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Author Topic: Lawrence Tseung sent a Prototype to test... any comments?  (Read 342854 times)
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Heck of a day...  The hard-drive on my lap-top went out -- ugh!   Trying to recover.   :-X

I'm borrowing a lap-top and that is much appreciated!   I see responses, again much appreciated, .99 ::

While having a running Po/Pi ratio (COP) would be ideal, it is not necessary, unless attaching the scope probes has a significant effect on the power levels. In such a case, then a 4-channel scope, or 2x 2-channel scopes would be preferable.
As mentioned, if the DPO3032 is a 2-channel scope, you will have to obtain another scope that performs multiplication, preferably the same model, or get a 4-channel scope.

The DPO3032 (being a 2-channel scope) will only allow you to make one power measurement at a time.

The absolutely ideal scenario is to have a 4-channel scope, 2 current probes, and 2 differential voltage probes.

Here is what I suggest:

Place the entire JT in a metal enclosure, and attach BNC (or something suitable) connectors to the enclosure so you can measure the required points in the circuit. This should minimize influence on the JT operation and allow for using a single 2-channel scope to make your measurements.

Also, see if you can borrow a current and differential probe. I wouldn't be surprised if the electrical engineering department had them.

.99

  On this -- "current probe and differential probe"... sorry for my ignorance, can you take a few minutes and enlighten me on how these are used?   I am quite certain I can borrow these all right, at the university.

@ MileHigh: 
Quote
Personally if I was to do the testing I would try the capacitor emulation of the supply battery and the thermal profiling of the output.  For the very low power this system is running at I am assuming that you can get thermometers or thermocouples that would work fine in this application.  Since it is low power you can put the output load components in a small insulated box so that the increased thermal resistance to the outside world results in higher and easier to measure temperature differentials.  If the COP is greater than 2 then you should be able to generate conclusive data without the need for any fancy equipment.  All that you need is the right test and measurement strategy and a high quality multimeter and a high quality temperature measurement device.

As I have indicated before, I'd like to perform different methods of measurement as a check. 
  Now, would you kindly explain this a bit more?  -- " the right test and measurement strategy and a high quality multimeter"  -- where does the multimeter come in with your approach? 

Again, much appreciated.

@ Lawrence:  rather than calculating "FLEET Index" values, let me provide Vin and voltage drop across the input resistor, then Vout across wires 5&6 along with V across a 1 ohm resistor in the out put chain (between wires 5&6), thus 4 measurements in that order.  You can calculate the FLEET index if you wish; perhaps the raw values actually give information that is more useful to us for comparison purposes.
 
 For sure, I will feel more comfortable when I get the Tektronix 3032 going on this, and ideally a thermal measurement as a check.  The more checks and tests the better -- I'm sure you will agree -- although these take time.  Then a hard-disk crashes...  :-\

  The values from our latest runs on our replication device, last evening, are interesting I think.  But will have to wait till tomorrow to post.
   
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PhysicsProf:

The reason I say a "high quality multimeter" is that you need one to make an accurate measurement of the voltage drop across the current bleeding resistor in the capacitor-based emulation setup of the supply battery.  You also need to make an accurate measurement of the capacitor voltage and the resistance of the bleeder resistor.

Again, the true argument is that if you are assuming a system with a COP of 2 or greater, you don't literally need a high quality multimeter with three or four digits of precision after the decimal point.  However, it would be "nice" to have a high quality multimeter just the same.

MileHigh
   

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It's not as complicated as it may seem...
 On this -- "current probe and differential probe"... sorry for my ignorance, can you take a few minutes and enlighten me on how these are used?   I am quite certain I can borrow these all right, at the university.

Professor,

You may recall this post which I previously referred you to and which I encourage you to read, including the attached document. It contains good information pertaining to what current and differential probes are and how to properly use them.

In short, a current probe is a non-invasive inductive-pickup, and a differential probe allows for a floating voltage difference measurement, and can often eliminate the use of ground leads. Both probes use only one channel each on the scope.

Feel free to ask if you have further questions about them.

