I thought this would add a little more info:
It was posted by Romo (i hope you don't mind ) and I think it falls in line with what Armagdn03
Sorry in advance for the long post
It was posted by Romo (i hope you don't mind ) and I think it falls in line with what Armagdn03
Originally posted by petar113507
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I have been looking where to fit this information into some of these connective, integrative topics.
Dave, thank you for giving me the oppourtunity to do so.
I have recently scanned a book called "Dielectric breakdown in solids". I hope some of this will be useful for your experiments.
Title page:
As you can see in the table of contents -- I have highlighted some of the topics which simply snagged my attention.
Earlier in the day I was musing over several high voltage phenomena -- and stumbled upon this book by "chance". (I was on autopilot, my focus remaining on the high voltage phenomena -- and I found my feet leading me to the shelf, where the books gold lettering caught my attention)
I would not consider this chance -- that I have found some suggestions and answers to the exact questions which I have desired to understand. Perhaps we can also discuss (elsewhere?) the mental state that al humans can remain in, to "attract" the answers that they seek.
Table of contents:
Thermal Breakdown:
Few things struck me here -- Even higher oscilations than our current electromagnetic spectrum "dampen". Heat is just a wave in the EM spectrum. Higher frequnencies than we can measure can be "recieved" to create EM oscilations. This sounds a lot like tapping into cosmic (read: higher) frequencies with superconductors.
Note: Too quick of alternating currents don't let the dielectric "relax" -- and dissapate heat as waste. Pulse DC too quickly, and it behaves the same as AC. More hints in the book are on this later -- effectively telling me why I need a sharp rise/fall, rapid (microsecond) DC pulse.
When dielectric breakdown ocurrs the "random" breakdown paths, mean that we don't know how to predict where the breakdown goes. Interesting discharge paths in pictures on the left page.
"High frequency" means smaller waves. that tells me that when you have a sharp/fast enough impulse, temperature does not rise as much in the dielectric (wasted energy into heat).
In frohlich's theory...
When the electric voltage potential below the critical value, the "probabillity" of getting "fast electrons" (Electron avalanche = Energy gain). Seeing the energy gain only happens after a critical voltage level has been reached. (Critical voltage level = phase transition into plasma?)
"fast electrons" do not produce heat -- thermal ionization (heat) lags behind.
We should be able to keep the dielectric cold. Cold, means the dielectric is not damaged by thermal decay -- which means we should be able to strike it for repeated energy gains.
AC -- maximum stable temperature
DC -- "infinite" temperature -- as long as it is confined within a small enough space. The average temperature seems normal.
Dielectric becomes a semi-conductor under AC -- Same conditions as DC
The hottest part of the temperature gradient must change more sharply
This tells me what is happening during that unidirectional DC pulse at the apex of the sharp wave gradient.
This confirms (one of many confirmations) what bearden/bedini have been saying about "the spike". When we average values over time -- it seems "normal/linear" -- but during short impulses, we have non-linear situations happening on a small scale.
Theoretically infinite = non linear
Thermal breakdown happens in AC at a "lower value" because the difference between the voltage fluxuations still reach the "critical value" for breakdown to happen.
======================
I see that under conditions of dielectric breakdown -- in discreet unidirectional DC pulses, you create for a fraction of a second -- a plasma, or "superconductor" which receives frequencies at the highest (or above) our current EM spectrum -- Producing a large pulse of energy, and the dampening oscilations ocurring thereafter can produce use-able OU energy.
Dave45, I can find the exact post tomorrow, but 'powerme' suggested a very similar setup to produce dielectric breakdown in a silicon/metglass torrid.
Dielectric breakdown can be induced by only voltage potential -- making that caduceus/pancake coil seem like a good lead.
========================
Will finish posting parts of this book tomorrow.
Glad to be enlightened by other sincere perspectives,
==Romo
========================
Dave, thank you for giving me the oppourtunity to do so.
I have recently scanned a book called "Dielectric breakdown in solids". I hope some of this will be useful for your experiments.
Title page:
As you can see in the table of contents -- I have highlighted some of the topics which simply snagged my attention.
Earlier in the day I was musing over several high voltage phenomena -- and stumbled upon this book by "chance". (I was on autopilot, my focus remaining on the high voltage phenomena -- and I found my feet leading me to the shelf, where the books gold lettering caught my attention)
I would not consider this chance -- that I have found some suggestions and answers to the exact questions which I have desired to understand. Perhaps we can also discuss (elsewhere?) the mental state that al humans can remain in, to "attract" the answers that they seek.
Table of contents:
Thermal Breakdown:
Few things struck me here -- Even higher oscilations than our current electromagnetic spectrum "dampen". Heat is just a wave in the EM spectrum. Higher frequnencies than we can measure can be "recieved" to create EM oscilations. This sounds a lot like tapping into cosmic (read: higher) frequencies with superconductors.
Note: Too quick of alternating currents don't let the dielectric "relax" -- and dissapate heat as waste. Pulse DC too quickly, and it behaves the same as AC. More hints in the book are on this later -- effectively telling me why I need a sharp rise/fall, rapid (microsecond) DC pulse.
When dielectric breakdown ocurrs the "random" breakdown paths, mean that we don't know how to predict where the breakdown goes. Interesting discharge paths in pictures on the left page.
"High frequency" means smaller waves. that tells me that when you have a sharp/fast enough impulse, temperature does not rise as much in the dielectric (wasted energy into heat).
In frohlich's theory...
When the electric voltage potential below the critical value, the "probabillity" of getting "fast electrons" (Electron avalanche = Energy gain). Seeing the energy gain only happens after a critical voltage level has been reached. (Critical voltage level = phase transition into plasma?)
"fast electrons" do not produce heat -- thermal ionization (heat) lags behind.
We should be able to keep the dielectric cold. Cold, means the dielectric is not damaged by thermal decay -- which means we should be able to strike it for repeated energy gains.
AC -- maximum stable temperature
DC -- "infinite" temperature -- as long as it is confined within a small enough space. The average temperature seems normal.
Dielectric becomes a semi-conductor under AC -- Same conditions as DC
The hottest part of the temperature gradient must change more sharply
This tells me what is happening during that unidirectional DC pulse at the apex of the sharp wave gradient.
This confirms (one of many confirmations) what bearden/bedini have been saying about "the spike". When we average values over time -- it seems "normal/linear" -- but during short impulses, we have non-linear situations happening on a small scale.
Theoretically infinite = non linear
Thermal breakdown happens in AC at a "lower value" because the difference between the voltage fluxuations still reach the "critical value" for breakdown to happen.
======================
I see that under conditions of dielectric breakdown -- in discreet unidirectional DC pulses, you create for a fraction of a second -- a plasma, or "superconductor" which receives frequencies at the highest (or above) our current EM spectrum -- Producing a large pulse of energy, and the dampening oscilations ocurring thereafter can produce use-able OU energy.
Dave45, I can find the exact post tomorrow, but 'powerme' suggested a very similar setup to produce dielectric breakdown in a silicon/metglass torrid.
Dielectric breakdown can be induced by only voltage potential -- making that caduceus/pancake coil seem like a good lead.
========================
Will finish posting parts of this book tomorrow.
Glad to be enlightened by other sincere perspectives,
==Romo
========================
Sorry in advance for the long post
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