JP2011147199A - Method of obtaining permanent battery without using any electrolyte - Google Patents
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本発明は金属の伝導電子に永久磁石の磁場を作用させ運動を与えることにより、電解質を用いない永続的な電池を得る方法に関するものである。 The present invention relates to a method for obtaining a permanent battery without using an electrolyte by applying a motion by applying a magnetic field of a permanent magnet to conduction electrons of a metal.
電磁気学によると磁場は静止している電荷には影響を及ぼさない。従って磁場は静止している電荷には運動等の物理的事象は及ぼさない。 According to electromagnetism, the magnetic field does not affect the static charge. Therefore, the magnetic field does not exert physical events such as motion on the static charge.
磁場は運動している電荷にはロ−レンツ力という力の作用を及ぼす。 The magnetic field exerts a force action called Lorentz force on the moving charge.
複数の永久磁石の同磁極を点、線、面で接触又は近接させたときの磁場即ち素数磁場では素数磁束は縦方向と横方向に振動している。素数磁束の振動は電圧の振動を発するので静止している電荷に運動等の影響を及ぼす。 In a magnetic field when the same magnetic poles of a plurality of permanent magnets are brought into contact with or close to each other by points, lines, or surfaces, that is, a prime magnetic field, the prime magnetic flux vibrates in the vertical and horizontal directions. Since the vibration of the prime magnetic flux generates the vibration of the voltage, it influences the stationary charge such as motion.
素数磁場は静止している電荷に運動を与えることにより素数磁場は金属の伝導電子に運動を与える。 A prime magnetic field imparts motion to a stationary charge, and a prime magnetic field imparts motion to a metal conduction electron.
伝導電子の運動はその方向が無秩序であったり相反するものであると打ち消し合い巨視的に運動は零に近いものとなり有効な電流は取り出せない。 If the directions of conduction electrons are disordered or contradictory, they cancel each other macroscopically and the movement is close to zero, and an effective current cannot be extracted.
発明が解決しようとする課題は素数磁場を金属の伝導電子に作用させ伝導電子に秩序性を有する運動そして等方向性を有する運動を与え有効な電流を得ることにあり従って永久磁石の磁場エネルギ−を直接的に電気エネルギ−に変換する方法つまり電解質を用いない永続的な電池を得る方法である。 The problem to be solved by the invention is to apply a prime magnetic field to the conduction electrons of a metal to give the conduction electrons an orderly motion and an isotropic motion to obtain an effective current, and therefore the magnetic field energy of the permanent magnet. Is a method of directly converting the energy into electric energy, that is, a method of obtaining a permanent battery that does not use an electrolyte.
本出願の課題は永久磁石の磁場の作用により金属の伝導電子に秩序性を有した等方向性の運動を与え有効な電流を得ることにあるから磁場は静止した電荷には影響を及ぼさないとする電磁気学の考えとは反することになる。 The subject of this application is to obtain an effective current by giving an orderly isotropic movement to the conduction electrons of the metal by the action of the magnetic field of the permanent magnet, so that the magnetic field does not affect the static charge. This is contrary to the idea of electromagnetism.
従って課題を解決するためには電磁気学とは概念を異にする理論を求める必要があり本出願人は数論上の素数を用いて記述される数論式は複数の永久磁石の同磁極を点、線、面で接触又は近接させたときの磁場即ち素数磁場と対応する関係にあるとする素数場理論を考えた。 Therefore, in order to solve the problem, it is necessary to obtain a theory that is different from the concept of electromagnetism. The prime field theory is considered to be in a corresponding relationship with the magnetic field, ie, the prime magnetic field, when contacting or approaching with a point, line, or plane.
素数場理論により素数磁場は通常の磁場とは異なる幾何学構造、物理的特性を保有し素数磁場での磁束を素数磁束と名称すれば素数磁束は幾何学構造であるト−ラス、球面上にル−プ状となって整列分布しそして物理的特性として振動している。 According to the prime field theory, the prime magnetic field has a geometric structure and physical characteristics different from those of the normal magnetic field, and if the magnetic flux in the prime magnetic field is named prime magnetic flux, the prime magnetic flux is on the geometrical structure of the truss or sphere. It is looped, aligned and oscillating as a physical property.
