What you say would only be true provided that the device were not generating 
most of the heat that lead to the self destruction.  It is too bad that they 
did not remove the drive and let it prove that it can run away which would have 
been quite convincing to most skeptics.  Or would it have been?


I suspect that the results would have been much the same in either case.  The 
device was out of control.


Dave



-----Original Message-----
From: Andrew <[email protected]>
To: vortex-l <[email protected]>
Sent: Sat, May 25, 2013 1:50 pm
Subject: Re: [Vo]: ECAT Drive PWM Issues



I should add that I don't believe that currently we have any hard evidence for 
the existence of thermal runaway occurring spontaneously. The (in)famous photo 
of the device in meltdown was taken under the condition of continuous supply of 
substantial input power. For all we know, we are looking at a photo of a 
resistor overheating.
 
Andrew
  
----- Original Message ----- 
  
From:   Andrew 
  
To: [email protected] 
  
Sent: Saturday, May 25, 2013 10:43   AM
  
Subject: Re: [Vo]: ECAT Drive PWM   Issues
  


  
Dave,
  
 
  
You therefore answer in the affirmative - i.e. it looks possible in   principle 
to operate with sporadic negative power input (cooling) and at zero   input 
power, once the reaction set point has been established.
  
 
  
This is exactly what is required to nail down the   existence of the effect. No 
shenanigans with input power are then possible,   and there's only one 
conclusion possible - that, at steady-state, energy   is being generated when 
no energy is being input. This is crucial in my view   for universal acceptance 
of the vailidity of the effect - whatever the details   of that effect might be.
  
 
  
Andrew
  
    
----- Original Message ----- 
    
From:     David     Roberson 
    
To: [email protected] 
    
Sent: Saturday, May 25, 2013 10:30     AM
    
Subject: Re: [Vo]: ECAT Drive PWM     Issues
    


Andrew,     


    
My model demonstrates that a periodic waveform is required in order to     keep 
the ECAT within stable bounds and at a good COP.  If the drive is     totally 
eliminated then there are two states that can exist.  One is     for the device 
to cool off and reach room temperature and the other is for     it to continue 
rising in temperature until it can no longer be controlled by     the drive 
waveform.  You can use the final drive state to     determine which direction 
the ECAT ultimately heads.  That is, you can     give the ECAT a push toward 
one of those two conditions.  The positive     feedback mechanism takes over 
after that final push and carries the order to     completion.
    


    
Of course, if someone applies super cooling tubes to extract the excess     
heat then the thermal resistance will be reduced.  Enough of this type     of 
cooling could reverse the process.  If sufficient reduction in     thermal 
resistance is achieved, the positive feedback instability can be     defeated.  
If the loop gain becomes less than unity the device would     begin to cool 
toward room temperature.   It is a complicated system     with many subtle 
points to consider.
    


    
There may exist some situations where negative feedback occurs, but     this is 
speculative.  I am fairly confident that a limiting mechanism     must exist 
where the temperature can become no higher.  As this     temperature is 
approached the positive feedback loop gain must become less     than unity.  
When the gain is reduced below unity stable operation     begins and a real SSM 
occurs.  I suspect that any attempt to gain     control by drive alone is 
hopeless at these temperatures and the only way     possible to cool the device 
would be to flush it with coolant.
    


    
Dave
    


    



    
-----Original     Message-----
From: Andrew <[email protected]>
To: vortex-l     <[email protected]>
Sent: Sat, May 25, 2013 12:47 pm
Subject:     Re: [Vo]: ECAT Drive PWM Issues

    
    
    
Dave,
    
 
    
Does this model allow a stable energy production regime to exist when,     
after initiation via initial heating has begun, the device can be run at     
zero input power, and regulation to prevent runaway is achieved by the     
application of sporadic cooling via (say) cooling tubes?
    
 
    
For if the device can indeed be continuously operated at zero (or     indeed 
negative) input power, then one has unambiguously demonstrated the     
production of "something from nothing", and there's no getting away from     
that. 
    
 
    
Andrew
    
      
----- Original Message ----- 
      
From:       David       Roberson 
      
To: [email protected] 
      
Sent: Saturday, May 25, 2013 9:36       AM
      
Subject: Re: [Vo]: ECAT Drive PWM       Issues
      


Fran, my model takes       into account the rate of heat transfer out of the 
device by using a       parameter that simulates a thermal positive feedback 
loop.  And, as       you suggest this depends greatly upon the rate of heat 
generation with       temperature and the thermal resistance that it delivers 
that heat into.        Another way to think of this effect is to consider what 
would happen       to a block of active material which is surrounded by a 
perfect heat       conductor.  In this special case, any additional heat that 
is       generated is immediately absorbed by the conductor and can not raise 
the       temperature of the block.  This would be a stable condition and the   
    COP would be low.  Now, if you modify the surrounding heat conductor       
by increasing its thermal resistance then any newly generated heat from       
within the block would result in an increase in its internal temperature       
in a positive feedback manner.  The resistance can be increased until       it 
reaches a point such that a tiny incremental input of heat to the block       
results in a temperature increase of the block that causes additional heat      
 generation slightly larger than the initial increment.  Rossi appears       to 
operate above this resistance point when his device has the desired       
performance.       


