So far we have not seen any clear excess energy out of the cell during this Helium test. Since our baseline was from a run with the exact wire being tested here, we did get a nice, close calibration curve, though. More accurately, we did not see any significant deviation in temperatures from the base line run.
One of the results from last night's run of the Loaded Celani Wire in Helium is that we got a glimpse into the impedance changes of the Celani wire pre-loading and post loading. That's what I want to talk about now.
This is the results for the very first run with the Celani wire after installing it in the cell. With every increase in power, the impedance went up in a nice step. It looks like the first 6 steps maintain a positive slope, though. The last 3 steps level out more at the top.
The second run was done at at 0.5 bar. Notice a difference?
The step in the middle of the range displays a strong negative slope. That occurred approx T_mica = 228C.
Then on this run, we saw the following curve.
A couple of interesting things here. The downward slope appears again on the 4th and 5th step. This was about 225 and 245C on T_mica, though the wire was probably higher temp. On the highest step (T_mica=265) the slope continued positive, though. Upon reducing the power back down to match the 225 T_mica, again, the impedance dropped well below the previous level at that temperature.
Questions these data raise:
If impedance is a measure of loading, is the wire somehow gaining Hydrogen in this Helium environment? It is possible there was some residual hydrogen available in the cell. Perhaps it was dissolved in the NiChrome wire, or the copper wire, or the Mica wire supports.
Or is it a migration of Hydrogen with the wire? Or is it some other metallurgical thing? It's possible it has little to do with hydrogen and may be a function of cycling the wire temperatures. Thoughts?
Why did we see some "loading" in the Run2He? Again, maybe residual hydrogen from other things in the cell. When we installed the Celani wire, we also replaced the Nichrome wire, so that probably was not a factor, but the other items may have been.
What is with the sudden drop as the power is turned on at the very beginning? This I think we have an answer for. At that time, the wire was powered by the power supply in automatic mode. This new power supply (that replaced the one we damaged yesterday) has an improved control interface that actually goes all the way to zero when asked to. That makes the impedance measurement very inaccurate. Additionally, the sensor inputs that measure the current and voltage have an option for a zero offset calibration that we have never had to worry about. Now calibrating that offset is on our to-do list. All these little improvements add up after a while to some real good technique.
It'll be interesting to see how the impedance changes by morning. Once again, I am up past my bedtime. Good night.
Comments
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I'm sure some of us would be keen to donate for its travel expenses. I would.
The process of taking off the lid and measuring temperatures does cause a slight drop in cell temperatures, though. Or at least, it did each time you said you were doing so.
Excess power calculation currently seems in line with that of the previous power step.
I did increase the power to see if the excess power increases with the temperature and the increased current.
In
www.nist.gov/.../jpcrd221.pdf
Page 235 is interesting too. It is a long read!
We have been discussing the potential for annealing to modify or disable the Celani wire. I guess as we start testing more wires in both the US and EU, running SEM on them afterwards - we will build up a pool of evidence we can dip into to understand what is happening. With the live and near live publishing of raw data and images and the help of people like those interested in looking at it on here we will together form a good understanding of what is going on.
lenr-canr.org/.../...
We speculate that the electrically self-heated wire method, is probably helpful in
obtaining higher loading values.
There's some research on alloy resistance across temperature that may be interesting to some.
www.nist.gov/.../jpcrd221.pdf
On page 53 there are graphs of electrical resistivity of Nickel/Copper alloys at different ratios across temperature.
There's also some interesting information about annealing of Ni in the temperature range that the wire has seen already. (just something to look at while waiting on the experiment! : )
I'm also thinking that once an active wire has been well-loaded with Hydrogen at a high pressure, afterwards it might not be necessary anymore to keep it at 7 bar.
So I'm asking: are there plans to try this "high pressure path", which anyway would be more faithful to Celani's testing conditions? Can your reactors withstand them?
(There are also potential safety issues with this, btw)
This would reduce the wire resistivity, even if no additional hydrogen/proton s are loaded in the wire.
I keep forgetting to tell you how to simply add a large ballast vessel. We used to use an empty gas bottle (big nitrogen ones) and connect directly to the laser (in your case the cell). In this way you have a very large reservoir (>1000:1 ratio) filled to the gas pressure you require and you can simply use this to accurately refill and keep your cell at the required pressure.
Good points as ever David - this is why we planned the internal replications first, to identify and iron out any doubts or bugs in the system in a public way to form a tight understanding of what affects certainty and how to deal with it.
Thanks for your diligent attention.
There appears to be a step down in ambient at that time - but pressure and impedance are both dropping.
Sorry for my poor english.
What happens to power-out on October 16 at 7:05 am? (HUGnetView™ time)
Sudden increase of 2.5 W ?
Thanks for your great job
Regards
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