.99


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I am going to respond to Ion's quick test that he did with a blocking oscillator a.k.a. Joule Thief in his lab.  Note that he tested the pulsing output of the JT transformer and did not wrap an extra energy pick-up winding around the toroid as in the Lawrence Tseung configuration.

If you go back to his original posting you can see the block diagram.  He is using a large capacitor on the input, to convert the pulsing current load of the JT into smooth DC current that can be easily measured by a multimeter.  On the output of the JT he takes the pulsing current output of transformer's secondary winding and also converts that into smooth DC current so the output current and voltage across a load resistor can also be easily measured by multimeters.  The logic here is simple:  He is measuring the average energy output from the discharging secondary transformer winding in the JT.

Quote
While all the arguing was going on, I built up a crude blocking oscillator and tested its efficiency at 75.0% using the method in post #168 of the Tseung thread. This took less than an hour.

I drew up a two step method outlined in the attachment and had intended to post it early in the Tseung thread, but as the existing described methods were misunderstood by many, I realized the purpose of the thread seemed more about discussion.

This should be a very sobering moment for anybody that thinks a JT circuit in whatever configuration is a potential over unity device.  The numbers don't lie.

MileHigh
   
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I missed this.  Output?  Output from the battery or output from the load resistor?  the output on the scope across the load resistor is related to voltage measurements.  Those voltage measurements need to be related to the Ohms value of the resistor to establish volts times amps (vi) to establish its wattage.  The Ohms value is impossible to determine.  Or nearly impossible.  So it's a meaningless exercise.  I am still not sure of your point.  But there is absolutely no way that the voltage measurements are wrong.  They are usually correct within certain very small error margin parameters.  It would be entirely feasible to determine the energy dissipated at the resistor - which is what I think you mean - provided only that it's determined calorimetrically.  It's heat will be a precise measure of the energy it is dissipating. Are we even on the same page here Gibbs?  I seem to be missing your point here.

Rosemary
Rosemary  :)

I think earlier you are talking about the battery capacity.  If a current flow out and in of the battery, it must be subtracted from each others while back and forth a resistor is an addition.  If this is what you're talking about, then I am sorry.

On the bright side, I was talking about the load resistor.  Yes, scope reading is unreliable in this case.  I have a different opinion that the current is nearly impossible to determine, not Ohms.  However, your thinking is not wrong.  If V=IR and you hold I constant while varying R yields the same result as holding R constant and varying I.  Yes, the best way to determine current/ohms function is to take the rate of change of the temperature vs time function.  We're not in contradiction.  :)

GH
   
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Thanks for the responses, .99 and MH.  Very instructive.

MH:
Quote
I am going to respond to Ion's quick test that he did with a blocking oscillator a.k.a. Joule Thief in his lab.  Note that he tested the pulsing output of the JT transformer and did not wrap an extra energy pick-up winding around the toroid as in the Lawrence Tseung configuration.

Of course, it is the "energy pick-up winding" that is the basis of Lawrence Tseung's innovation.  

As I wrote before:
Quote
@ Lawrence:  rather than calculating "FLEET Index" values, let me provide Vin and voltage drop across the input resistor, then Vout across wires 5&6 along with V across a 1 ohm resistor in the out put chain (between wires 5&6), thus 4 measurements in that order.  You can calculate the FLEET index if you wish; perhaps the raw values actually give information that is more useful to us for comparison purposes.

  During our tests Friday evening, we set up a Tseung-replica with everything mounted on a breadboard and found the following 4 measurements as described above;

 1.42 V / 0.040 V // 1.29 V // 0.004 V  

I checked the connections on the breadboard -- and found all the connections to be good (no higher resistances on the output circuit, in particular).  The output LED showed an extremely dim glow -- barely there but observable in reduced lighting.

