Jonathan Lansey's Alternate Resume

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Analysis of a Harmonograph I Built:

NJIT Art Show, Oct, 8:
I displayed 3 of these drawings at the NJIT art show (the three in the middle column of picture at right). They asked for names so I called the top one:
,
the middle one: "Harmonic" and the bottom one "As b approaches 1"

Abstract:
An apparatus to draw to graph some lovely pictures. (pictures, seen at right, are called Lissajous Figures, with damping). Since I understood what was going on, I could change certain things to get different looking graphs. In the end, I put the equations on paper then graphed them on a computer.
I plan to make a poster about this for a math conference next year.

Page Index:
Introduction, Basic Analysis, Analog Output, Digital Graphs, Pictures of the Apparatus.

Description: 2003 (click here to see a short video clip)
After a short push, a barbell hanging from a ladder would swing around and around for 10 minutes with the a pen drawing on the paper.
Complete List of Materials:

pen and paper
strings
45 kg of weights
a ladder
tape
paper clips
thermometer.

Motivation:
I tried to emulate this thing I saw at the "Exploratorium" at The Museum of Natural History (NYC). At the end, my apparatus far surpassed the exhibit's both in magnitude and flexibility.

Click for larger Version.

Introduction:

I mathematically describe the motion of an experimental two stringed pendulum. Graphs were drawn mechanically with a pen attached an actual pendulum. The pendulum’s motion can be approximated as complex harmonic motion with linear damping. Similar graphs were first made by Jules Antoine Lissajous in the 19^th century, but required a bulky harmonograph (a complicated device with multiple connected pendulums). My apparatus is simpler with only one pendulum, while an added degree of freedom allows for more interesting output. Different parameter combinations were tested, and the results modeled with equations.

I first recognized this type of motion in a hanging bench swing but it is present to a small degree in almost everything that hangs on two strings. After seeing a double pendulum harmonograph at The Museum of Natural History (in the visiting exhibit The Exploratorium) I decided to build my own. After a few trial versions, my apparatus far surpassed the exhibit's both in magnitude and flexibility.

Apparatus

A short barbell with removable weights totaling 45 kg (about 100 pounds) hung from a ladder by equal strings tied at each end of the barbell.
A pen is loosely held on one end of the barbell by two paper clip rings allowing the pen to slide vertically (to compensate for changing distance to the paper underneath as the pendulum swings). The thermometer seen in the picture served no temperature reading purpose.

Conceptual Analysis:

When the pendulum swings in a direction perpendicular to the barbell, figure 2 (the green arrows in figure 3), the effective radius for measuring period is the red point (center of mass).When the pendulum swings parallel to the barbell as in figure 1 (the red arrows in figure 3), the effective radius is the distance to the point where the string is tied. These two different radii result in two different values for period if one breaks the motion into x and y components.
What I call a “third oscillation,” also harmonic, is found in the twisting of the pendulum shown by the blue arrows in figure 3 and determined by the moment of inertia of the barbell along a vertical axis.

Friction between the pen and paper is assumed to be the main source of damping. Since the friction force is independent of velocity damping will be constant.

A More Mathematical Analysis:
Call the red arrows the y axis and the green arrows the x axis. Since the pendulum is oscillating approximately harmonically it can be described by the following parametric equation:
b=(close to zero); multiply by (k*t) for damping; a=amplitude;
x(t)=a*cos(t*b)(k*t)
y(t)=a*cos(t)(k*t)
Some people say the damping should be logarithmic. I think it should be linear because the main source of damping (kinetic friction of the pen sliding on the paper) is constant regardless of amplitude and velocity. I cannot calculate the damping by the ladder, this is a problem.
Note: It's a good idea to have 't' go from - to 0. This way the thing slows to a stop.

That is the type of pictures drawn in the museum. My contraption was more complicated because it also oscillated along the blue arrows. Unlike the others, the period of this oscillation depends mostly on the moment of inertia of the weights along a vertical axis. I could change 'I' easily and very precisely by moving some smaller weight further or closer to the center (see the gray weight in the first figure). It was convenient to set this oscillation to be around twice the other oscillations.

