GB2386764A

GB2386764A - Magnetic engine

Info

Publication number: GB2386764A
Application number: GB0221261A
Authority: GB
Inventors: Mark Andrew Newman
Original assignee: Individual
Current assignee: Individual
Priority date: 2001-09-14
Filing date: 2002-09-13
Publication date: 2003-09-24
Also published as: GB0221261D0

Abstract

A magnetic engine includes a housing 6 and a dynamo 4 or alternator. The engine may include a ring magnet 1, a ring of magnets 2, a magnetic shield 3, magnetic bearings 5, superconductors and electromagnet coils. The components may be latched together and the housing may include a vacuum. Alternative arrangements are also disclosed.

Description

-1- 2386764

I' - Magnetic Engine/Dynamo [] The invention seeks to provide a machine which transforms a high velocity kinetic energy into a low velocity kinetic energy, to a end to create a electrical energy by the said low velocity kinetic energy. A high velocity kinetic energy exists within any magnetic field.

A permanent magnets magnetic field degrades (magnetic fields emit as a

result of a magnetic materials self destructive chemistry i stray magnetic / electrical fields), this machine / invention is not a perpetual machine.

The invention utilises a magnetise magnetic materials incredibly high frequency' / 'tiny mass' active field, to provide a incredibly

efficient machine. A magnetised magnetic material should be classed a tiny wavelength (radio) active material: It will equalise and stop being active, or disappear as a consequence of.

Energy = matter; kinetic force = a velocity a matter has: A kinetic force without matter can achieve nothing (a kinetic force without matter is nothing): A energy without a kinetic force cannot achieve a field: A magnetic field

is a kinetic energy (has a mass and a kinetic force).

A magnetic field cannot be created by nothing: A high

velocity kinetic energy which exists within a magnetic field is transformed into a

low velocity kinetic energy by this machine / invention (not efficiently i incredibly efficiently compared to a combustion engine).

Alternate (to current theories) accurate theory has been filed separately to describe a realistic accurate physics / chemistry concept. Its relevance to these machines / inventions is it states indepth magnetic fields are like that of them

described above. This said theory has been filed separately to accommodate machines which validate its statements. '

A magnetic engine/dynamo provides a great amount of free and pollution free energy. Applications range from boiling of water for sanitation in third world countries to environment cleaning machines. ' A implementation of a engine/dynamo requires to be void of excessive magnetic radiation: Its efficient use will be in outer space.

The machine has been created to benefit wildlife, plantlike and environment [to become the property of (sold by) wildlife, plantlike and environment].

A licence for a engine/dynamo / its components, will be available to anyone'; anyone with a said license may create, develop and sell a engine/dynamo; ' a said licence will only contract fifty percent of such licensed peoples profits or a preset sum to said preset beneficiaries. A said preset sum will enforce when said -

profits become too small (too much competition will not aid to these said beneficiaries). Given the engine does not operate as intended by any implementation described herein, its components alone shall be licensed by a said license.

. I had only been able to financially afford a United Kingdom patent: I declare anyone in the UK may exploit this scenario equally to anyone outside the UK. Indirect exploitation of a engine/dynamo / its components will not benefit these said beneficiaries. A said alternate accurate physics} chemistry concept should be read before thinking to exploit this scenario...DTD: The invention will be described by function' referencing the accompanying drawings: Drawings Page: Figure I: see the Hugh plan -co-ed of the r.. acine.

Below this: A section cut side view of the machine.

Figure 2: A plan view of a alternate magnetic engine.

Each figure will reference certain components: -

Component 1: The ring magnet (a magnetic field source).

Component 2: A rotor magnet (a magnetic tibia sources.

-- Component 3: Shielding (biases magnets [1,2] to each others.' ' Component 4: A ring shaped conductor (a dynamos pickup). '.

Component 5: A ring magnet (a magnetic bearing).' - ' Comcnent5: The machines housing.: -

Equal shading-of a unmarked component to a marked component of a ';''-''' '''-

similar shape represents a like / equal component. Shading is individual drawing -' -.

specific. ,.

_ 2 f -. genetic en-tine definitions: (references [Figure 1]) Ring magnet [1] is magnetised vertically (a typical ring magnet (a unlike pole exists between its [1] flat top and bottom surfaces)).

Rotor magnets [2] are magnetised vertically completely respecting the magnetization direction of ring magnet [1] (they [1,2] will repel to each other when placed side by side).

Shielding [3] is a superconductor material or a ferroAntiFerro magnetic material. Its [3] purpose is to exclude / expel (superconductor) or neutralism (ferroAntiFerro) the rotor magnets [2] and ring magnets [1] magnetic fields from

passing though it [3].

A superconductor materials properties definition:, Superconductor (London Penetration Depth): The London equation can be shown to require a external magnetic field to exponentially decay to zero inside a superconductor.

The London penetration depth refers to a exponentially decaying magnetic field at the surface of a superconductor.

Superconductor (Meissner): 7hen a superconductor is subject to a external magnetic field

currents will be induced inside it which generate a magnetic field of their own,

neutralizing the external field.

If the external field is strong enough, however, some of

the external field lines will be able to penetrate the superconductor, although

only by organising themselves into flux vortices of discrete sizes.

That is, if an external magnetic field applied to a

superconductor exceeds a critical field, the flux will penetrate into the material

causing it to return to a non superconducting state.

[The accuracy of, and correct interpretation of the London equation and Meissner effect, are required properties of the shield material described herein (see 'magnetic field analyses ')j

A ferroAntiFerro magnetic material definition: A ferroAntiFerro shield [3] material is a material composed of a equal amount of antiFerroMagnetic particles to ferromagnetic particles: They may be particles held densely together in a chemical resin (to form a shield [3]), or thin layers of antiFerroMagnetic and ferroMagnetic materials layered together (to form a shield [33).

- A ferroAntiFerro material will posses the ability to change a magnets [1,2] magnetic fields which enter it, into a magnetic field consisting of two equal

and opposite magnetic fields: Creating a magnetic field which has no perceptive

- affect upon another magnets [1,2] when it [3] is placed between them [1, 2].

A ferroAntiFerro materials antiFerroMagnetic particles will generate a equal and opposite magnetic field to its ferromagnetic particles.'

A ferroMagnetic material will generate a attraction force (all ferromagnetic particles will generate a attraction force) A antiFerroMagnetic material will generate a repulsion force (all antiFerroMagnetic particles will generate a repulsion force).

The magnets L1,2] magnetic fields which enter it [3j will be

transformed into a fully neutral magnetic field:

Attraction (ferromagnetic) + Repulsion (antiFerroMagnetic) = A neutral magnetic field

- The gain of a ferroAntiFerro shield material is the amount of magnetic field lost to it [3] from magnets [1,2] (that [1,2] which becomes transformed into

a attraction repulsicl, field,' ne-t'^aJecto'sec' (see 'pe',.eable J l.. agne'c

materials' and 'magnetic field analyses ')j: A shield [3j should be as dense and

thick as possible.

