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A Practical Guide to 'Free-Energy' Devices

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An arm 9, is fastened <strong>to</strong> a flat face of the flat plate 3a, which supports the pin 10a, which carries the ball bearing<br />

10, as it rolls on the eccentric disc 11. The off-centre disc 11, is fastened <strong>to</strong> the slow speed shaft of the gear<br />

reduction unit 12, which is driven by the small DC mo<strong>to</strong>r 13. A return tension spring 14, is connected <strong>to</strong> the<br />

oscillation plate 3a, by eyelet 3e. The opposite end of the return tension spring 14, is retained by the post 15,<br />

which is pressed in<strong>to</strong> the base plate 4. Mo<strong>to</strong>rs 13, are powered by multiple arrays of silicon pho<strong>to</strong>voltaic solar<br />

cells 16. Electrical leads 16a, conduct solar converted electricity <strong>to</strong> the mo<strong>to</strong>rs 13, with any excess current s<strong>to</strong>red<br />

in the batteries 16b.<br />

The mo<strong>to</strong>r driven oscillation stations become the master stations for this invention 1, from which three <strong>to</strong> five slave<br />

oscillation stations are driven. The reciprocating motion is transmitted by straight links 17, which are pinned <strong>to</strong> the<br />

link arms 18, which in turn are secured <strong>to</strong> the flat plates 3a.<br />

All of the slave oscillation stations must be precisely adjusted <strong>to</strong> exactly the same angular position as the master<br />

driving oscillation station so that all stations are synchronised <strong>to</strong> allow proper functioning of the rotating disc 2.<br />

For very large discs 2, with many disc magnets, several master oscillation stations, with a fixed number of slave<br />

oscillation stations will be required. All of the master oscillation driving-stations will have <strong>to</strong> be electrically<br />

synchronised <strong>to</strong> maintain overall synchronisation, with all of the eccentrics 11, set at the same angle at start-up of<br />

the disc.<br />

Either end of the drive shaft 5, may be connected with a speed step-up belt drive arrangement, which is not<br />

shown here.<br />

Plastic deflec<strong>to</strong>rs 19, are added <strong>to</strong> either side of the oscillation plates 3a, adjacent <strong>to</strong> the opposite magnets<br />

segments 3b, and 3c, their exact position depending on the direction of rotation of disc 2. These act as an antijamming<br />

device for the magnets.<br />

Magnetic field bias angles 3f and 3g (Fig.3), are required for the sides of plates 3a, in order <strong>to</strong> assure an optimum<br />

"pull-push" sequence on the large drive disc 2, as the magnetic oscillation pairs 3, are actuated. The bias angle<br />

3f, is matched <strong>to</strong> the magnet segment 3b, while bias angle 3g is matched <strong>to</strong> magnet segment 3c.<br />

None of the load components which are external <strong>to</strong> the device, such as an electric genera<strong>to</strong>r or alterna<strong>to</strong>r, are<br />

shown as a part of this invention, since a variety of load devices and arrangements are possible for the magnetic<br />

disc drive.<br />

A - 1125

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