A Practical Guide to 'Free-Energy' Devices
A Practical Guide to 'Free-Energy' Devices
A Practical Guide to 'Free-Energy' Devices
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This magnetic disc drive represents a practical solution in applying permanent magnetism in the development and<br />
commercialism of a decentralised, silent, fuel-free, household-sized alternate power system. While the power<br />
output from an individual magnetic disc unit may be small, the power output is constant and does not generally<br />
depend on the intensity of an external energy source, as do present solar energy systems.<br />
SUMMARY OF THE INVENTION<br />
The magnetic disc drive unit is comprised of a large driving disc made of non-magnetic metal on which several<br />
permanent magnets are equally spaced around the rim. The disc drive shaft rotates on trunnion supported ball<br />
bearings and may revolve in nearly any conventional position, and may be constructed with any practical large<br />
diameter.<br />
The identical oscillating magnet pairs are the driving component of the disc drive and consist of flat, non-magnetic<br />
plates on which, pairs of identical permanent magnets are secured at both sides of the oscillation plates. These<br />
magnet pairs have opposite pole faces facing each other. The disc's direction of rotation is determined by the<br />
polarity of all the disc's magnets relative <strong>to</strong> the polarity of the oscillating magnet pairs.<br />
The oscillating pair of magnets make a full back and forth oscillation while each ro<strong>to</strong>r disc magnet passes by.<br />
This produces a pull on the disc magnet as it approaches the oscilla<strong>to</strong>r magnet and then when the oscilla<strong>to</strong>r<br />
moves that magnet away, a push force is applied <strong>to</strong> the magnet on the rotating disc by the second magnet of the<br />
oscillating pair of magnets. The synchronisation of the disc and the oscillating magnet pairs must be maintained<br />
for continuous and smooth rotation of the disc. This movement is similar <strong>to</strong> the action of a clock escapementmechanism.<br />
The method of moving the oscillating pairs of magnets is one or more solar-powered DC mo<strong>to</strong>rs. These mo<strong>to</strong>rs<br />
drive push rods which are in contact with ball bearings mounted on the oscillation plates. Since the eccentrics<br />
must move at relatively slow speeds, suitable gear reduction units must be used between the mo<strong>to</strong>rs and the<br />
rocker arms.<br />
In order <strong>to</strong> maintain proper synchronisation of all of the oscillating components, straight links are used <strong>to</strong> connect<br />
all of the driven oscillation shafts <strong>to</strong> the driving oscillation shaft. Four or five oscillation stations can be driven from<br />
one driver oscillation shaft so that a disc drive with a large number of oscillation stations will require several D.C.<br />
mo<strong>to</strong>rs <strong>to</strong> drive all of the other oscillation shafts.<br />
It is important that the multiple, identical oscillation plates and their magnet pairs be slightly shorter in width than<br />
the space between two adjacent disc magnet segments, so that an optimum pull and push force is induced on the<br />
local disc magnet segments. One side of the oscillating magnet couple "pulls" on the disc's permanent magnet<br />
and then the other oscilla<strong>to</strong>r magnet "pushes" the disc's permanent magnet onwards as it has been moved in<strong>to</strong><br />
place by the oscillation.<br />
All of the oscillating magnet pairs oscillate on stationary rods, or shafts, and all of the eccentrics and DC mo<strong>to</strong>r<br />
drives remain fixed on a base plate. The other ends of the oscillating rods or shafts must be supported by some<br />
form of bracket <strong>to</strong> keep the oscillation plates parallel <strong>to</strong> the disc magnet segments. Each eccentric which moves a<br />
ball bearing attached <strong>to</strong> arms on the oscillation plates must make one full 360 degree revolution within the angular<br />
displacement arc between two adjacent ro<strong>to</strong>r disc magnet segments. Two small pivot brackets are attached <strong>to</strong><br />
the extreme, non-magnetic ends of the oscillation plates <strong>to</strong> allow these plates <strong>to</strong> oscillate freely with a minimum of<br />
friction.<br />
The basic rotational relationship between the magnetic oscillating pairs, and the magnetic segmented disc, will<br />
have a bearing on the gear reduction ratio required for the gear drive unit coupled <strong>to</strong> the small DC mo<strong>to</strong>rs. Fairly<br />
rapid oscillation is necessary <strong>to</strong> maintain a reasonably acceptable disc speed which will be required for most<br />
power applications. The size of the eccentrics which oscillate the oscillating magnet pairs will be determined by<br />
the full oscillating arc needed and the mechanical advantage required by the oscillation plate in order <strong>to</strong> cause the<br />
optimum rotation of the magnetic disc drive unit.<br />
Proper magnetic disc drive functioning requires the pulling magnets of the oscillating magnet pairs <strong>to</strong> enter the<br />
disc's interference circle within the mutual magnetic field zone between the two local interacting magnets on the<br />
disc's rim. Since the disc will revolve continuously, the withdrawing phase of the "pulling" magnets brings the<br />
"pushing" magnets of the couple in<strong>to</strong> the disc's interference circle within the mutual magnetic field zone, for<br />
effective interaction with the adjacent disc magnet segment.<br />
All of the magnet segments on the oscillation plates which form the magnetic couples must be in line with the<br />
corresponding disc magnet segments in order <strong>to</strong> maintain an optimum interaction between them.<br />
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