I suggested to my colleague Les that we remove the output circuit from the pick-up winding from the breadboard -- to see what would happen.  Lawrence had noted that changes might be observed in so doing and he ascribes the changes to resonance conditions or lack thereof.  So we simply took the output wires from the pick-up winding and connected these directly to the 1-ohm output resistor and LED.   The change was remarkable, see if you agree:

  1.4 / 0.04 // 1.3 / 0.07

And now the output LED glows quite bright, indicating an increase in power in the output circuit.
Conclusion:  the Tseung circuit is very sensitive to what appear to be small changes... as he previously noted.
Perhaps the breadboard affects a resonance condition, I'm beginning to think he may be right about that.

Next, we will check whether the circuit stays the same when we turn it on again tomorrow.
   
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From the prof:

Quote
Of course, it is the "energy pick-up winding" that is the basis of Lawrence Tseung's innovation.  

This is not Lawrence Tseung's innovation. Multiple windings are used on the secondary of most all switching power supply designs.

A fixed amount of energy is stored in the inductor per cycle of operation. It is released to whatever coil or coils are there to grab it when the field collapses.

You do not get more energy by adding more windings, the energy divides up according to the burden load on each winding.

You folks and LT need to get a serious primer on switching magnetics and power supply design.

Do a little  reading and you won't be groping in the dark. This stuff is so old hat and quite elementary.

« Last Edit: 2011-01-17, 03:47:08 by ION »


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Quote
While all the arguing was going on, I built up a crude blocking oscillator and tested its efficiency at 75.0% using the method in post #168 of the Tseung thread. This took less than an hour.

This should be a very sobering moment for anybody that thinks a JT circuit in whatever configuration is a potential over unity device.  The numbers don't lie.

I believe the person who built a crude blocking oscillator did not try to tune for the pseudo resonance condition.  PhysicsProf is doing a great job in finding and trying to understand this pseudo resonance phenomenon.

Doing crude experiments and jumping to conclusions may not be the most scientific approach when we are dealing with controversial and potentially world-shaking inventions.

May God open the eyes and minds of the researchers and replicators.  Amen.
   
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I believe the person who built a crude blocking oscillator did not try to tune for the pseudo resonance condition.  PhysicsProf is doing a great job in finding and trying to understand this pseudo resonance phenomenon.

Doing crude experiments and jumping to conclusions may not be the most scientific approach when we are dealing with controversial and potentially world-shaking inventions.

May God open the eyes and minds of the researchers and replicators.  Amen.


hmmm now where have I heard this kind of talk before......"pseudo resonance condition"

suddenly the new parameter requirement is thrown into the hat after being pulled out of you know where.

OK Larry I'll play...exactly where does the extra energy you claim come from in the simple but now "tuned to pseudo resonance" Joule Thief? (in engineering terms, no lead in  bring out doubletalk).

and what is a "pseudo resonance condition" as opposed to a "real resonance condition"

Third, how can you claim something you took from another website as your own invention, when these things are in the public domain and have been for many many years.

Fourth: You are sending out units claiming they work and deliver OU "out of the box" and not requiring any tuning as all resistors are fixed. Now you are changing the rules?
« Last Edit: 2011-01-17, 04:38:00 by ION »


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...

...and what is a "pseudo resonance condition" as
opposed to a "real resonance condition"

...

Has anyone yet come up with an authoritative definition
for "real resonance condition" yet?

("Double Yet" intentional)


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I just did a quick review on the Joule Thief circuit on Wikipedia and noticed the following:

Quote
The circuit works by rapidly switching the transistor. Initially, current enters the transistor base terminal (through the resistor and secondary winding), causing it to begin conducting collector current through the primary winding. This induces a voltage in the secondary winding (positive, because of the winding polarity, see dot convention) which turns the transistor on harder. This self-stoking/positive-feedback process almost instantly turns the transistor on as hard as possible (putting it in the saturation region), making the collector-emitter path look like essentially a closed switch (since VCE will be only about 0.1 volts). With the secondary winding now virtually directly across the battery, the secondary winding current increases until it approaches the battery's short-circuit current. This enormous current drain on the battery reduces the battery's output voltage to the point where it can no longer forward bias the Base-Emitter junction of the transistor. (This Thévenin-equivalent resistance  of the source is actually a requirement for oscillation). When this happens, the transistor goes into the cutoff region (and opens the collector-emitter "switch"). The magnetic field collapses, inducing however much voltage is necessary to make the load conduct, or for the secondary-winding current to find some other path.

