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Author Topic: Flea Power Measurements  (Read 8324 times)

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Dear ION.

I found... wires.com seems to stock most of everything, great for experimenters this side of the pond.

With regards to Verpies's circuit I could ask my friend Richard at RM Cybernetics about building it.

If a suitable PCB layout was produced and presented to him the price shouldn't be too prohibitive.

Cheers Graham.


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Dear Verpies.

Would a " K " type thermocouple bead Epoxied to the resistor body affect results?

Cheers Graham.


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Would a " K " type thermocouple bead Epoxied to the resistor body affect results?
It would make it slower to respond but it would be more immune to the magnetic induction/interference from the current flowing in the resistor.
   

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OK,i have just had a brain wave-or brain fart  :D

Wont say now,but will throw it together tomorrow,and present a video of my idea here,and you guys can tell me what you think.

This will eliminate any inductive problem,and can be fine tuned to be exact-to show us the smallest difference in actual current on the input,and output.

Should cost all of about $5.00 to put together,but i would think we would all have the required parts lying around,and any DMM should work ok in showing us the difference,as the amplitude would be in mV,not uV


Brad.


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Wrapping the resistors with the thermocouple wire is not a good idea because that thermocouple winding will pick up the magnetic flux variations from the current flowing in the resistors and the induced voltage will swamp the thermocouple signal approximately 100000 times.

See the scopeshot below for a 10Ω ¼W THT resistor wrapped with 7 turns of wire while a 1MHz 340mAP-P square AC is flowing through it.
Green trace is the current through the resistor and the yellow trace is the voltage induced in the 7 turns of wire (4.8VP-P).

Dear Verpies

I'm trying to figure out how you got (7 turns) from the picture I posted, since it only shows one half turn of the twisted portion of the junction. Also you do not explain what load you had on the 7 turns. As you know an unloaded coil will have quite a self resonant rise and tend to exaggerate the voltage produced across it, even by just capacitance coupling from a nearby object.

1) I never suggested anyone should use 7 turns of TC lead wire around the resistor, I don't know where that came from. I use only one half turn of the twisted portion that forms the thermocouple junction. Since it is twisted it is immune to current in the resistor except perhaps  for some common mode signal capacitively coupled. The common mode as well as series mode AC signal is rejected by most good DC uV meters, as generally it would be very high frequency, low level. The output of the thermocouple is DC voltage or current depending on how it is used.

2) The resistor you used may have been "spiral cut" to trim it's value. This creates a few turns on the resistor film which can indeed inductively couple to the 7 turns, As you know, a wire passing through the center of a coil cannot induce current into the coil by Faraday induction because it is at right angles 90 degrees to the coil. It can however excite the turns capacitively, which is what I see in your scope  shot.

3) As I said earlier, there are improvements that I would discuss at a later time so as not to overly complicate the basic device. A couple of the improvements are to add ferrite beads to the thermocouple leads both series mode and common mode to attenuate any capacitive or inductive coupling effects. I did not complete the fine points of advanced construction yet.

4) Depending on the skill of the constructor at forming  a tiny thermocouple junction, it as not at all necesary to wrap the junction or it's associated wires around the body of the resistor. A tiny bead of epoxy will thermally connect the tiny junction to the resistor.

5) There is a well known  technique  that should the constructor wish to add a turn or two of the wires around the body of the resistor, it can be done in a  in a non-inductive manner. It is the same method used to make non-inductive wirewound resistors. Why would an extra turn or two help?
The value of the extra turn is more precise temperature reading by also heating the thermocouple wires leading to the junction so that the leads do not adversely drain heat from the junction.
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There seems to be an intent on killing this method before it is "off the ground". Trying to warn others that it is a bad method is probably working, having it's effect by now.  :(

 I have not yet had a chance to post the finer details of the method such as the HF rejection curves.
Sorry for that, I have a lot of domestic and health related issues to deal with right now.

P.S Brad

As I mentioned in the beginning there are many ways to sense the temperature of the resistors e.g. thermistors, Thermal IC chips, diodes. You could build a bridge that uses any of those devices but it will not be passive, will need a power supply, and will have a propensity to pick up HF noise that would not be easily filtered due to the non-linearity and rectification of some of the devices.

I chose thermocouples because I am quite experienced in using them and they solve a lot of the problems that would be introduced with other temperature sensing methods and it is a passive method, not requiring a power supply, which could introduce additional capacitance coupling.

 Also I have a lot of good uV meters and measuring instruments in the shop. Nowadays they are very common. Back 50   years ago they were more difficult to construct, usually requiring chopper stabilised DC amplifiers.
When I get time I will try to demonstrate using a passive analog 50-0-50 uA meter.

