US2019292070A1PendingUtilityA1

System for and method of affecting molecules and atoms with electromagnetic radiation

Assignee: BLANCHETTE KATHLEENPriority: Jul 31, 2006Filed: Jun 14, 2019Published: Sep 26, 2019
Est. expiryJul 31, 2026(~0 yrs left)· nominal 20-yr term from priority
Inventors:Gregory Young
C02F 1/461C01B 2203/0855C02F 1/48C02F 1/005C02F 1/34C01B 3/042B01J 19/129B01J 19/128B01J 19/126B01J 19/10Y02E60/36
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Claims

Abstract

A system for and method of cleaving a bond between a first atom and a second atom in a molecule of a material are presented. One embodiment of the technique includes selecting a first electromagnetic radiation frequency, the first electromagnetic radiation frequency including a product of a golden mean and a base frequency associated with at least one of the first atom and the second atom. Such an embodiment further includes directing a first electromagnetic radiation at the material, where the first electromagnetic radiation has a frequency equal to the first electromagnetic radiation frequency, and where the first electromagnetic radiation frequency is sufficient to cleave the bond between the first atom and the second atom.

Claims

exact text as granted — not AI-modified
We claim: 
     
         1 . A method of strengthening a bond between a first atom and a second atom in a molecule of a material, the method comprising:
 selecting a first electromagnetic radiation frequency, the first electromagnetic radiation frequency comprising a product of a golden mean and a base frequency associated with at least one of the first atom and the second atom; and   directing a first electromagnetic radiation at the material, the first electromagnetic radiation having a frequency equal to the first electromagnetic radiation frequency, wherein the first electromagnetic radiation frequency is sufficient to strengthen the bond between the first atom and the second atom.   
     
     
         2 . The method of  claim 1  wherein the first electromagnetic radiation frequency (v1) is defined by the equation:
     v   1   =A   fr ·Φ n   ·e· 10 m  
 
 wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, n is an integer, and m is an integer. 
 
     
     
         3 . The method of  claim 1  further comprising:
 selecting a second electromagnetic radiation frequency, the second electromagnetic radiation frequency comprising a product of a golden mean and a base frequency associated with at least one of the first atom and the second atom; and 
 directing a second electromagnetic radiation at the material, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, wherein the first electromagnetic radiation frequency and the second electromagnetic radiation frequency are sufficient to strengthen the bond between the first atom and the second atom. 
 
     
     
         4 . The method of  claim 3  wherein the first electromagnetic radiation frequency (v1) is defined by the equation:
     v   1   =A   fr ·Φ n   ·e· 10 m ,
 
 wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, n is an integer, and m is an integer; and wherein the second electromagnetic radiation frequency (v 2 ) is defined by the equation:
     v   2   =B   fr ·Φ j   ·e· 10 k ,
 
 
 wherein B fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, j is an integer, and k is an integer. 
 
     
     
         5 . The method of  claim 4  wherein n and j are negative integers. 
     
     
         6 . The method of  claim 2  further comprising:
 selecting a second electromagnetic radiation frequency (v″), the second electromagnetic radiation frequency being defined by the equation:
     v″=A   fr ·Φ x   ·e   −Lt ·10 y ; and
 
 
 directing a second electromagnetic radiation at the material, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, L is the natural log of two, t is equal to n, x is an integer, and y is an integer. 
 
     
     
         7 . The method of  claim 2  further comprising:
 selecting a second electromagnetic radiation frequency (v′″), the second electromagnetic radiation frequency being defined by the equation:
     v ′″=( A   fr ·Φ a   ·L   −1 )·10 b   e   −L ; and
 
 
 directing a second electromagnetic radiation at the material, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, wherein wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, L is the natural log of two, a is an integer, and b is an integer. 
 
     
     
         8 . The method of  claim 6  wherein the first electromagnetic radiation and the second electromagnetic radiation are directed at the material concurrently. 
     
     
         9 . The method of  claim 7  wherein the first electromagnetic radiation and the second electromagnetic radiation are directed at the material concurrently. 
     
     
         10 . A method of facilitating the formation of a bond between a first atom and a second atom, the method comprising:
 selecting a first electromagnetic radiation frequency, the first electromagnetic radiation frequency comprising a product of a golden mean and a base frequency associated with at least one of the first atom and the second atom; and   directing a first electromagnetic radiation at the first and second atoms, the first electromagnetic radiation having a frequency equal to the first electromagnetic radiation frequency, wherein the first electromagnetic radiation frequency is sufficient to facilitate the formation of the bond between the first atom and the second atom.   
     
     
         11 . The method of  claim 10  wherein the first electromagnetic radiation frequency (v 1 ) is defined by the equation:
     v   1   =A   fr ·Φ n   ·e· 10 m ,
 
 wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, n is an integer, and m is an integer. 
 
     
     
         12 . The method of  claim 10  further comprising:
 selecting a second electromagnetic radiation frequency, the second electromagnetic radiation frequency comprising a product of a golden mean and a base frequency associated with at least one of the first atom and the second atom; and 
 directing a second electromagnetic radiation at the first and second atoms, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, wherein the first electromagnetic radiation frequency and the second electromagnetic radiation frequency are sufficient to facilitate the formation of the bond between the first atom and the second atom. 
 