So in my proposed trickle-charged capacitor circuit for emulating the 1.5 volt battery and measuring the power consumption of the Joule Thief, you must put in an output impedance resistor, it is not optional like I was originally suggesting.  As you can see from above, the Joule Thief has to momentarily short out the battery so that it's voltage output drops to nearly zero.  Hence you must have a series output impedance resistor for the capacitor emulation of the battery.

As far as the oscillations go:

Quote
The oscillating frequency (in Hz) is approximately equal to the battery (or source) voltage (in volts) multiplied by the battery's Thévenin-equivalent resistance (or output impedance) (in ohms), divided by the transformer's mutual inductance (in Henrys).

Frequency of oscillation is approximately equal to:  V_battery x R_battery_output_impedance / Transformer_mutual_inductance

In the above example, given a 1.5v battery with a 1 ohm output impedance, the transformer's mutual inductance needs to be approximately 14 uH for the circuit to oscillate at 50 kHz. The oscillating frequency is principally a function of these three parameters, and is approximately linear, although this equation is only an approximation.

So Lawrence, we are operating in full reality mode now.  When you say "pseudo resonance condition" it's a false statement.  The Joule Thief circuit will resonate at it's resonance frequency.  As you can see above the resonance frequency is primarily determined by the battery voltage and output impedance and the mutual inductance between the windings of the Joule Thief transformer.

I know that you want to believe that resonance causes "something special" to happen.  This notion that resonance may be a source of over unity is seen everywhere on the free energy forums.  However, if you study resonance in thousands of physics and electronics and electrical and civil engineering books, you will not see a single reference to any kind of over unity phenomenon.  Passive resonance is simply the accumulation and storing of energy in a system from an outside energy source where the energy is provided to the system at the resonant frequency.  In addition, the actual storage of the energy in a resonance condition means that the stored energy is cycling back and forth between two different storage elements.  The first example that comes to mind is the ringing of a bell.  On storage element is the fact that the bell can be deformed and the energy is stored in the bell like a compressed spring.  The other storage element is when the mass of the bell is moving and the energy is stored as kinetic energy in the moving mass.  Energy moves back and forth between compressed spring energy and kinetic energy at the resonant frequency and nothing special is going on in this passive resonance example.  The Joule Thief circuit is an example of an active resonator that only resonates because there is an external power source that provides the energy required to keep it resonating.  At the same time the Joule Thief operates on somewhat similar principles to a passive resonator.

So, we are hopefully embarking on the measurement phase now.  All of the pieces of the puzzle are in place and it's just a question of collecting the data and seeing what it tells us.

MileHigh
   
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Quote
The circuit works by rapidly switching the transistor. Initially, current enters the transistor base terminal (through the resistor and secondary winding), causing it to begin conducting collector current through the primary winding. This induces a voltage in the secondary winding (positive, because of the winding polarity, see dot convention) which turns the transistor on harder. This self-stoking/positive-feedback process almost instantly turns the transistor on as hard as possible (putting it in the saturation region), making the collector-emitter path look like essentially a closed switch (since VCE will be only about 0.1 volts). With the secondary winding now virtually directly across the battery, the secondary winding current increases until it approaches the battery's short-circuit current. This enormous current drain on the battery reduces the battery's output voltage to the point where it can no longer forward bias the Base-Emitter junction of the transistor. (This Thévenin-equivalent resistance  of the source is actually a requirement for oscillation). When this happens, the transistor goes into the cutoff region (and opens the collector-emitter "switch"). The magnetic field collapses, inducing however much voltage is necessary to make the load conduct, or for the secondary-winding current to find some other path.

So in my proposed trickle-charged capacitor circuit for measuring the power consumption of the Joule Thief, you must put in an output impedance resistor, it is not optional like I was originally suggesting.  As you can see from above, the Joule Thief has to momentarily short out the battery so that it's voltage output drops to nearly zero.  Hence you must have a series output impedance resistor for the capacitor emulation of the battery.

