Re: [Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-28 Thread Alan Fletcher
Most of the audio is just reading from the slides, with little extra 
information.


Questions at the end were mostly to do with the nickel .. purity, 
surface area, power density. There were no pulses applied to the 
nickel wires : the only controls are the heater temperature and gas 
pressure, which were stepped up and then left stable for days.


A few comments on gamma (etc) .. with the response : come to JCF 15 
!  (Nov 2014)


I would have asked if the 1kW (Scarlet) and 10kW (Catherine) were 
actually working. 



Re: [Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-28 Thread Jed Rothwell
Alan Fletcher a...@well.com wrote:


 I would have asked if the 1kW (Scarlet) and 10kW (Catherine) were actually
 working.


I do not think they are working yet. The equipment actually exists, as you
see from the photos, but I do not think they have tested them yet. Before I
got the photos I asked Mizuno do you really plan to test a 10 kW reactor?
He said, yes. I think he would have said if he had already tested it.

My wife does not think much of naming reactors with English female code
names. I was surprised to see such names.

- Jed


[Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-27 Thread Jed Rothwell
Finally! The slides are here:

http://lenr-canr.org/acrobat/YoshinoHreplicable.pdf

I will replace a few of the graphs that still have Japanese text in them
later.

- Jed


Re: [Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-27 Thread Ruby

Thank you Jed, I have added your version to the Audio files page:

http://coldfusionnow.org/2014-cflanr-colloquium-at-mit-audio-files/

Ruby


On 3/27/14, 7:40 AM, Jed Rothwell wrote:

Finally! The slides are here:

http://lenr-canr.org/acrobat/YoshinoHreplicable.pdf


--
Ruby Carat
r...@coldfusionnow.org
Skype ruby-carat
www.coldfusionnow.org




Re: [Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-27 Thread David Roberson
Thanks Jed.  I reviewed the slides and find them most interesting.  Slide 23 
shows the metal after activation.  Does the HV discharge lead to bubbles or are 
the visible structures holes left in the metal?  Could bubbles be a result of 
local melting of the nickel followed by surface tension drawing the molten 
metal into blobs?  This is a process that I am not familiar with and perhaps 
someone might explain the structure.


Also, how critical is the amount of electrical energy released during each 
discharge?  Does too much energy lead to bumps that are too large?  Likewise, 
would too little energy cause the structures to cease to form?  Of course I 
have to wonder how consistent the surface features are among the many mesh 
particles.  Here, I am curious about how the inner particles are effected by 
the discharge when they are shielded by the outer ones.



Dave



-Original Message-
From: Jed Rothwell jedrothw...@gmail.com
To: vortex-l vortex-l@eskimo.com
Sent: Thu, Mar 27, 2014 10:41 am
Subject: [Vo]:Yoshino slides from 2014 MIT Colloquium



Finally! The slides are here:


http://lenr-canr.org/acrobat/YoshinoHreplicable.pdf



I will replace a few of the graphs that still have Japanese text in them later.


- Jed






Re: [Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-27 Thread Axil Axil
This surface preparation very similar to what Piantelli does to the surface
of his nickel bars.

Polaritons will be localized in a vortex by either cavities or bumps or
both. This is called Anderson localization.

http://en.wikipedia.org/wiki/Anderson_localization


On Thu, Mar 27, 2014 at 1:15 PM, David Roberson dlrober...@aol.com wrote:

 Thanks Jed.  I reviewed the slides and find them most interesting.  Slide
 23 shows the metal after activation.  Does the HV discharge lead to bubbles
 or are the visible structures holes left in the metal?  Could bubbles be a
 result of local melting of the nickel followed by surface tension drawing
 the molten metal into blobs?  This is a process that I am not familiar with
 and perhaps someone might explain the structure.

  Also, how critical is the amount of electrical energy released during
 each discharge?  Does too much energy lead to bumps that are too large?
  Likewise, would too little energy cause the structures to cease to form?
  Of course I have to wonder how consistent the surface features are among
 the many mesh particles.  Here, I am curious about how the inner particles
 are effected by the discharge when they are shielded by the outer ones.

  Dave



 -Original Message-
 From: Jed Rothwell jedrothw...@gmail.com
 To: vortex-l vortex-l@eskimo.com
 Sent: Thu, Mar 27, 2014 10:41 am
 Subject: [Vo]:Yoshino slides from 2014 MIT Colloquium

  Finally! The slides are here:

  http://lenr-canr.org/acrobat/YoshinoHreplicable.pdf

  I will replace a few of the graphs that still have Japanese text in them
 later.

  - Jed




Re: [Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-27 Thread Alain Sepeda
It remind me some reports of tritium being produced then consumed...
experiments in BARC ?

result are strange... interesting.


2014-03-27 15:40 GMT+01:00 Jed Rothwell jedrothw...@gmail.com:

 Finally! The slides are here:

 http://lenr-canr.org/acrobat/YoshinoHreplicable.pdf

 I will replace a few of the graphs that still have Japanese text in them
 later.

 - Jed




Re: [Vo]:Yoshino slides from 2014 MIT Colloquium

2014-03-27 Thread Jed Rothwell
I uploaded a new version with some minor changes.

- Jed