A Practical Guide to 'Free-Energy' Devices

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energy density will be E x H / 2C and it will have the appearance of a steady E-field. In the same way, if the E fields cancel out, the result will appear to be a steady "H" field. Modern physics is based on the faulty assumption that electromagnetics contains two kinds of energy: electric and magnetic. This leads to the Baroque view of physical reality. Under that view, energy seems to be associated with the square of the field intensity, rather than a more reasonable view that it is directly to the field intensity. It is worth remembering that neither Einstein nor most modern physicists were, or are, familiar with the concept of "energy current" described here. However, their work still survives by ignoring the energy current concept, scalar electromagnetics, the works of Tom Bearden, kaluza-Klein and others who dispute Heaviside's interpretations of Maxwell's equations. The Fallacy of Displacement Current: Conventional electromagnetic theory proposes that when an electric current flows down a wire into a capacitor, it spreads out across the plate, producing an electric charge on the plate which in turn, leads to an electric field between the plates of the capacitor. The valuable concept of continuity is then retained by postulating a displacement current "after Maxwell". This current is a manipulation of the electric field "E" between the plates of the capacitor, the field having the characteristics of electric current, thus completing the flow of electricity in the circuit. This approach allows Kirchoff's laws and other valuable concepts to be retained even though superficially, it appears that at the capacitor there is a break in the continuous flow of electric current. The flaw in this model appears when we notice that we notice that the current entered the capacitor at only one point on the capacitor plate. We are then left with the major difficulty of explaining how the electric charge flowing down the wire suddenly distributes itself uniformly across the entire capacitor plate at a velocity in excess of the speed of light. This paradoxical situation is created by a flaw in the basic model. Work in high-speed logic carried out by Ivor Catt has shown that the model of lumped capacitance is faulty and displacement current is an artefact of the faulty model. Since any capacitor behaves in a similar way to a transmission line, it is no more necessary to postulate a displacement current for the capacitor than it is necessary to do so for a transmission line. The removal of "displacement current" from electromagnetic theory has been based on arguments which are independent of the classic dispute over whether the electric current causes the electromagnetic field or vice versa. The Motional E-Field: Of all of the known fields; electric, magnetic, gravitational and motional E-field, the only ones incapable of being shielded against are the induced motional E-field and the gravitational field. The nature of the motionally-induced electric field is quite unique. In order to understand it more fully, we must start by discarding a few misleading ideas. When magnetic flux is moved perpendicularly across a conductor, an electromotive force ("e.m.f.") is electromagnetically induced "within" the conductor. "Within" is a phrase which comes from the common idea of comparing the flow of electric current within a wire to the flow of water in a pipe. This is a most misleading comparison. The true phenomenon taking place has little been thought of as involving the production of a spatially- distributed electric field. We can see that the model's origins are likely to have arising from the operation called "flux cutting" which is a most misleading term. A better term "time-varying flux modulation" does not imply any separation of lines of flux. Truly, lines of flux always form closed loops and are expressed mathematically as line integrals. It is a fallacy to use the term "cutting" which implies time-varying separation which does not in fact ever occur. A motionally-induced E-field is actually created within the space occupied by the moving magnetic flux described above. The field is there whether or not a conductor is present in the space. In terms of a definition, we can say that when magnetic flux of vector intensity B-bar is moved across a region of space with vector velocity V-bar, an electromagnetically induced electric field vector B x V appears in the space at right angles to both B-bar and V-bar. Therefore: E = B-bar x V-bar . . . . . . . . . . . . . . . . . . . (1) It is this field which is related to gravity and which is virtually unshieldable. This field may be called the Motional E-field. According to Tom Bearden, "It seems that the charged particles in the atom act like tiny magnets and their motion in the space surrounding the atom would create this motional E-field". The fields created by both the positive and negative charges would cancel to some degree, but due to the high orbital velocity of the negative electron relative to that of the positive proton, the induced field of the electron would dominate the resulting field. The field produced as a result of these charges would vary in proportion to the inverse square of the distance as gravity does. The field produced by the translational motion of the charges would vary inversely as the cube of distance. This concept totally unites the A - 1204
electromagnetic and gravitational field theories and accounts for the strong and weak force within the atom. Field Super-Position and the Vacuum Triode: Electromagnetic induction with no measurable magnetic field is not new. It is well known that in the space surrounding a properly wound toroidal coil, there is no magnetic field. This is due to the superposition of the fields. However, when alternating current is surging through a transformer, an electric field surrounds it. When we apply the principle of super-position to the vacuum triode, it becomes more obvious how the device is operating. The principle of super-position states that "in order to calculate the resultant intensity of superimposed fields, each field must be dealt with individually as though the others were not present" The resultant is produced by the vector addition of each of the fields considered on its own. Consider for a moment, the construction of the triode which includes two bi-filar coils located within the fields of two conditioned magnets. When the current in one half of the conductors in the