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A Practical Guide to 'Free-Energy' Devices

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Whereas, the field in a direction perpendicular <strong>to</strong> the axis of the electron produces a quadrature phased<br />

electromagnetic radiation. Thus, instead of utilising the output of electron precession for energy purposes, it may<br />

be utilised for field radiation of either light or electromagnetic waves, such as indicated by the arrows in Fig.9. In<br />

this case, the output will be coherent field radiation.<br />

In reference <strong>to</strong> the arrangement of Fig.6, the electron emission is shown <strong>to</strong> occur within the central magnetic field<br />

of the focusing magnet M5. It may be practically desired, however, that these electrons are injected in<strong>to</strong> the<br />

central field of the cylindrical magnet from a gun assembly, as shown in an exemplary arrangement of Fig.10. In<br />

this case, the vacuum chamber C is flanged at the right hand side, for mounting an electron emitting cathode 1<br />

(the filament not being shown), and a curved electron-accelerating gun 2. The central part of this flange is<br />

recessed for convenience of mounting an electron-tilting magnet (as shown), as close as possible <strong>to</strong> the electron<br />

beam. In operation, when current is passed through the filament, and a positive voltage is applied (not shown) <strong>to</strong><br />

the gun 2, the emitted electrons from the cathode are accelerated and injected in<strong>to</strong> the central field of the magnet<br />

11. Assuming that the open end of the gun 2 overlaps slightly the open end of the cylindrical central field of the<br />

magnet M1, and the positive accelerating voltage applied <strong>to</strong> the gun 2 is very low, the accelerated electrons will<br />

enter the central field of the magnet M1, and travel <strong>to</strong> the other end of the field. Due <strong>to</strong> the low speed acceleration<br />

of the electrons, however, they cannot spill out of the field, and become permanently entrapped therein.<br />

In regard <strong>to</strong> the direction in which the coil L1 is positioned, its winding should be in a direction perpendicular <strong>to</strong> the<br />

longitudinal axis of the beam <strong>to</strong> which the polar axes of the electrons are aligned uniformly in parallel. In one<br />

practical mode, the coil L1 may be wound in the shape of a surface winding around a tubular form fitted over the<br />

cylindrical vacuum chamber.<br />

In regard <strong>to</strong> the operability of the apparatus as disclosed herein, the illustration in Fig.7 shows that the field output<br />

in a direction parallel <strong>to</strong> the polar axis of the electron is singular phased, and it produces the effect of light when<br />

the precessional frequency is at a light frequency. Whereas, the output in a direction perpendicular <strong>to</strong> the polar<br />

axis of the electron is quadrature phased, which is manifested in practiced electromagnetic field transmission.<br />

In regard <strong>to</strong> experimental references, an article entitled "Magnetic Resonance at high Pressure" in the "Scientific<br />

American" by George B. Benedek, page 105 illustrates a precessing nucleus, and indicates the direction of the<br />

electromagnetic field radiation by the precessing nucleus. The same technique is also used in the medical<br />

apparatus "Nuclear magnetic resonance" now used in numerous hospitals for imaging ailing tissues (see "High<br />

Technology" Nov. Dec. 1982. Refer also <strong>to</strong> the technique of detecting Electron Spin Resonance, in which<br />

electrons (called "free radicals") are precessed by the application of external magnetic field <strong>to</strong> the tissue matter. In<br />

all of these practices, the electromagnetic field detecting coils are directed perpendicular <strong>to</strong> the polar axes of the<br />

precessing electrons or the nuclei.<br />

In regard <strong>to</strong> the production of light by a precessing electron, in a direction parallel <strong>to</strong> the polar axis of the<br />

precessing electron, see an experimental reference entitled "Free electrons make powerful new laser" published<br />

in "high Technology" February 1983 page 69.<br />

In regard <strong>to</strong> the aspect of producing and s<strong>to</strong>ring the electrons in a vacuum chamber, it is a known fact by practice<br />

that the electrons are entrapped within the central field of a cylindrical permanent magnet, and they will remain<br />

entrapped as long as the magnet remains in position.<br />

With regard <strong>to</strong> the performance of obtaining precessional resonance of the electron, the simple example of a<br />

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