素数磁束のト−ラス、球面上でのル−プ状の整列分布そして振動は電荷に運動を与える。そして幾何学構造であるト−ラス、球面も整列分布し、素数磁束の整列分布並びにト−ラス、球面の整列分布を保持するために力の作用が生じる。その力はク−ロン力、反ク−ロン力、万有引力に対応すると考える。 The prime magnetic flux truss, the loop-like alignment distribution on the sphere, and the vibration give motion to the charge. Then, the torus and spherical surface which are geometric structures are also aligned and distributed, and the action of force is generated to maintain the alignment distribution of the prime magnetic flux and the aligned distribution of the torus and spherical surface. I think that the force corresponds to cron force, anti-cron force, universal gravitation.
従って素数磁場内に金属を配設すれば伝導電子はク−ロン力、反ク−ロン力、万有引力によりト−ラス、球面という幾何学構造上でル−プ状で整列分布している素数磁束に沿って円運動とか対数スパイラル運動という秩序性を有した運動即ち整列運動をする。 Therefore, if a metal is arranged in a prime magnetic field, the conduction electrons are distributed in a loop in the geometrical structure of a truss and a spherical surface due to the Cron force, anti-Clon force, and universal gravitation. A movement having an ordering, that is, a circular motion or a logarithmic spiral motion, that is, an alignment motion is performed.
素数磁束はそのすべてがト−ラス、球面上に整列分布しているのではなく素数磁場に垂直方向にスパイラル状で整列分布している素数磁束も存在する。円運動とか対数スパイラル運動をしているト−ラス、球面上の伝導電子は垂直方向にスパイラル状で整列分布している素数磁束に沿って金属表面に配位しようとする。 Not all of the prime magnetic fluxes are aligned and distributed on the torus and spherical surface, but there are also prime magnetic fluxes that are aligned and distributed spirally in the direction perpendicular to the prime magnetic field. A circular or logarithmic spiral truss or conduction electron on a spherical surface tries to coordinate to the metal surface along a prime magnetic flux that is spirally aligned in the vertical direction.
垂直方向の素数磁束に沿って金属表面に配位しようとする伝導電子を直接的に有効な電流として取り出すことは困難である。 It is difficult to directly extract conduction electrons that are to be coordinated to the metal surface along the prime magnetic flux in the vertical direction as an effective current.
素数磁場内の金属の表面をホ−ル（穴）とフラット（平坦）とすることによりホ−ル底部では伝導電子の円運動とか対数スパイラル運動による磁気モ−メントの整列が乱れることより伝導電子はホ−ル底部に集積する。 By making the surface of the metal in the prime magnetic field into a hole (hole) and flat (flat), the conduction electron is disturbed at the bottom of the hole due to disturbance of the alignment of the magnetic moment due to circular motion of the conduction electron or logarithmic spiral motion. Accumulates at the bottom of the hole.
ホ−ル底部に集積した伝導電子はエントロピ−力によりフラットに流れる。つまり伝導電子はホ−ル底部よりフラットに流れ、電流はフラットよりホ−ル底部に流れる。 The conduction electrons accumulated at the bottom of the hole flow flat due to entropy force. That is, conduction electrons flow flat from the bottom of the hole, and current flows from the flat to the bottom of the hole.
従って素数磁場内の金属の表面をホ−ルとフラットとすることにより金属は電池機能としての性質を保有し、ホ−ル底部はアノ−ド極、フラットはカソ−ド極となる。 Therefore, by making the surface of the metal in the prime magnetic field into a hole and a flat, the metal has the property of a battery function, the hole bottom is an anode pole, and the flat is a cathode pole.
１個のホ−ル、フラットの対から得られる電流は微弱でも多数のホ−ル、フラットの対から得られる電流を合計すれば有効な電流が得られる。例えば５平方ｃｍの金属表面に２ｍｍ間隔で格子状のホ−ルを作成すれば６２５個のホ−ル、フラットの対ができる。 Even if the current obtained from a single hole / flat pair is weak, an effective current can be obtained by summing the currents obtained from a number of hole / flat pairs. For example, if a grid-like hole is formed on a metal surface of 5 cm 2 at intervals of 2 mm, a pair of 625 holes and flats can be formed.
用いる金属は良導体であるアルミニウム板とか銅板が適している。 The metal used is an aluminum plate or a copper plate which is a good conductor.