Dear MileHigh,

Thank you for the information.  It made my day.  I was stipulating that the Joule Thief circuit itself forces an oscillating frequency.  If there were a small momentary disturbance, the JT circuit would get back to the oscillating frequency.

That was the logic I had in mind in putting on the secondary windings.  “Take out some energy in a pulsing mode and let the system swing back into the resonance condition”. 

We still differ in our opinion that I hypothesized that surrounding energy (electron motion energy) was brought-into the system at resonance.  But we can lay that difference aside and wait for our dear PhysicsProf to master the oscilloscope.  The best scenario is that he can borrow another identical one to show Input and Output Instantaneous Power simultaneously.

Let us give him some breathing space.  I like your too many cooks scenario.

Lawrence
   
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A fixed amount of energy is stored in the inductor per cycle of operation. It is released to whatever coil or coils are there to grab it when the field collapses.

You do not get more energy by adding more windings, the energy divides up according to the burden load on each winding.

You folks and LT need to get a serious primer on switching magnetics and power supply design.

Do a little  reading and you won't be groping in the dark. This stuff is so old hat and quite elementary.



MileHigh similarly appeals to existing technology and text-book primers:


Quote
I know that you want to believe that resonance causes "something special" to happen.  This notion that resonance may be a source of over unity is seen everywhere on the free energy forums. However, if you study resonance in thousands of physics and electronics and electrical and civil engineering books, you will not see a single reference to any kind of over unity phenomenon.

Now just a minute...  Are we to bound to what is already known, such that we cannot proceed with experiments that might show a NEW effect?  Is that what you guys are saying?    

  OR -- can EXPERIMENTS, quite apart from theoretical understanding, establish a new effect -- even when the source of the incoming energy remains for the moment unknown?

If your rules, gentlemen, require us to find our effect in existing textbooks, or in counting the number of windings, then I for one see little reason to proceed with discussion of empirical data here.  We should spend our time, if I understand you, reading the textbooks rather than doing experiments.
 Please clarify.


@Lawrence -- I think we need experiments and data to guide our research at the stage.  IF the energy output is greater than energy input -- IF this is demonstrated empirically and repeatably, then we can proceed to study and talk about where the extra energy comes from.  That is my suggestion.
   
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Before you throw out the books, I am merely suggesting you will have a better reach in searching for something new when you are well grounded in established switchmode design.

Otherwise, without the understanding you will be looking at something you are deluded to believe is new, when actually it is quite ordinary.

This is the current state of things.

For the record, I spent many years designing  Blocking Oscillators very similar to the one LT lifted and claimed as his baby and many more advanced and exotic versions.

I have been well down the road that you are only at the entrance ramp of.

Continue in your delusion if you like. LT is another pied piper of free energy and has led many of the entranced over the cliff with his hypnotic music.

Best of Luck in your research....you will need it.



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Before you throw out the books, I am merely suggesting you will have a better reach in searching for something new when you are well grounded in established switchmode design.

Otherwise, without the understanding you will be looking at something you are deluded to believe is new, when actually it is quite ordinary.

This is the current state of things.

For the record, I spent many years designing  Blocking Oscillators very similar to the one LT lifted and claimed as his baby and many more advanced and exotic versions.

I have been well down the road that you are only at the entrance ramp of.

Continue in your delusion if you like. LT is another pied piper of free energy and has led many of the entranced over the cliff with his hypnotic music.

Best of Luck in your research....you will need it.



My delusion?  What delusion?  I am conducting experiments to determine whether or not there is an effect here in Lawrence's particular design of input energy from an unknown source such that the output energy exceeds the KNOWN input energy.
 Are you saying it is delusional to do experiments -- that you know, in advance of taking data, that such an effect does not exist? 
   
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My delusion?  What delusion?  I am conducting experiments to determine whether or not there is an effect here in Lawrence's particular design of input energy from an unknown source such that the output energy exceeds the KNOWN input energy.
 Are you saying it is delusional to do experiments -- that you know, in advance of taking data, that such an effect does not exist? 

