2007 AAPT Summer Meeting
Greensburo, NC
Coupled Oscillations with a Suspension Bridge Model
Thomas
B. Greenslade, Jr.
Department of Physics
Kenyon College
Gambier, Ohio 43022
740 437-2989
GREENSLADE@KENYON.EDU
Abstract
A flexible
metal sash chain is suspended between supports, and hanging weights are
suspended uniformly at horizontally-spaced locations along the chain. The
original intent was to show that the catenary formed by the freely-hanging
cable is transformed into the parabola of the uniformly-loaded bridge.
Serendipitously, I discovered that pairs of equal length weight suspensions
symmetrically located on either side of the center acted as coupled pendulums.
Construction of Apparatus:
The model bridge was first constructed
for an enrichment lecture during the 1972-3 academic year at the University of
the West Indies, Kingston, Jamaica campus. The lecture on suspension bridges was
then taken on tour to high schools in Jamaica and the Cayman Islands. The
picture below shows it with some of my Jamaican students, and was published in
an article on suspension bridges in the January 1984 issue of The Physics
Teacher.
A length of about 4 m of metal
sash chain is suspended freely from laboratory stands on either end. At equal
distances, as measured along the horizontal, eleven identical weights are
suspended from strings attached to opened-up paper clips passing through the
links of the chain. The lengths of the strings are adjusted to make all of the
masses the same height above the table, thus simulating the deck of the bridge.
Today I would estimate that the
cost of the sash chain would be no more than $5. Instead of the collection of
identical hooked weights that I had available, I would use large steel nuts,
which might cost $0.50 apiece.

Use of Apparatus:
In my original lecture
demonstration I used the light from a slide projector to cast a shadow of the
freely-hanging chain onto the blackboard, and traced it with chalk. The
students could then see that the parabola formed by the loaded bridge was
slightly deeper in the center than the catenary of the same length.
When I set this demonstration up
in early May 2007 for my annual end-of-the-year demonstration lecture at, I
noted that setting the extreme left-hand suspension string swinging as a
pendulum in a direction perpendicular to the length of the string caused only
the corresponding pendulum on the right-hand side to start swinging. Clearly
this was an example of resonant coupled oscillations, with only the pendulum of
the proper resonant length responding. As expected, the two pendula came
alternately to rest and then started swinging once more. This behavior was
noted with all of the longer pendula.
So, here we have examples of geometric form (catenaries and
parabolas), coupled oscillations and resonance – three demonstrations for
the price of one!