To each his own.

I'm gonna take a break from this jousting session, it's bad for my health.


« Last Edit: 2017-05-09, 17:09:46 by ION »


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Dear ION.

I found... wires.com seems to stock most of everything, great for experimenters this side of the pond.

With regards to Verpies's circuit I could ask my friend Richard at RM Cybernetics about building it.

If a suitable PCB layout was produced and presented to him the price shouldn't be too prohibitive.

Cheers Graham.

Dear Graham

I would recommend that you not bother with building the thermal RMS bridge, that I have used over the years with success. Apparently, it has been deemed to have too many theoretical problems that I have yet been able to locate.  ;)
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Regarding the circuit that verpies posted, attached is the pdf with the circuit and PCB layout for the evaluation board right from the manufacturer of the IC. Notice the use of a few chokes and capacitors to keep HF out of the device and to provide transformation, which have not been included in the circuit verpies posted, and may not even be necessary. You may wish to read this document and evaluate their need or not and modify appropriately before boards are produced. Maybe check with verpies on that. I believe the chokes are intended for singled ended to balanced transformation for AC signals but may be removed for DC operation so they may not be needed.

Regards
« Last Edit: 2017-05-09, 19:54:20 by ION »


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Maybe check with verpies on that.

Dear ION.

That's probably a good idea....

I can't seem to find the Carburettor anywhere.....  :o

Cheers Graham.


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I would recommend that you not bother with building the thermal RMS bridge.
Grum is probably going to throw up his hands and run away from his monitor when he reads that in my opinion the dual thermal bridge is right up his alley and in my opinion he should build it because he understands heat flow well and a sub milimeter precision of mechanical assembly is not anything new to him. He also has intuitive understanding that closely spaced parallel wires interfere with each other.

Regarding the circuit that verpies posted, attached is the pdf with the circuit and PCB layout for the evaluation board right from the manufacturer of the IC. Notice the use of a few chokes and capacitors to keep HF out of the device, which have not been included in the circuit verpies posted. You may wish to read this document and evaluate their need or not and modify appropriately before boards are produced. Maybe check with verpies on that.
That evaluation board is not DC-coupled, it performs a different function and uses more pins of the multiplier chip.
Anyway, I do not recommend that Grum gets involved in  building it until  he can have a debugged version  of the Watt2Volt converter PCB sent to him for the "A" version of the chip.
« Last Edit: 2017-05-09, 18:37:09 by verpies »
   

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I'm trying to figure out how you got (7 turns) from the picture I posted, since it only shows one half turn of the twisted portion of the junction.
It  was a low resolution picture and it looked to me this way. With half a turn I would expect the induced EMF to be 14 times smaller but that is still a lot  compared to the  thermocouple signal.

Also you do not explain what load you had on the 7 turns.
Just the scope probe.

As you know an unloaded coil will have quite a self resonant rise and tend to exaggerate the voltage produced across it,
Not with a 1MHz signal which  is  far away with such resonance.

...even by just capacitance coupling from a nearby object.
I use only one half turn of the twisted portion that forms the thermocouple junction. Since it is twisted it is immune to current in the resistor except perhaps  for some common mode signal capacitively coupled. The common mode as well as series mode AC signal is rejected by most good DC uV meters, as generally it would be very high frequency, low level. The output of the thermocouple is DC voltage or current depending on how it is used.
3) As I said earlier, there are improvements that I would discuss at a later time so as not to overly complicate the basic device. A couple of the improvements are to add ferrite beads to the thermocouple leads both series mode and common mode to attenuate any capacitive or inductive coupling effects. I did not complete the fine points of advanced construction yet.
Capactive coupling could be an issue, too. 
You  should post scopeshots of thermocouple interference tests with a 1MHz 100mA square AC current flowing through the heater/resistor.

2) The resistor you used may have been "spiral cut" to trim it's value. This creates a few turns on the resistor film which can indeed inductively couple to the 7 turns,
Not in this case but it is a valid concern and you should warn potential builder about such Gotcha.

Why would an extra turn or two help?
Because the EMF from the extra turns can be arranged to cancel  itself, as in a bifilar coil of the  3rd kind.
Also if half of the coil has an equal and opposite pitch then it also cancels the helix's axial current.

As you know, a wire passing through the center of a coil cannot induce current into the coil by Faraday induction because it is at right angles 90 degrees to the coil.
Yes, but when the distances are comparable to the diameer of the wire, the near field  is so twisted that it can still cause induction.  Even the pitch of the helix can matter.
« Last Edit: 2017-05-09, 18:59:37 by verpies »
   
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Dear Verpies
Quote
Quote from: ION on Today at 15:34:58

    Why would an extra turn or two help?

