Image Gallery

Mike Henderson



One of the things I like best is to be able to take a mathematical object and visualize it. Other pages at this site deal with the math, this page is just a bunch of pictures that I have made.

Also check out the pages (mine)


Click on the images to see a larger version (or in some cases an animation).




These first are from a study of the equilibrium configurations of an elastic rod which is clamped in such a way that the two ends of the rod lie on a common line. A force can be applied (either pushing the ends together or pulling them apart), and two torques (one twisting the rod and the other bending it).


The result is a surface in the parameter space (force and two torques). The surface is complicated, and each point on the surface corresponds to a shape of the rod. The surface does not cross itself, but in this projection onto the parameter space it appears to,


The following images give some idea of the shape of the surface.


Image of the surface of twisted rod configurations

Image of the cnfiguration space of the twisted rod

Another view




The next example is the motions of a pair of pendula on a common axle, coupled with a spring. There are three parameters, the strength of the spring (k, fixed in the images below) and two torques (I1, I2) applied to each pendulum respectively (the horizontal plane in the images below). The vertical axis bellow is the period of the motion.


The first image is the surface of stationary points (where the pendula don't move) and show the separation of the pendula as a function of I1 and I2.


Surface of fixed points of the coupled pendulua



In the image above the spring strength k is fixed. If the surface is projected down onto the (I1,I2) plane and the fold lines are drawn (i.e. where the number of stationary points change), and k is allowed to vary, we obtain the image below.


Surface of folds on the surface of fixed points



Finally (for the pendula) is the surface of period as a function of (I1,I2) for fixed k.


The surface of period as a function of the two torques



And some snapshots of the algorithm used to compute the surface:


An incomplete computation of the surface




Sphere Computation
Torus
Spacing Points on a Plane

A piece of the surface of clamped rod configurations

The union of a set of balls on three different trajectories of a flow and the corresponding dual

Coordinate and parameterization surfaces computed  for an invariant torus

Simplicial Continuation (isosurface) applied to a sphere

The (2,4) mode interaction in Taylor-Couette flow

An invariant torus

A view of a (1,4) resonance tongue

Points on a sphere with cubes of a set radius at each point

Points on a sphere with cubes of a set radius at each point. The outer faces have been removed to show the decomposition of IR^3

The same as previous, but with different colors

The cubes clipped against a slightly larger sphere. The fences are geodesics (the cubesare of a set radius)