従って課題を解決するための手段は素数磁場内に、表面に多数のホ−ルとフラットを格子状に配置した金属を配設することにあり、ホ−ル底部はアノ−ド極、フラットはカソ−ド極となることから多数のホ−ル底部とフラットから得られる電流を合計することにより電解質を用いない永続的な電池を得る方法が解決できる。 Therefore, a means for solving the problem is to arrange a metal having a large number of holes and flats arranged in a lattice on the surface in a prime magnetic field. The bottom of the hole is an anode pole, and the flat is Since it becomes a cathode electrode, a method of obtaining a permanent battery without using an electrolyte can be solved by summing up currents obtained from a large number of hole bottoms and flats.
本発明によれば、永久磁石の磁場エネルギ−を何らの電気的、機械的操作を与えなくても直接電気エネルギ−に変換できる。 According to the present invention, the magnetic field energy of the permanent magnet can be directly converted into electric energy without giving any electrical or mechanical operation.
電気エネルギ−を電気分解に利用することにより、アルカリ水溶液中で水を電気分解してホ−ル底部のアノ−ド極で酸素、フラットのカソ−ド極で水素を発生させることができる。 By utilizing electric energy for electrolysis, water can be electrolyzed in an alkaline aqueous solution to generate oxygen at the anode electrode at the bottom of the hole and hydrogen at the flat cathode electrode.
本発明は素数場理論から導かれることより、発明を実施するためには素数磁場での素数磁束の整列分布、素数磁場でのク−ロン力、反ク−ロン力、万有引力の出現、そしてそれらの力による電荷の整列運動を説明する必要がある。 Since the present invention is derived from the prime field theory, in order to implement the invention, the alignment distribution of the prime magnetic flux in the prime magnetic field, the Kron force in the prime magnetic field, the anti-Kron force, the appearance of universal gravitation, and those It is necessary to explain the electric charge alignment movement by the force of.
素数磁束の整列分布とは素数磁束が素数磁場の幾何学構造であるト−ラス、球面上でル−プ状で秩序性を有して分布していること、そして素数磁場に垂直方向にスパイラル状で秩序性を有して分布していることを意味する。電荷の整列運動とは整列分布してい素数磁束に沿う電荷がク−ロン力、反ク−ロン力、万有引力により円運動とか対数スパイラル運動という秩序性を有した運動を意味する。 Alignment distribution of prime magnetic flux is a truss that is a geometric structure of a prime magnetic field, a magnetic flux that is distributed in a looped and ordered manner on a spherical surface, and a spiral perpendicular to the prime magnetic field. It means that it is distributed with order and order. The charge alignment motion means a motion in which the charge along the prime magnetic flux, which is aligned and distributed, has ordering such as circular motion or logarithmic spiral motion due to Clone force, anti-Clone force, and universal gravitation.
先ずト−ラス、球面上で素数磁束がル−プ状で整列分布することを説明する。素数磁束の整列分布を説明するためには複素変数の関数論とその絶対値関数、そして整列分布を意味するζ（ｓ）関数が重要でありζ（ｓ）は幾何学的にはル−プを意味する関数である。 ζ（ｓ）を（数式１）で定義する。ζ（ｓ）の絶対値｜ζ（ｓ）｜を複素平面上の点ｓより垂直上方に整列分布するル−プであると考えるとζ（ｓ）は概念的には素数磁束の静的な整列分布を意味する。素数磁束の静的な整列分布を求めるには素数磁束とζ（ｓ）の関数の絶対値との対応関係を求める必要がある。 First, it will be explained that the prime magnetic flux is arranged and distributed in a loop shape on the truss and spherical surface. In order to explain the alignment distribution of the prime magnetic flux, the function theory of complex variables, its absolute value function, and the ζ (s) function meaning the alignment distribution are important. Ζ (s) is geometrically looped. Is a function that means ζ (s) is defined by (Formula 1). Considering that the absolute value | ζ (s) | of ζ (s) is a loop that is aligned and distributed vertically above the point s on the complex plane, ζ (s) is conceptually a static of a prime magnetic flux. Means an ordered distribution. In order to obtain the static alignment distribution of the prime magnetic flux, it is necessary to obtain the correspondence between the prime magnetic flux and the absolute value of the function of ζ (s).