A ferroAntiFerro magnetic engine described herein may not operate: This said material may only posses the perceptible properties of a nonpermeable malarial. however, dependent upon this said materials density, it may' (will sea to its ability to re-trajectorise intercepting magnetic fields) operate (see

magnetic field analyses'). i':-'

: ' ' I'.'', - ' i :.- : :...: .

erconductor shield operating principles (references [Figure 1]) - A superconductor shield [3] actively" excludes and expels a external magnetic field from within it (Meissner; London equation), and therefore from passing

through it [3]. This achieves a mutual magnetic bias between the ring magnet [1] and the rotor magnets [2].

Energy is not used to make the superconductor [3] superconduct: It [3] will become a superconductor when placed in a environment free of excessive magnetic radiation.

Ring magnet [1] and rotor magnets [2] have a much lower superconducting temperature to their shield material [3] (they [l,2i will be as -

free of excessive magnetic radiation as the superconductor [3], but they [1,2] will not become superconductors).

Rotor magnet [2] will repel to the ring magnet [1] where the superconductor [3] does not exist. This will effect a anticlockwise force.

Rotor magnet [2] will not repel to the ring magnet [1] where the superconductor [3] exists, its [2] magnetic field is excluded / expelled from

passing through it [3].

Ring magnet [1] will repel to the rotor magnet [2] where the superconductor [3] does not exist. This will effect a anticlockwise force.

Ring magnet [1] will not repel to the rotor magnet [2] where the superconductor [3] exists, its [1] magnetic field is excluded / expelled from

passing through it [3].

-- Ring magnet [1] will repel to the superconductor [3] where the,,, superconductor [3] exists. This will effect a clockwise force.

Ring magnet [1] will repel to the superconductor [3] where the superconductor [3] exists (after passing though the rotor magnet [2]). This will effect a anticlockwise force.

Rotor magnet [2]s force: -

Repels to ring magnet [1] producing a anticlockwise force.

- Cannot pass though the shield [3] to act upon ring magnet [1].

Ring magnet [1]s force: Repels to rotor magnet [2] producing a anticlockwise force.

Repels to shield [3] producing a clockwise force.

Repels to shield [3] producing a anticlockwise force.

Cannot pass through the shield [3] to act on rotor magnet [2].

This produces a magnetic force bias: 3(AC)Magnetic forces - l(C)Magnetic force = Magnetic forces.: FerroAntiFerro shield operating principles (references [Figure 1]) I, A ferroAntiFerro shield [3] neutralizes / retrajectorises any magnetic field [1,2] which enters it [3]. This achieves a mutual magnetic bias between the

ring magnet [1] and the rotor magnets [2]. ' Rotor magnet [2] will repel to the ring magnet [1] where the shield [3] does not exist. This will effect a anticlockwise force.

Rotor magnet [2] will neutralise through the shield [3] where the shield [3] exists. This will not effect any directional force.

Ring magnet [1] will repel to the rotor magnet [2] where the shield [3] does not exist. This will effect a anticlockwise force.

Ring magnet [1] will neutralise through the shield [3] where the shield [3] exists. This will not effect any directional force.

Rotor magnet [ids force Repels to ring magnet [1] producing a anticlockwise force.

Neutralises through shield [3], to not effect [1].

Ring magnet [1]s force: -

Repels to rotor,magnet [2] producing a anticlockwise force.

Neutralises through shield [3], to not effect [2].

. This produces a magnetic force bias:, 2(AC)Magnetic forces -,O(C) Magnetic force = 2(AC)Magnetic forces. A : - -.. ' ', ,....

, -':' it,, ', ' ' -', ' -:" ' _. '. ,..: a, - - ':

( C eld design (references [Figure 1]) The shields [ 3] shape has been mutually designed to the shape of the rotor magnets [2] and ring magnet [1]: To achieve a efficient anticlockwise rotation of the rotor system [2, 3]. Simple mathematics create the shields [3] and rotor magnets [2] shapes, as shown in [Figure 1].

Superconductor shield implementation: The superconductor shielding [3] has been designed such that the magnetic fields from both the rotor magnets [2] and the ring magnet [1] do not

combine to produce a great magnetic field at ar,y point toward the supercorductc-

[3]. A great magnetic field would otherwise breakdown the superconductor [3], to

prevent it being a superconductor.

A uniform magnetic field [1,2] is distributed toward the

superconductor [3] by way of its [3] and the magnets [1,2] designed shapes.

FerroAntiFerro shield implementation: The shielding [3] itself is both dense and thick, this allows a tiny amount of magnetic field [1,2] which enters it [3] to be fully converted into a

neutral magnetic field [1,2].

Shield [3] density and thickness determine the gain of a ferroAntiFerro magnetic engine. The stated gain of 2Magnetic forces is a multiple to the actual amount of neutralization achieved.

-Rotor magnet design (references [Figure 1]) _ Rotor magnets [2] have a specifically designed shape such that they are not bonded to a superconductor shielding [ 3].

Rotor magnets [2] have a specifically designed shape such to enhance their [2] bonding to a ferroAntiFerro shielding [3].

They [2] provide a physical latch to the shielding [3] which prevents them [2] escaping horizontally (the latch is the section of rotor magnet [2] furthest away from the ring magnet [1] (appearing beneath the magnetic bearings [5])).

They [2] are held in place vertically by two ring magnets [5], both [5] mutually repel to the rotor magnets [2] said latches.

Rotor magnets [2] are insulated by a non magnetic non electrically conducting material. This prevents them [2] becoming demagnetized by the electrical current induced into the shielding [ 3] by ring magnet [1].

Friction free bearings (references [Figure 1]) Magnetic bearings [5] are magnetized vertically (a typical ring magnet (a unlike pole exists between its flat top and bottom surfaces)).

The rotor system [2,3] is supported vertically by two ring magnets [5].

Ring magnets [5] are latched to the housing [6] (their [5] outer circumferences are of a very slight elliptical shape, this prevents them [5] slipping within the housing [6]).

Superconductor shield implementation: The rotor system [2,3] supports itself horizontally: Both the rotor magnets [2] and the shielding [3] repel to ring magnet [1] (ring magnet [1] is latched to the housing [6]).

When the system is assembled, ring magnets [5] (located top and bottom to the rotor system [2,3]) will both [5] mutually repel to the rotor system components [2,3] (like poles exist between magnets [5,2]; the superconductor [3] will mutually repel to magnets [5]), keeping it [2, 3] vertically stable, mutually holding ring magnets [5] in place.

rerroAntiFerro shield =plerentaton The rotor system [2,33 supports itself horizontally: The rotor magnets [2] repel to the ring magnet [1] (ring magnet [1] is latched to the housing [6]).

When the system is assembled, ring magnets [5] (located top and bottom to the rotor system [2,3]) will mutually repel to the rotor magnets [2] (like poles exist between magnets [5,2]), keeping it [2,3] ([2] is bonded to [3]) vertically -

stable, mutually holding ring magnets [b] in place.

