System for and method of affecting molecules and atoms with electromagnetic radiation
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-modifiedWe 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.Join the waitlist — get patent alerts
Track US2019292070A1 — get alerts on status changes and closely related new filings.
We store only your email — no account needed. See our privacy policy.