A Practical Guide to 'Free-Energy' Devices

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Fig.8 illustrates the actuator 36 for reciprocating the actuator arm 38 in response to rotation of the rotor shaft 10 and the alternating polarity of the solenoid 74. The actuator 36, includes the solenoid 74, the toroidal permanent magnet 90, an elastic flexible spider 92 for supporting the solenoid above the plane of the magnet, and a basket or frame 94, to which the spider is secured. The actuator arm 38 is secured to solenoid 74. The polarity of the solenoid 74 changes as rotor shaft 10 rotates, causing the solenoid and actuator arm 38 to reciprocate due to the alternating polarity of the solenoid relative to that of the toroidal permanent magnet 90. As the solenoid polarity changes, the actuator arm 38 reciprocates linearly due to the alternating forces of attraction and repulsion of the solenoid 74 relative to the poles of the magnet 90. The actuator arm 38 is secured to the oscillator arms 20, 22 and 24 causing them to pivot, and the reciprocating magnets 50 – 52, secured to the oscillator arms, to reciprocate. Alternatively, the reciprocating magnets 50 – 52 can be secured directly to the arm 38 , so that the magnets 50 – 52 reciprocate without need for an intermediary oscillating component. It is important to note at this point in the description that, when two magnets approach each other with their poles of like polarity facing each other but slightly offset, there is a tendency for the magnets to rotate to the opposite pole of the other magnet. Therefore, in the preferred embodiment of the instant invention, the angular position at which the switch assembly of the actuator 36 changes between the states of Fig.4 and Fig.5 is slightly out of phase with the angular position of the rotor shaft 10 to help sling or propel the actuator arm 38 in the reverse direction at the preferred position of the rotor shaft. The optimum phase offset is approximately 5–8 degrees. This way, advantage is taken of each rotor magnet's tendency to rotate about its own magnetic field when slightly offset from the respective reciprocating magnet, and the repulsive force between like poles of the reciprocating magnets and the rotor magnets is optimised to propel the rotor magnet about the rotor axis 11, thereby increasing the motor's overall efficiency. Fig.12 is a graph showing the angular displacement 96 of the rotor shaft 10 and linear displacement 98 of the reciprocating magnets 50 – 52. Point 100 represents the end of the range of displacement of the reciprocating magnets 50 – 52 shown in FIGS. 2 and 9, and point 102 represents the opposite end of the range of displacement of the reciprocating magnets 50 – 52 shown in FIGS. 3 and 10. Point 104 represents the angular position of the A - 984
otor magnets 42 – 49 when in the horizontal plane shown in FIGS. 2 and 9, and point 106 represents the angular position of the rotor magnets 42 – 49 when rotated one-half rotation to the horizontal plane shown in Fig.3 and Fig.10. Preferably, the reciprocating magnets 50 – 52 and rotor magnets 42 – 49 are out of phase: the reciprocating magnets lead and the rotor magnets lag by several degrees. The reciprocating magnets 50 – 52 reach the respective extremities of their range of travel before rotor rotation moves the rotor magnets 42 – 49 into the horizontal plane. When the reference poles 54 and opposite poles 56 of the rotor magnets 42 – 49 and reciprocating magnets 50 – 52 are arranged as shown in Fig.2 and Fig.3, the rotor position is stable when the rotor magnets are in a horizontal plane. The rotor position is unstable in any other angular position, and it moves towards horizontal stability from any unstable position, and is least stable when the rotor magnets 42 – 49 are in a vertical plane. The degree of stability of the rotor shaft 10 is a consequence of the mutual attraction and repulsion of the poles of the rotor magnets 42 – 49 and reciprocating magnets 50 – 52 and the relative proximity among the poles. In Fig.2, the reciprocating magnets 50 – 52 are located at a first extremity of travel. In Fig.3, the reciprocating magnets 50 – 52 have reciprocated to the opposite extremity of travel, and the rotor magnets have rotated one-half revolution from the position shown in Fig.2. When the rotor is stopped, its rotation can be easily started manually by applying torque in either direction. Actuator 36 sustains rotor rotation after it is connecting to its power source. Rotation of rotor shaft 10 about axis 11 is aided by cyclic movement of the reciprocating magnets 50 – 52, their axial location between the rotor magnet pairs 42 – 43 , 44 – 45 , 46 – 47 and 48 – 49, the disposition of their poles in relation to the poles of the rotor magnets, and the frequency and phase relationship of their reciprocation relative to rotation of the rotor magnets. Actuator 36 maintains the rotor 10 rotating and actuator arm 38 oscillating at the same frequency, the phase relationship being as described with reference to Fig.12. With the rotor magnets 42 and 49 as shown in Fig.2, when viewed from above, the north poles 54 of the rotor magnets on the left-hand side of axis 11 face a first axial direction 110, i.e., toward the actuator 36, and the north poles 54 of the rotor magnets on the right-hand side of axis 11 face in the opposite axial direction 112, away from actuator 36. When the rotor magnets 42 – 49 are located as in Fig.2, the north poles 54 of reciprocating magnets 50 – 52 are adjacent the south poles 56 of rotor magnets 45, 47 and 49 , and the south poles 56 of reciprocating magnets 50 – 52 are adjacent the north poles 54 of rotor magnets 44, 46 and 48. Furthermore, when the rotor shaft 10 rotates to the position shown in Fig.2, the reciprocating magnets 50 – 52 are located at, or near, one extremity of their axial travel, so that the north poles 54 of reciprocating magnets 50 – 52 are located close to the south poles 56 of rotor magnets 45, 47 and 49, respectively, and relatively more distant from the north poles 54 of rotor magnets 43, 45 and 47, respectively. Similarly, the south poles 56 of reciprocating magnets 50 – 52 are located close to the north poles of rotor magnet 44, 46 and 48, respectively, and relatively more distant from the south poles of rotor magnets 42, 44 and 46, respectively. With the rotor magnets 42 and 49 rotated into a horizontal plane one-half revolution from the position of Fig.1B, when viewed from above as shown in Fig.3, the north poles 54 of reciprocating magnets 50 – 52 are located adjacent the south poles of rotor magnets 42, 44 and 46, and the south poles 56 of reciprocating magnets 50 – 52 are located adjacent the north poles 54 of rotor magnets 43, 45 and 47, respectively. When the rotor 10 shaft is located as shown in Fig.3, the reciprocating magnets 50 – 52 are located at or near the opposite extremity of their A - 985
