Come to think about it, the High School reactor also uses a stark discharge
into a liquid emulation of random diameter tungsten micro/nano powder and a
potassium salt. They claim a COP of 4.**

* *


On Wed, Jul 10, 2013 at 2:16 PM, DJ Cravens <djcrav...@hotmail.com> wrote:

> ?? yes it produces sparks or arcs or discharge....  I am not sure of the
> technical variations.
> I am using a modified strobe light circuit. I cannot see into the "good"
> brass sphere.  I do have a cut away mockup of the sphere (I will have that
> with my demo).  The terminal ending moves among the various locations.
> Most of the time the "sparks" terminate on one of the metal containing
> carbon particles. They are "higher" than the binder that holds them.
>
> There is a little more to it than that- actually the lower half of the
> sphere has an internal insulation layer to help it from too much heat loss,
> a conductive connection between the brass sphere and the conductive binder
> holding the particles.  The upper half is "empty" or should I say filled
> with gas so there can be convection movement of the gas.  One think I did
> learn from Les Case is that there must be convection or flow of H through
> the material, or mixing of the powders in the gas.
>
> (note: as mentioned in some of my earlier post, I am using "mesopore"
> carbon to contain my metal host lattice - which is a "doped" metal to lower
> its E of vac. formation - I have not bought into the transmutation of
> Nickel idea and am using mostly D not H)
>
> The sphere I will have at the NI demo is "self sustaining" at low power.
> But only when brought up in temp.  I will be holding it at 75C in an Al
> bead dry bath. You can compare its temp to the control sphere.
>
> I hope to have one infinite COP (the spheres in a constant temp bath)
> device and a low COP higher power device. I will be lucky to get to 1.33.
> I have not evaluated the COP level for that one.  Again, it is just for the
> unwashed masses and not as a science item to produce data.
>
> It took me a while to figure out something visual for the public to show
> heat production and compare it to a control.  Something that does not
> require any calculation- just comparisons.  (but yes, a passerby could put
> on a clamp amp meter if they enjoy that kind of thing.)
>
> I know it will tick of Jed, but it is just for fun and to stimulate public
> interest in the field - nothing more.
>
> D2
>
> ------------------------------
> Date: Wed, 10 Jul 2013 13:28:09 -0400
>
> Subject: Re: [Vo]:DGT or ECAT? Same Process?
> From: janap...@gmail.com
> To: vortex-l@eskimo.com
>
>
> *Yes, think of the plasma globe type lights.  I have a central electrode
> (actually W rod held by a Cu tube).  It is within a brass sphere holding my
> material. But the material is only "stuck" to the lower half on the wall.
> *
> **
> *If this info is not closely held, does this electrode produce a spark?
> If not what does it do?*
>
>
> On Wed, Jul 10, 2013 at 10:42 AM, DJ Cravens <djcrav...@hotmail.com>wrote:
>
>
>
> ------------------------------
> To: vortex-l@eskimo.com
> Subject: Re: [Vo]:DGT or ECAT? Same Process?
> From: dlrober...@aol.com
> Date: Tue, 9 Jul 2013 22:38:55 -0400
>
> That is very interesting Dennis.  If I understand you correctly, you solve
> the thermal run away problem by extracting heat fast enough to keep the
> thermal positive feedback loop gain below unity.  That should work provided
> there is enough energy released per pulse of drive to achieve a high enough
> COP.
>
> *Yes, that is the way I look at it.  You can get large COP at lower
> outputs and lower temps.  For example I have a small unit with no sparking
> that has infinite COP but only fractional watts of excess. *
>
> The behavior that you describe would not depend upon very much gain being
> augmented by thermal feedback as I suspect that Rossi is relying upon.  Do
> you understand why a spark would be so efficient at producing LENR?  You
> mention local heating as a possible factor, which certainly could cause
> small hot regions to develop.  Is this the key to high gain without
> meltdown?