I'm saying I have done the research, collected the data, there is no effect, continue on, have fun it's a great and very steep learning curve.


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It's not as complicated as it may seem...
Professor,

I think you should expect some skepticism, in light of the experience that exists here. However, as far as the comments go, don't let them discourage you from your experimenting and testing. Rarely is this done at all in these circles, so it is refreshing to have someone actually attempting to discover the truth, all the while actually taking to heart the advice being offered along the way. In this I commend you, and it is my hope that this may lay the groundwork and perhaps become a template for similar testing in the future, for here, and at other forums where the checks and balances simply are not enforced.

So in short, carry on, and don't feel rushed or pressured. I and hopefully others will help along the way. I sense that you are open and unbiased, and that is exactly the approach to take. Let the resulting indicators speak for themselves.

.99


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ION:  
Quote
I'm saying I have done the research, collected the data, there is no effect,

Before you say this -- Have you actually built a replica of the Tseung device, as shown in photographs earlier in this thread?
Or just the Joule Thief device without the added winding and output circuit? 
[/b]


Professor,

I think you should expect some skepticism, in light of the experience that exists here. However, as far as the comments go, don't let them discourage you from your experimenting and testing. Rarely is this done at all in these circles, so it is refreshing to have someone actually attempting to discover the truth, all the while actually taking to heart the advice being offered along the way. In this I commend you, and it is my hope that this may lay the groundwork and perhaps become a template for similar testing in the future, for here, and at other forums where the checks and balances simply are not enforced.

So in short, carry on, and don't feel rushed or pressured. I and hopefully others will help along the way. I sense that you are open and unbiased, and that is exactly the approach to take. Let the resulting indicators speak for themselves.

.99

Well and nicely said, .99.     I will continue on.  "Some skepticism" is expected and is alright of course.  I don't know what the results will be yet regarding "unknown input energy".  

I have been reviewing the waveform traces this morning, and learning.
   
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Where the energy is coming from is not important at this stage? How much energy in and out is what is needed to confirm. What is the operating frequency of the DUT. Since all components are fixed values that were "supposedly matched to achieve a form of resonance with the complete circuit as is, meaning proper feed supply, unhindered device operation, normalized output, then ANY form of additional side pick up coils or probes will change this resonance. So maybe such questions should not be asked on small DUTs.

I have been trying to explain that same thing in my last few post, about using capacitors. @Milehigh "seems" to agree with this also.

With low energy DUTs, it would be best to simply use a high enough mF cap as feed, another dioded (germanium diode) capacitor as output and just let it run. The feed capacitor will have the same flyback throughput as a battery, it will eliminate the time factor you would have to equate if run by a battery, then dealing with depleted batteries, you will not have to poke and prod or apply near field pick-up coils to the DUT causing any unknown adverse effects or causing or being a potential additional energy source. The output capacitor will stabilize the final energy count regardless of running frequencies, etc. Just put your volt meter probes on the feed cap, measure and remove the probes quickly, then do the same to the output cap never leaving the meter on the cap while running the DUT.

This would provide at least a quick enough method of qualifying a "potential" small OU device for further scrutiny, based solely on how the first method results are. If the results of this first method are so obviously OU or so obviously not OU, then you can just stop there and provide the results. Only if the result of the first method is too close to call, would you then consider doing some more precise analysis.

Also, if such a capacitor run method can be standardized, then potential inventors of small potential overunity devices will have an easy method of doing this test themselves before they even consider sending it in for confirmation.

Now I clearly understand that a high level measurement of any "purported" OU device is desirable including caloric accouting but in many instances, the inventor claims OU without the inclusion of such values. If an easy method was available for all to do, without having to invest in rather expensive equipment and know-how and credibility, then maybe, just maybe that would be a good way to start. The inventor makes his device, tests it with this simple and "accepted" method, reports the results quickly, sends a few sample devices out, testers quickly corroborate those results and that gives you a solid basis to move forward or not to more advanced methods.