coils (that is, just one strand of the twin windings in each coil) is increasing, both the current and the magnetic field follow the right-hand rule. The resulting motional E-field would be vertical to both and directed inwards. At the same time, the current in the other strand of each winding is decreasing and both the current and the magnetic field also follow the right-hand rule. The resulting motional E-field is again vertical to both, and directed inwards. So, the resultant combined field intensity is double the intensity produced by either one of the conductors considered on its own. Expressed mathematically, this is: E = (B x V) + (-B x -V) or E = 2 (B x V) . . . . . . . . . . . . . . . . . . . . . . . (2) Where: E is the electric field intensity B is the magnetic field intensity and V is the electron drift velocity (B x V), the first term in the equation, represents the flow of the magnetic field when the electrons are moving in one direction, while (-B x -V), the second term in the equation, defines the flow of the magnetic field when the electrons are moving in the other direction. This indicates that field intensity is directly proportional to the square of the current required by the load placed on the device. This is due to it's proportional relationship with the virtual value of the magnetic field which theory states is proportional to the current. Electrometer readings were always close to parabolic, indicating that the source was of infinite capacity. It was further determined through experiment, that the magnetic field does not change with temperature. Also, there is no reason yet identified, which would lead one to believe that electron drift velocity changes. It has been found remarkable that the vacuum triode runs approximately 20 O F below ambient. Induced Electromotive Force - Positive Energy: When an e.m.f. ("electromotive force") is applied to a closed metallic circuit, current flows. The e.m.f. along a closed path "C" in space is defined as the work per unit charge (that is, W / Q) done by the electromagnetic fields on a small test charge moved along path C. Since work is the line integral of Force ("F"), the work per unit charge is the line integral of force per unit charge (in Newtons per Coulomb) we have: The scalar product "(F/Q) x dtdl" is the product of (F/Q) x Cosθ x dl where θ denotes the angle between the vectors F/Q and dl. The electric force per unit charge is the electric field intensity ("E") in volts per metre. The magnetic force per unit charge is V x B where "V" denotes the velocity of the test charge in metres per second and "B" denotes the magnetic flux density in webers per metre squared. In terms of the smaller angle θ between V and B, the cross product of V and B is a vector having the magnitude VBSinθ. The direction of vector V x B is at right angles to the plane which contains vectors V and B in accordance with the right-hand rule (that is, V x B is in the direction of the thumb while the fingers curl through the angle θ from V towards B). Since the total force per unit charge is E + VB, the total e.m.f. in terms of the fields is: A - 1205
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JUAN AGUERO Patent Application EP04
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the exhaust manifold. This heats so
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combustion chambers. The hydrogen i
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21. The system of claim 20, charact
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electrolysis of water at such a rat
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Fig.4 is an elevation view of the h
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Fig.10 is a cross-section on the li
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Fig.16 is a cross-section on the li
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Fig.23 is an enlargement of part of
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Fig.33 is a perspective view of a v
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A - 843
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through a resistor R4 to provide tr
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The installation of the above circu
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cathode in the upper region of the
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transformer and, assuming an input
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valve apparatus to control engine s
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. a first hollow cylindrical electr
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CHRISTOPHER ECCLES UK Patent App. 2
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Fig.1 is a circuit diagram of fract
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If a large electric field is applie
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The pulses R1 and S1 are of the sam
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DISCLOSURE OF THE INVENTION The inv
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A - 867
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Fig.5B shows a stylised representat
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Fig.6 shows a gas collection system
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Fig.8A and Fig.8B are views of a se
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A - 875
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Figs.16-30 are graphs supporting th
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A - 887
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If it is the case that the hydrogen
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plate shown in Fig.1A and Fig.1B an
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is in equilibrium where the 10 watt
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The previously mentioned prior art
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The stores of high pressure gases c
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unit to retain operational gas pres
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HENRY PAINE This is a very interest
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Henry Paine’s apparatus would the
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some form of distortion of space. I
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superconductive disk is made part o
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Fig.2A and Fig.2B are diagrams, pre
