Take your time Gigi, we want to get to the facts.  I am very impressed by the 
simulations that you have shown and how well they match the curves made by Jed. 
 Now, we need to verify that things add up as they should by combining thermal 
resistance and capacities of two parts to get to the whole.

They must combine according to normal physical laws.  My first attempt using 
your models did not seem to match properly.  That is what I want you to show.

And, if the thermal time constant is large, then average power due to the test 
itself will show up.  As you know, you are assuming that there is nothing 
except for the input drive signal of 20 watts and the pump leakage power.  I 
want to see how those parameters impact your results.  Then, we need to 
determine whether or not we can match the curves of Jed with a actual input 
signal due to LENR using your model.

I also still believe that the pump power is less than you are considering.  
Nevertheless, I will keep an open mind and give your model an opportunity to 
show its strength.

Thanks,

Dave

 

 

 

-----Original Message-----
From: Gigi DiMarco <[email protected]>
To: vortex-l <[email protected]>
Sent: Tue, Jan 13, 2015 4:35 pm
Subject: Re: [Vo]:"Report on Mizuno's Adiabatic Calorimetry" revised


Ok, we need some time to perform the full set of simulations. But please do not 
take for sure that the pump only test had exactly the same configuration than 
the test run had. We will present them as soon as we are confident that all the 
problems have been settled.



2015-01-13 22:18 GMT+01:00 David Roberson <[email protected]>:

Gigi,

I have another issue that you might be able to discuss.  You made two 
independent simulations of the behavior of the Dewar temperature and reactor 
body over time.  In one case the pump was working and in the other if had 
failed.  I took the values that you calculated for the thermal components of 
your model and get very different results for the combined time constant than 
what you have shown for the individual ones.

The thermal masses should be added in parallel directly which you seem to have 
done.  I combined the thermal impedances in what I consider the proper manner.  
When a final calculation of the time constant is computed by using the two 
others, the number does not come very close to matching what you are using for 
the first case.

Please take time to perform that combination on this forum for us to view and 
analyze.  Also, please turn that answer into an actual hour figure for us.  
This will be very important as we attempt to understand the impact of residual 
drive signal and any additional due to LENR activity.

Begin with the time constant you calculate in hours.

Regards,

Dave

 

 

 

-----Original Message-----
From: David Roberson <[email protected]>
To: vortex-l <[email protected]>

Sent: Tue, Jan 13, 2015 3:27 pm
Subject: Re: [Vo]:"Report on Mizuno's Adiabatic Calorimetry" revised


I may have answered my own question below.   The drop in ambient acts much like 
a negative signal as I have proposed before.  Eventually the delta will become 
zero for both signals. 

Forget the first question and concentrate upon the next one.

I notice that in both curves that you use to determine the pump power leakage 
actual true signal power due to the 20 watt drive and any device LENR power was 
contributing to the total.   The shape of the temperature curves with time 
clearly show an initial rise during the first few hours that affect your final 
answer.

What have you done to subtract this effect from your determination of the 
constant average power presumed to be leaking from the pump?   It would be 
useful if you include this heat input into your model and see how that would 
modify the average power that is coming form the pump.  Since you know the 
shape of this heat signal and you assume that no additional power is added by 
the LENR effect, it should be easy to model it as an additional heat source.  
Spice would handle this nicely.

Dave


 

-----Original Message-----
From: David Roberson <[email protected]>
To: vortex-l <[email protected]>
Sent: Tue, Jan 13, 2015 2:49 pm
Subject: Re: [Vo]:"Report on Mizuno's Adiabatic Calorimetry" revised


Dear Gigi,

I have begun to analyze your report and find something that does not seem 
logical according to my understanding of heat flow.  On your figure A2 I see 
that you have overlaid your simulation results upon Jed's figure.  The 
correspondence between the curves is remarkable and you should be commended for 
your work.

The issue that I need to resolve is that the delta temperature between the 
Dewar and ambient is actually increasing during this time.  Also, the delta for 
the reactor is becoming less with time as I was expecting.  In order for the 
temperature delta to increase you would have to supply some form of heat power 
to that device.  The model that you are using is extremely simple and certainly 
does not suggest that anything more complex would be happening.

How do you explain that the delta is increasing?  Is there some process that is 
supplying extra power into the Dewar once the pump is turned off?

Regards,

Dave

 

 

 

-----Original Message-----
From: Jed Rothwell <[email protected]>
To: vortex-l <[email protected]>
Sent: Tue, Jan 13, 2015 2:06 pm
Subject: Re: [Vo]:"Report on Mizuno's Adiabatic Calorimetry" revised



Gigi DiMarco <[email protected]> wrote:

 



The refrigerator example is quite evident, but is unfit to our situation, by 
various causes. The main one is that there you have an abrupt change of air 
temperature, while in the 18h test the air temperature is falling at a modest 
rate of 0,36 °C/h that is very simple to follow for the calorimeter.






No, it isn't. That is why a gap opens between the room temperature and the 
calorimeter, and the gap persists until early morning.


 




If from now on the losses are equal to the pump power, since you have


Loss = K * deltaT    and  PumpPower = loss = constant

and since K is valid over a broad range of deltaT you should have a constant 
deltaT.





No, it isn't. See Newton's law of cooling.


 



So going back to the plots in the missing file you considered only the first 
1.5 hour only because just after the ambient temperature starts decreasing. 
What have it happened if the ambient did not change for 5-6 hours? Can you 
answer this question?




Yes, I can. If ambient stays stable, the reactor and water temperature will 
remain stable at 0.6 deg C above room 


 


 Where in the data do you see that 0.6 °C is the maximum?




It goes no higher after 1.4 hours. You can see this in other data sets as well, 
such as early in the morning with this data set. Whenever ambient remains 
stable for a few hours or more, the reactor temperature always settles 0.6 deg 
C warmer.






 


Please don't be contemptuous and dismissive; it is not the case. If someone 
does't understand calorimetry it is not me.





You do not understand Newton's law of cooling and you cannot tell the 
difference between ambient cooling and heat generation in a cell. In my 
opinion, you are terribly confused and totally unqualified to do calorimetry.


- Jed











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