I know of no single paper that describes how cracks are formed. However, a huge 
literature exists that describe how cracks are produced in materials and how 
this destructive process can be avoided. I have 69 papers in my collection that 
address this issue.  Unless you are prepared to do a lot of study, an answer to 
your question is not easy to supply.

Ed Storms
On Mar 22, 2014, at 1:39 PM, James Bowery wrote:

> Is there a paper describing the technique(s) for generating a wide 
> distribution of crack sizes?
> 
> 
> 
> On Sat, Mar 22, 2014 at 2:11 PM, Edmund Storms <[email protected]> wrote:
> Tritium can not be detected easily using a beta detector. The best way is to 
> convert the gas to water and measure the tritium using the scintillation 
> metaod. The allows the sample to be studied over a period of time by many 
> people if they wish. 
> 
> Ed Storms
> 
> On Mar 22, 2014, at 1:02 PM, James Bowery wrote:
> 
>> Perhaps I can illustrate by avoiding thermal detection and going with 
>> tritium:
>> 
>> Since tritium production is inherently time integrated, setting up a Cravens 
>> style dual experiment with a one treated to have a wide range of crack 
>> sizes, and both identical in all other respects, puts the primary cost 
>> constraint on the beta-emission counter.  Can such counters be made 
>> economical?
>> 
>> 
>> On Sat, Mar 22, 2014 at 1:56 PM, James Bowery <[email protected]> wrote:
>> Ed, I'm attacking a different problem:  Cost.
>> 
>> Since we're in a quasi-Edisonian phase of scientific research, keeping the 
>> cost per experiment as low as possible seems to be the bottleneck to getting 
>> a protocol that has reproduces the FPE to any statistically significant 
>> degree.
>> 
>> Developing a different kind of experimental set up may be the key.
>> 
>> 
>> On Sat, Mar 22, 2014 at 1:47 PM, Edmund Storms <[email protected]> wrote:
>> James, I feel much more comfortable using a calorimeter design I can trust 
>> and that has been used in the past. The Cravens device is a nice 
>> demonstration but it proves nothing. I have made calorimeters that do the 
>> job much better and give absolute values for power.  No need exists to 
>> reinvent. 
>> 
>> Ed Storms
>> 
>> On Mar 22, 2014, at 12:27 PM, James Bowery wrote:
>> 
>>> If you are running a Cravens style simultaneous, colocated control 
>>> experiment with infinite COP your odds of detecting a tiny temperature 
>>> difference economically are vastly improved.  Basically you just integrate 
>>> the voltage out of a bimetallic (thermocoupling) wall separating the 
>>> treated material from the untreated material in a common vessel that 
>>> provides a small amount of gas communication between the chambers for 
>>> pressure equalization.  This is not an expensive device.
>>> 
>>> 
>>> On Sat, Mar 22, 2014 at 12:46 PM, Edmund Storms <[email protected]> 
>>> wrote:
>>> Yes, getting a wide variety of sizes is easy. Getting enough of the right 
>>> size in this distribution is the problem. Only a few of the right size will 
>>> not give enough energy to be detected. When radiation or tritium is used to 
>>> detect the occurrence of LENR, the effect can be seen using fewer active 
>>> sites.  However, these methods have not been used very often, probably 
>>> because the tools and skill are not common.
>>> 
>>>  Cracks either want to grow larger or sinter and disappear.  As a result, 
>>> production of LENR is unstable.  This makes the effect occur for brief 
>>> times, but not long enough to be sure LENR is actually happening rather 
>>> than a random event. 
>>> 
>>> Ed Storms
>>> 
>>> On Mar 22, 2014, at 11:28 AM, James Bowery wrote:
>>> 
>>>> 
>>>> 
>>>> 
>>>> On Sat, Mar 22, 2014 at 11:35 AM, Edmund Storms <[email protected]> 
>>>> wrote:
>>>> 
>>>> Based on my theory, the active material are nano-cracks. Making these at 
>>>> the require size is the challenge. Cracks can be made many different ways, 
>>>> but getting the right size is the problem.
>>>> 
>>>> Might there be a technique that generates a wide distribution of crack 
>>>> sizes? 
>>>> 
>>> 
>>> 
>> 
>> 
>> 
> 
> 

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