(Magnetism excerpt)
by
Sean Sinjin
© Copyright 2003, Sean Sinjin.
All rights reserved. Edition 1.5
ISBN 0-9762271-0-X
No
part of this writing may be reproduced, stored in a retrieval system, or
transmitted by any means, electronic, mechanical, photocopying, recording, or
otherwise, without the express written permission of the author.
Meme,
much like our perspective on reality, is an ever-evolving story. Be sure to visit us on the Internet at:
for
revisions, as Meme continuously changes to reflect reality as accurately as
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{Note to reader: Please be aware that the target audiences for this writing are people that are not very well educated in the sciences, and as such the nomenclature may not be representative of typical scientific literature. This is in the attempt to express these complicated theories with terminology that would be more familiar and digestible to the typical layperson. In order to best understand the concept of ‘Relativistic Bether’, please read the Gravity Web Excerpt prior to reading the text below}
Some atoms can be magnetic. When electrons spin
around the nucleus (or any particles moving through bether for that matter, but
for our example we’re going to focus on the electron), they cause a “drag” on
the bether that they pass through. This
is not to say that they experience friction, but rather the temporary
displacement of the bether that their presence causes is not equally shaped in
front and behind the path of the electron (from a point of reference where the
electron is moving; we’ll get to that in more detail later). This causes a little bit of bether
to stretch with the electron before more slowly returning to its original
position.
Particle speeding through bether
The same amount of bether is displaced in front as it is
behind, however,…
A: …bether behind the particle expands slower than the rate
it was originally stretched…
B:
…in front of the particle, hence bether is “dragged” somewhat behind the particle
The
net energy used to displace the bether in front of the electron is perfectly
balanced with the returned energy behind it so the electron does not lose any
energy; however, because of the extremely small radius of atoms, the bether is
constantly being pulled and stretched around the atom in the direction of the
electrons’ rotation.
Electron
“drag” causes the bether within its circumference to be somewhat twisted
You may be wondering what keeps these electrons moving in and between shells.
Bether is constantly in a fluctuating state, in regards to its ambient pressure. At the resolution that
we humans can physically sense the dynamics of bether (as in gravity, or light
waves), it feels pretty consistent, but at the atomic level, there is a
constant bombardment of alternating waves of high and low pressure bether (just like a buoy bobs
around on a ceaseless ocean). There are
magnetic fields (regions of twisted bether), as well, that the electrons are
perpetually compelled to react to, keeping them actively seeking the best
balancing point within their current shell.
It may seem that this dragging bether along with an
electron might slow it down but everything is relative, meaning that if you
were capable of rotating your point of observation to match that of the
orbiting unpaired electrons around an atom (as absurd as that notion is), that
atom would not be magnetic, relative to you, and the electron would also no
longer be dragging any bether, relative to you.
So, what may seem like friction from one perspective, is frictionless
from another. More on “frame of reference” is coming
up.
Now for simpler atoms, the electrons will fill each shell’s orbitals (an orbital is kind of like a subshell within a shell)
in pairs, and each half of a pair opposes and cancels the effect of the other
half's drag. Hence, the atom balances
out to having no charge (neutral).
A: Shell
B: Orbital
C:
Each orbital has a maximum of 2 electrons that orbit in opposite directions so
as to counteract each other’s bether drag
It should be noted that orbitals are not necessarily
spherical but that some orbitals are discrete regions within a shell where an
electron may be found. For our purposes,
it will suffice to simplify their structure to spheres for clarity.
In
the heavier elements however, electrons will not always fill in the shell’s
orbitals in pairs, and instead some orbitals will have just one electron. These solitary electrons are responsible for
shifting the atom’s balance from a non-charge state to a magnetic charge state since
their bether-drag is not being counteracted by an opposing electron in their
same orbital. The bether is forever
chasing these solo electrons in the attempt to equalize the imbalance of bether
pressure caused by the electron’s drag. The net result of this chase is that a magnet is formed from the
perpetually twisted bether in the atom.
The more unpaired electrons you have that are orbiting in a common
direction, generally the farther the bether will be twisted
around the atom and hence the greater the magnetic charge.
An analogy would be to place a ball on our blanket (the ball representing the entire atom) and then rolling it to
wrap itself up in the blanket, forming opposing twists in the blanket on each
side of the ball. This isn’t to say that
the blanket keeps getting twisted indefinitely around the ball, but that
eventually the blanket will not stretch any further and the ball will just spin
inside the wrap of blanket.
A: Blanket wraps around the ball much like bether wraps
around atoms with unpaired electrons
B: Ball rolls in this direction
C:
Blanket wrapping the ball forms opposite twists on each side of it. This demonstrates how bether is twisted to
form negative and positive charges, hence a magnet
This
example simulates how an electron’s drag within an atom can wrap bether around
the atom. Put gagillions of magnetic
atoms together into an object with the majority of these atoms all aligned in
the same direction, and you will now have a large “sum of parts” magnet as all these atoms combine their bether twisting
efforts into one large twist that wraps the entire object.
The atoms of most metals have a large number of
electrons orbiting about their nucleuses and this makes them natural candidates
for being magnets; however, in solid metal, the atoms are mostly jammed all
together haphazardly and are pointing in all directions, fighting each other
for their individual preferred magnetic orientations.
A: Magnetically neutral object (e.g., an iron bar)
Disarrayed
magnetic atoms cancel the magnetic effects of each other on a large scale
Some
metals, however, were formed in high temperatures where the metal was molten
for a long enough period of time that the magnetic pull of the earth aligned
the atoms before the metal had a chance to cool and solidify. When these metallic pieces cooled, their
atoms remained aligned, locked in position, and as a whole became a large
powerful natural magnet with all the atoms pointing together in a common
direction.
