Spatial Energy Coherence
   
 Copyrights(c) 2005-2011, Dr. R. R. Stiffler  

DO NOT attempt replication of my research, unless you are fully aware of the dangers involved in working with Hydrogen gas. You must insure that the Hydrogen and Oxygen are not allowed to mix. Mixtures of H2 and O2 are reactive in concentrations from ~4% > 74%. All apparatus should be vaccum tested and evacuated of Oxygen before Hydrogen production is commenced. Stiffler Scientific is not responsible for, or holds any libility for damage or injury to person or property resulting from the duplication of our work.

In 1995-1996 I looked into the production of fuel hydrogen using standard configuration plated electrolyzer cells. It was not until the middle of 1996 that I devoted considerable research time to exploring how one might produce on demand hydrogen. The initial research looked at what is sometimes called Rhodes(a) gas, Browns(b) gas or HydroOxy (also known as OxyHydrogen) gas, which is a very dangerous mixture of hydrogen and oxygen produced by non-separation (single duct) electrolyzer cells. (Dr. Rhodes(a) and Prof. Yull Brown(b) have both made statements the gas is less dangerous than tank H2 and O2 when combined. I do not dispute their claims, although my experience, possibly do to my own errors, indicates otherwise.)

Additionally I performed a number of experiments with a somewhat controversial Pulsed cell arrangement  using a low voltage pulsed power supply. The pulsed power method I am referring to is attributed to a Stanley Meyer (somewhat controversial individual, do Internet search for further information on Stanley Meyer) that developed a circuit using high voltage pulsed power.

Not wanting to duplicate the work of Meyer, I constructed a switching (pulsed) power supply running at 12 volts DC that was switched into a two plate electrolyzer cell. The switching rate was adjustable and the circuit itself was a rather simple circuit overall. Initial testing did not produce surprising or unexpected results. The cells action and output performed as expected and calculated.

A number of experiments were conducted with resonant circuits (both parallel and series) in the cells return power leg (anode).  A number of configurations were tested before even the slightest indication of something different was observed. A slight oscillation in the circuit and a visible increase (although small) in gas production, without seeing increased input was the first indication of something different in the test runs. What was different was this particular circuit had a feedback path from the resonant components back to the cathode side of the cell.

Many hours were spent under the mistaken assumption that this oscillation was in some way tied into some frequency component of the molecular bonds of H2O itself, which was helping in the disassociation. Only through a mistake in misreading a capacitor value did I realize that the observed action was not a result of a frequency connection to the molecules themselves. The incorrect selection of a capacitor shifted the frequency of interest by many orders of magnitude lower

Gas production increased significantly while maintaining the same input to the cell. Something was taking place in this particular circuit that indicated a generation efficiency of over 100%, but appeared to be outside of any direct molecular interaction..

I constructed a large cell, one that would allow for a large volume of gas so that exact output measurements could be performed and appropriate calculations performed.

Because of a mistake in staying with the Rhodes(a) gas mixture I set the stage for what was to be a near tragic yet avoidable accident. Stating again that the Rhodes(a) gas, an evolved combination of Hydrogen and Oxygen in my opinion is extremely dangerous and should be avoided without exception. (This gas mixture and its apparent dangers arise from the storage of the gas, rather than the generation and real time usage of the gas, provided safety standards are carefully followed.)

With an improved design while storing close to a liter of this highly volatile mixture, it happened. Some how the mixture became catalyzed and Bang!. The entire cell was blown apart with the lid and hose fixtures embedding into the soft lab ceiling. Pieces of the cell were found some 10 meters away from where the explosion took place. The hose fitting on the lid to the cell pushed one half inch into the ceiling tile. Further testing was stopped while consideration was given to the hazards involved in this type of research being conducted in a general research lab.

In mid 2004 after reading numerous articles on the direction alternate energy production was taking, I again decide to resume research into real time hydrogen fuel production. This time I chose to use separation cells (dual duct) and implement strict production, storage and handling procedures.

My goal was to be able to produce hydrogen on a demand basis with equipment easily obtainable and assembled, while using common tap water as the H20 source and consuming less power in the electrolyzer than I obtained back in H2.

I began with a common or standard cell design composed of anode and cathode electrodes (1/4" carbon rods) without membrane separation, yet fully separating the H2 from the O2. Pressure adjustments and balancing were not of initial concern. Once establishing a base line for comparative measurements I looked into the design of the electrodes and what if any impact different geometry had on overall production efficiency.

Initial research results were text book, output was without a doubt a function of input, even though I did see some minor increases in production efficiencies from different electrode designs, shape and feed points. Electrodes

One of my early circuits contained a resonant circuit, a few capacitors and some high speed switching diodes. Scope traces and pulse timing measurements indicated that the resonant circuit was not a contributor to the process owing to its resonance. Rather it was acting as a time delay for pulses being reapplied to the input of the cell. Once this was understood I began to form a conceptual picture of how the CRE was working.

