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Electron Entrapment

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    t the moment we e!ploit electrons " generally " by burning stuffto generate electrical streams which we then distribute over gridsand circuits in order to get them to do wor#$ to power-up our lives.

    %ut why should we need to generate electricity at all when the

    electron is so abundantly " and freely " available&

    'e do not need to generate electricity.

    'hat we do need is to devise a way to simply collect it.

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    (ow are we loo#ing at a comple! methodology here&

    )o we need to devise an intricate device manufactured from rare,

    e!otic materials to achieve our desire&

    'hy would it have to be so&

    *erhaps there is " already in e!istence " a phenomenon that we could

    imitate. Some natural propensity or even a physical law that we couldturn to our advantage.

    'ell " we are here tal#ing about harvesting electrons right&

    nd there is " indeed " a model, a paradigm upon which we couldbase our own design.

    +his model lies hidden in plain sight. ou will have missed it becauseyou happen to be standing on it. Its called *lanet arth.

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    *lanet arth receives " or collects " electricity: in the form of*lanet arth receives " or collects " electricity: in the form of

    charged particles /electrons0, from the Sun all the time.charged particles /electrons0, from the Sun all the time.

    Most of this electricity arrives in a fairly steady stream that we callMost of this electricity arrives in a fairly steady stream that we callthe Solar 'ind.the Solar 'ind.

    +here are times, however, when this electrical material1energy+here are times, however, when this electrical material1energy

    arrives in massive blasts. +his happens when the arth ta#es aarrives in massive blasts. +his happens when the arth ta#es a

    direct hit from a 2oronal Mass 3ection /2M0: a huge cloud "direct hit from a 2oronal Mass 3ection /2M0: a huge cloud "which can weigh many millions of tons " of charged particles andwhich can weigh many millions of tons " of charged particles and

    super-heated gas.super-heated gas.

    Our focus here, though, is on the interaction between the electronsOur focus here, though, is on the interaction between the electrons

    that arrive from the Sun and the arths magnetic field.that arrive from the Sun and the arths magnetic field.

    +his is the model that we need to emulate.+his is the model that we need to emulate.

    Magnetism is the KeyMagnetism is the Key

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    Some curious and rather fortunate facts

    about magnetism and electrons.

    Magnetic flux will always take the shortest route possible to get

    where it needs to go.

    Electrons are attracted by magnetic fields.

    Electrons will flow spiral around magnetic force lines in the

    direction of the magnetic flux.

    Electrons moving through space or some other medium

    generate a magnetic field.

    rgo:

    Magnetism and electrons are self-reinforcing phenomena.

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    *ut simply:

    The stronger the magnetic field the

    more electrons will be attracted to it.

    The more electrons that are attracted

    the stronger that magnetic field

    becomes.

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    So using lanet Earth as our template let!s devise a way

    to entrap electrons.

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    Our first component isa hollow silica glasssphere.

    Silicate mineralsma#e up 456 of thearths 2rust.

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    (ow we need a component designed to emulate the arths moltencore.

    +he problem here is that nobody has ever seen it.

    In fact " we dont actually knowanything for sure about it either.

    ll we have are theories about the composition of the core and the

    way in which it generates the arths magnetic field.

    (ot to worry.

    I thin# I have found a solution to this dilemma.

    Instead of the postulated ball of molten iron " we will, instead, utili7ethe configuration and properties of a /toroidal0 ring magnet.

    My reason for choosing this configuration will " I hope " become clearas we progress.

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    So here we see ourring magnet within theglass sphere.

    It will be held inposition usingmagnetic

    repulsion1suspension.

    *lease note: all magnetspossess a (orth andSouth *ole.

    Our ring magnets (orth*ole corresponds with

    the rings upper surface.

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    'e now need to loo# at other configurations of magnet andunderstand something of the way in which magnetic forces /flu!0move both through and around magnets.

    +his image represents a simple bar magnet and the way in which themagnetic flu! " represented by the flow lines " travels from the magnets(orth *ole to its South *ole. +he direction of flow between the two poles isalways the same. 'hen travelling through the magnet the flow is South to(orth. 'hen travelling around it " through the air " the direction is always

    (orth to South.

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    The !"! Magnet.

    Ive chosen this shape /NBwhich will be modified as we progress0 for our third

    element: the 2 magnet, because with it we can physically model the actualshape of the arths magnetic field - which is essentially the shape of a ringdoughnut /tech spea#: torus0.

    'ith the 2 magnet, magnetic force flowing around it is negligible due to thepro!imity of the (orth and South *oles to each other. ll the (orth to South flu!is: instead, concentrated directly between the poles. /Indicated by the redtriangles0

    'e will be using multiple instances of the 2 magnet in our design.

    (orth *ole

    South *ole

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    However, before we ta#e a loo# at how the 2 magnets are to be arrangedwithin our electron trap we need a little more information on how magnetsbehave when in close pro!imity to one another.