Assuming that the Blue arrow oscillation is harmonic (like a normal pendulum it is not, but very close at small angles) then the angle 's' that the pen will move is:
f=(constant, depends on 'I', f is almost 2); j=damping (Note: this motion was somewhat less damped by the ladder than the green and red, so it gets its own constant);
s(t)=cos(t*f)*(j*t)
When the green and red arrows are zero:
r=(distance from center to pen); m=(amplitude);
y(t)=r*sin(cos(t*f)(j*t))m
x(t)=r*cos(cos(t*f)(j*t))m

To get the complicated motion simply add these to the original parametric formula.
x(t)=a*cos(t*b)(k*t)+r*cos(cos(t*f)(j*t))m
y(t)=a*cos(t)(k*t)+r*sin(cos(t*f)(j*t))m

So to get different output, I simply tied the string to a different weight (thus changing 'b') or moved the small weight around (changing 'f').

I could also push and twist harder or softer (changing a, and m respectively). Another way to change the output without changing the string arrangement was to change the direction of the initial push (ranging between tangent to the center and directed at the center). This simply adds two constants (h,g) on the inside of the parenthesis, one for initial twist position/velocity and another for initial amplitude/velocity.
x(t)=a*cos(t*b+h)(k*t)+r*cos(cos(t*f+g)(j*t))
y(t)=a*cos(t+h)(k*t)+r*sin(cos(t*f+g)(j*t))

Calculating all these constants would have been rather difficult considering that the only measuring device I had was a thermometer. Instead I just guessed from the way the graphs looked (with practice, a quick look at the graph will shout out what is happening).

Heres an example.
With 2 Axis's of motion (red and green): x(t)=cos(t*1.03)*t
y(t)=2*cos(t)*t

x(t)=cos(t*1.005)*2*t
y(t)=cos(t)*2*t

With 3 Axis's of motion (red green & blue)
x(t)=cos(t*1.01)*2*t-25*sin(cos(t*2.06)*0.001*t)*5
y(t)=cos(t)*2*t+25*cos(cos(t*2.06)*0.001*t)*5

Procedure

To raise the heavy weights to the exact height of the pen, the legs of that ladder could be slowly pushed together, with amazing leverage, raising the weights hanging from it to very precise heights.
Fresh paper was taped to the floor and the pen put in place.
Once set up, a short push was given to the pendulum; moments later, the pen was dropped to the paper. It would swing for about 10 minutes before coming to rest in the center.

Parameters I Could Change

The amplitude of the push and the amount of weight can be changed to decrease or increase the time before friction stops the motion.
The push could initially direct the pendulum in approximately a straight line, an ellipse, or anything in between.
The strings could be tied to weights of different heights to adjust the difference in frequencies. Tying with the green string in figure 1, will result in a longer period than tying with the blue string.
The amplitude and initial conditions of the third oscillation (the blue arrows in figure 3) could be set in the same way as the previous two.
The frequency could also be easily tweaked by sliding the weights along the barbell, changing its moment of inertia. It was convenient to set this frequency to about twice the others, but with an extra barbell I managed to get them about equal. This made very different looking graphs.

Discussion

The assumption of linear damping is not completely correct. The swaying ladder and possibly air resistance damped the motion as some function of the amplitude.
The assumption of simple harmonic motion is not a perfect model for a pendulum. It is only a good approximation only for small amplitudes. The same applies to the third oscillation.
In the earlier models with low weight, and a considerable frequency differences, the lines were spaced far enough apart that the third oscillation could be largely ignored. Upon increasing to 45 kg, the lines were so closely spaced they overlapped no matter how carefully I tried to minimize its motion, see figure ___. By setting this frequency to match one of the others, the same error margin is still there, it is only very difficult to see.
I say it was hung from two strings but in reality it was hung from two string loops, making four. Since I bound the two strings together at the base and top, I thought it would not make much of a difference. In general though, the frequency difference would lessen slowly over time as the knots loosened. This is because the motion described by figure 2 began to look just a bit like the motion in figure 1. This increased the frequency ever so slightly, but the effects were quite noticeable in the graph. For example. figures __ and __ were made with the same arrangement, but at different times.
If you really read all this, I'm flattered, so make sure to let me know.

The Output Hung Up In My Living Room

Click for larger Version.
I have lots more of them. If you want to see, ask and I'll scan some more in.

Some Computer Graphs:

Note: I'll find the constant parameters much more carefully when I have more time.

The Apparatus:s:

While Drawing

Close up while drawing

I attached to pens at the same time here.

A setup with less weights

A setup with a large difference in frequencies

This shows what I did to lower the twisting frequency (f) to equal the back and forth frequency instead of being double it. The pictures it drew with this configuration were significantly different.

See the old version of this page Here.