     
     
         13 . The method of  claim 12  wherein the first electromagnetic radiation frequency (v 1 ) is defined by the equation:
     v   1   =A   fr ·Φ n   ·e· 10 m ,
 
 wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, n is an integer, and m is an integer; and wherein the second electromagnetic radiation frequency (v 2 ) is defined by the equation:
     v   2   =B   fr ·Φ j   ·e· 10 k ,
 
 
 wherein B fr  is a base frequency associated with either the first or second atom, .PHI. is a golden mean, e is a natural log base, j is an integer, and k is an integer. 
 
     
     
         14 . The method of  claim 12  wherein n and j are negative integers. 
     
     
         15 . The method of  claim 11 , further comprising:
 selecting a second electromagnetic radiation frequency (v″), the second electromagnetic radiation frequency being defined by the equation:
     v″=A   fr ·Φ x   ·e   −Lt ·10 y ; and
 
   directing a second electromagnetic radiation at the material, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, L is the natural log of two, t is equal to n, x is an integer, and y is an integer.   
     
     
         16 . The method of  claim 11  further comprising:
 selecting a second electromagnetic radiation frequency (v′″), the second electromagnetic radiation frequency being defined by the equation:
     v ′″=( A   fr ·Φ a   ·L   −1 )·10 b   e   −L ; and
 
 
 directing a second electromagnetic radiation at the material, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, wherein wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, L is the natural log of two, a is an integer, and b is an integer. 
 
     
     
         17 . The method of  claim 15  wherein the first electromagnetic radiation and the second electromagnetic radiation are directed at the material concurrently. 
     
     
         18 . The method of  claim 16  wherein the first electromagnetic radiation and the second electromagnetic radiation are directed at the material concurrently. 
     
     
         19 . A method of mimicking the presence of a molecule, the molecule having at least a first atom and a second atom, in a material, the method comprising:
 selecting a first electromagnetic radiation frequency, the first electromagnetic radiation frequency comprising a product of a golden mean and a base frequency associated with at least one of the first atom and the second atom; and   directing a first electromagnetic radiation at the material, the first electromagnetic radiation having a frequency equal to the first electromagnetic radiation frequency, wherein the first electromagnetic radiation frequency is sufficient to mimic the presence of a molecule in a material.   
     
     
         20 . The method of  claim 19  wherein the first electromagnetic radiation frequency (v 1 ) is defined by the equation:
     v   1   =A   fr ·Φ n   ·e· 10 m ,
 
 wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, n is an integer, and m is an integer. 
 
     
     
         21 . The method of  claim 20  further comprising:
 selecting a second electromagnetic radiation frequency (v″), the second electromagnetic radiation frequency being defined by the equation:
     v″=A   fr ·Φ x   ·e   −Lt ·10 y ; and
 
 
 directing a second electromagnetic radiation at the material, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, L is the natural log of two, t is equal to n, x is an integer, and y is an integer. 
 
     
     
         22 . The method of  claim 20  further comprising:
 selecting a second electromagnetic radiation frequency (v′″), the second electromagnetic radiation frequency being defined by the equation:
     v ′″=( A   fr ·Φ a   ·L   −1 )·10 b   e   −L ; and
 
 
 directing a second electromagnetic radiation at the material, the second electromagnetic radiation having a frequency equal to the second electromagnetic radiation frequency, 
 wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, L is the natural log of two, a is an integer, and b is an integer. 
 
     
     
         23 . The method of  claim 21  wherein the first electromagnetic radiation and the second electromagnetic radiation are directed at the material concurrently. 
     
     
         24 . The method of  claim 22  wherein the first electromagnetic radiation and the second electromagnetic radiation are directed at the material concurrently. 
     
     
         25 . A method of electrolyzing water, the method comprising:
 frequency (v 1 ) is defined by the equation:
     v   1   =A   fr ·Φ n   ·e· 10 m  
 
   wherein A fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, n is a nonnegative integer, and m is a nonnegative integer;   selecting a second frequency (v 2 ) defined by the equation:
     v   2   =B   fr ·Φ j   ·e· 10 k ,
 
   wherein B fr  is a base frequency associated with either the first or second atom, Φ is a golden mean, e is a natural log base, j is a nonnegative integer, and k is a nonnegative integer;   causing the water to cavitate;   directing a first electromagnetic radiation having the first frequency at the water;   directing a second electromagnetic radiation having the second frequency at the water, wherein the step of directing the first electromagnetic radiation occurs substantially simultaneously with the step of directing the second electromagnetic radiation; and   causing electrical current to flow through the water.   
     
     
         26 . The method of  claim 11  wherein at least one of m and k is equal to zero. 
     
     
         27 . The method according to  claim 1 , further comprising the processes of Formula VI, Formula VII and Formula VIII for attenuating EMFs and cancelling possible aberrant feedback or cavitation waves during processing of the method.

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