素数磁束とζ（ｓ）の関数の絶対値との対応関係を求めるには素数磁束の整列分布という概念より考えてζ（ｓ）の関数は三角関数表示が適切である。（数式１）より関数ＳＩＮＬｎζ（ｓ）に関する数式（数式２）が求まる。（数式２）より（数式３）が求まる。（数式３）の実数値表示として数値計算を満足する（数式４）が求まる。そして（数式３）の絶対値関数として（数式５）が求まる。 In order to obtain the correspondence between the prime magnetic flux and the absolute value of the function of ζ (s), the function of ζ (s) is appropriately represented by a trigonometric function in view of the concept of the alignment distribution of the prime magnetic flux. From (Expression 1), an expression (Expression 2) relating to the function SINLnζ (s) is obtained. (Expression 3) is obtained from (Expression 2). (Numerical expression 4) that satisfies the numerical calculation is obtained as the real numerical value display of (Numerical expression 3). Then, (Expression 5) is obtained as an absolute value function of (Expression 3).
（数式５）の絶対値関数は、数論的観点から（ζ（ｓ））×（ζ（ｓ）の複素共役）＝素数磁束という置換を考えれば特許文献３の数論式（数式６）により書き換えられて（数式７）となる。絶対値関数は曲面を表現しているので（数式５）と（数式７）とにより絶対値関数のグラフを描くことにより、素数磁束は曲面上でル−プ状となって秩序性を有して分布している。曲面をト−ラス、球面とすると素数磁束はト−ラス、球面上で静的な整列分布をしている。 The absolute value function of (Formula 5) is the number theoretic formula (Formula 6) of Patent Document 3 considering the substitution of (ζ (s)) × (complex conjugate of ζ (s)) = prime magnetic flux from the number point of view. Is rewritten as (Equation 7). Since the absolute value function expresses a curved surface, by drawing the graph of the absolute value function using (Equation 5) and (Equation 7), the prime magnetic flux is looped on the curved surface and has an order. Distributed. When the curved surface is a torus and a spherical surface, the prime magnetic flux has a static alignment distribution on the torus and spherical surface.
次に素数磁場に垂直方向に素数磁束がスパイラル状で整列分布することを説明する。素数磁束の垂直方向の整列分布を考えるとき、素数磁束の縦方向と横方向への振動を考慮に入れて素数磁束の縦方向と横方向への取り替えに対し数論上自由な形式となる数論式を新たに求める必要がある。新たな数論式は当然数値計算を満足する必要があり、その数論式を（数式８）とする。（数式８）の１／ζ（ｓ）は概念的には素数磁束の動的な整列分布を意味している。 Next, it will be described that the prime magnetic flux is arranged and distributed in a spiral shape in a direction perpendicular to the prime magnetic field. When considering the vertical distribution of prime magnetic fluxes, a number that is free in terms of number theory for the replacement of prime magnetic fluxes in the vertical and horizontal directions, taking into account the longitudinal and lateral vibrations of the prime magnetic flux. It is necessary to obtain a new theoretical formula. The new number formula must naturally satisfy the numerical calculation, and the number formula is represented by (Formula 8). 1 / ζ (s) in (Expression 8) conceptually means a dynamic alignment distribution of prime magnetic fluxes.
（数式８）は素数磁束の縦方向と横方向への取り替えに対し自由な形式となっており、又φ（ｋ）は数論上φ（ｋ）〜（１／素数磁束）が成立するから（数式８）のφ（ｋ）を素数磁束に置換しても物理的内容は変化しない。（数式８）の右辺の複素変数の関数について、その絶対値関数を（数式９）としてそのグラフを描くことにより、素数磁束は垂直方向にスパイラル状で秩序性を有して分布している。つまり素数磁束は垂直方向に動的な整列分布をしている。 (Equation 8) is a free format for the replacement of the prime magnetic flux in the vertical direction and the horizontal direction, and φ (k) holds from φ (k) to (1 / prime magnetic flux) in number theory. Replacing φ (k) in (Equation 8) with a prime magnetic flux does not change the physical contents. By plotting the graph of the function of the complex variable on the right side of (Formula 8) with the absolute value function as (Formula 9), the prime magnetic flux is distributed in a spiral and orderly in the vertical direction. That is, the prime magnetic flux has a dynamic alignment distribution in the vertical direction.