When reading this paper, one must keep in mind that for proper disassociation of H2 and O2 through electrolysis that the electron conduction is ionic, not resistive in the conventional sense. This fact is significant in the understanding and operation of the CRE. The CRE supplies electrode voltages of from 2 volts to 4 volts, depending on the composition of the water and electrolyte. The more conductive the water the higher the applied electrode voltage will be.

Let me offer an explanatory mind picture of how CRE is working. Picture a fire brigade using buckets with a central supply of water some distance away from a particular fire. To fight the fire each man runs to the water supply, fills his bucket, runs back to the fire and disperses the water over the fire. The men must then run back to the water supply for the next bucket of water and keep repeating the process until the fire is out. In this process each man expends X amount of energy for each bucket of water he obtains and throws upon the fire.

One day a rather tired fire fighter noted that not all of the water thrown onto a fire was evaporated from the fires heat and some water ran off and pooled in a ditch a few feet from the fire. The fire fighter reasoned that one bucket of water was just as good as the next so he saved the long run to the supply pool and drew his buckets from the closer source of the ditch, thereby recycling some of the water while expending less of his own energy. When the fire was finally out, our industrious fire fighter that took water from the ditch used X' energy during the event, while the rest of the fire fighters each used X energy. Our fire fighter saved (X - X')energy by recycling the water.

What is important here is the fire fighter was recycling water and saving energy he would have otherwise used if all of the water had to come from the supply pond. It should be easy to see why energy was saved from this process.

So how does this apply to the CRE? Simple, the water is replaced by electrons from the power source to the electrolyzer and the CRE is the smart fire fighter that uses some of those electrons over in the process of the disassociation of the H2 and O2. As far as the power source is concerned it cares less how many times a particular electron is used before being returned to the anode. Neither does the power source care how long it really takes for a particular electron to travel from the cathode back to the anode, provided it does return.

I may need to clear up a possible connection between energy and efficiency that could lead to a misunderstanding. Assume a standard two plate electrolyzer cell that is capable of producing 1 liter of H2 per hour with an electrical input of ( Xb Joules) at an efficiency of  80%. This same cell under the control of a CRE controller could easily produce 1.8 liters per hour with the same input of (Xb Joules). The additional energy comes from the CRE controller recycling electrons back through the cell for a second trip. The cell efficiency has crossed the magic 100% barrier because I are now disassociating additional gas over and above that which would be produced by the source (Xb Joules) alone.

The increased production cannot exceed 200%, limited by the fact that I can only use a single electron over one time. Current test CRE's run comfortably around 80% to 91% over source input.

Consider the following two reactions that take place at the cell electrodes.

Cathode:           4H2O + 4e-  => 4OH- + 2H2
Anode:              2H2O => O2 + 4H+ + 4e-
Net Reaction:    6H2O => 4OH- + 4H+ + 2H2 + O2

The two electrons come from the cells power source entering the cathode and exiting the anode through ionic conduction. Once entering the anode side of the power source, the electrons are gone, and become part of the total power used by the cell in the production of gas. But with CRE these two electrons are captured before returning to the source and are fed back through the cell a second time, thereby producing twice the evolved gas from the same source input.

In its simplicity the CRE is a circuit that recycles electrons and does not violate thermodynamics in the application of this method in the disassociation of the H2 and O2 gases. The CRE will not work for recycling of electrons in a purely resistive load as the entropy will prevent an efficiency gain. It must be mentioned again that electrolysis does not depend on the generation of heat and therefore is not subject to the thermodynamic limitation on efficiency.

The switching circuits in the CRE use energy supplied by the power source, which lowers overall efficiencies by from 10%-20%, although new designs using MOSFETs and Opto Switches can limit this loss to below 20%. Current test CRE's are using a switch controlled by a CMOS 555 adjustable timer that allows a maximum of 191% effective gain. In a production cell I feel the effectiveness will be in the range of 170% to 180% in order to keep circuit complexity and module cost low.

03/11/2006

Current CRE switches now use four MOSFET's with two in a multi-vibrator circuit and the remaining two with two high speed, high current switching diodes form the capacitor switch. The new arrangement allows for the timing and switch components (not including capacitor bank) to be priced at less than $5 (US). For a high volume CRE , the cost of the capacitors can run into the hundreds of dollars and require that additional MOSFET switches be used.

The CRE will work on conventional and PEM cells although with the PEMs a 2W output cell remains a 2W cell because its production limitations are more or less built into the cell itself. Although you would with the CRE be able to max out the PEM production limit with less input power than is normally be required.

CRE circuit diagram? Not shown are the required switching components.

When the power source is initially connected the electron pressure at the cathode supplies an electron to an H+ ion. (H+ although not truly correct is used for illustration.) While at the anode a HO- ion is giving up an electron. During this continued process the H2(g) and O2(g) are produced. The electrons flowing through the cell and causing the Redox reaction are also storing energy in capacitor C1. When C1 has reached 1T, the switching circuit disconnects the power source and connects C1 across the cell. C1 dumps its stored energy in the form of recycled electrons back into the cell to continue the Redox reaction. The switching circuit keeps switching back and forth between the power source and C1.

