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Magnet Keeper

A magnet keeper is ferromagnetic bar placed across the poles of a permanent magnet that helps preserve the strength of the magnet by completing the magnetic circuit, and are particularly useful for magnets which have a low magnetic coercivity, such as AlNiCo magnets.

Keepers also have a useful safety function as they stop external metal being attracted to the magnet. Wikipedia, Magnet Keeper


Keely
"[Sympathetic Outreach] Is not induction. They are quite foreign to each other in principle. Sympathetic outreach is the seeking for concordance to establish an equation on the sympathetic disturbance of equilibrium. When a magnet is brought into contact with a keeper, there is no induction of magnetism from the magnet into the keeper. The static force of the magnet remains unchanged, and the action between the two may be compared to a sympathetic outreach of a very limited range of motion. The sympathetic outreach of the moon towards the earth, has a power strong enough to extend nearly a quarter of a million of miles to lift the oceans out of their beds. This is not the power of induction. [SYMPATHETIC OUTREACH - Snell]

"The keeper is first placed on the magnet, which has an attachment whereby a transmitter can be centrally associated with it; the other terminal having three connections that can be attached to this medium. The impulse is given simultaneously to the three leads after setting the instrument to represent forty-two thousand eight hundred vibrations on the harmonic, the same on the enharmonic and on the diatonic." [The Operation of the Vibratory Circuit]

"When a magnet is brought into contact with a keeper, there is no induction of magnetism from the magnet into the keeper. The static force of the magnet remains unchanged, and the action between the two may be compared to a sympathetic outreach of a very limited range of motion." [More on Keelys Theories]

"A magnet does not induct magnetism in its keeper this is merely sympathetic outreach of a very limited range."

"The time approaches when electric magnetic waves will be produced with an outreach of two feet, as powerful at that distance as is now shown when the keeper is almost touching the poles. These waves will demonstrate a radiating force too stupendous for measurement with present instruments." [POLARIZATION AND DEPOLARIZATION]

"The time is approaching when electromagnetic waves with an outreach of two feet will be produced, having an energy equal to that now shown up on the magnet when it is about to kiss its keeper, and showing a radiating force too stupendous for actual measurement." [ELECTROMAGNETIC RADIATION - Snell]

"A magnet does not induct magnetism in its keeper - this is merely sympathetic outreach of a very limited range." [7B.20 - Magnetism]

"''Maxwell's theory is correct that the plane of polarized light is the plane of magnetic force. The sympathetic vibrations associated with polarized light constitute the pure coincident of the plane of magnetism. Therefore, they both tend to the same path, for both are interatomic, assimilating sympathetically in a given time, to continue the race together, although one precedes the other at the time of experimental evolution. The time is approaching when electromagnetic waves with an outreach of two feet will be produced, having an energy equal to that now shown up on the magnet when it is about to kiss its keeper, and showing a radiating force too stupendous for actual measurement.’' ELECTROMAGNETIC RADIATION - Snell


A magnet keeper, also known historically as an armature, is a ferromagnetic bar made from soft iron or steel, which is placed across the poles of a permanent magnet to help preserve the strength of the magnet by completing the magnetic circuit; it is important for magnets that have a low magnetic coercivity, such as Alnico magnets.

Keepers also have a useful safety function, as they stop external metal being attracted to the magnet.

Most magnets do not need a keeper, only those with low coercivity, meaning that they are easily susceptible to stray fields.

Magnet can be considered as the sum of many little magnetic domains, which may only be a few micrometers or smaller in size. Each domain carries its own small magnetic field, which can point in any direction. When all of domain are pointing in the same direction, the fields add, yielding a strong magnet. When these all point in random directions, they cancel each other, and the net magnetic field is zero.

In magnets with low coercivity, the direction in which the magnetic domains are pointing is easily swayed by external fields, such as the Earth's magnetic field or perhaps by the stray fields caused by flowing currents in a nearby electrical circuit. Given enough time, such magnets may find their domains randomly oriented, and hence their net magnetization greatly weakened. A keeper for low-coercivity magnets is just a strong permanent magnet that keeps all the domains pointing the same way and realigns those that may have gone astray. Wikipedia, Magnet Keeper

See Wikipedia, Electropermanent Magnet

See Also


See Also


Cathode
Cohesion
Electropermanent magnet
Figure 16.08 - Two bar magnets becoming one magnet
Figure 17.03 - Analysis of the Octave Gravity Bar
Figure 17.04 - Gravity Pressure Recorder - Bar Magnet
Figure 7B.16 - Bar Magnets shown separate then joined as one
Figure 7B.17 - Multiplying Force to Poles of a Bar Magnet
Figure 7B.18 - Four Poles of a Bar Magnet
Magnet
Magnetism
Sympathetic Negative Attraction
sympathetic outreach

Created by Dale Pond. Last Modification: Friday September 30, 2022 07:37:16 MDT by Dale Pond.