,' i.-.

:: . i, I. --;

r NATO (references [Figure 1]) As the rotor system [2,3] rotates, ring magnet [1] will induce a magnetic field (electrical current)-into the shielding [3], the shielding [3] will induce a

magnetic field (electrical current) into the dynamos pickup [4].

A direct electrical current may be taken from the pickup -[4] flat top and bottom surfaces.

The dynamos pickup [4] may be a aluminimm ring (ferroAntiFerro shield implementation), or a aluminium or superconductor ring (superconductor shield implementation) material [4].

Housing: (references [Figure 1]) The machines housing [6] is made from a non magnetic non electrically - -

conducting material. It [6] is a doughnut shape, to use its material [6] to a greater efficiency.

It [6] consumes every non rotating component, with every non rotating component being latched to it [6]. This latching avoids the need for the machines components to be chemically bonded to the housing [6].

All of the machines non rotating components will be designed with physical latches (protrusions or elliptical shapes) to latch into a respectful equal and opposite' latch in the machines housing [6;.

Ring materials [1, 5] outer circumferences are of a very slight elliptical shape, they [1,5] are not bonded to the housing [6]: Their [1, 5] Hatchable shape prevents them slipping within the housing [6].

The dynamos ring pickup [4] inner circumference is of a very slight elliptical shape, this prevents it [4] slipping within the housing [6].

Each component [1,4,5] is fully insulated by the housing [6]. Each components [1,4,5] insulation [6] toward the rotor system [2,3] reduces eddy currents between them [1,4,5]-[2,3] (the insulation [6] layer between components [1,4,5]-[2,3] is too thin to be shown in [Figure 1]).

With the single exception of a ferroAntiFerro shields [3] rotor magnets [2] being bonded to their shielding [3]: No component [1,2,3,4,5,6] of the machine is bonded, each [1,2,3,4,5] provides a physical latch into a equal and opposite latch into the housing [6]..

The housing [ 6] is cast (melted) around the machines components: The required air gap surrounding the rotor system [2,3] and the temporary support needed to the machine whilst the housing sets, will be provided by a temporary (deteriorating) structure (maybe copper): This temporary structure will deteriorate -

when a liquid (copper = ferric chloride) poured through a single tiny hole left in the machines housing (once the housing has set) comes into contact with it.

A machines efficiency equally equates to a great life span: A cast housing [6] provides a extremely solid structure, to effect a life of hundreds of years. A complete vacuum exists within the housing [6] to prevent friction acting upon any rotating component housed within it [2,3] . It [6] may be vacuumed (once assembly is completed) by a tiny hole left in the machines housing [6].

The machines housing may emit gases (dependent upon housing material and machines location), the machine will require to be vacuumed regularly (a machine connected to the machine may accomplish this task).

.. : ':. -." '.:..DTD: : - ' it; ' '- '.'';',.-..,'.;: ....,,.:

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-6- . Alternate I. plementations The implementations / statements which follow are not independently written

into the 'Claims', they allow me to write the 'Claims' to a accurate scope.

Many and numerous magnetic engines may be made from the principles set out in this patent: Equal inverse operations of operations described in this patent should be covered by this patent (equal principles of operation with back to front / numeral component configurations (many different engines may be made; all will obey the same base principles)). Patent applications claimed to by this patent are this patent (this patent is a detailed rewrite of these said replaced rewritten development applications).

Alternate magnets (references [Figures 1,2]) All and any of the magnets us-cd in this-machine may be electromagnets rather than permanent magnets, or not: Given electromagnets are used as magnets [1,2] in a self feeding loop (electrical energy generated is used to power magnets [1,2]): A kinetic force is not matter and cannot be turned into matter: A dynamo transform a magnetic field (which is matter) into a electrical current: A

magnetic field breaks doves a conductors material, producing (from broken bits of

its material) electrons (a result of a disturbing moving magnetic field toward a

conductor). Matter effects matter: A kinetic force without matter can achieve nothing (a kinetic force without matter is nothing): A magnetic field is matter.

.,. . _..

If electromagnets [1,2] emit a magnetic field which is

proportional to a ratio ('electric currents magnetic field' + 'materials mutual

consequentially generated magnetic field'), to the electrical energy directed into

them [1,2]. Given a kinetic force is not matter and cannot therefore create matter, the electromagnets will degrade as a consequence of the kinetic energy (matter) released from them.

A electromagnet outputs a greater energy than the electrical current energy delivered to it. A electromagnet is a temporary permanent magnet. If electromagnets [1,2] emit a magnetic field directly

proportional to the electrical current directed to it (if it were said a electromagnets magnetic field were a single product of the electrical currents

magnetic field), a rotation of the machine will not occur (if the engine described

herein were one hundred percent efficient, the engine would rotate, but it would have no 'gain' (it would rotate until stopped by a external force).

A electromagnet is unlike a permanent magnet. A permanent magnet is self destructive (requires no external energy for it to emit a magnetic field).

Alternate rotation (references [Figure l]) The stationary ring magnet [1] mutually causes the rotor system [2,3] to rotate. This would imply ring magnet [1] should rotate if the rotor system [2,3] were stationary. If this implication were accurate this would create a machine where the only moving component would be a ring magnet [1].

The ring magnet [1] could be supported by two tiny ring magnets (or superconductors (superconductor shield implementation)) situated top and bottom to the ring magnet [1] (fixed to the housing [6]), repelling to it [1], supporting it vertically. It [1] would support itself horizontally, it is being repelled to by the rotor magnets [2] (and the shield [3] (superconductor shield implementation)).

A electrical current could be generated in conductors placed around the now rotating ring- r.Zagre. [1], using the ring magnets,1] magnetic field

to induce electrical current into them (the said superconductor ring magnet bearings which support the now rotating ring magnet [1] will have a electrical current induced into them). The shield [3] itself has a electrical current induced into it by ring magnet [1]: Electrical current can now be directly taken from the shield [3].

:: :. i..., ::: ':. '- - ':",.. "'

,.. -:. .

,, ...

l - Alternateequal inverse operations A inverted component layout of [Figure 1] will produce a component configuration where the rotor system [2,3] rotates around the ring magnet [1] (the rotor system [2,3] will have a greater internal diameter to the ring magnets [1] external diameter, to enable it [2,3] to rotate around its [1] external circumference). The ring magnet [1] itself may rotate, as described in 'alternate rotation'.. A inverted component layout of [Figure 1] will produce a component configuration where the rotor system [2,3] is situated / rotates above and below the flat top and bottom surfaces of the ring magnet [1]. The ring magnet [1] itself may rotate, as described in 'alternate rotation T. Alternate dynamo (references [Figure 1]) --

A ring magnet could be fixed (latched) to the inner circumference of the shield [3], where a ring shaped conductor could be placed (latched to the housing [6]) top and bottom to it, or inside it: As the rotor system [2,3] rotates the dynamo ring magnet will rotate, this will induce a direct current into the pickups placed above and below it, or inside 'it.