    +a#e a loo# at the diagram above. ou will see that when the (orth andSouth *oles of two individual magnets are brought together the magneticforce between them is one of attraction.

    +he opposite becomes true when li#e poles /(orth to (orth1South to

    South0 come into contact. +he force becomes repulsive.

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    'e are now ready to integrate our third element: the 2 magnets, into ourdesign.

    +his illustrates how the ring magnet is suspended within the system. Its(orth /(0 pole /upper surface0 is repulsed by the 2 magnets ( poles and its

    South /S0 pole /lower surface0 is " li#ewise " repulsed by the 2 magnets.

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    *lease note the 2 magnets shown here are fi!ed: actually embedded in theglass sphere, whilst the ring magnet is left free to rotate.

    +here will also be more than 3ust two 2 magnets used in the system.

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    *lease be aware that the diagrams I am showing you are only intended toillustrate the principles related to electron entrapment in a general way. nactual " nuts and bolts " system might loo# a lot different to what I amshowing you here.

    'e need now, also, to modify the configuration: the physical shape, of the2 magnets in that ring above so that the twelve individual magnetseffectively become one.

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    +his 2 magnet configuration is crucial to the success our design.

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    +his is what it allows for. +he magnetic flu! originating from the(1pole of one magnet now flows to the S1pole of the ad3acentmagnet. 89 individual magnets have now become a single, circular/closed0 magnetic heli!.

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    Here we see the magnetic flu! flowing from the 2 magnets (1polebeing flared-out /ie: forced to go around0 by the flu! flowing from thering magnets (1pole.

    In both cases theflu! has to reachthe respectiveS1poles of bothmagnets.

    )irection offlow indicatedby arrows.

    /cross-section0

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    Here we are loo#ing at the ring magnet in cross-section. (ow we can seethat " although the respective flu! flows from both magnets originate from(1poles " both are travelling in the same direction.

    +he red arrowsindicate 2

    magnet flow.

    +he whitearrows indicate

    ring magnet flow.

    The pink arrows indicate the combined flow of both magnets.

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    *in# arrowsindicate directionalflow of combined

    flu!.

    'e need to#now...

    ...what happensto the combined

    flu! flow in thatcentral area.

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    'ith the three diagrams that you have 3ust seen we first loo#ed at the flow ofmagnetic flu!: from both the 2 and ring magnet (1poles, and how oneaffected the other.

    (e!t we loo#ed at the mid region " where the flow direction of the flu! fromboth types of magnet essentially merges or comes-into-phase.

    inally we loo#ed at the lower region where the flow from the magnetsreaches its target destination: the S1poles. %ut what " e!actly " is going onhere isnt immediately apparent.

    'e #now that the flow from both magnets has to reach their targetdestinations " but how is this to be achieved when it would mean that the in-phase, combined flow has to move in two seperate, e!actly opposite,directions to do so&

    +here is really only one answer here. t the point where the combined flow isforced to split into two seperate streams a region of e!tremely low magneticdensity forms as a result of the split.

    /NB: *lease remember that a magnetically repulsive region needs to be

    maintained in this area.0

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    +his leads us on to another ;uestion. 2an a magnetic field tolerate thee!istence of such a region within it& 'e all #now nature abhors a vacuum.2an a relatively dense magnetic field tolerate the presence of such adrastically lower density volume&

    +he answer is " most certainly " no: it cannot.

    So how is this situation to be resolved&

    Simple.

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    'hat needs to be understood here is that this system: although constructedfrom several components, only e!ploits a single magnetic field. ll thecomponents are connected by the magnetic flu! flowing both through anaround them.

    Once the only moving part in this system: the ring magnet, is set in motion itneed never stop.

    s it spins it will accelerate. +he magnetic field around the ring magnet will

    become a vorte!. +he vorte! will reach out beyond the confines of the systemto draw in electrons. s more and more electrons are drawn into the systemthe ring will accelerate faster and faster and the magnetic field will begin tointensify e!ponentially.

    %efore long the electrical charge within the system will need to e;uali7e$ to

    discharge.

    So now Id better show you how we are going to get that electricity out of thesystem and into the 'orld.

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    +his is how well do it.

    lectricity: li#e magnetic flu!, will always follow the line of leastresistance. So we simply provide a preferred route for it to follow out ofthe system.

    +erminals embedded inthe sphere allow power tobe harvested.

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    (ow I have a favour to as# of you.

    If you thin# the the ideas that I have set out here have any merit whatsoever$

    could you please help me transmit these ideas to the 'orld&

    2ould you please save a copy of this pdf to your drive and send it on to a fewof your friends&

    +he design that I have illustrated here represents an idea whose time hascome.

    +he 'orld is ready.

    +he time is now.


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