次に素数磁場の幾何学構造であるト−ラス、球面の整列分布を説明する必要がある。ト−ラス、球面の整列分布とは、例えばト−ラス、球面が直線上に配位していることを意味する。ト−ラス、球面が無秩序に分布していれば、素数磁束がト−ラス、球面上に整列分布していても巨視的にみて素数磁束は無秩序分布となり電荷は整列運動を為しえない。電荷が整列運動を為すためにはト−ラス、球面の整列分布が必要である。 Next, it is necessary to explain the torus and spherical alignment distribution, which is the geometric structure of the prime magnetic field. The alignment distribution of the torus and the spherical surface means that the torus and the spherical surface are aligned on a straight line, for example. If the torus and sphere are distributed randomly, even if the prime number magnetic flux is aligned and distributed on the torus and sphere, the prime number magnetic flux has a disordered distribution when viewed macroscopically, and the charges cannot perform an alignment motion. In order for the electric charges to make an alignment motion, a torus and spherical alignment distribution is required.
ト−ラスと球面を特許文献６のＭ関数によりト−ラスをＭ（λ（ｋ））、球面をＭ（｜Ｌｎ φ（ｋ）｜）と書くと、ト−ラスと球面は（数式８）を用いて、数値計算を満足する（数式１０）が求まる。 When a truss and a spherical surface are written as M (λ (k)) and a spherical surface is written as M (| Lnφ (k) |) according to the M function in Patent Document 6, ) Is used to obtain (Expression 10) that satisfies the numerical calculation.
（数式１０）の右辺の｜ζ（ｓ）｜は複素平面上の点ｓより垂直上方に整列分布するル−プであると考えると（数式１０）はト−ラス、球面が素数磁場に垂直方向に配位する位置を違えて整列分布していることを示している。つまりト−ラス、球面は素数磁場に垂直方向に整列分布している。 Considering that | ζ (s) | on the right side of (Equation 10) is a loop that is aligned and distributed vertically above the point s on the complex plane, (Equation 10) is a truss, and the spherical surface is perpendicular to the prime magnetic field. It shows that the distribution is aligned with different positions coordinated in the direction. That is, the truss and spherical surface are aligned and distributed in the direction perpendicular to the prime magnetic field.
以上の説明により素数磁場の幾何学構造ト−ラス、球面上での素数磁束の整列分布とト−ラス、球面の整列分布を（図１）に示す。但し（数式４）の条件により素数磁束はト−ラス、球面の全曲面上で整列分布しているわけではない。素数磁束が整列分布していない曲面を（図２）に示す。（図２）の斜線部分は整列分布していない曲面である。 As described above, the geometrical structure truss of the prime magnetic field, the alignment distribution of the prime magnetic flux on the spherical surface, and the alignment distribution of the torus and spherical surface are shown in FIG. However, the prime magnetic flux is not arranged and distributed on the entire curved surface of the torus and spherical surface under the condition of (Equation 4). A curved surface in which the prime magnetic flux is not aligned and distributed is shown in FIG. The hatched portion in FIG. 2 is a curved surface that is not aligned and distributed.
次に電荷の整列運動を説明するために必要な要因である素数磁場でのク−ロン力、反ク−ロン力、万有引力の出現について説明する。素数磁束のト−ラス、球面上での整列分布、ト−ラス、球面の整列分布は素数磁場の作用により整列分布しているが素数磁場の作用を物理上の力の作用に対応させることにより素数磁束並びにト−ラス、球面の整列分布を保持するための力が具体的に表示できる。 Next, the emergence of the Kron force, the anti-Kron force and the universal attractive force in the prime magnetic field, which are necessary factors for explaining the charge alignment motion, will be described. Truss of prime magnetic flux, alignment distribution on sphere, alignment distribution of truss and sphere are aligned by the action of prime magnetic field, but by making the action of prime magnetic field correspond to the action of physical force The force for maintaining the alignment distribution of the prime magnetic flux, the torus and the spherical surface can be specifically displayed.