A alternator may be formed by replacing the said dyn&..o ring magnet with a ring magnet composed of alternating pole sections. Independent pickups may then be placed (latched to the housing [6]) top and bottom to it, or inside it (each pickup would be insulated from each other, by the housing [6]).

........DTD: A ring shaped conductor (pickup) could be placed above and below the rotor magnets [2]: As the rotor system [2, 3] rotates, the rotor magnets [2] will induce a magnetic field (electrical current) into the ring pickup. This will effect

a varying direct current to be induced into the pickup by rotor magnets [2].

Each ring pickup may be segmented, with each segment being insulated [6] from each other, to achieve a greater and more efficient magnetic induction into them, by both the rotor magnets [2] end 'tine shielding [3] (superconductor implementation). However, this will not be a smooth induction, and will result in the rotor system [2,3] jittering: A efficient machine is equally one with a long life, this dynamo implementation will have a greatly shortened life. If each ring pickup were segmented into thousands of pieces it would better the machines life span (and the induced current capability), but the machine will still have a very short life (compared to' other implementations)).

Alternate shielding materials Ferromagnetic / antiFerroMagnetic / diamagnetic / permeable / dense metals(Lead(pb) a denser material) shielding materials [3] may be implemented each biasing a magnet(s) to another magnet(s) in like ways: FerroMagnetic (references [Figure 2]) This shield [3] material is designed to provide a magnetic force bias of magnets [1,2] by shielding [3] them [1,2] with a unlike pole orientated magnetic material [3]. The shielding [3] has been designed and placed to eliminate all clockwise rotational forces.

A given thickness of shield material [Figure 2] [3] is used to produce a neutral 'attraction + repulsion' force between a rotor magnet [2] and ring magnet [1]: From the point of view of the ring magnet [1]: The ring magnet [1] will attract to the shielding [3], and repel to a rotor magnet [2]. This will achieve a neutral repulsion force to a rotor magnet [2] where the shield [3] exists between them [',2] (ring magnet [11 attracts the shield [3J and repels a rotor magnet [2], this creates a neutral force (attraction + repulsion = neutral)' given a exact thickness of shield material [3] between them [1,2]). Where the shield [3] does not exist between magnets [1,2] a full magnetic repulsion between magnets [1, 2] will occur.

As shown in [Figure 2] the depth of the shields [3] thickness at any point is proportional to now far the rlug magnet [1] is away from a rotor magnet [2] at any point. The distance at which a neutralization occurs is determined by the power and distance the ring magnet [1] is away from the power and -

distance of a rotormagnet [2], shield thickness is resultantly determined by this simple calculation. ' ' ' ' -. ',.,,'. ', ':

.-, i: at,.. -:, .. !

-8 - AntiFerroMaqnetic / diamagnetic (references [Figures 1,2]) This shielding material is designed to provide a magnetic force bias of magnets [1,2] by shielding them [1,2] with a like pole orientated magnetic material [3]. Unlike other types of this same engine type, a rotor magnet [2] attracts to the ring magnet [1] (this produces a clockwise rotation by magnets [1,2] biasing [3], given how [Figures 1,2] have been drawn). The shielding [3] has been designed and placed to eliminate a31 anticlockwise rotational forces.

A given thickness of shield material [Figure 2][3] is used to p'-oduce a neutral 'attraction + Repulsion' force between a Notch magnet [2] and ring magnet [1]: From the point of view of the ring magnet [1]: The ring magnet [1] will repel to the shielding [3], and attract to a rotor magnet [2] -This will achieve a neutral repulsion force to a rotor magnet [2] where the shield [3] exists between them [1,2] (ring magnet [1] repels the shield [3] and attracts a rotor magnet [2], this creates a neutral force (repulsion + attraction = neutral), given a exact thickness of shield material [3] between them [1,2]). Where the shield [3] does not exist between magnets [1,2] a full magnetic attraction between magnets [1, 2] will occur.

As shown in [Figure 2] the depth of the shields [3] thickness at any point is proportional to how far the ring magnet [1] is away from a rotor magnet [2] at any point. The distance at which a neutralization occurs is determined by the power and distance the ring magnet [1] is away from the power and distance of a rotor magnet [2], shield thickness is resultantlydetermined by this simple calculation; A tiny percentage of the shield material [3] itself will generate a fully neutral magnetic field: It [3] achieves two unlike poles in the

same material (magnets [1,2] have unlike poles to each other): Ring magnets [1] and rotor magnets [2] magnetic forces will have been truly neutralized by the shield [3]. A shield [3] material can be used in excess [Figure 1][3]: To achieve a greater repulsion between ring magnet [1] and the shield [3] (the shield [3] will repel ring magnet [1] greater than ring magnet [1] is attracted to a rotor magnet [2]): From the point of view of the ring magnet [1]: The ring magnet [1] will greatly repel to the shielding [3] r and slightly attract to a rotor magnet [2] where the shield [3] exists between them [1,2]: A repulsion force indirectly acting toward a rotor magnet [2] where the shield [3] exists between magnets [1, 2] occurs (ring magnet [1] repels the shield [3] greater than it attracts to a rotor magnet [2], this creates a biased repulsion force (great repulsion + small attraction = a repulsion)). Where the shield [3] does not exist a full magnetic attraction force between magnets [l,2] will occur.

Permeable / magnetic materials (references [Figure 1]) Tiny gains in using a permeable / magnetic shield materials [3] are the magnets [l'2] magnetic fields will be partially re-trajectorised when

passing it [3].

A permeable / magnetic shield [3] will re-trajectorise a magnets [1,2] magnetic field (which were heading for each other [1,2]) to another

trajectory (when passing through it [3]), which may consequentially not intercept each other [1,2] (many will still intercept each other [1,2l, is dependent upon shield [3] thickness). A magnetic bias is achieved to where the shield [3] material does not shield between the rotor magnet [2] and ring magnet [1].

Although magnetic fields [1,2] which would not have

intercepted each other magnet [1,2] will now intercept them [i,2]' a bias will still favour a gain: Magnetic fields [1,2] which were not headed for each other

magnet [1,2] (but still passed though a section of the shield [3]) will not be as many as those magnetic fields which were heading for each other magnet [the tiny

bias is reduced by this even tinier effect].

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Dense metals(Lead(pb)...) (references [Figure 1]) This shield [3] material will bias a magnets [1,2] magnetic field by inhibiting a amount of their [1,2] magnetic fields from passing though it

[3]. Lead(pb) is know to inhibit short wavelength magnetic fields

(X-rays...), but does not so influence incredibly tiny wavelengths (magnetic fields).

However, a incredibly tiny inhibitance of a magnets magnetic field may occur, and therefore the most simplest magnetic bias is

achieved: Lead(pb) (a denser material) [3] will inhibit a magnets [2] magnetic field from only partially escaping through it [3] to reach

magnet-[1]. -.

