. Examine modes 1, 4, 16 and determine the frequency
for each mode. Are the phase velocities the same?
- c.
- Repeat [a.] for the Klein-Gordon equation but set the ends of
the medium to be at
. Try modes 1,
4, 16. Are the phase velocities the same?
- d.
- The functional relationship between wave number,
and the angular frequency,
for a harmonic
wave is called a dispersion function. Determine the dispersion
relationship,
, for the equations in
Table
that exhibit oscillatory behavior. A
wave equation is said to be nondispersive if
and k are
proportional. Which of the equations in
Table
are nondispersive? Which are
dispersive?
- e.
- Repeat [a.] for the diffusion equation. Even though these
solutions do not oscillate, there is a time associated with each mode,
called the characteristic time, that determines how long it takes for
the function to decay to
of its initial value at a point.
Determine the characteristic time for modes 1, 4, 16.
- Periodic-Boundary Eigenfunctions
Change the boundary to Periodic
and examine the modes as in the
previous exercise. It is important to note that these modes are not
the same as for Fixed
boundaries.
- a.
- How do the eigenfunctions change when you switch to periodic boundary conditions? Try both positive and negative modes. Write the analytical
form of the eigenfunctions for periodic boundaries.
- b.
- Using Periodic
boundary conditions with an
[Electromagnetic]
wave, place the system simultaneously in modes
4 and -4 and run the simulation. Is it possible to write
the eigenfunctions for Periodic
boundaries in terms of the
functions listed in
? Is the reverse
possible?
- Beats
The phenomena of beats is usually covered in introductory physics
texts for the classical wave equation. You should now be familiar enough
with the program to construct simulations that demonstrate the
phenomenon of beats for other equations. Do you notice differences in
the beat patterns when the simulation is run for the Schrödinger
equation? The Klein-Gordon eqution?
Hint: Set the medium to
for interesting effects with the Klein-Gordon equation.
Next: Fourier Analysis
Up: Exercises
Previous: Visualization and Analysis
Wolfgang Christian
Fri Apr 14 08:22:30 EDT 1995