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#10. Principles of the Magnetic Trapping
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(Files in red–history)  Index
7. Plasma
7a. Fluorescent lamp
7H. Langmuir, 1927
8. Positive Ions
8H. Arrhenius, 1884
9. Magnetic trapping
9H. Poincaré, 1896
10. Trapped Motion
10H. Einstein, 1910
10a. Particle Drift
11. Explorers 1/3
11a. Geiger Counter
12. Rad. Belts
12H. Argus 1958
12a. Inner Belt
12b. Outer Belt
13. Fast Particles
14. Synch. Orbit
15. Energy
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Circular Motion
Because the force is perpendicular to the velocity, it can only change the direction of motion, not its speed or energy. Because no energy is needed to keep up the motion, it can (in principle) persist indefinitely.
In addition, however, there will also exist a small force parallel to the axis, repelling the particle away from the tip of the cone. That added force gradually slows down the particle's advance down the axis and finally reverses it, causing it to "mirror" and bounce back.
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Throughout all this, the total speed of the particle stays unchanged. Out in space, it usually takes electric forces, not just magnetic ones, to change the total speed and energy of the particles.
It turns out that the product T x E, the period T times the energy E, is
almost a constant. It is not an exact constant, like total energy in a system, but if the rate of change is slow enough, e.g. if the string is pulled rather slowly, it comes very close.
The motion of electrons and ions spiraling around magnetic field lines is also periodic. While the period of a pendulum changes when its string gets longer or shorter, that of a spiraling ion or electron changes as it moves into regions where the magnetic field is weaker or stronger. Just as for a pendulum the product T x E stays very nearly constant, so here too, a certain quality, an "adiabatic invariant," is almost kept at a constant value. From that constancy it is possible to deduce the "mirroring" of particle and many other properties of their motion.
That is somewhat similar to the case of the lowered support, but the calculation gives a diferent rate. With the lowered support, work is also done--but that happens when the weight is pulled in from the sides to swing in a shorter arc, not at the bottom of the swing.
The process described here is related to the way children "pump" a swing to make it go higher. The child moves arms, legs and body in a way that works against the centrifugal force, and the energy invested in overcoming this force ends up producing a more energetic swinging motion.
(This is a highly simplified explanation and assumes that from the point of view of the child in the swing, nature behaves exactly the same as anywhere else, only a centrifugal force is added. The actual situation can be more complicated.)
Furthr Explorations The "Exploratorium" science museum in San Francisco has a small swing (too small to carry a person) that can be "pumped" from the outside. The seat of the swing, instead of hanging by two ropes or chains, is attached to the axis by two smooth parallel rods.
Above the regular swing seat is a second seat, with two wide holes threaded by the two rods. Under normal circumstances, the second seat will drop to the bottom, on top of the regular one. However, a rope is connected to its middle, going over the bar from which the swing hangs and down again, and a person standing next to the swing can pull that string or let it go, making the second seat rise along the rods or fall down again.
With your hand, you set the swing moving with moderate motion. Now, by pulling the rope or letting go at suitable times in the oscillation, you can easily "pump up" the motion. You only need to pull the swing up when it passes the lowest part of its motion, and let it down again at the extreme ends of its motion, when for a brief instant it is at rest.
Next Stop: #10H. Motion of Trapped Radiation--History Author and Curator: Dr. David P. Stern
Adiabatic Invariants
There exists a different and somewhat more abstract manner of reaching the same result. The period T of rotation, the time required by the particle for one circuit around its guiding field line, becomes shorter as the particle approaches the tip of the cone. After all, the total speed of the particle is unchanged, its rotation speed nearly so, while the distance covered by one circuit gets shorter and shorter near the tip.
In the theory of motions, this is an example of a periodic motion whose period gradually decreases. The best-known periodic motion is the back-and-forth swing of a pendulum, say of a weight suspended by a string (drawing). The shorter the string, the shorter the time of each swing ("period"), which goes like the square root of the length. One can replace the support point with a pulley wheel, which is gradually lowered and its string shortened (ignore the word "pull" which is explained further below). The bottom of the swing stays in the same height, but the period gets shorter and shorter.
Note on the above illustration
Many books give this example but state that the string is pulled up, over the wheel, while the pendulum is swinging. This is a more complex situation. As the pendulum swings, it generates a centrifugal force, and the pull on the string, besides lifting the weight to a higher average position (which increases the potential energy), also has to overcome the resistance of the centrifugal force. That requires an extra input of energy from the force pulling the string, and since energy has to go somewhere, it makes the swing of the pendulum more vigorous.
Last updated 25 November 2001
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Mail to Dr.Stern: education("at" symbol)phy6.org
Co-author: Dr. Mauricio Peredo
Spanish translation by J. Méndez
Re-formatted 9-28-2004
