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Old 06-02-2009, 04:05 PM
Peter Lindemann Peter Lindemann is offline
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Join Date: Apr 2007
Location: Liberty Lake, Washington
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Electric Heater with COP>20

Quote:
Originally Posted by Aaron View Post

Aaron,

Thanks for re-invigorating this older thread. I was about to start a new thread about Rosemary's work. I have also posted her major contributions to a new page on my site at: Free Energy | Rosemary Ainslie On this page, I have collected her papers and put them all in simple, downloadable PDF files, for ease of handling.

This material clearly shows how to build an electric heating device that produces 17 times more heat than the "equivalent" amount of electricity. It accomplishes this by using a resistive heating element that also has inductive properties, and by "recycling" the energy of the inductive collapse.

Rosemary's original test circuit is shown in the article she tried to have published in a "refereed" scientific journal, but the submission was always rejected. In the last 5 months, I have had extensive email correspondence, and numerous telephone conversations with Rosemary, who lives in South Africa. After studying her work, I was absolutely thrilled with her discovery of the super-efficient heating effect. In mid-February of this year, I proposed to her an "idealized" schematic of her DC resonance circuit to produce the effects she had discovered. That circuit diagram is here:


Based on the circuits and work done in the Electric Motor Secrets thread, this circuit should be easy enough to understand.

For those that do not understand it, I will describe its function in a later post.

There are broad implications connected with the proper understanding of the functions of this circuit. We all owe Rosemary Ainslie a deep debt of gratitude, both for her discoveries, and for her willingness to publish her results for the betterment of Science and the human condition.

Peter
Hi guys,

OK, Here is an explanation of the schematic diagram above, for the creation of an Electric Heater with a COP>20.

PS = the Power Supply. This is the Primary Supply of energy to the circuit. Any NEW ENERGY required to run the circuit must come from here. It can be a battery, or any source of DC current.
RL = the heating element (load) that has the electrical characteristics of both resistance and inductance. Electrically, the component is operated as an INDUCTOR to be charged and discharged in sequence.
C = a Capacitor of sufficient capacitance to act as a secondary power supply to power the circuit and to act as a reservoir to receive the energy returned by the inductive collapse of RL.
D1 = a Diode to make sure that energy can only move in one direction, in this case, FROM the power supply TO the capacitor. This component prevents any of the energy returning from the inductive collapse from traveling all the way back to the primary power supply. So, in operation, this Diode will allow the Capacitor C to rise to a voltage that is higher than PS, but it will never allow C to drop to a voltage below PS.
SHUNT1 = a low value, calibrated resistor used to measure the currents leaving the Power Supply PS. Current pulses measured here, times the voltage of PS, represent ALL of the energy the circuit is "dissipating".
Q1 = a Power MOSFET, or any appropriate switching device to allow currents to magnetize the inductive load RL. This includes all of the timing circuitry for the circuit's proper function.
D2 = a Diode to complement Q1, to allow currents from C to energize the load RL.
D3 + D4 = Diodes to direct the energy of the inductive collapse of RL back to Capacitor C so this energy may be re-used.
SHUNT2 = a low value, calibrated resistor used to measure the currents supplied from C (through Q1 and D2) to the load RL. Current pulses measured here, times the voltage of the Capacitor C, represent ALL of the energy supplied to the load RL.

The circuit is designed to operate in the following manner. Q1 is timed to produce current pulses which magnetize RL and then shut off, based on the inductive "current rise-time" of the component. The exact timing of this depends on the inductance of RL and the voltage of the Power Supply. RL then discharges as an inductor through Diodes D3 and D4 back to Capacitor C. This represents "one cycle" of the circuit. As soon as this cycle is completed, the process repeats.


RL is meant to be a Resistor Element made of NiChrome Wire, wrapped in a spiral shape around a ceramic frame, as pictured above. Every time there is both voltage and current present at RL, heat is produced. This includes both when currents are being supplied by Capacitor C and when currents are being returned to Capacitor C. Since the inductance of RL does not change during this charge and discharge cycle, the total amount of energy capable of being recovered from the inductive collapse should be on the order of 95% of the amount of energy supplied, during each cycle.

In this situation, currents can be supplied to RL and returned to C rapidly, with very little "real energy" lost to the circuit. Any energy that is actually dissipated, such as voltage drops on the switching devices (Q1, D2, D3, and D4), will be made up for by energy provided by the Primary Power Supply PS.

This "schematic" is provided without specific values, and is meant to provide a theoretical basis for understanding how an Electric Heater with a COP>20 could work.

Peter
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Last edited by Peter Lindemann; 06-02-2009 at 05:10 PM.