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 <andrew...@att.net>
To: vortex-l <vortex-l@eskimo.com>
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: vortex-l@eskimo.com 
  
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 <froarty...@comcast.net>
To: vortex-l   <vortex-l@eskimo.com>
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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