370 lines
17 KiB
Plaintext
370 lines
17 KiB
Plaintext
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| File Name : FLEXFLO.ASC | Online Date : 12/07/95 |
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| Contributed by : Anonymous F/E Guy| Dir Category : ENERGY |
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| From : KeelyNet BBS | DataLine : (214) 324-3501 |
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| KeelyNet * PO BOX 870716 * Mesquite, Texas * USA * 75187 |
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| A FREE Alternative Sciences BBS sponsored by Vanguard Sciences |
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| InterNet email keelynet@ix.netcom.com (Jerry Decker) |
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| Files also available at Bill Beaty's http://www.eskimo.com/~billb |
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The following text files were sent to KeelyNet anonymously with the intent of
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stimulating experiments with this type of circuit. The information is being
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honestly presented and believed to be worthy of further investigation. These
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circuits have presented anomalies which need to be investigated by many people
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and are offered in the spirit of sharing information.
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They represent the 'state of the art' as per the contributor and are subject
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to revision based on future enhancements or refutations. Please be fair and
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constructive in your comments, preferably based on personal experiments.
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If you choose to experiment using this information, please share your
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observations or findings with KeelyNet and others. Thanks!......>>> Jerry
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The files are listed as : FLEXFLO.ASC - this text file
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PROOF1.GIF - proof of overunity circuit
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FLEXWAT1.GIF - water analog to how FlexFlo works
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FLEXFLO1.GIF - simplified conserver circuit
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FLEXFLO2.GIF - advanced conserver circuit
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FLEXFLO.ZIP - all the above files zipped into one
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The Wiseman Theory of Energy Conservation
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by
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Anonymous F/E Guy
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(who takes no credit for this idea)
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Concept origin:
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George Wiseman
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H and A Industries
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Rt. 2 Box E-35
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Bowling Green, MO 63334
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If you are interested in true F/E principles, I recommend that you contact "H
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& A Industries" for a catalog of their products. Specifically, order the books
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entitled:
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"The Energy Conserver Method, Book 1" $15
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"The Energy Conserver Method, Book 2" $15
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handling $3
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---------------------
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Total $33
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The book money goes into furthering Mr. Wiseman's research which will result
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in more info for US to use. Please purchase these books if you are interested
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in studying this device. There is much more information contained in the books
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that I don't plan to delve into in this extremely short text.
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Mr. Wiseman explains his process of experimentation fully and also notes the
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many strange effects of his devices. His ideas seem to FULLY explain the true
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nature of electricity.
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I am in no way affiliated with Mr. Wiseman or H & A Industries, but I do
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HIGHLY recommend these books for your personal library.
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The principle behind this circuit is simply this:
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This circuit takes an initial charge from a power supply or battery (12vdc for
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this circuit). That charge is recycled several times through a resistive load
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(a bulb, for this demonstration).
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The circuit produces the same mysterious "pulsating" lightbulb effect that the
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"Sweet Vacuum Triode" and the "Testatika" produce through the bulbs that they
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power in their respective videos.
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These circuits are ONLY TWO POSSIBLE FORMS for this power recycling. I would
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like to encourage anyone who would be kind enough to make this into a solid-
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state circuit that the capacitors could simply be "plugged into".
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A MOSFET switching device using digital timing for duty-cycles and pulse
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frequency would be a fantastic boon for further research using this little
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toy. This recycling can be accomplished at any voltage, as long as your
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components can handle it. High Voltage arc contacts might be used instead
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of solid state switches.
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Well, now the rest is up to YOU. Get the books. Study the books. Let's get
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this F/E boat rockin'!
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Principles of FLEXFLO circuits
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Theories and original
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circuit concepts
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from
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" The Energy Conserver Method "
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by
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George Wiseman
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For Complete info, order a catalog from
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H & A Industries
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Rt. 2 Box e-35
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Bowling Green, MO 63334
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Mr. Wiseman's books contain much more information than I an provide in this
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short text. I highly recommend ordering and reading the "energy conserver"
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books.
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from
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the anonymous F/E guy
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see files: PROOF1.GIF
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FLEXFLO1.GIF
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FLEXFLO2.GIF
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FLEXWAT1.GIF
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The first and most important principle of these circuits is the understanding
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that a resistive 'Load' DOES NOT CONSUME electricity.
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This is easily illustrated by examining ANY school text on electrical theory.
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They always show several examples. I have emphasized a few points in these
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examples to demonstrate my point.
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1. Electrons flow from a battery's negative pole, to a batteries positive
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pole. ALWAYS. Once the electrons (current) complete the circuit and
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enter the positive pole, some of the battery's potential is destroyed.
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The more current that flows, the faster the battery goes "dead".