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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
Page 25 and 26:
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 - 879
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A - 881
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A - 883
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A - 885
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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
Page 109 and 110:
A low-speed or idling jet 25 has it
Page 111 and 112: DESCRIPTION OF THE DRAWINGS Fig.1 i
Page 113 and 114: Fig.5 is a detail sectional view on
Page 115 and 116: Vapour formed by air bubbling throu
Page 117 and 118: From the foregoing description it w
Page 119 and 120: Fig.2 is an enlarged view of the de
Page 121 and 122: Fig.6 is a section taken along line
Page 123 and 124: ROBERT SHELTON US Patent 2,982,528
Page 125 and 126: Fig.4 is a transverse sectional vie
Page 127 and 128: HAROLD SCHWARTZ US Patent 3,294,381
Page 129 and 130: 182,420 now abandoned. The present
Page 131 and 132: DESCRIPTION OF THE INVENTION The ca
Page 133 and 134: THOMAS OGLE US Patent 4,177,779 11t
Page 135 and 136: In accordance with other aspects of
Page 137 and 138: Fig.3 is a sectional view of the va
Page 139 and 140: Fig.7 is a partial side, partial se
Page 141 and 142: The cooling system of the vehicle c
Page 143 and 144: Upon initial starting of the engine
Page 145 and 146: (f) A filter positioned in the vapo
Page 147 and 148: with the magnitude of the current a
Page 149 and 150: Fig.1B is a perspective view of the
Page 151 and 152: Fig.3 is a top view of the motor of
Page 153 and 154: Fig.7 is an isometric view showing
Page 155 and 156: Fig.10 is a top view showing the ro
Page 157 and 158: Fig.13 is a top view of a pair of r
Page 159 and 160: Extending in opposite diametric dir
Page 161: Fig.5 shows the state of the switch
Page 165 and 166: Fig.9 and Fig.10 show a second arra
Page 167 and 168: constructed otherwise than as speci
Page 169 and 170: 12. The motor of claim 11 wherein t
Page 171 and 172: timer or a control mechanism mounte
Page 173 and 174: Fig.4 is a view similar to Fig.3 bu
Page 175 and 176: Fig.10 is a view similar to Fig.3 f
Page 177 and 178: Fig.13 is a schematic circuit diagr
Page 179 and 180: Fig.16 is a simplified embodiment o
Page 181 and 182: Fig.22 to Fig.25 are similar to Fig
Page 183 and 184: Referring to Fig.2, the permanent m
Page 185 and 186: Fig.7 shows a modified embodiment w
Page 187 and 188: them, will depend upon the order in
Page 189 and 190: Fig.14, shows another embodiment 14
Page 191 and 192: Fig.18 shows the air coil 210 posit
Page 193 and 194: Figs. 22-25 show four different pos
Page 195 and 196: movement with the first permanent m
Page 197 and 198: a shaft and means journaling the sh
Page 199 and 200: CLAUDE MEAD and WILLIAM HOLMES US P
Page 201 and 202: Fig.2 is a front elevation of the w
Page 203 and 204: impactors and drills. The turbine d
Page 205 and 206: (a) fourth rotating means responsiv
Page 207 and 208: path to the other side of the perma
Page 209 and 210: Fig.3 is an oscilloscope waveform t
Page 211 and 212: 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
Page 283 and 284:
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
Page 299 and 300:
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
Page 305 and 306:
Fig.2 is a vertical transverse cros
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Fig.6 is a vertical, longitudinal,
Page 309 and 310:
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
Page 315 and 316:
Fig.6 is a cross-sectional view of
Page 317 and 318:
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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
Page 325 and 326:
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:
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Fig.12 is a cross-sectional view si
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Fig.14 is a schematic diagram of an
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A - 1163
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A - 1165
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Figs.20A-20F are schematic diagrams
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Note: Corresponding reference chara
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Integral with the piston bodies are
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The piston has a generally semi-tor
Page 353 and 354:
Referring back to Fig.13A, for engi
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As piston 39A reaches BDC, distribu
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mixture and do not combine because
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These wires are about twelve gauge,
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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 and 382:
Energy cannot enter a space of zero
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electromagnetic and gravitational f
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
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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
Page 433 and 434:
http://www.free-energy-info.co.uk/M
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A Practical Guide to 'Free-Energy' Devices

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