Skip to main content
Sandbox Physics

Drawing mechanisms · Perpendicular slides

Trammel of Archimedes

On a trammel of Archimedes, where should the pen sit to draw a circle? At the midpoint of the arm, halfway between the two shoes. Each shoe slides back and forth in its own slot, and a pen on the arm combines the two motions: its sideways swing equals its distance from the shoe in the vertical slot, and its up-down swing equals its distance from the other shoe. Halfway, the swings are equal and the ellipse becomes a circle. A pen on a shoe draws a straight line.

Two shoes slide in perpendicular slots, joined by a rigid arm. Move the pen along the arm to draw a slender ellipse or turn it into a circle, or put the pen on a shoe and watch the path collapse into a line.

Interactive modelTrammel of Archimedes
Pen horizontal position00
Pen vertical position00
Pen speed00
Pen acceleration magnitude00
Shoe pivot distance00
Path eccentricity00
Local path curvature00
Largest constraint residual00

Physics tutorial

A rigid arm makes a family of curves

BackgroundThe links and joints of a mechanism can build a geometric construction into its motion.

Why it mattersFollow the pen first, then check the rods that hold it on its path.

Start with the essentials

Focus question
Where must the pen sit to draw a circle instead of an ellipse?
One-sentence intuition
The two shoes give the pen two perpendicular sinusoidal components, and where the pen sits on the arm sets their amplitudes.

Core mathematical model

Positions of the two shoes

A=(Lcos⁡θ,0),B=(0,Lsin⁡θ)\mathbf A=(L\cos\theta,0),\quad\mathbf B=(0,L\sin\theta)

The distance between their pivots stays fixed. The arm's angle is the supplement of the parameter angle, which keeps increasing.

A pen fixed along the arm

Q=(1−t)A+tB\mathbf Q=(1-t)\mathbf A+t\mathbf B

The fraction is measured from the horizontal shoe toward the vertical shoe.

Semiaxes of the ellipse

a=L∣1−t∣,b=Lta=L|1-t|,\quad b=Lt

When the two semiaxes are equal and nonzero, the curve is a circle. When one semiaxis is zero, the curve is a line, not a regular ellipse.

Velocity and acceleration

Q˙=Lω(−(1−t)sin⁡θ,tcos⁡θ),Q¨=−ω2Q\dot{\mathbf Q}=L\omega(-(1-t)\sin\theta,t\cos\theta),\quad\ddot{\mathbf Q}=-\omega^2\mathbf Q

The angular rate is constant and positive, but the pen's speed is generally not constant.

Common difficulties

The pale curve is not a measurement

Typical misconceptionThe pale curve is an independent experimental check.

Better mental modelIt is the full path of the ideal model. The constraint residuals and independent geometric tests check that the model is consistent; no real data are acquired.

The motion is set directly

Typical misconceptionA smooth trace proves that a real mechanism can be driven safely at this rate.

Better mental modelMass, friction, contact forces, clearances and drive dynamics need a separate analysis. The thicknesses of the three-dimensional parts only show how the pieces are assembled.

Run the experiment

  1. 01

    Trace the default path

    Use the drawing-plane view, then play or drag the coral handle.

    What to observe: Each shoe stays in its slot while the pen follows an ellipse.
  2. 02

    Move the pen

    Compare the midpoint, slender and shoe presets.

    What to observe: The midpoint draws a circle; the shoe draws a line.
  3. 03

    Separate geometry from speed

    Increase the angular rate and export the phase sweep.

    What to observe: The pen covers the same path faster. Velocities grow in proportion to the angular rate, and accelerations grow with its square.

Geometry & apparatus: Il Giardino di Archimede · Peaucellier · Caltech · Elliptical Trammel

FeedbackSomething broken, confusing, or missing on this page?Tell us
What kind of feedback?

Sent with this page’s address, its Lab ID, the site language and your device type. Please leave out personal details. Feedback is kept for up to 12 months.Privacy policy