It's been a while since our last electromagnetic adventure, and hope the few weeks in between have
provided enough time to have your batteries recharged (no pun intended). This week we explore the phenomena
of magnetic levitation in the realm of a superconductor. Since the topic may be foggy for many people (pun
intended this time), click here to
show further explanation on the topic.
About Magnetic Levitation
Magnetic levitation can be achieved either one of two ways. The naive approach (and I say that from
experience) is to take two magnets and attempt to balance them with like poles repelling each other.
As anyone who has tried this knows, the magnets never balance quite completely and the attempt is rather futile.
This can be slightly improved upon by using a gyroscope to balance to the hovering magnet, as is done in the
popular Levitron--though this too is rather finicky and
frustrating at moments. The bottom line is such contraptions are inherently unstable, and the unstable
equilibrium of such approaches is summarized mathematically by Earnshaw's Theorem.
The second and better way to go is to induce an electromagnet that will repel the physical magnet instead.
This is achieved through magnetic induction: as a magnet is lowered towards a conductor eddy currents
are induced according to Faraday's and Lenz's Law to repel the magnet being lowered. Why might this way be
more stable you ask? The induced electromagnet effectively allows for more "degrees of freedom" as the
eddies are induced in all directions, in just the right way to repel the magnet. In short, Nature does the work
and she always does it perfectly.
Alternate high-res version.
Magnetic levitation is not confined to superconductors and can be achieved, for brief moments of time,
even with highly cooled, non-superconducting materials such as copper.
The eddy currents induced under normal circumstances however die out quickly as a result of the electrical
resistance present within all conductors (like aluminum, copper, gold, etc). However in a superconductor--a
material in which there is zero (yes, exactly zero) electrical resistance--these currents persist
and continue to levitate the magnet perpetually. These persistent currents allow the electromagnet to push
on the physical magnet indefinitely, and thus are the critical advantage to magnetic levitation
using superconductors.
A copper stand is bathed in a sea of liquid nitrogen, supporting a curious, black disc
of Yttrium Barium Copper Oxide (YBCO). The copper being an excellent conductor, chills the YBCO that rests
above it to liquid nitrogen temperatures while safely keeping it from being submerged in the liquid.
YBCO, a manmade superconducting material discovered in 1987, is
unique among its kind due to its relatively high superconducting-transition temperature of 93 K; though that is
still colder than our South Pole, temperature is "high" enough for scientists! YBCO's high
transition temperature saves scientists the trouble of procuring unwieldy
novel methods to study superconductivity, and instead enables them to use the readily available supply of
liquid nitrogen, whose boiling point is mere 77 K in comparison.
A levitating magnet is surely fun in its own right, but sadly does not make an interesting question.
A non-conducting piece of plastic is used to give the magnet a small torque allowing it to spin freely
in midair, as can be seen in the video above. Two pieces of white tape are used to mark the direction of rotation.
The question: What would happen instead if the levitating magnet were given a torque along
the other axis of rotation?
You must, of course, explain your answer to the best of your ability
using physics laws and ideas.