P5: Resonance
Adapted from Joe Rogers, Fall 1996
If you have limited time at the computer, you can do parts
(a) and (c) first, and part (b) later...
(P5a) Waves, Forcing, and Resonance
Start up the program pythag in the default
configuration, set the left boundary Forcing
to Wave, Initialize, and Run.
This shows the kind of forcing we will be using in this problem:
the left boundary is wiggled up and down with an amplitude 0.05 m
at a frequency omega:
y(0,t)- (0.05 m) sin(omega t)
(except that the sine wave is made to turn on slowly, in order
that the curve doesn't develop any kinks.)
Now load the preset OffRes. Launch the Configure
menu, and notice that we've lowered the frequency by a factor of ten,
to omega=30 radians/sec.
Notice that the vertical scales on the plots are expanded, so the
amplitude 0.05 of the forcing is now a small fraction of the range.
Notice that the wiggles build up a bit, but don't keep growing.
Calculate the frequency omega of the lowest frequency
standing wave in this simulation. Show your calculation
in your solution, and enter this frequency in the
Configure window under Omega. (If you're
insecure about your answer, you can check it with the preset Reson.)
Run for the full time (2.8 seconds). Forcing the boundary
at a resonant frequency produces a large response (as you will see or
perhaps have seen in the Tacoma Narrows Bridge video).
Make a table of the times at which y reaches
a maximum and the value of y at each maximum by reading
these from the Y vs. T graph. (Clicking the mouse on a point should
show the numbers: don't bother zooming and such.) Leave room in your graph
for two more columns. On what kind of curve do your
versus t points fall? Explain why
they should fall on this kind of curve.
(P5b) Total Energy, Average Power, and Power Input
We want to find out how fast the string is gaining energy.
Add another column to your table for the total energy U.
At the times when the displacement reached its maximum, the displacement
was approximately a sine function with
in the middle
and zero at the ends. Write out this function and use it to calculate
the total energy as a function of
(Hint: why don't
you need the kinetic energy density?) Fill in the total energy
column U, by computing it using your formula and your values
from the
column in your table. Now find the
average power entering the string during the past oscillation
and enter that into a fourth
column for
. Sketch a graph of U
and
as a function of t. Is
constant, or is it increasing linearly with time?
Explain why it behaves that way in terms of the
equation for the power entering the left end of the string:
(P5c) Off Resonance
Initialize the program again, but this time enter a frequency
omega which is 30% or 40% larger, and run the program.
Describe what you see and explain
why it is different from what you saw in the first part of this
problem.
Links Back
- Traveling Pulse
- Energy and Power
- Boundary Conditions and Colliding Pulses
- Reflection and Transmission
- Resonance
- Reflectionless Coatings
Statistical Mechanics: Entropy, Order Parameters, and Complexity,
now available at
Oxford University Press
(USA,
Europe).