What could be devised is a simple table where based on the devices required feed, test duration and anticipated output levels would be replaced with set capacitors of predefined values, set diode values or model numbers, etc.

So if you have a feed cap of 10,000mf 6 volts, charged to 1.500 volts and you have another identical cap on your output at 0 volts, but now, after you run the test you have 4 volts stored in output cap and 0 volts stored in the input cap, then you know it's OU. Simple and sweet. But if your output shows 1.501 volts, then the inventor may decide to tweak the device further to improve on those results before considering declaring it as OU.

wattsup

PS: Keep it simple.
That's what we need.

Question: Is there a formal build spec on this device that one can use to make a unit and test it ourselves? Not just a picture. Maybe this should always be provided when the inventor supplies his device.


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If your rules, gentlemen, require us to find our effect in existing textbooks, or in counting the number of windings, then I for one see little reason to proceed with discussion of empirical data here.  We should spend our time, if I understand you, reading the textbooks rather than doing experiments.
 Please clarify.


You will be hard-pressed to find any useful effect in textbooks, and if you first find an effect, you will be hard-pressed to explain it.

When we turn on an electrical circuit, what really occurs?  We are performing work to move electrons. 

Are the electrons the soruce of the energy in the circuit, or is the source imbalanced energy?

So, if our conventional method of induction requires 10 units of work and we devise a method of induction that produces the same amount of power for 1 unit of work, then we have devised a more efficient method if induction and no laws are broken and no additional energy is required.

I suggest everyone look for a more efficient method of induction rather than "additional energy".
   
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@wattsup
Quote
So if you have a feed cap of 10,000mf 6 volts, charged to 1.500 volts and you have another identical cap on your output at 0 volts, but now, after you run the test you have 4 volts stored in output cap and 0 volts stored in the input cap, then you know it's OU. Simple and sweet. But if your output shows 1.501 volts, then the inventor may decide to tweak the device further to improve on those results before considering declaring it as OU.
That was a good post, however I would like to point out one issue in regards to using capacitors to measure input/output. Let's say our input is a capacitor which feeds a black box circuit and the output charges another capacitor, now if our black box has any capacitance or capacitive effects we then have two capacitors in series. At this point the law of inverse squares applies and we magically lose one half or more of the energy initially present in the system. This is why it is important to consider the effects of every field present as well as the standard current, voltage and time functions.

@Ion
Your last post was priceless, you seem to be implying that if we do not think just like you then we are delusional and that you know all the facts before any data has even been presented, which does not sound much like science to me. Unfortunately being an expert counts for nothing unless you can improve a technology which is kind of odd, all those self-proclaimed "experts" who never actually improve anything,lol. Which raises the question what good are they?

Regards
AC


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Comprehend and Copy Nature... Viktor Schauberger

“The first principle is that you must not fool yourself and you are the easiest person to fool.”― Richard P. Feynman
   

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As far as the oscillations go:

So Lawrence, we are operating in full reality mode now.  When you say "pseudo resonance condition" it's a false statement.  The Joule Thief circuit will resonate at it's resonance frequency.  As you can see above the resonance frequency is primarily determined by the battery voltage and output impedance and the mutual inductance between the windings of the Joule Thief transformer.

I know that you want to believe that resonance causes "something special" to happen.  This notion that resonance may be a source of over unity is seen everywhere on the free energy forums.  However, if you study resonance in thousands of physics and electronics and electrical and civil engineering books, you will not see a single reference to any kind of over unity phenomenon.  Passive resonance is simply the accumulation and storing of energy in a system from an outside energy source where the energy is provided to the system at the resonant frequency.  In addition, the actual storage of the energy in a resonance condition means that the stored energy is cycling back and forth between two different storage elements.  The first example that comes to mind is the ringing of a bell.  On storage element is the fact that the bell can be deformed and the energy is stored in the bell like a compressed spring.  The other storage element is when the mass of the bell is moving and the energy is stored as kinetic energy in the moving mass.  Energy moves back and forth between compressed spring energy and kinetic energy at the resonant frequency and nothing special is going on in this passive resonance example.  The Joule Thief circuit is an example of an active resonator that only resonates because there is an external power source that provides the energy required to keep it resonating.  At the same time the Joule Thief operates on somewhat similar principles to a passive resonator.