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2. Electron flow (current) THROUGH a wire "causes" a magnetic field around
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that wire. The field strength is in direct proportion to the amount of
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current. The electrons don't DISAPPEAR in the wire. They go IN one end
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AND OUT the other.
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3. Electron flow THROUGH a bulb produces light and heat. The current does
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not DISAPPEAR inside the bulb. The same current flows on both sides of
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the filament. The current going into the bulb is the same as the current
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that leaves the other side of the bulb.
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Nobody ever seems to notice the obvious contradiction between electricity
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passing COMPLETELY THROUGH a load and electricity being CONSUMED WITHIN a
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load. It has to be one or the other, not both.
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Resistive loads only slow down the current, they don't consume it. If they
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did, your battery would last longer on devices that consumed more electricity
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because the electrons would vanish inside the load and never reach the
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positive pole of the battery. In the real world a circuit works like this, one
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electron goes in, one electron comes out. That's just the way it works.
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The FLEXFLO circuits are designed to hold a volume of electricity and "pour"
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it from one bank of capacitors to another bank through a load. If the circuit
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in FLEXFLO2.GIF is constructed using standard grade electrolytic capacitors,
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it should move approximately 3 to 4 times as much electricity through the load
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area than what is actually drawn from the battery. (based on actual circuit
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measurements and calculations.)
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The Charge of a Capacitor is figured in coulombs:
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Q=CE
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where:
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Q = electric charge (coulombs)
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C = capacitance (farads)
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E = voltage (V)
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A coulomb is a measure of electrical VOLUME contained in a capacitor.
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Using this formula with the capacitances and voltages in a circuit, we can
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calculate approximately how much energy will move through that circuit.
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See Flexflo2.gif in relation to the following example. Measurements taken from
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an actual prototype in operation. Energy used for switching was on a separate
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circuit and is not used in the calculations.
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My prototype used four 110,000uF @ 25v capacitors, Four DPDT relays, one
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microswitch to activate relays, one 13.6 volt car battery, and many bits of
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colored wire.
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C1 and C2 make Bank 1. C3 and C4 make Bank 2.
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Step one:
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Battery was connected to bring charge across C1 to 13.6 volts. At this point
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C1 and C2 are in parallel while C3 and C4 are in series. Battery was then
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disconnected.
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Total capacitance of Bank 1 is .22 farads @ 13.6 V = 2.992 coulombs
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Bank 2 is .055 farads @ 13.6V = .748 coulombs
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-------------------------------------------------
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Total system charge = 3.740 coulombs
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Step two:
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C1,C2 placed in series. C3,C4 placed in parallel. This caused a VOLTAGE
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imbalance which caused 2.244 coulombs of charge to pass through the load
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point to equalize voltages of the two banks.
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( 2.992 ) - ( .748 )= 2.244 coulombs moved through load point.
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Bank 1 is now .055 farads @ 11.15 volts = .613 coulombs
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Bank 2 is now .220 farads @ 11.15 volts = 2.453 coulombs
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-----------------------------------------------------------
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Total system charge = 3.066 coulombs
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At this point the voltage across C3 was measured at 11.15 volts.
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Total system charge is now calculated to be 3.066 coulombs. System charge
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loss from step 1 to step 2 calculated to be .674 coulombs.
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Step three:
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C1,C2 placed in parallel. C3,C4 placed in series. This causes another
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VOLTAGE imbalance which causes 1.840 coulombs of charge to pass through
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the load point in order to equalize voltage potential between the two
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banks.
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( 2.453 ) - ( .613) = 1.840 coulombs moved through load point.
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At this point the voltage across C1 was measured at 8.7 volts.
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Total system charge is now calculated to be 2.393 coulombs. System charge
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loss from step 2 to step 3 calculated to be .773 coulombs.
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Bank 1 is now .220 farad @ 8.7 volts = 1.914 coulombs
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Bank 2 is now .055 farad @ 8.7 volts = .479 coulombs
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-------------------------------------------------------
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Total system charge = 2.393 coulombs
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The battery is now connected to recharge C1,C2 through the load, and C3,C4
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directly. This moves another 1.078 coulombs through the load point while
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charging C1,C2. Total charge taken from battery to recharge whole system
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to 13.6 volts is 1.347 coulombs.
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( 3.740 ) - ( 2.393 ) = 1.347 coulombs used from battery.
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Charge passed through load point:
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step 1 = 2.244 coulombs
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step 2 = 1.840 coulombs
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During Recharge = 1.078 coulombs
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------------------------------------
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total = 5.162 coulombs
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Charge taken from battery = 1.347 coulombs
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---------------------------------------------
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Over-Unity output = 3.815 coulombs or 383% "efficiency"
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Several tests were conducted without any load resistance present in the
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circuit (dead short across load point), and several tests were performed with
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various types of resistive loads (electromagnet, bulbs, motor).