A: Magnetized object (e.g., a magnetic iron bar)
Symmetrically
aligned magnetic atoms create a large magnetic object overall
Natural
magnets will attract non-magnetized metals since the magnetic field is strong
enough to force some of the non-magnetized metal’s particles to break their
position and rotate into proper orientation (negative facing positive), and
this passes on a little bit of that magnetism from the magnet to the other
metal.
Around anything magnetic exists invisible “force” lines
A:
Force lines are formed around magnets
caused
by the layers of wrapped bether that surround a magnet, like our previous blanket-wrapping
analogy. What differentiates magnetized
from non-magnetized metal is that a magnet simply has a significant number of
its atoms aligned so that these atoms collectively twist bether around the
object, all in the same direction; and it does this on such a scale that we can
actually see it with our own eyes. This
effect of magnetism can be observed by placing a magnet under a piece of paper
and then spreading metal filings on the paper. The
metal filings will be attracted to the regions of strongest magnetic pull,
which are between the layers of overlapped bether that wrap the magnet.
So how exactly does a magnet attract or repel other
objects? Using our rope again, hold it stretched between your two hands, then have another person grab
it in the middle and start twisting it by rolling their fist backwards so that
the halves of the rope start forming opposite twists. They shouldn’t twist so far as to create
loops (particles) but just enough to add significant twisting strain to our
rope. Their twisting action simulates
the effect of unpaired electrons orbiting around an atom, and the rope
demonstrates the twisting that the bether around the atom endures because of
the electrons’ motion.
A: Person A holding the rope at both ends
B:
Person B rotates hand to add twisting strain to rope
Now you have a magnet, or at least the simulated
effect of forming a magnet from bether.
Note that the rope does not shorten in length as it would if you
continued to twist until a loop formed.
Now get a couple more people to do exactly the same thing but with
another rope, and now you have two “rope” magnets.
A: Person A holding the rope at both ends
B: Person B twisting rope
C: Person C holding an identical rope to person A’s
D:
Person D twisting rope identically to person B
Take
the end of the rope in your right hand and attach it to the end of the rope in
the left hand of the person holding the ends of the other rope, and then both
of you let go of the newly attached ends.
E: Attach ends of twisted ropes
F:
Since they are opposite twists (charges, poles, etc.) they unwind themselves,
relieving the twisting strain
The
rope section between the middle pair of hands immediately unwinds itself,
releasing all the twisting strain that was applied there. This is the same as what happens when you
bring opposing ends of magnetically charged atoms together (remember, charges
are simply twists of bether); they unwind each other’s adjacent charge. The closer the magnets are together, the
greater the relief to the twisted bether, and so the magnets are elastically pulled together with great force as the bether untwists—unlike gravity, which pinches things together from outside.
To continue where we left off, now the two attached
ropes as a whole act like a single larger magnet due to the fact that the two
hands that added the twisting to each individual rope now combine in their
twisting efforts. To parallel this to
our magnetic atoms, bringing the oppositely charged ends of these atoms
together will combine the bether twisting effects of the unpaired electrons of
both atoms, essentially creating a larger unified magnetic field. Unlike our rope, however, it is impossible
with bether to separate the attached ends to end up with a single charge (a
monopole) on each side because once the magnetic charges (the ropes) are
separated again, they each reform into individual bipolar magnets since there
no longer is a proximal opposing charge to counter the twisted bether (magnetic
field) that forms on both sides of a magnetic atom. So to emulate this in our rope example,
return the hands that were removed and as the ropes are separated, re-twist
them to re-form the original charges.
E: Re-twist the rope, then…
F:
…separate the ends. This simulates the
effects on bether from pulling magnets apart
This
simulates the resistance that you feel when pulling real magnets apart, which
is the bether resisting the re-twisting motion.
The exact opposite happens should you bring similar
magnetic poles together. The closer you
bring them, the more the bether has to contain the same number of twists within
a decreasing distance; these twists being the same direction, they can’t unwind
each other.
E: Person C rotates the entire length of the rope, such that
the opposite hand is now adjacent to the end of Person A’s rope
F: Hands and twists are now opposite
G: Attach the ends
H: Ropes can’t unwind because twists are in same direction
(same charges)
I:
Sliding B and D’s hands together along the rope will shorten the length of rope
between them but not the number of twists.
The closer the hands are together, the more the twisting strain
increases on this section of rope, which resists the action of bringing the
hands together. This simulates how
bether resists being twisted. When two
same-charged magnetic ends of atoms (or objects) are brought together, bether
will try to push them apart to relieve the twisting strain being imposed by the charges
Ultimately,
with enough strength, the magnets could be forced into direct contact with each
other and this would provide the greatest amount of bether twisting resistance,
better known as magnetic repulsion. Bether
can provide powerful resistance to being so twisted, and the instant the
magnets are released from their forced proximity, the twisted bether
immediately acts like a spring, pushing the two magnets apart.
Photons are largely unaffected by magnetic fields because although the bether
is twisted, it still occupies the same volume as if it weren’t forming a
magnetic field, and therefore it’s still the same average pressure as untwisted
bether. It’s only when photons go
through a gravitational field where the bether is actually stretched, like the
gravity field that surrounds an object, that photons will pursue the path of
least pressure towards the most stretched bether. This gives observers the impression that the
photon was attracted by the object when in fact it was pinched toward the
object by the higher pressure bether on the outer side of its path.
A: Photon unaffected by magnetic field since the average
bether density in the magnetic field has not changed, despite it being twisted
B:
Photon pushed towards object as it passes between the object and the less
stretched bether on the outside of its path
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