Captured Lightning - Lichtenberg Figures

Lichtenberg Figures are branching electric discharges (or electrical trees) that are sometimes preserved on the surface or the interior of a solid dielectric. They are named after the German physicist Georg Christoph Lichtenberg, who originally discovered and studied them.

One way that they can be produced is as follows: A sharp-pointed needle is placed perpendicular to a non-conducting plate, such as of resin, ebonite, or glass, with its point very near to or in contact with the plate, and a high voltage Leyden jar (a type of capacitor) or a static electricity generator is discharged into the needle. The electrification of the plate is now tested by sifting over it a mixture of powdered flowers of sulfur and red lead (Pb3O4 or lead tetroxide).

The negatively electrified sulfur is seen to attach itself to the positively electrified parts of the plate, and the positively electrified red lead to the negatively electrified parts. In addition to the distribution of color thereby produced, there is a marked difference in the form of the figure, according to the polarity of the electrical charge that was applied to the plate. If the charge was positive, a widely extending patch is seen on the plate, consisting of a dense nucleus, from which branches radiate in all directions; if negative, the patch is much smaller and has a sharp circular boundary entirely devoid of branches.

Modern Lichtenberg Figures can also be created within solid blocks of acrylic plastic (polymethyl methacrylate or PMMA) using a beam of electrons from a linear electron beam accelerator (or Linac, a type of particle accelerator). Inside the Linac, electrons are focused and accelerated to form a beam of high speed particles. Electrons emerging from the accelerator are moving an appreciable fraction (95 - 99+ percent) of the speed of light (relativistic velocities). The electron beam is then aimed towards an acrylic specimen. When the relativistic electrons hit the acrylic, they easily penetrate the surface, slowing down as they collide with the molecules inside the plastic, and finally coming to rest deep inside the specimen. Since acrylic is an excellent electrical insulator, the electrons inside the specimen are temporarily trapped. Under continued irradiation by the beam, the excess electrons form a plane of negative charge inside the specimen. As the charge builds, the effective voltage inside the specimen can reach millions of volts. Ultimately the huge electrical stress exceeds the dielectric strength of the plastic, causing it to suddenly become conductive in a process called dielectric breakdown.