Because the EMF from the extra turns can be arranged to cancel  itself, as in a bifilar coil of the  3rd kind.
Also if half of the coil has an equal and opposite pitch then it also cancels the helix's axial current.


In this statement, I was asking the question rhetorically as a prelude to the follow up sentence and you did not have to answer, as I had already stated how to create the non inductive wind  in the prior sentence:

 "it can be done in a  in a non-inductive manner. It is the same method used to make non-inductive wirewound resistors."

"Why would an extra turn or two help?" I asked (rhetorically)

I was posing different  reason for adding one or two turns and why you would even want to do it, namely:

"The value of the extra turn is more precise temperature reading by also heating the thermocouple wires leading to the junction so that the leads do not adversely drain heat from the junction."

Maybe we have a language barrier here.

Regarding the interference of the RF signal by injection into the thermocouple, I can assure you it is not a problem.

I tested it with both a Kiethley 155 Null Microvolt meter and a Fluke 87. I  had a steady readout of around 4 mV with the full input of 6.72 volts from the FG  into the resistor, up to 5 MHz. Quickly switching on and off the generator did not affect the readings on either of the meters. The readings only changed if there was a long interval after switchoff, as the resistor cooled down, the readings were not visibly affected by the RF.

I looked at the actual signal on the scope and at 5 MHz it was in the range of 30 mV AC, but this is not a problem, as you see, most good instruments that are designed to read low level uV DC also reject HF AC quite well, and 30mV of AC is nothing.

I have worked in the temperature and process control industry for half a lifetime as a chief engineer designing equipment that used thermocouples and the  front end amplifiers had to reject everything from noise on a 480 volt mains to HF RF from local transmitters. These were sometimes difficult problems to solve, but solve them we did, and usually very simply.

I see the problems you keep bringing and your concerns as quite  trivial by comparison and if my time were not so valuable right now,  I would flood this page with information showing that your concerns are not an issue.

This exercise very much reminds me of the numerous exchanges I had with customers that were Ph.D's that had a lot of  theoretical but very little practical experience. It is becoming tiresome to say the least. What do you gain by continuing on like this? Why don't you just  build it and see that it works just fine and is not affected  by your caveats or just stand by and watch this fail and have a good laugh (it won't, I can assure you).

Regards





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The value of the extra turn is more precise temperature reading by also heating the thermocouple wires leading to the junction so that the leads do not adversely drain heat from the junction.
Maybe we have a language barrier here.
We don't.  Notice, that I did not disagree with the above - I just added more advantages from my perspective.

Regarding the interference of the RF signal by injection into the thermocouple, I can assure you it is not a problem.
I tested it with both a Kiethley 155 Null Microvolt meter and a Fluke 87. I  had a steady readout of around 4 mV with the full input of 6.72 volts from the FG  into the resistor, up to 5 MHz. Quickly switching on and off the generator did not affect the readings on either of the meters. The readings only changed if there was a long interval after switchoff, as the resistor cooled down, the readings were not visibly affected by the RF.
I looked at the actual signal on the scope and at 5 MHz it was in the range of 30 mV AC, but this is not a problem, as you see, most good instruments that are designed to read low level uV DC also reject HF AC quite well, and 30mV of AC is nothing.
So you are aware that there is 30mV AC HF interference superimposed on several μV/ºC thermal signal in your system.
Wouldn't an ounce of prevention (avoiding the interference) be worth more than a pound of cure (low pass filtering)?  The latter is not infallible.
 
Did you test it with asymmetrical HF waveforms, that create a DC component after low pass filtering?


What do you gain by continuing on like this?
Exploration. Advancement of knowledge.
Qualitative and quantitative characterization. Perfection of the design.
List of Gotchas for future builders. 

Aren't these the very reasons for existence of forums like this ?

Why don't you just  build it and see that it works just fine and is not affected by your caveats
My caveats?  I thought that caveats were not personal...
A 1 turn wrap around a 10Ω resistor produces interference like this:
   
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From Verpies

Quote
Did you test it with asymmetrical HF waveforms, that create a DC component after low pass filtering?

Asymetrical signals do not communicate a DC signal through a capacitance nor through a transformer by induction, even after filtering. I'm sure you know this or you could rewrite the physics books by being able to pass DC through a transformer or a capacitor. After the capacitor or transformer the average of the wave is always zero DC regardless of the input waveshape.
Only when there is leakage, rectification or asymetrical saturation of a device could the result have a DC component.