Lead(pb) (a denser material) [3] will inhibit a magnets [1] magnetic field from only partially escaping through it [3] to reach

magnet [2].

A incredibly tiny (but still) magnetic bias is achieved between a full repulsion (where the Lead(pb) (a denser material) does not block a magnets [1,2] magnetic field) and the magnets [1,2] magnetic fields being slightly

inhibited by the shielding [3] (when their [1,2] magnetic fields attempt to pass

through it [3]).

The shielding [3] has been designed and placed to eliminate all clockwise rotational forces.

......DTD: Magnetic biasing of magnetic fields via materials definitions

Superconductors / DiaMagnetic / FerroMagnetic / AntiFerroMagnetic Permeable / Dense materials(Lead(pb) or denser) shield materials each bias a magnets magnetic field when they are placed beside a magnet.

A magnetic bias is the ability to manipulate a magnets magnetic field,

to another magnets magnetic field, by a material, such that this manipulation of

the magnets magnetic fields does not appear uniform (to that that the magnet(s)

would naturally achieve; toward another magnet(s)): To use this advantage to create a mutually biased magnetic motion (as similarly described herein for a t.

superconductors [3] ability to bias a magnets [1,2] magnetic fields).

A single magnet itself may be magnetized in a multiple direction, to achieve a biased / shielded magnetic field of itself. A single electromagnet may be

wound to achieve a biased / shielded magnetic field of itself.

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. . ...

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-10 f., -..

. I Kinetic field analyses

I have written a magnetic field analyses program two ways (only applys to

magnetic'/'permeable' materials (does not apply to a superconductor material)): 1. A particle analyses will clearly point out placing a shield material anywhere will create a equal and opposite force: A neutralization is achieved, but the same particles magnetic field will emit in a equal and opposite

direction, to indirectly counter the neutralization achieved. [A bias is not achieved] 2. A global particle analyses operates how a person would naturally perceive these types of shields to operate (projecting acc,. ulting field lines

across the whole magnetic engine array (to accumulate the magnetic forces they accumulate)): A magnetic force gain does result. [This result / program is assumed to be of a error] I have not been able to write a computer simulation of a superconductor, as as far as I am aware T superconductor chemistry is unknown. I am sceptical to the theory of a externally applied magnetic field exponentially decaying at the surface

of a superconductor, however, this is a requirement of the shields property described herein.

It is most likely the external magnetic field becomes neutralised by

the superconductor' but, as all 'shielded' J 'neutralized' magnetic fields, the

magnetic field still exists, completely uninhibited, and, completely unchanged:

They exist as unlike magnetic fields (a north pole orientated

magnetic field + a south pole orientated magnetic field = a neutral magnetic

field): The magnetic fields still exist, they only appear not to.

Example: A permeable material will not attract to a shielded magnetic field, not because the said magnetic field has been 'conducted away' /

inhibited' / 'removed' (made to 'not exist'), but because two unlike magnetic fields are made present to it ('magnetic field source' + 'inverted magnetic field

source (a permeable material will create a unlike orientated magnetic field to the

magnetic field source it is shielding)'): These unlike orientated (north + south =

neutral) magnetic fields will equally attract and repel to a permeable material

(attraction + repulsion = neutral).

A permeable material subject to a shielded magnetic field

(two equal and opposite magnetic fields) will mutually and equally establish two

unlike oriented magnetic fields of its own (north orientated field + south

orientated field = a neutral field), creating again a actual but neutral magnetic

fields.

The permeable materials created equal and opposite (attraction + repulsion = neutral) magnetic fields will equally attract and repel

(attract + repel = neutral) to other permeable materials, and the two magnetic field sources themselves (the shielded magnet): Each and all magnetic fields exist,

each completely uninhibited / completely unaffected by each other: Many unique independent magnetic fields independently achieve a 'in total' (as many attractions

to repulsions) neutral effect.

No known natural materials inhibit effect or change a magnetic field,

where, like gravity, magnetic fields penetrate all known natural materials, except

maybe' superconductors.

A superconductor has been practically shown to exclude / expel (decay) a tiny fraction of Gravity, greatly validating a superconductor achieves to expel (decay) magnetic fields.

A superconductor magnetic engine described herein will require to be made: Either result will be required: Magnetic fields do / do not decay through a

superconductor material: If they do, the magnetic engine will rotate, if they do not, it Will not.

Claims

Art 1. A magnetic engine, utilising a mutually biased magnetic fields of a

magnet(s), by way of a shield(s), toward a magnet(s), to create a mutual magnetic propulsion / consistent kinetic motion, between the magnet(s) and/or shield(s); A friction free embedded dynamo/alternator; A friction free embedded magnetic bearing; Latches, A non-chemical 'latched' bond between machine components; A machine housing, A non chemical 'latched' bond to the machines components, possessing a vacuum internal to it.
2. A 'Shield' claimed within any preceding/proceeding Claim(s): A superconductor material, acting to actively exclude and expel magnetic fields from

within it; to achieve a magnetic bias of a magnetic field(s).
3. A 'Shield' claimed within any preceding/proceeding Claim(s): A ferroantiferro magnetic material, acting to neutralise / re-trajectorise magnetic fields which pass through it; to achieve a magnetic bias of a magnetic field(s).
4. A 'Shield' claimed within any preceding/proceeding Claim(s): A apparently not magnetic - conductive material, acting to re-trajectorise magnetic fields which pass through it; to achieve a magnetic bias of a magnetic field(s).
5. A 'Shield' claimed within any preceding/proceeding Claim(s): Either or any combination of materials: ferromagnetic / antiferromagnetic / diamagnetic / permeable / magnetic material(s); where each shield material acts to neutralize a magnetic field by placing a exact fixed amount of it beside a magnet(s), to achieve

a neutralization at a given distance away from the shielded magnet(s); by the shield material having/producing a equal-opposite / unlike magnetic field to each

respectful magnet(s) it is placed beside/between; to achieve a magnetic bias of a magnetic field(s).
6. A 'Shield' claimed within any preceding/proceeding Claim(s): A as dense or denser material to Lead(pb), acting to partially/fully inhibit magnetic fields from passing through it; to achieve a magnetic bias of a magnetic field(s).
7. A 'Shield' claimed within any preceding/proceeding Claim(s): Any material with magnetic properties or properties which inhibit, affect or change a magnetic field / perceptive magnetic field; to achieve a magnetic bias of a

magnetic field(s).
S. A 'Shield' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations ó and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.
9. Any 'Magnet' / 'Magnetic Field Source' claimed within any

preceding/proceeding Claim(s): A or any number of any particularly arranged/combination of permanent magnet(s) / electromagnet(s) / superconductor(s) / magnetic material(s) / any direct/indirect magnetic field source(s).
10. A 'Biased Magnetic Field' claimed within any preceding/proceeding

Claim(s): A 'shield' placed beside a 'magnet', where the shield partially surrounds the magnet; the magnets magnetic field becoming biased between where the shield is

placed, to where it is not, around the magnet.
11. A 'Biased Magnetic Field' claimed within any preceding/proceeding

Claim(s): A 'shield' placed between 'magnets', where the shield partially surrounds between these magnets; the magnets magnetic fields becoming biased between where

the shield is placed, to where it is not, between these magnets.
12. A 'Biased Magnetic Field' claimed in/within any preceding/proceeding

Claim(s): A 'shield' partially placed between/beside/around any number of any particularly arranged 'magnet(s)'; the magnet(s) magnetic fields becoming biased

between where the shield is placed, to where it is not, between these magnet(s).
13. A 'Biased Magnetic Field' claimed in/within any preceding/proceeding

Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.

