Low Energy Nuclear Reactions on the Cathode
- f a Chemical Cell
New Energy Times Archives
Low Energy Nuclear Reactions on the Cathode of a Chemical Cell New - - PowerPoint PPT Presentation
Low Energy Nuclear Reactions on the Cathode of a Chemical Cell New Energy Times Archives A. Widom Y.Srivastava S. Sivasubramanian E. Del Giudice G. Vittiello D. Cirillo R Germano, V. Tontodonato New Energy Times Archives Contents:
New Energy Times Archives
Y.Srivastava
R Germano,
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Bulk Water is a Fluid Colloidal Suspension
Floating Within a Background of Normal Water with no Net Ordered Polarization.
Skim Milk is a Dilute Colloidal Suspension
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Interfacial Water is a Liquid Crystal Ferro- electric Wherein Overlapping Polarized Domains Yield a Net Polarization
Cream is a Dense Colloidal Suspension
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Milk from a Cow Phase Separates into Cream Floating on Top of Skim Milk.
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Interfacial Water Floats on Top of the Normal Water Emulsion and a Copper Coin Floats
Interfacial Water
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A Bulk Water Droplet Floats on an Interfacial Water Layer Which in Turn Floats on Top of the Bulk Water Emulsion. The Droplet Remains Floating for Seconds
Suddenly Falling Down into the Water.
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Formation of a Water Bridge Across Two Glass Containers. The Container with the Lower Level Has the Cathode while the Container with the Higher Level has the Anode. V is about 15
when storing electronic negative charge .
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Liquid Crystal Interfacial Layer Stores Negative Charged Electrons Pushing Protons Into the Metallic Cathode Making a Metal Hydride and Pushing Positive Ions into the Bulk Water.
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For zero electric field, the ferroelectric state has neighboring polarization domains leave a configuration
+ - + - + - + - + - For strong electric fields, the downward polarization leaves only positive charges ++++++++++
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The - + charged ion pairs on the Interfacial water bulk water surface annihilate leaving a neutral molecule while another Electron runs from the cathode to replace the lost electron. The neutral object then ionizes radiating optical photons. The ionized electron then makes it through to the anode yielding
discharge) glow plasma ( photon ) anode ( ) water bulk ( ) crystal liquid ( ) cathode ( eV e e e e
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) gas ( 2 ) cathode ( 4 ) l interfacia ( 2 ) cathode ( 4 ) l interfacia ( 2 ) cathode ( 4
2 2
H H O H H e
) l interfacia ( 2 ) Emulsion Bulk ( 2 ) anode ( 2 ) gas ( ) Emulsion Bulk ( 2 Emulsion) Bulk ( 4 Emulsion) Bulk ( 4 l) interfacia ( 4 l) interfacia ( 4 ) l interfacia ( 2 ) l interfacia ( 2
2 2 2 2 2
O H O H e O O H HO HO HO HO O H O
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) anode ( 4 ) gas ( ) gas ( 2 2 ) cathode ( 4
2 2 2
e O H O H e
Faradays Law :For every 4F of charge which passes through the cell, two moles of hydrogen gas and one mole of oxygen gas will be produced F=96,485 Coulomb
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discharge) glow plasma ( photon ) anode ( ) water bulk ( ) crystal liquid ( ) cathode ( eV e e e e
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~100 Volt
~220 Volt
Radiation Subtracts From Faraday’s Law
discharge) glow plasma ( photon ) anode ( ) water bulk ( ) crystal liquid ( ) cathode ( eV e e e e ) anode ( 4 ) gas ( ) gas ( 2 2 ) cathode ( 4
2 2 2
e O H O H e
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Important Physics Requires
Production of Neutrons by Weak Interactions
2 2)
e
2 2 2 2 2 2 2 4 2
EE
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1 1 ) (
2 2 2 2 2 2 2 2 2
mc c m E e mc W Mc c M W n p e
e
The glow discharge excites surface plasma modes At mean frequency which n turn yields a fluctuating electric Field E. These quantum electrodynamics fluctuations renormalize the electron energy.
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volt/cm 300 Gauss 1 Gauss 10 ~ 5 ~ 3 | | 4 1 1 ) (
7 2 2 2 3 2 2 2 2 2 2 2
E E E me a a mc e E E Mc c M mc n p e
e
u
With u as the amplitude of the surface plasma mode displacement, the glow discharge is past the threshold for neutron production.
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2 14 2 12 2 hreshold 2 2 hreshold 2 2 2 2 2 2 2 2 hreshold
10 10 2 3 531 . 2 cm Hz cm Hz n mc c m G g g m M M
t t F A V p n t
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Nuclear Sequences are of the form shown below.
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Transmuted Deposit on the Cathode after Prolonged Discharge glow Grain Size ~ 10microns
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Neutrons Have Now Been Directly Observed
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modes
as a nuclear power source is under investigation.
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