Quote
Wouldn't an ounce of prevention (avoiding the interference) be worth more than a pound of cure (low pass filtering)?  The latter is not infallible.

The filtering is already in the instruments I use to measure the TC signals. If additional filtering were necessary, I would certainly use it. I did mentioned using common mode and series mode ferrite beads.
I haven't even gotten to the finer points in the method of discussing additional filtering, where and why it might be needed, because I didn't want to cloud the basic understanding of the principle.

Quote
So you are aware that there is 30mV AC HF interference superimposed on several μV/ºC thermal signal in your system.
Wouldn't an ounce of prevention (avoiding the interference) be worth more than a pound of cure (low pass filtering)?  The latter is not infallible.

If it were needed I would certainly us it, the 30mV AC is well filtered by the low pass filter of the measuring instrument. Precaution noted.

Quote
Exploration. Advancement of knowledge.
Qualitative and quantitative characterization. Perfection of the design.
List of Gotchas for future builders. Aren't these the very reasons for existence of forums like this ?

*I'm beginning to believe forums serve a different, not so benign purpose, and what I wrote recently about brotherhood was indeed very naive of me.

Quote
My caveats?  I thought that caveats were not personal...

Answered in part in prior sentence* They can be subtly personal.

Quote
A 1 turn wrap around a 10Ω resistor produces interference like this:
You call it interference when seen on a scope but it's only interference if it can register an effect on the thermocouple DC measuring instrument. Most DC measuring instruments (even common DMM's) are designed to handle much larger interfering signals and reject them quite well, allowing only the expected DC component of the TC to pass.

Regarding your scope shot, it shows the typical signal I would expect to find on the TC leads, or even just an unconnected scope probe in the vicinity of the resistor, and it is of little consequence compared to the much larger AC signals on TC leads that I have successfully coped with in the past without difficulty as most skilled in the art have.

Regards
 
« Last Edit: 2017-05-10, 00:11:36 by ION »


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Well i didnt get time to get the whole current differential device together,due to a late finish at work,and friends turning up.

But i did get to test the current input side,and the results are better than expected  O0
For every mA of current increase,i can get a 5mV increase on the DMM-so 5mV for every mA increase  ;)

HF,stray inductance,and the likes,will have no effect on this devices measurements.

Being that it works so well,and with the twist of a knob,can be calibrated with ease,i am going to spend the money,and get all new parts,and build it properly.

So,in saying that,i will hold of on the video,until such time as i have a presentable device.


Brad


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Well i didnt get time to get the whole current differential device together,due to a late finish at work,and friends turning up.

But i did get to test the current input side,and the results are better than expected  O0
For every mA of current increase,i can get a 5mV increase on the DMM-so 5mV for every mA increase  ;)

HF,stray inductance,and the likes,will have no effect on this devices measurements.

Being that it works so well,and with the twist of a knob,can be calibrated with ease,i am going to spend the money,and get all new parts,and build it properly.

So,in saying that,i will hold of on the video,until such time as i have a presentable device.
Brad

Brad
It will be very interesting to see what you have come up with. O0

 Meanwhile attached is a block diagram of how to test a common JT or Blocking Oscillator using the thermal bridge. It will give a fairly accurate indication of true RMS power output. Accuracy depends on how well your bridge is constructed, and how well insulated with respect to ambient and each side of the bridge (crosstalk). There are many ways to improve the basic idea and it's performance, but what I have presented thus far is for conceptual and initial  understanding purposes, by no means a finished, perfected device.

As you know the output of a JT presents an asymmetrical current pulse into a load resistor. Use this method as a backup to the values you are getting on a scope measuring the output.
 Input to the JT is measured the usual way, since it is DC.

Regards


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It's not as complicated as it may seem...
Nice setup Ernie, with the TC bridge.   :)

Is there any calibration involved?


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Brad
It will be very interesting to see what you have come up with. O0

 Meanwhile attached is a block diagram of how to test a common JT or Blocking Oscillator using the thermal bridge. It will give a fairly accurate indication of true RMS power output. Accuracy depends on how well your bridge is constructed, and how well insulated with respect to ambient and each side of the bridge (crosstalk). There are many ways to improve the basic idea and it's performance, but what I have presented thus far is for conceptual and initial  understanding purposes, by no means a finished, perfected device.

As you know the output of a JT presents an asymmetrical current pulse into a load resistor. Use this method as a backup to the values you are getting on a scope measuring the output.
 Input to the JT is measured the usual way, since it is DC.

Regards

Looks good ION,and i believe that my setup can be used to calculate the P/out of a JT.