      
That was a lot of words and I suspect is not clearly written.        The meat 
of the description is that there will be a temperature that       depends upon 
the heat sinking where the device becomes unstable and begins       to proceed 
toward melting.  My model suggests that this is the       temperature above 
which Rossi should operate his device to achieve good       COP.   The model 
further indicates that you can maintain control of       the device while 
operating above this point as long as you reverse the       process before a 
second temperature trip point is reached that leads to       run away.  It is 
important to realize that operation within this       region is unstable unless 
a drive waveform is applied with the proper       characteristics.
      


      
In the radio world this type of device would be referred to as a       negative 
resistance component.  Rossi must be relying upon the energy       generated in 
this mode for his large gain.  The hard part is to keep       the ECAT from 
getting out of control since he is operating on a sharp       balance to obtain 
good COP.
      


      
I am not modeling any process that occurs beyond the two temperature       
trips that I described since operation above the second one is       
destructive.  Operation below the first temperature point results in       a 
COP that is too low to be useful.  I have included energy loss due       to a 
4th order radiation process in some of my runs, but so far I find       that 
control issues occur before this has significant effect.
      


      
I believe as you do that operation with a heat exchange fluid will be       
easier to control.  This also allows Rossi to adjust the flow rate       which 
could be used to modify the thermal resistance factor and thus total       loop 
dynamics.  For example, he could raise the temperature at which       the core 
become unstable thereby compensating for different core       activities.
      


      
My model operates upon the average behavior of an ECAT type device.        It 
assumes that the design has been developed by good engineering       processes. 
 If the design team allows the system to harbor       inconsistent heat 
transfer such as would occur with too many and too large       in size hot 
spots, then there is no control technique that will work       effectively.  I 
suspect that much effort will center around making       sure this issue is 
handled.
      


      
Dave


      
-----Original       Message-----
From: francis <[email protected]>
To:       vortex-l <[email protected]>
Sent:       Sat, May 25, 2013 7:16 am
Subject: re: [Vo]: ECAT Drive PWM       Issues

      
      
      
      
Dave, I think you we are both in agreement with the       initial post of Ed’s 
thermal analysis, 
http://www.mail-archive.com/vortex-l%40eskimo.com/msg80803.html        but it 
does not mention the difference between the destructive test       in open air 
and the unit in normal operation which is constantly bathed in       a heat 
extracting fluid.. are you modeling this in your SPICE calculation?       The 
thermal circuit in the destructive test only has air cooling to keep       the 
runaway at bay and represents a softer – more fragile target for the       
waveforms to temporarily exceed while I think the reactor in heavy        heat 
sinking mode would have much higher tolerance for controlled        PWM 
excursions into areas that would be considered runaway if not       for the 
steady drain.
      
Fran
      
 
      
[Vo]: ECAT Drive PWM Issues 
      
David Roberson Fri, 24 May 2013 23:30:52 -0700 
I was adjusting my spice model of the ECAT when I decided to determine how 
important it is to keep the device operating within the normally unstable 
region at all times.  Here I refer to the unstable region as that operation 
range where the ECAT would tend toward over heating unless under control.
 
There is no end to the questions which keep arising as to how heat can be 
applied in the proper format to keep an unstable device operating under control 
when it is capable of putting out more heat than required to drive it.   And, 
the ECAT tends to operate best when the COP is equal to 6 which clearly is 
within this mode.
 
One day this will be accepted.  For now, I want to mention that it is important 
to keep the ECAT operating near the ultimate thermal run away region.  If the 
device temperature is allowed to drop too far before the drive returns then the 
COP degrades significantly.  And, as is somewhat demonstrated by the waveforms 
shown in the recent report,  the length of time that the temperature hesitates 
at its greatest level is determined by how  by Coupon Companion" 
id="_GPLITA_0"close to that ultimate run away 
temperature the device operates.
 
My test runs demonstrate that the ECAT needs to be operating at a maximum 
temperature near to its ultimate thermal run away point and that the variation 
in output temperature needs to be maintained low by timing of the PWM drive.
 
Both of these requirements should be met if the ECAT is to deliver the desired 
COP of 6 and remain stable.  My spice model offers good guidance even though it 
can only approximate a real device.
 
Dave
      
 








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