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14. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed within any - preceding/proceeding Claim(s): A mutually 'biased magnetic field' between at least

two 'magnetic field sources', where each magnetic field source mutually attracts or

repels greater to each other through a particular direction-trajectory not passing through a 'shield', to any said particular trajectories equalopposite countering direction-trajectory that passes through a shield; a direction-trajectory bias created by a design/shape/placement of a shield(s) and magnets; to achieve a mutually biased magnetic propulsion between these shielded magnetic field sources.
15. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claim 14: Magnetic field sources(s)' magnetised/wound a unlike mutually-attractive pole to

each other, to achieve a attraction/propulsion between these magnets.
16 A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claim 14: Magnetic field sources(s)' magnetised/wound a like mutually-repulsive pole to each

other, to achieve a repulsion/propulsion between these magnets.
17. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claims 15, 16: 'Magnetic field sources(s)' magnetised/wound a vertical direction 'up

through them', or, circular about their centre-column; to achieve a like pole around a magnets circumference; to achieve a 'always' 'like/repulsive pole' / unlike/attractive pole' toward another magnet(s).
18. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claims 14, 15,16,17: A mutually 'biased magnetic fields' between a ring of 'shielded

magnet(s)' and a/any outer-circumference/inner-circumference/above/below surrounding 'ring magnet(s)'; to achieve a mutually biased magnetic propulsion between the 'shielded magnet(s)' / 'ring magnet(s).
19. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claim 18: A ring of shielded magnets' being a single solid shield structure; where the 'ring of shielded magnets' 'magnet(s)' are 'latched'/bonded/embedded into it.
20. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claims 14, 15,16,17,18,19: A 'ring magnet' surrounding the outer-circumference of a 'ring of shielded magnets'; where any particular 'shield' materials respective shield(s) '-'magnet(s) ' designed/shapes/placements directiontrajectory-

bias/'magnetic engine' are of that substantially described and two illustrated in the accompanying descriptions and drawings.
21. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.
22. A 'Embedded Dynamo' claimed within Claim 1: A stationary magnetic field source(s) inducing a magnetic field / electrical current into a rotating

shield'; the shield inducing a magnetic field / electrical current into a

stationary conductive material(s) placed beside/around it; where the 'shield(s)' and/or 'magnetic field source(s)' are/are-not facilitated by a 'magnetic engine'.
23. A 'Embedded Dynamo/Alternator' claimed within Claim 1: A rotating ring of 'shielded magnets' facilitated by a 'magnetic engine', where the ring of shielded magnets 'magnets' and/or 'shields' induce a magnetic field / electrical

current into a stationary conductive material(s) placed beside/around it/them.
24. A 'Embedded Dynamo' claimed within Claim 1: A rotating 'ring magnet(s) ' facilitated by a 'magnetic engine', inducing a magnetic field /

electrical current into a stationary conductive material(s) placed beside/around it/them.
25. A 'Embedded Dynamo/Alternator' claimed within Claim 1: Traversing / rotating 'magnetic field source(s)' facilitated by a machine/'magnetic engine' for

other purposes, inducing a magnetic field / electrical current, by its/their

traversion/rotation into a stationary conductive materials(s) placed beside/around it/them.
26. A 'Embedded Dynamo/Alternator' claimed in Claims 22,23,24,25: A stationary conductive material being a/any 'conductive material' / 'shield' / magnetic bearing'; where a conductive material(s) are/are-not stationary.

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27. A 'Embedded Dynamo/Alternator'/'magnetic bearing' claimed within Claim - 1: A stationary superconductor(s) / antiferromagnetic(s) / magnetic-material(s) material placed beside/around a magnetic spindle / rotating magnetic component(s) required to be supported; the magnetic spindle / component(s) inducing a electrical current into the materials(s) ; the magnetic spindle / component(s) being mutually repelled / supported by the material(s).
28. A 'Embedded Dynamo/Alternator' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and one illustrated in the accompanying descriptions and drawings.
29. A 'Embedded Magnetic Bearing' claimed within Claim 1: A ring of shielded magnet(s)' 'magnet(s)' and/or 'shield(s)' mutually repelling to a 'ring magnet(s)'; to mutually support 'the ring of shielded magnets' / 'ring magnet(s)'; where any of the 'ring of shielded magnets '-'shields ''magnets ' / 'ring magnet(s)' are/are-not facilitated by a 'magnetic engine';
30. A 'Embedded Magnetic Bearing' claimed within Claim 1: A 'magnet(s)' and or 'shield(s)' mutually repelling to a 'other magnet(s)', to mutually support each 'magnet(s)' / 'shield(s)' / 'other magnet(s)'; where any of the 'magnet(s)' / shield(s)' / 'other magnet(s)' are/are-not facilitated by a 'magnetic engine'.
31. A 'Embedded Magnetic Bearing' claimed within Claim 1: A rotating 'ring magnet(s)' facilitated by a 'magnetic engine', having stationary 'respectfully magnetized magnetic' / 'antiferromagnetic' / 'superconductor' ring magnet shaped material(s), placed 'above and below its flat top and bottom surfaces' and/or around its inner and/or outer circumference(s)'; to achieve a mutual repulsion/support between them.
32. A 'Embedded Magnetic Bearing' claimed within Claim 1: Rotating / traversing magnetic field source(s) facilitated by a machine/'magnetic engine' for:

other purposes / equally required to be supported, having stationary 'respectfully magnetised magnetic material' / 'antiferromagnetic material' / 'superconductor material' placed around it/them; to achieve a mutual repulsion/support between them.
33. A 'Embedded Magnetic Bearing' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.

i,
34. 'Latches'/'Latched' claimed within any preceding/proceeding Claim(s): Machine components non-chemically bonded/'latched' together; each respective component(s) having equal and opposite latches set into them, to achieve each component(s) latching into each other components equal-opposite latch; these latches may be elliptical shapes of the components themselves or oddities sticking out of' or 'in to' these components; to a end to achieve a non-chemical 'equal-

opposite latched' bond between components.
35. 'Latches' claimed in Claim 34: A 'shielded magnets' 'shield(s)' and magnet(s)' created with equal-opposite 'latches' set into them, such that a magnet may latch into a shields equal-opposite latch; these latches may be elliptical shapes of the magnets / shields themselves or oddities sticking 'out of' or 'in to' these components; to achieve a non-chemical bond between the shield(s) and magnet(s).
36. 'Latches' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.
37. A 'Machine Housing' claimed in Claim 1: A non magnetic non electrically conducting material such as a plastic or glass, with 'latches' internally inset/moulded into it, such that the machines components this housing supports latch into its latches; these latches may be elliptical shapes of the components themselves or oddities sticking 'out of' or 'in to' these components, to a end to achieve a non- chemical 'equal-opposite latched' bond between a machines components and housing.

