Ed--Bob Here--

I would note that testing by the manipulation of spin is possible by changing 
the static magnetic fields or the oscillating fields given known nuclear 
magnetic resonance parameters.  You suggest that energies associated with spin 
are not found to involve the magnitude of energy involved.  Who determined this 
situation?  Is there a reference supporting  this conclusion other that mere 
assertion?   


I know of Japanese researcher data regarding the formation of various heavier 
isotopes after forcing  D gas through thin films.  However, I am not familiar 
with the data you suggest for the splitting of Pd and Ni.  A couple references 
would be good.

When do you expect to finish your book on the subject?  If you have a partial  
bibliography of references, maybe that would give me the pertinent leads.  

Bob Cook


  ----- Original Message ----- 
  From: Edmund Storms 
  To: [email protected] 
  Cc: Edmund Storms 
  Sent: Saturday, February 08, 2014 7:12 AM
  Subject: Re: [Vo]:MIT Course Day 5 -- NiH Systems


  Bob, we are presented with a complex puzzle. A solution requires testing 
possibilities against what is observed. A solution is made difficult if 
mechanisms are proposed that can not be tasted. For example, spin coupling can 
not be tested against what is known and, in addition, it is not found to 
involve the magnitude of energy involved. KThe human mind can imagine an 
infinite number of possibilities. Some way must be used to limit these 
possibilities.


  I do this my making as few assumptions as possible and then limit these to 
the most basic possibilities. If this approach fits the data, then we have the 
answer. If the data are not fit, then additional assumptions are added only 
where absolutely necessary as exceptions. 


  To start, you need to stop thinking of the LENR process as being caused by 
ordinary nuclear reactions. For example cross-section data have no application. 
This data is based on use of high energy particles for which a reaction rate is 
determined as this energy is changed. This process does not happen during LENR. 
If this process were operating, LENR could not happen. In fact, rejection of 
the claim results because this kind of thinking is used. We are dealing with a 
new kind of nuclear reaction. The challenge is to discover the rules that apply 
to this reaction, not keep using rules that apply to conventional reactions. 
The rules of conventional reactions make LENR impossible. 


  The data show that Pd and Ni split into smaller parts.  This data results 
from hundreds of studies and is not in doubt. This fact is the starting point 
for a search for an explanation. The first assumption results from the need to 
have something cause this result. That event is assumed to be addition of 
either one or more d or p to the nucleus by some unknown process, followed by 
fragmentation. Such a process requires the number of p and n in the initial 
nucleus to equal the total number in the fragments.  As a result, if 2d entered 
the Ni, the fragments would have to contain a total of 30 p. This limits the 
element combinations that can result. Such calculations can be called nuclear 
chemistry because the same rule applies to chemical reactions. 


  In the case of nuclear reactions, unlike chemistry, the number of neutrons 
also has to remain unchanged. Each isotope of an element has a different number 
of neutrons.  Therefore, different isotope combinations  are possible.  At this 
point, we need one more assumption. This assumption says the isotope 
combination must always be non-radioactive, because that is what is observed 
most of the time. When this assumption is applied, the combinations are further 
limited, with some isotopes of Ni having many element combinations and some 
having only a few possibilities.  The periodic table can be searched to 
discover which elements between He and Ni satisfy these two conditions.  I have 
done this and obtained a distribution. This distribution matches what is 
observed.  Therefore, the two assumptions appear to be correct. Once this 
information is obtained, the energy from each reaction can be calculated along 
with the frequency of each reaction, with no other assumptions being required. 


  So you ask how the d or p got into the Ni nucleus. This is a separate 
question requiring different assumptions.  First, energy must be available and 
it must be applied at the time and place where the nuclear event occurs. In 
addition, this energy must have a form that does not interact with the 
surrounding chemical structure. This requirement is unique to LENR, unlike what 
can happen in plasma.  I propose a structure forms I call a Hydroton in which 
the fusion process takes place. This reaction, and only this reaction, has 
enough energy to overcome the Coulomb barrier for Ni or Pd.  This fact further 
limits what can be proposed to happen.  Of course, a person can imagine all 
kinds of novel quantum process that might operate, but these can not be tested 
and they all conflict with basic natural laws, which I will not explain here. 


  I can test the consequence of the fusion reaction using the method applied  
above. I can add one or more d to the Ni or I can add one or more p. It turns 
out adding 2 d fit the observations. The question is, what kind of fusion 
reaction can generate two d?  This can only happen as a result of a p-e-p 
reaction.  Having 2d enter means the Ni had to be attracted to two Hydrotons, 
each of which produced and added 1d.  


  Here we have used a few basic assumptions to explain transmutation and to 
describe the fusion reaction by showing how they are connected. No additional 
assumptions are required and no novel or untestable processes have to be 
suggested. This is how, I suggest, LENR be explored. If this approach is used, 
LENR can be explained and all the previously unexplained behavior makes sense. 
That is what I'm attempting to do in the book.  No math is required. Only 
knowledge of what has been observed, simple logic, and knowledge of basic 
chemistry and nuclear behavior is required. The lesson is keep it simple and 
basic. KISABS


  Ed Storms



    Ed--Bob Cook here

    Spin states of a quantum system reflect the angular momentum of the system 
and hence the energy associated with that angular momentum.  High spin quantum 
numbers reflect the higher energy of the system.  The allowable states are 
quantized.  In magnetic fields the direction of the spin is controlled more or 
less depending upon the field strength.  The allowable number of states is 
reduced from the situation where there is no magnetic field.  Resonant magnetic 
oscillating fields input to a nucleus with a magnetic moment and non-zero spin 
state for  its ground state, can add energy to the quantum system by changing 
the spin number of the quantum system.  This is the basis for the MRI 
technology which is an accounting of the energy absorption  at a given 
resonance frequency at well determined locations, identifying the nucleus with 
the specific resonance frequency absorption .       

     If there is spin coupling, (a basic assumption is that spin is conserved 
in any nuclear reaction at the end of the reaction)  a coupling between various 
 particles subject to integer, J, quantum seems probable.   Thus, any He-4* 
with a high spin integer J quantum number and excess energy--say 10 mev--would  
distribute this high angular momentum to  electrons or other particles in the 
quantum system--all the many electrons  and particles at the same time.  The 
electrons (and other particles) in turn would distribute their excess spin 
energy (angular momentum) to the lattice as electromagnetic field oscillations 
or  radiation and hence lattice heat.  In the end the net spin would be what it 
was to start with.  The reaction would be fast and cause results of the 
distribution of quantum angular momentum and lattice motion instantaneously.   
No energetic (kinetic energy) particles are  involved, only angular momentum 
with its corresponding rotational energy.  The rotational energy may actually 
be rotating electric and or magnetic fields associated with the particle with 
the high spin quantum state. 

    Again I do not understand the details of spin coupling, the actual timing 
nor the most likely fractionation of the spin/angular momentum among the 
particles of the quantum system.  The basic idea is that the energy associated 
with the mass loss first shows up as angular momentum or spin of the newly 
found He-4*  and this spin is distributed to the rest of the system.     

    Bob Cook



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