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Fig.4A and Fig.4B are diagrams, pre
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#1 hollow superconductive shield #2
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Fig.2B shows the counter-clockwise
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In this example, the difference bet
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CHARLES POGUE US Patent 642,434 12t
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Fig.3 is a horizontal sectional vie
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Fig.9 and Fig.10 are detail section
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having a valve 52 in it. Chamber 50
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CHARLES POGUE US Patent 1,997,497 9
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Fig.4 is a detail sectional view of
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A low-speed or idling jet 25 has it
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DESCRIPTION OF THE DRAWINGS Fig.1 i
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Fig.5 is a detail sectional view on
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Vapour formed by air bubbling throu
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From the foregoing description it w
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Fig.2 is an enlarged view of the de
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Fig.6 is a section taken along line
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ROBERT SHELTON US Patent 2,982,528
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Fig.4 is a transverse sectional vie
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HAROLD SCHWARTZ US Patent 3,294,381
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182,420 now abandoned. The present
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DESCRIPTION OF THE INVENTION The ca
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THOMAS OGLE US Patent 4,177,779 11t
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In accordance with other aspects of
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Fig.3 is a sectional view of the va
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Fig.7 is a partial side, partial se
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The cooling system of the vehicle c
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Upon initial starting of the engine
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(f) A filter positioned in the vapo
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with the magnitude of the current a
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Fig.1B is a perspective view of the
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Fig.3 is a top view of the motor of
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Fig.7 is an isometric view showing
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Fig.10 is a top view showing the ro
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Fig.13 is a top view of a pair of r
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Extending in opposite diametric dir
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Fig.5 shows the state of the switch
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otor magnets 42 - 49 when in the ho
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Fig.9 and Fig.10 show a second arra
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constructed otherwise than as speci
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12. The motor of claim 11 wherein t
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timer or a control mechanism mounte
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Fig.4 is a view similar to Fig.3 bu
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Fig.10 is a view similar to Fig.3 f
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Fig.13 is a schematic circuit diagr
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Fig.16 is a simplified embodiment o
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Fig.22 to Fig.25 are similar to Fig
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Referring to Fig.2, the permanent m
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Fig.7 shows a modified embodiment w
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them, will depend upon the order in
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Fig.14, shows another embodiment 14
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Fig.18 shows the air coil 210 posit
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Figs. 22-25 show four different pos
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movement with the first permanent m
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a shaft and means journaling the sh
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CLAUDE MEAD and WILLIAM HOLMES US P
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Fig.2 is a front elevation of the w
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impactors and drills. The turbine d
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(a) fourth rotating means responsiv
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path to the other side of the perma
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Fig.3 is an oscilloscope waveform t
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DETAILED DESCRIPTION OF THE PREFERR
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although it is by no means obvious
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second diode connected at its posit
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In the present invention, a permane
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Fig.4 is a circuit diagram, illustr
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and Fig.3. In practice, this coil m
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y a simultaneous magnetic accelerat
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Mr. P.G. Mallory started out in 191
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All models have a 30 Watt power rat
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In the auto racing circles it has a
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BATTERY + _ SIMPLIFIED MULTIVIBRATO
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Schematic Wiring Diagrams for two P
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motor. What is not generally known,