>
> *There must be a thermal path out of the region to take away the heat at
> the right "speed".  I assume that that could be done by adjusting the
> particle size and "packing", but in my case, the metal host occupies pores
> within carbon.  *
>
> Once a hot spot is initiated, what prevents the heat from spreading
> rapidly into the adjacent material and causing a sudden extreme burst of
> energy?  Perhaps the distribution of active hydrogen in the NAE is such
> that areas capable of spreading the heat only exist in small patches and
> are easy to extinguish.  If this is true, new active regions would need to
> form in time to take over the process as others die out.
>
> *Again, I believe the rates have an exponential them. coef.  Notice in my
> case the active regions are isolated via the carbon.  So as the heat
> spreads other regions would not be at as high a temp. and have a much lower
> heat production rate.  The slowly extinguish as the spark moves to other
> regions*.
>
> So what functions does the spark perform in a system of this type?
> Heating of a small region makes a great deal of sense as each spark strikes
> the surface.  Also, do you expect that the spark breaks apart the hydrogen
> molecules as a second function?  I can imagine a rain of protons falling
> upon the metal due to ionization as another possible piece of the puzzle.
>
> *The spark just causes very high local temps. I don't really see the
> spark functioning to ionize the H (my case D and H).  I think it is the H
> already in the lattice that reacts.*
>
> Has there been evidence of enhanced reaction caused be the magnetic field
> associated with the currents entering or leaving the metal surfaces?  If I
> recall, DGT speaks of dipole behavior of Ryndberg hydrogen helping out.
> Can you describe any evidence of this?
>
> *Yes, it seems that the reaction is almost linear in respect to the B
> field.  (also linear with mass, and expon. in terms of Energy of vacancy
> formation.  (that is why Ag helps Pd system and Cu and Pd .....  helps Ni
> systems.)  I believe that the H occupies or must move through the
> vacancies. The occupation of H in a vacancy is likely in a controlling
> pathway. *
>
> Your bowl shaped targets are quite interesting to consider.  Does the bowl
> tend to spread out the spark contact region?
>
> *Yes, think of the plasma globe type lights.  I have a central electrode
> (actually W rod held by a Cu tube).  It is within a brass sphere holding my
> material. But the material is only "stuck" to the lower half on the wall.
> *
>
> From what you describe it appears that your reaction is almost entirely a
> surface effect.  Would you expect a very thin layer of active metal to work
> in the same manner?  A thin coating layered upon another passive metal
> might be helpful in preventing a large scale thermal event.  Maybe one of
> Axils heat pipes underneath could extract the heat quickly enough to
> enhance the net energy density.
>
> *Yes, one configuration (I have 4) has variable heat conductive heat
> pipes.  I have to juggle the heat extraction and production. (changes
> contact areas)*
>
> Do you have to worry about the destruction of your active material as the
> process operates?
>
> *If I "turn it up" to much my material is destroyed.   In one device, I
> use internal B fields (added Sm 2 Co 17 powder) and it will demagnetize. *
>
> Are you planning to demonstrate one of your devices at the conference?
>
> *At NI Week (Booth 922).  It will be just a "golly gee" type of demo not
> a science "prove it" demo.  Small in the few watt range. I hope to be
> upstaged by Defkalion.  *
> * *
> * *
> Dave
>  -----Original Message-----
> From: DJ Cravens <djcrav...@hotmail.com>
> To: vortex-l <vortex-l@eskimo.com>
> Sent: Tue, Jul 9, 2013 9:29 pm
> Subject: RE: [Vo]:DGT or ECAT? Same Process?
>
>
> My take on their process is that the control and the sparks are related to
> the positive heat coef. of the reaction and the rate at which the heat is
> extracted.
>
> My best empirical model shows an almost exponential increase in max power
> output with temperature (due to vacancy production).  A few very hot
> regions can produce a large fraction of the output.