In order to obtain the greatest gain from the CRE, the charge and discharge time constants which, are adjusted by the switching rate (duty cycle), must be correctly selected, otherwise the average cell output will drop and the gas production will decrease. C1 itself is a limitation to the cells output in that we are bound by J=1/2CV2, therefore very large C1 values are required for high production cells.

The following is a picture of a working test model CRE.

The follow circuit indicates the construction of a low current solid state CRE driver. Using a solid state driver removes the draw back of the mechanical relay which would only offer limited service do to the high number of contact closures per minute that would be required in a fully operational system. There is a waste of power in the solid state unit and that is the dissipation of diodes D1 and D2. With 1A of current each will dissipate 0.7 watts. D1 and D2 are used although in that they reduce the complexity of the overall switching circuit and reduce cost.

crem12cir

12/15/2006
When selecting the switch frequency and the recycle capacitor ( C1) , keep in mind that the desired and most efficient time constant should be as close to ( 0.7T ) as possible. This selection places you at the cross over of voltage and current from the discharge of ( C1 ).  Trying to extend the discharge past this value can reduce the overall average gas production. Of course you must factor in the supply voltage as you do not wish to drop below a level of ~1.9 volts across the cell when the capacitor discharge reaches the ( 0.7T ) point.

To illustrate what a CRE looks like in operation I set up a simple demonstration with two carbon electrodes in a lab beaker, driven by a CRE. As you will see in the video this is not a separation cell and is releasing all gases into the open air. What is important is looking at the cathode or H2 electrode on the left side of the picture. You will observe bursts of gas as the CRE pulses. Each alternate burst is charge recycled during the preceding power cycle. Remember that CRE disconnects the power source from the cell for 50% of the time. The remaining time, recycled charge is flowing through the electrolyte.

This video is MPEG and 600k in size.

09/02/2006
Almost all standard cells will experience a decline in input current once the ion concentration of the cell has reached equilibrium. This is seen in a new cell slowly building in input current until a peak is reached at which point the current will be seen to decrease. This decrease can be attributed to only one or many factors, the primary being the cell ion concentration and the cell temperature. Increased cell temperature is not desired as the ideal cell would generate minimal heat during operation. Yet, ion concentration is a desired element of cell operation.

Once the input current decreases, production also decreases and overall decrease in efficiency. This decrease is easily overcome by the addition of a second electrode. In a three electrode cell system the electrical anode is maintained at +V, while the two electrical cathodes are alternately switched to -V with the duty cycle of 50% alloted to each electrode. What will be seen is that the cell will maintain its peak input current and overall efficiency will be much improved.

What aids in the increase of production is not obvious at first, yet is a mix of jarring bubbles from the electrodes and a fracturing of the ion cloud around each electrode (a form of directed mixing). During the switch period, one electrode sees a reversal in polarity that tends to push the attached gas bubbles from the electrode surface as well as away from the electrode. At the same time the other electrode is moving upward in voltage in the correct polarity.

The following image is a simple diagram of this type of switch circuit.

12/15/2006
After receiving a number of requests on how I eliminated the double diode loss in the initial CRE and how it might be applied to the double cathode cell, I am including the following circuit.

Care is required so that the switch frequency is kept as low as possible to obtain the increase in efficiency, yet not increase the cell heat by a significant amount. Because the molecules are shifting direction there will be additional collisions and heat. Strangely enough the cell seems to learn what is taking place and the additional heat will decrease over a period of time. This decrease can be observed if the switch frequency is adjusted slowly upward. There will be a point where the heat will continue to rise with no fall back. The optimal frequency is of course below this level.

It should be obvious that you can not just place two electrodes in a cell with a switching circuit and obtain optimal results. The entire cell must be taken into consideration in the design and the ability to determine the electrode size and spacing from each other as well as the spacing of each from the electrical anode. Pure water or electrolyte also factors into the equation. At his time the number of variables involved in various cell parameters place this design into the art class leaning heavenly on empirical data from a limited number of controlled cells. The information is being provided as presented, informational only.



The following pictures are of the bubblers, scrubbers (or dryers) and flame traps (flame arrestors). I use three types of flame arrestors, bubblers, water filled U tubes and silicate sand supported by screens and fiberglass cloth. The following is a picture of a completed silicate sand arrestor .

H2 capture and pressure tank in leak testing

The electrolyzer generator cells used for laboratory testing

Checking how the system fits together

Full Unit Test, All Ready to go

First Complete Test a Success (1)

First Complete Test a Succes (2)

Dryer and Flame arrestor

Having hydrogen at half the cost still presents numerous problems, especially for the domestic user, just how will this cheaper hydrogen be used? Feeding hydrogen back into a fuel cell to obtain electricity, makes little sense, you end up paying more overall than just using the utility electricity and forgetting the hydrogen. One must factor in the cost of the electrolyzer, the cost of the fuel cell, water and all the maintenance that would be required. Currently fuel cells just are not efficient enough to make this a working configuration.

References:
aDr.William A. Rodes.
bProf. Yull Brown