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Mark McKay's investigation of Edwin
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Investor Photo #012D Popping a coil
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capacitors connected in series, wit
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PULSE WIDTH TIME IN mS went to the
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TOP DEAD CENTER 0° REFERENCE Accor
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The recovery and simple analysis of
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FILTER CAPACITOR + 2 OHM 200 WATT R
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Subject: CSET design Date: Sun Feb
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Date: Fri Feb 28, 2003 8:25 pm (Tim
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(Tad Johnson) I'm being as careful
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SANGAMO ENERGY DISCHARGE CAPACITOR
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(Alan Francoeur) But I also measure
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Subject: Progress Date: Sun Mar 30,
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● all electrical connections were
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Mark Gray claims that the heart and
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Mark Gray claims that some potentia
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Radio Frequency (RF) Generator Gene
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Some time during 1987 - 1988, Gray
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The two-channel trace from the osci
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What “maximum squareness” means
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Zo = 112 Ohms Td of 293 nS. 50 KV 8
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MIKE BRADY’S “PERENDEV” MAGNE
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Fig.3 is a perspective view showing
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Fig.7 is a perspective view showing
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In the rotor assembly 30 of Fig.2,
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Fig.7 shows a typical magnetic sour
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DONALD A. KELLY ABSTRACT Patent US
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This series of magnetic oscillating
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Because there is no natural, lock-i
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Fig.3 is an enlarged top view of on
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An arm 9, is fastened to a flat fac
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Fig.2 is a vertical transverse cros
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Fig.6 is a vertical, longitudinal,
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Working inside the cylinders 12 are
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Leroy K. Rogers Patent US 4,292,804
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Preferred embodiments of a method a
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Fig.6 is a cross-sectional view of
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Fig.8 is a cross-sectional view of
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tapped hole in the cylinder 20 typi
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A second embodiment of a valve actu
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otates faster, the other end 98 of
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In normal operation (as seen in Fig
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Eber Van Valkinburg Patent US 3,744
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Referring to the drawings in detail
Page 331 and 332: Since the pump depends for its supp
Page 333 and 334: Briefly, in one aspect the engine o
Page 335 and 336: Fig.5 is a cross-sectional view of
Page 337 and 338: Fig.12 is a cross-sectional view si
Page 339 and 340: Fig.14 is a schematic diagram of an
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Page 345 and 346: Figs.20A-20F are schematic diagrams
Page 347 and 348: Note: Corresponding reference chara
Page 349 and 350: Integral with the piston bodies are
Page 351 and 352: The piston has a generally semi-tor
Page 353 and 354: Referring back to Fig.13A, for engi
Page 355 and 356: As piston 39A reaches BDC, distribu
Page 357 and 358: mixture and do not combine because
Page 359 and 360: These wires are about twelve gauge,
Page 361 and 362: cold-cathode tube 391, and an x-ray
Page 363 and 364: Fig.17D), polariser 289, branch B17
Page 365 and 366: Robert Britt US Patent 3,977,191 31
Page 367 and 368: Fig.3 is an elevational view of the
Page 369 and 370: Fig.7 is an electrical schematic of
Page 371 and 372: Referring now to Fig.3 of the drawi
Page 373 and 374: and drives Q1 into conduction. The
Page 375 and 376: Floyd Sweet Recently, some addition
Page 377 and 378: The day when we witnessed the VTA d
Page 379 and 380: up to see Floyd. Floyd was with the
Page 381: Energy cannot enter a space of zero
Page 385 and 386: or in another form: So, the e.m.f.
Page 387 and 388: Example 2: Suppose the conductor wi
Page 389 and 390: Meguer Kalfaian There is a patent a
Page 391 and 392: Fig.2 illustrates a controlled top
Page 393 and 394: Fig.9 is a modification of Fig.6; a
Page 395 and 396: the outer periphery of the magnet,
Page 397 and 398: wobbling top is sufficient, as proo
Page 399 and 400: Theodore Annis & Patrick Eberly US
Page 401 and 402: BRIEF DESCRIPTION OF THE DRAWINGS F
Page 403 and 404: Fig.6 is a schematic diagram of a s
Page 405 and 406: DETAILED DESCRIPTION OF THE PREFERR
Page 407 and 408: Fig.5 is a detail drawing of an alt
Page 409 and 410: In the preferred implementation of
Page 411 and 412: William McDavid junior US Patent 6,
Page 413 and 414: This sloping floor causes the drive
Page 415 and 416: FIG.3 is a side elevational view of
Page 417 and 418: FIG.9 is a horizontal cross-section
Page 419 and 420: otational downstream annular chambe
Page 421 and 422: In Fig.5 is shown a perspective vie
Page 423 and 424: small hydro-electric version of the
Page 425 and 426: Fig.10 is a perspective view of a s
Page 427 and 428: longitudinally mounted in the upstr
Page 429 and 430: shaft in the central aperture, said
Page 431 and 432: Scientific Papers The following lin
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