Physics 103:  Fall 2005

 

Pendulums

 

With the invention of the pendulum clock, civilization suddenly had an accurate timekeeper, independent of the heavenly motions.  Before the pendulum, the best clocks were accurate to perhaps ˝ hour per day.  After the pendulum, clocks were routinely accurate to within a few seconds per day, and were rapidly improved after that.  How was it that such a simple and revolutionary invention escaped notice for so many centuries?  I have never heard a plausible answer.

 

A simple pendulum is just a mass m on a string.  Its length L is the length from the support to the center of the mass.  (Notice this means that if you try to change m holding L fixed, you might have to make little adjustments to allow for a different size m.)

 

About the only thing to measure for a given pendulum is its period T, or equivalently its frequency f=1/T, or equivalently its angular frequency =2f=2/T.  For many purposes the simplest quantity is the angular frequency.  (Try not to make your pendulums too short:  short ones can swing in a more complicated way, with the mass pivoting on the knot that holds it.  That is a more complicated pendulum, with internal motion in addition to the normal pendulum swing.)

 

(1)  The most important things about pendulums can be seen without measuring anything!  A priori, we might expect the frequency of a pendulum to depend on both m and L.   Find out how the pendulum frequency depends on mass by constructing two pendulums, using two different masses, one about twice the mass of the other.   Let the pendulums run at the same time, and adjust their lengths to make them have the same frequency.   What really matters, m or L?

 

(2)  To find what role the length L plays, adjust the lengths of two pendulums so that one has twice the frequency of the other (i.e., makes two swings while the other makes only one).  You will probably find that when the frequency goes up by a factor of 2, the length goes down by a factor of 4. 

 

(3)  Another variable, rather subtle, is the amplitude of the pendulum’s swing.  Galileo stated in writing that the frequency doesn’t depend on the amplitude, but this is not true!  In the decades following Galileo’s death, Christian Huyghens went to great effort to make a pendulum-like mechanism that would be truly isochronic, i.e., would have a frequency independent of amplitude.  See if you can tell just the sign of the small amplitude effect:  make two pendulums that have the same frequency for small swings, as nearly as you can arrange it, and then observe them if one of them has a larger amplitude.  Is it slower or faster?  Try reversing their roles.

 

(4)  Finally take some real data!  Measure T vs L, for some pendulum, and make a neat data table in Excel.  Use Excel also to find the corresponding f and .  Use the log-log idea to test for a power law relationship between  and L (find the power!).  Also, supposedly,

                                                                 

Here the constant of proportionality is supposed to be g!   Use your data to test this idea graphically, and if these things seem indeed to be proportional, determine g as the slope.

 

 

Data table:

 

 

 

 

 

 

 

 

 

 

 

 

Sketches of graphs, labeled:


Use your results from (1)-(4) to write a paragraph explaining everything one has to know about the pendulum:

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

OPTIONAL:  please comment on the lab, if you wish, -- suggested improvements?