So, we are hopefully embarking on the measurement phase now.  All of the pieces of the puzzle are in place and it's just a question of collecting the data and seeing what it tells us.

MileHigh

The Blocking Oscillator variants operate as
non-linear resonance (pulled) devices.

The resonance conditions are a combination
LC (high frequency) and RC (low frequency).

The inherent modulation process is capable
of being "tweaked" or "tuned" by various
electrical adjustments and/or influences.

Its operation is quite sensitive to loading changes.

I'm delighted that this "simple" circuit is being
fully explored and evaluated by the present team
of well qualified and thoughtful participants.

Please continue gentlemen;  who can say what
further experimentation will reveal?

allcanadian =>  Well said!
« Last Edit: 2011-01-17, 19:51:47 by Dumped »


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For there is nothing hidden that will not be disclosed, and nothing concealed that will not be known or brought out into the open.
   
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PhysicsProf:

I also encourage you to do your experiments and make your measurements.  Don't mind me making reference to established sources of information.  This is a place where we are looking for something new.

Wattsup:

Your general concept of using capacitors on the input and output of a DUT to make definitive power/energy measurements is a good one.  However this has to be evaluated on a case by case basis.  The DUT may or may not work properly with a capacitor as the load.  A Bedini motor output for example is a discharging inductor and would be very amenable to driving a capacitor as a load.  The Lawrence Tseung flavour of the JT circuit however has an output that is a transformer secondary coil.  In this case you could rectify the output and charge a capacitor.  As soon as the capacitor got charged to the maximum voltage output by the JT transformer secondary coil it would then stop charging and disappear as a "load" from the point of view of the JT secondary winding.  In this case a capacitor is not a suitable way of measuring the power or energy output from the Lawrence Tseung version of the Joule Thief circuit.

A little addendum here:  I should also add that if you use a very large capacitor for the load then it might not get charged to the maximum voltage of the JT secondary winding like I indicated above.  Instead it will look like a short circuit to the JT secondary transformer output and the capacitor voltage will slowly increase as the circuit runs.  Again, this is not an appropriate type of load for the circuit and it will not be a good indicator of the output power or energy.

MileHigh
« Last Edit: 2011-01-18, 05:29:33 by MileHigh »
   
Group: Guest
Rosemary  :)

I think earlier you are talking about the battery capacity.  If a current flow out and in of the battery, it must be subtracted from each others while back and forth a resistor is an addition.  If this is what you're talking about, then I am sorry.

On the bright side, I was talking about the load resistor.  Yes, scope reading is unreliable in this case.  I have a different opinion that the current is nearly impossible to determine, not Ohms.  However, your thinking is not wrong.  If V=IR and you hold I constant while varying R yields the same result as holding R constant and varying I.  Yes, the best way to determine current/ohms function is to take the rate of change of the temperature vs time function.  We're not in contradiction.  :)

Good stuff Gibbs.  I see we are on the same page.  Take care.
Rosemary
   
Group: Guest
Golly guys.  Am I seeing a sea change in general attitudes. What a pleasure are these last posts - and even MileHigh coming to the party with an open mind.  Well done Professor.  We all needed you.  My take is that LT's circuit will give the required proof.  Hopefully.  And if this forum acknowledges that proof then we've made deep inroads into some rigid paradigms.

Professor.  More to the point.  You'll have finally thrashed out a required method for measurement.  If this is done conclusively, on 'small values' then that is, indeed, a milestone.  And it will certainly 're-ignite' this rather commendable research.  I cannot tell you how well I respect your efforts here.  It is that rare that an academic openly acknowledge any kind of interest at all.  And your own efforts are just so thorough.  I personally hope that you're a trend setter.  LOL. 

 :)
Rosie

   
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