>
> My reoccurring problem is to balance the temperature of the reaction
> species with the rate at which I remove the heat.   You remove too much
> heat and the reaction sites cool down and the reaction slows.  Most
> people seem to be looking at the global average temperature of the bulk and
> not the temperatures of local areas.  By sparking to your sample you can
> have very high local temperatures and thus higher local reaction rates, IF
> your material is such that its resistivity increases with temperature.  Notice
> this is the case for most metals.  Since the sparks target the paths with
> greatest conductivity, the sparks are to new regions with lower
> temperatures and lower resistance.  i.e. you hit new regions.  I believe
> that they are basically sparking to a flat area within a cylinder.  I
> prefer to use a spark into a bowl shaped target.
>
> You just simply make sure that your heat flow out of the system is large
> enough to stop any runaway reactions. (you are also saved by the 4thpower law)
>  For my system, it is a balancing act between heat production and heat
> transfer out of the system.  I do that by both having a variable heat
> conductive path (variable contact areas by turning- think variable air
> caps) for rough tuning and then changing the spark rate (I use a strobe
> circuit).
>
>
>  Dennis
>
> ------------------------------
> To: vortex-l@eskimo.com
> From: dlrober...@aol.com
> Date: Tue, 9 Jul 2013 18:39:06 -0400
> Subject: [Vo]:DGT or ECAT? Same Process?
>
>  Whenever I read about the DGT device I get the impression that it
> behaves much differently than the ECAT.  The main difference I focus upon
> so far is the *method of control.*  We have discussed the ECAT thermal
> positive feedback control on many occasions and have developed models that
> appear to explain its operation.  The same is not yet true for the DGT
> beast.
>
> Thermal control such as that used by Rossi seems to have difficulty
> achieving a stable COP of 6 for the basic device excluding electrical power
> generation and feedback.   Of course it is expected that one will be able
> to use the fed back electrical power to drive the device one day and
> achieve a net COP of infinity.  This should become possible fairly soon and
> Rossi appears to be working hard to arrive at a reasonable design.
>
> DGT suggests that they potentially can already obtain a large COP, but I
> have questions about the design since little has been demonstrated in
> public.  My reservations can easily be disposed of by additional
> information and I anxiously await that time.
>
> The spark plug like ignition system of the DGT animal bears little
> resemblance to the thermal operation of Rossi's ECAT.  I have the suspicion
> that there is something important to be learned by the fact that these
> various devices both function.  How can that be?  What is it about the DGT
> design that appears to efficiently use the spark induced reactions while
> maintaining excellent control?  We certainly are not interested in hot
> fusion products which tend to be associated with high voltages such as
> spark discharges.  If acceleration due to high voltage is present then why
> does this not occur?  Does DGT balance the spark magnitude carefully enough
> to avoid this fate while achieving adequate LENR activity?
>
> I want to learn from the DGT device as well as the ECAT.  There appears to
> be an understanding among most of us that some form of NAE is present which
> allows LENR to proceed, but what form does it take?  Is it the same for
> both designs?  What does the spark of DGT offer that heat alone seems to
> neglect in the ECAT?  It seems as if the ECAT would love to thermally run
> away without much provocation while the DGT device does not seem to exhibit
> that behavior.  Perhaps DGT has done a good job of hiding this problem, but
> they offer information that suggests that this is not happening with their
> design.  I find the description that the DGT design can be turned on and
> off rapidly to potentially find applications that are diverse such as
> transportation, the gold standard of mine as evidence.  If thermal run away
> were a major issue, then the rapid control might not be so easy to
> demonstrate.
>
> From the information that I have gleaned, both systems appear to offer
> excellent energy density and good power output.  This is extremely
> important for future applications.  It will be interesting to witness the
> race between these two horses in the near future.  Of course, others might
> enter the fray soon and we all will benefit it that occurs.
>
> I realize that I have touched upon a multitude of interesting issues in
> this post and I hope that some of our esteemed members can add important
> information to the discussion.  And if the answers to some of my questions
> appear, then that would be fantastic.
>
> Dave
>
>
>

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