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38. A 'Mach.ne Uousing' climed in Claim 37: Manufactured to support its machines components by casting the housing material around the machines components; the machines components being supported by a temporary structure, while the housing is cast, the temporary structure being chemically broken down once the machines housing has set.
39. A 'Machine Housing' claimed in Claim 38: A temporary deteriorating structure being copper, chemically broken down by ferric chloride.
40. A 'Machine Housing' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and one illustrated in the accompanying descriptions and drawings.
41. A 'Ring Magnet' claimed within any preceding claim, A 'ring magnet' equally being a 'ring of magnets'.
42. Any preceding Claim(s): A 'Magnetic Engine / Dynamo/Alternator' machine implemented/created by any combinations of individual components, configurations and implementations of that substantially described and some illustrated in the accompanying descriptions and drawings.

43. A 'Magnetic Engine / Dynamo/Alternator' machine implemented/created by any combinations of individual components, configurations and implementations of that substantially described and some illustrated in the accompanying descriptions

and drawings.

is Amendments to the claims have been filed as follows 1. A magnetic engine, utilising a mutually biased magnetic fields of a

magnet(s), by way of a shield(s), toward a magnet(s), to create a mutual magnetic propulsion / consistent kinetic motion, between the magnets and/or shield(s); A friction free embedded dynamo/alternator; friction free embedded magnetic bearing; Latches, A non-chemical 'latched' bond between machine components; A machine housing, A non chemical 'latched' bond to the machines components, possessing a vacuum internal to it.

2. A 'Shield' claimed within any preceding/proceeding Claim(s): A superconductor material, acting to actively exclude and expel magnetic fields from

within it, as a result of a high speed rotation of it, or not; to achieve a magnetic bias of a magnetic field(s).

3. A 'Shield' claimed within any preceding/proceeding Claim(s): A ferroantiferro magnetic material, acting to neutralize / re-traectorise magnetic fields which pass through it; to achieve a magnetic bias of a magnetic field(s).

4. A 'Shield' claimed within any preceding/proceeding Claim(s): A apparently not magnetic - conductive material and/or any permeable/magnetic material(s), acting to re-trajectorise magnetic fields which pass through it; to

achieve a magnetic bias of a magnetic field(s).

5. A 'Shield' claimed within any preceding/proceeding Claim(s): Either or any combination of materials: ferromagnetic / antiferromagnetic / diamagnetic / permeable / electromagnetic / magnetic material(s); where each shield material acts to neutralise a magnetic field by placing a exact fixed amount of it beside a

magnet(s), to achieve a neutralization at a given distance away from the shielded magnet(s); by the shield material having or producing a equalopposite/unlike magnetic field to each respectful magnet(s) it is placed beside/between; to achieve

a magnetic bias of a magnetic field(s).

. 6. A 'Shielded Magnet' claimed within Claim 5: A electromagnet wound/consisting a 'source magnetic field winding' and 'shield winding', to achieve

a self shielded electromagnet, of a single intertwined coil, which may or may not be wound over a core.

7. A 'Shielded Magnet' claimed in Claim 6: A single electromagnet consisting one or more individual intertwined 'magnetic source(s)' / 'magnetic shield(s)' coils.

8. A 'Shield' claimed within any preceding/proceeding Claim(s): A as dense or denser material to Lead(pb), acting to partially/fully inhibit magnetic fields from passing through it; to achieve a magnetic bias of a magnetic field(s).

9. A 'Shield' claimed within any preceding/proceeding Claim(s): Any material with magnetic properties or properties which inhibit, affect or change a magnetic field / perceptive magnetic field; to achieve a magnetic bias of a

magnetic field(s).

10. A 'Shield' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.

11. Any 'Magnet' / 'Magnetic Field Source / Material' claimed in/within

any preceding/proceeding Claim(s): A or any number of any particularly arranged/combination of permanent magnet(s) / electromagnet(s) / superconductor(s) / magnetic material(s) / any direct/indirect magnetic field source(s); a

electromagnet(s)' being wound respectfully to any magnetic field described for a

magnet(s)'. 12. A 'Biased Magnetic Field' claimed within any preceding/proceeding

Claim(s): A 'shield' placed beside a 'magnet', where the shield partially surrounds the magnet; the magnets magnetic field becoming biased between where the shield is

placed, to where it is not, around the magnet.

13. A 'Biased Magnetic Field' claimed within any preceding/proceeding

Claim(s): A 'shield' placed between 'magnets', where the shield partially surrounds between these magnets; the magnets magnetic fields becoming biased between where

the shield is placed, to where it is not, between these magnets.

!

It - - 14. A 'Biased Magnetic Field' claimed in/within any preceding/proceeding

Claim(s): A 'shield(s)' partially placed beside/between/around any number of any particularly arranged 'magnet(s)'; the magnet(s) magnetic fields becoming biased

between where the shield(s) are/is placed, to where it is not, beside/between/around these magnet(s).

15. A 'Biased Magnetic Field' claimed in/within any preceding/proceeding

Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.

16. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed within any preceding/proceeding Claim(s): A mutual 'biased magnetic field' / motion, between

at least two 'magnetic field sources', where each magnetic field source mutually

attracts or repels greater to each other through a particular directiontrajectory not passing through a 'shield', to any said particular trajectories equal-opposite countering direction-trajectory that passes through a shield; a direction-

trajectory bias having been created by a design/shape/placement of a shield(s) and magnets. 17. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claim 16: Magnetic field sources(s)' magnetised/wound a unlike mutually-attractive pole to

each other, to achieve a attraction/propulsion between these magnets.

18. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claim 16: Magnetic field sources(s)' magnetised/wound a like mutually-repulsive pole to each

other, to achieve a repulsion/propulsion between these magnets.

19. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claims 17, 18: 'Magnetic field sources(s)' magnetised/wound a vertical direction 'up

through them', or circular about their centre-column; to achieve a like pole around a magnets side-circumference; to achieve a 'always' 'like/repulsive pole' / unlike/attractive pole' toward another magnet(s).

20. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claims 16, 17,18,19: A mutually 'biased magnetic fields' between a ring of 'shielded

magnet(s)' and a/any outer-circumference/inner-circumference/above/below surrounding 'ring magnet(s)'; to achieve a mutually biased magnetic propulsion between the 'shielded magnet(s)' / 'ring magnet(s).

21. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claim 20: A ring of shielded magnets' being a single solid shield structure; where the 'ring of shielded magnets' 'magnet(s)' are 'latched'/bonded/embedded into it.

22. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in Claims 16, 17,18,19,20,21: A 'ring magnet' surrounding the outer-circumference of a 'ring of shielded magnets'; where any particular 'shield' materials respective shield(s) '-'magnet(s)' designed/shapes/placements directiontrajectory-

bias/'magnetlc engine' are of that substantially described and two illustrated in the accompanying descriptions and drawings.

23. A 'Consistent Kinetic Motion'/'Magnetic Engine' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.

24. A 'Embedded Dynamo' claimed within Claim l: A stationary magnetic field source(s) inducing a magnetic field / electrical current into a rotating

shield'; the shield inducing a magnetic field / electrical current into a

stationary conductive material(s) placed beside/around it; where the 'shield(s)' and/or 'magnetic field source(s)' are/are-not facilitated by a 'magnetic engine'.

25. A 'Embedded Dynamo/Alternator' claimed within Claim 1: A rotating ring of 'shielded r,agnets' facilitated by a 'magnetic engine', where the ring of shielded magnets 'magnets' and/or 'shields' induce a magnetic field / electrical

current into a stationary conductive material(s) placed beside/around it/them.

26. A 'Embedded Dynamo' claimed within Claim 1: A rotating 'ring magnet(s) ' facilitated by a 'magnetic engine'' inducing a magnetic field /

electrical current into a stationary conductive material(s) placed beside/around it/them.

i? . 27 A 'Embedded Dynamo/Alternator' claimed within Claim 1: Traversing / rotating 'magnetic field source(s)' facilitated by a machine/'magnetic engine' for

other purposes, inducing a magnetic field / electrical current, by its/their

traversion/rotation into a stationary conductive materials(s) placed beside/around it/them. 28. A 'Embedded Dynamo/Alternator' claimed in Claims 24,25,26,27: A stationary conductive material being a/any 'conductive materiel '/component facilitated by a machine; where a conductive material(s) may or may-not be stationary. 29. A 'Embedded Dynamo/Alternator'/'magnetic bearing' claimed within Claim 1: A stationary superconductor(s) / antiferromagnetic(s) / magnetic-material(s) material placed beside/around a rotating/traversing magnetic component(s) required to be supported; the magnetic component(s) inducing a electrical current into the material(s); the magnetic component(s) being mutually repelled / supported by the material(s). 30. A 'Embedded Dynamo/Alternator' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and one illustrated in the accompanying descriptions and drawings.

31. A 'Embedded Magnetic Bearing' claimed within Claim 1: A ring of shielded magnet(s)' 'magnet(s)' and/or 'shield(s)' mutually repelling to a 'ring magnet(s); to mutually support 'the ring of shielded magnets' / 'ring magnet(s)'; where any of the 'ring of shielded magnets'-'shields ''magnets ' / 'ring magnet(s)' are/are-not facilitated by a 'magnetic engine'; 32. A 'Embedded Magnetic Bearing' claimed within Claim 1: A 'magnet(s)' and or 'shield(s)' mutually repelling to a 'other magnet(s)', to mutually support each 'magnet(s)' / 'shield(s)' / 'other magnet(s)'; where any of the 'magnet(s)' / shield(s)' / 'other magnet(s)' are/are-not facilitated by a 'magnetic engine'.

33. A 'Embedded Magnetic Bearing' claimed within Claim 1: A rotating 'ring magnet(s)' facilitated by a 'magnetic engine', having stationary 'respectfully magnetised magnetic' / 'antiferromagnetic' / 'superconductor' ring magnet shaped material(s), placed 'above and below its flat top and bottom surfaces' and/or around its inner and/or outer circumference(s)'; to achieve a mutual repulsion/support between them.

A.., 34. A 'Embedded Magnetic Bearing' claimed within Claim 1: Rotating / traversing magnetic field source(s) facilitated by a machine/'magnetic engine' for

other purposes / equally required to be supported, having stationary 'respectfully magnetized magnetic material' / 'antiferromagnetic material' / 'superconductor material' placed around it/them; to achieve a mutual repulsion/support between them. 35. A 'Embedded Magnetic Bearing' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.

36. 'Latches'/'Latched' claimed within any preceding/proceeding Claim(s): Machine components non-chemically bonded/'latched' together; each respective component(s) having equal and opposite latches set into them, to achieve each component(s) latching into each other components equalopposite latch) these latches may be elliptical shapes of the components themselves or oddities sticking out of' or 'in to' these components; to a end to achieve a non-chemical 'equal-

opposite latched' bond between components.

37. 'Latches' claimed in Claim 36: A 'shielded magnets' 'shield(s)' and magnet(s)' created with equal-opposite 'latches' set into them, such that a magnet may latch into a shields equal-opposite latch; these latches may be elliptical shapes of the magnets / shields themselves or oddities sticking 'out of' or 'in to' these components; to achieve a non-chemical bond between the shield(s) and magnet(s). 38. 'Latches' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and two illustrated in the accompanying descriptions and drawings.

/S 39. A 'Machine Housing' claimed in Claim 1: non magnetic non electrically conducting material such as a plastic/Perspex or glass, with [latches' internally inset/moulded into it, such that the machines components this housing supports latch into its latches; these latches may be elliptical shapes of the components themselves or oddities sticking 'out of' or 'in to' these components, to a end to achieve a non- chemical 'equal-opposite latched' bond between a machines components and housing.

40. A 'Machine Housing' claimed in Claim 39: Manufactured to support its machines components by casting the housing material around the machines components; the machines components being supported by a temporary structure, while the housing is cast, the temporary structure being chemically broken down once the machines housing has set.

41. A 'Machine Housing' claimed in Claim 40: A temporary deteriorating structure being a metal/copper, chemically broken down by a chemical/ferric chloride. 42. A 'Machine Housing' claimed in/within any preceding/proceeding Claim(s): Implemented/created by any combinations of individual components, configurations and implementations of that substantially described and one illustrated in the accompanying descriptions and drawings.
43. Any Magnetic / Permeable / Conductive component(s) claimed in/within any preceding/proceeding Claim(s): Each magnetic / permeable / conductivecomponent being laminated to reduce mutual magnetic resistance forces between itself and other traversing/rotating magnetic / permeable / conductive components.
44. A 'Lamination' claimed within Claim 43: Implemented as the machine housing fully-thinly encompassing around stationary components it already supports/latches-to.
45. A 'Ring Magnet' claimed within any preceding claim: A 'ring magnet' equally being a 'ring of magnets'.
46. Any preceding Claim(s): A 'Magnetic Engine / Dynamo/Alternator' machine implemented/created by any combinations of individual components, configurations and implementations of that substantially described and some illustrated in the accompanying descriptions and drawings.
47. A 'Magnetic Engine / Dynamo/Alternator' machine implemented/created by any combinations of individual components, configurations and implementations of that substantially described and some illustrated in the accompanying descriptions

and drawings.