One thing to note though.
You cant place a resistor where the LED go's in a JT,as you have in your schematic.
You would need to add a diode in series with the resistor,and then some how account for the power dissipated by that diode as well as the resistor.

With my design,you would only need the LED,as per the standard JT.

I should be collecting my new 4 channel scope on friday,and hopefully my copper tape rolls will arrive in the mail on friday also.

So this weekend is going to be full on,as i want to build this equivalent to your thermocouple device as well.

I see a late friday night coming on  C.C


Brad


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Ah..... oh to be a little younger Brad...

I love the elegance in its simplicity ION, nice one.  O0

Regarding calibration, well it's all a bit " hit n miss " without a visit to your local standards laboratory but, most modern test instruments are pretty good, aren't they?

I spent some time in the test and standards lab calibrating what were called " sub standard " instruments for field use. The " standard volt and amp " meters were kept in amazing housings!!  Oh they were all analogue back then, those were the days!

Gotta go.... back later.


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Nice setup Ernie, with the TC bridge.   :)

Is there any calibration involved?

The really interesting thing about the bridge is that the resistors don't have to be matched in resistance, just in size. In fact, they can be widely different in resistance as long as they are the same approximate physical size and power rating e.g. for power measurements under
 250 mW 1/4 or 1/8 watt resistors are ideal. For higher power measurements, the resistors can be scaled up accordingly in size.

I know this all sound counter intuitive, but once you begin thinking in the realm of heat production and EMF from heat, it will start to make sense.

I imagine it should be possible to build a device that can measure levels in the  0 to 50 mW range with acceptable accuracy.

At some point I want to build one that uses tiny surface mount resistors and see how low it can go, and maintain some decent level of accuracy.

I'm sure you know the technique of using heat and thermocouples to generate mV to drive a meter movement is actually used in some older RF ampmeters.

Because the bridge is immune to small resistance changes, we don't have to worry about slight drifts in the resistors. It may be difficult to understand this but once you begin thinking in terms of the final result of generating heat, the value on the right side R2  can be anything that matches the voltage range your power supply, and the value of R1 can be roughly impedance matched to the DUT.

If you wish to see how well the bridge balances, you can apply the same power level to each resistor, you should get a null output if the bridge is properly constructed, if not there are ways to trim and calibrate the TC mV output of the system. I will get into that later, but calibration should not be required if physical symmetry of the constructed device is maintained.

Regards

P.S. Thermocouples are used in some vacuum measuring bulbs where the filament temperature is related to the number of molecules the filament can transfer heat to,
 so a higher vacuum = higher filament temperature=more TC output.
« Last Edit: 2017-05-10, 19:34:34 by ION »


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Here are a few graphs from two different builds, using different components. One is a round styrofoam chamber, the other is flat sandwich construction.

As you can see from the graphs, there is  a healthy output even under 50 mW.

Tracking was also very good, as I put voltage into both resistors in parallel to observe the deviation at several points (which was acceptable) .

I'll be moving on from this to some new ideas, but will continue to work in the background perfecting the method and going to even lower values of milliwatts.

Some of the ideas I will be working on in background:
a)  Eliminating the need for a thermocouple/heater combination by using a low slope PTC Thermistor or Platinum RTD of the non inductive thin film type as both load and sensor.

b) for very small mW measurement, using the tempco of a heating element (filament) inside a vacuum tube as both load and sensor. As you may know some of these bismuth coated filament rods are folded back and forth and are low inductance. Just a fun experiment.

c) measuring the emission vs filament voltage of e.g. a 6AL5 dual diode vacuum tube, both passively, Cathode to Anode mVolts or with a plate voltage applied. Initial tests look very interesting, very low to no emission under 3 Volts on the filament, but quite stable and high output above that approximately up to 500 mV at 6 volts on the filament, passively measured A to K.

d) using an infra red sensor to accurately read the IR energy from the load resistor in a non contact manner.

By the way, if you wish to know how small the power we are chasing really is, take a 100 Ohm 1/4 watt resistor and put 5 volts into it. This is 250 mW. You can just barely hold it to a spot slightly below the lower lip.(I found this to be an accurate spot on the body to detect temperature, there are probably others, but I won't go there, that's for your own private experiments) This is a reasonable amount of power as you almost can't keep it touching.

 Now keep reducing the voltage until you can no longer sense the heat. What mW did you find it to be? For me it was around 40 to 60 mW where any warmth was first detected, but I'm almost dead anyway so maybe someone else will get better results.

Probably better to run this experiment working up from zero.

Regards.


« Last Edit: 2017-05-15, 18:04:18 by ION »


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