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In every case, the measured charge potentials of the capacitors remained
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virtually the same at every testing stage. The fact that purely resistive
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loads don't "consume" electricity is shown in the circuit PROOF1.GIF.
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Diodes do cause a voltage drop across the load and do lower the measured
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voltages by about 1 volt per diode in series with the load.
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I attribute the constant voltage drops to mechanical stress loss inside the
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capacitors. Many small capacitors in parallel, as opposed to a large single
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capacitor, might help offset the losses to a degree.
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Bearden spoke of "laboratory grade" capacitors that have almost no internal
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stress losses. These might provide a nearly lossless flex circuit.
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Since there is a fixed amount of potential loss per cycle, it would be best
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to design a load that makes the most use of each charge cycle. I suggest a
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self-variable resistor in series with the load to maintain a constant useable
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voltage/current through most of the transfer cycle.
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The output is a high voltage spike that drops to zero over time in accordance
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to load resistance. (20 volts down to 0 volts)
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Using V=IR we should be able to construct a solid-state resistor that can be
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set at any desired current level so that it will maintain a steady current
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through the load during most of the charge cycle.
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Bulbs, heater elements and magnets are directly useable without the use of
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this variable resistance device.
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IDEAS FOR DEVICES:
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Build a motor that "flex's" power via the commutator. Collect the C.E.M.F.
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from the stator magnets to feed charge back into the system. Use mechanical
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torque of motor to drive generator. This motor should only need 4 stator
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electromagnets and 2 permanent magnets on the rotor.
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Build a "Testatika" device. Wheel is driven by HV pulses through stator
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magnets. Leyden jars are arranged as in FLEXFLO2.gif and commutator
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directs charges approprietly. Commutator is NOT full contact device; NO
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CONTACT FRICTION LOSS! HV spark jumps small gap to transfer charge.
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Meanwhile, charge is collected from static generator portion of device.
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------------------------------------------------------------------------------
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Tapping "Massless Displacement Current"
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using a capacitor as a "collector"
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by
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the anonymous F/E guy
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See PROOF1.GIF for circuit diagram
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This is a REAL EXPERIMENT that can be performed by anyone using only the
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following materials:
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- 3 electrolytic capacitors
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2 are >50,000uF and one small one for the "collector", 10,000uF
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- 12 volt D.C. power source (for charging 1 capacitor)
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- A good V.O.M. (digital preferred, or an O-scope)
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Connect the two large capacitors as in the circuit in PROOF1.gif. Leave out
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the variable resistor. This is where you'll be using the small capacitor.
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Leave the "load" point open so that a load can be added in order to complete
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the circuit.
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Step 1: Make sure C1 and C2 are completely discharged. Charge C1 with the
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battery. Check the voltage across C1 and write it down.
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Step 2: Short the connection across the load point to allow the charge
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from C1 to equalize with C2. Now check the voltage across C1 and
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also across C2. They should be the same. Write down the voltage
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readings.
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Step 3: Repeat step 1. Now, make sure your small cap is discharged. Then,
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place it in series in the load point. Remove it from the load
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point and check the voltage on it. Now discharge it into a bulb
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or something.
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Step 4: Place the small cap into the load point a few more times, each
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time removing, checking voltage, and discharging it. When it no
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longer goes above 0volts you can stop. That means that the
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potential differences in C1 and C2 have equalized. Check the
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voltage across C1 and then C2. They should be approximately the
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same readings that you found in step 2.
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This circuit plainly shows that Bearden's "massless displacement current" is a
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REAL and TANGIBLE substance. It can be extracted by repeatedly halting a D.C.
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circuit with a small, or large, capacitor.
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Explanation:
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Current flows through a capacitor until it reaches a full charge. The
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same current flows on both sides of the capacitor.
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The charged capacitor can then be removed from the circuit, the massless
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displacement current is drawn off, and the capacitor is then placed back
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into the circuit where it fills up again.
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The same amount of current flows through the circuit each time. This is a
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passive "electrical milking" that can be performed on just about any D.C.
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circuit.
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If the "milking" was done in microsecond pulses, a normal electronic
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circuit would never realize it's happening.
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This could mean that many conventional power supplies, heaters, lamps,
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etc..., could be made to run with nothing but a single input pulse.
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With several stages of the same circuit stacked on top of each other,
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many everyday devices could be made self powering.
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Well, there you go. I'm no electronic designer. I leave it up to those of
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you who can make this into a solid state device of some sort.
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Enjoy!
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