素数磁束並びにト−ラス、球面の整列分布を保持するための力は特許文献５の数式（数式１１）で表示される。（数式１１）は直感的には理解しずらい式であるため次のような写像を考える。複素平面上の点ｓを直交複素座標により複素平面上の点ｘ＋ｉｙに移す等角写像を考えることにより、この変換は単位円に関する反転を意味し、円は円に移る。反転を表示する変換式を（数式１２）とする。 The force for maintaining the alignment distribution of the prime magnetic flux, the torus, and the spherical surface is expressed by the equation (Equation 11) of Patent Document 5. Since (Expression 11) is an expression that is difficult to understand intuitively, consider the following mapping. By considering a conformal mapping that moves a point s on the complex plane to a point x + iy on the complex plane by means of orthogonal complex coordinates, this transformation means inversion with respect to the unit circle, and the circle moves to a circle. A conversion formula for displaying inversion is represented by (Formula 12).
｜ζ（ｓ）｜を幾何学的なル−プに、幾何学的なル−プをＭ関数に、更に特許文献５よりＭ関数を質量とか電気量に対応させて考えると（数式１１）と（数式１２）よりク−ロン力式、反ク−ロン力式そしてｓを万有引力定数Ｇに対応させて万有引力式を表示する概念式が求まる。従ってク−ロン力、反ク−ロン力、万有引力はト−ラス、球面上での素数磁束の整列分布並びにト−ラス、球面の整列分布を保持するために出現する力であると考えることができる。 Considering | ζ (s) | as a geometrical loop, a geometrical loop as an M function, and from Patent Document 5, the M function corresponds to a mass or an electric quantity (Formula 11). From (Equation 12), the Cron force equation, the anti-Clon force equation, and the conceptual equation for displaying the universal gravitation equation by correlating s with the universal gravitation constant G are obtained. Therefore, it can be considered that the cron force, anti-cron force, and universal gravitation force are the forces that appear to maintain the alignment distribution of the prime magnetic flux on the truss and sphere as well as the alignment distribution of the torus and sphere. it can.
素数磁場でのク−ロン力、反ク−ロン力の出現、特に反ク−ロン力の出現は物理の観点からは奇異に感じられる。反ク−ロン力の出現は素数磁場での素数磁束の縦方向と横方向への取り替えが自由であることに起因していることによるものであると考えられる。 The appearance of cron and anti-cron forces in a prime magnetic field, especially the appearance of anti-cron forces, seems strange from a physical point of view. The appearance of the anti-cron force is thought to be due to the fact that the prime magnetic flux in the prime magnetic field can be freely replaced in the longitudinal and transverse directions.
従って素数磁場ではク−ロン力、反ク−ロン力は時間振動して出現していると考えることができる。つまり素数磁場はク−ロン力、反ク−ロン力そして万有引力が混在している場であると考えられる。 Therefore, in the prime magnetic field, it can be considered that the Kron force and the anti-Khlon force appear by time oscillation. In other words, the prime magnetic field is considered to be a field in which cron, anti-cron, and universal attractive forces are mixed.
素数磁場でのク−ロン力、反ク−ロン力、万有引力は電荷に力の作用を及ぼし運動を与える。運動については運動の軌道が重要な要素であり、運動の軌道については重力の結合定数である万有引力定数Ｇとか電磁力の結合定数である微細構造定数の意味する幾何学的、物理的内容を知る必要がある。 The cron force, anti-cron force, and universal gravitation force in a prime magnetic field exert a force on the electric charge and give motion. For motion, the trajectory of motion is an important factor, and for the trajectory of motion, know the geometric and physical contents of the gravitational coupling constant G, which is the gravitational attraction constant G, and the fine structure constant, which is the coupling constant of electromagnetic force. There is a need.
先ほどの記述でｓをＧに対応させれば万有引力式の概念式が求まるとしたが、ｓをＧに対応させればＧも複素表示で記すことができる。Ｇの数値を満足する複素表示は数式（数式１３）で表わされる。（数式１３）は（数式１４）より（数式１５）となる。（数式１５）の右辺の複素関数は三角関数の複素変数で表わされるからＧはル−プ分布、即ち整列分布という概念を有している。 In the above description, if s is made to correspond to G, a universal gravitation formula can be obtained. However, if s is made to correspond to G, G can also be described in a complex display. A complex display satisfying the numerical value of G is expressed by an equation (Equation 13). (Formula 13) becomes (Formula 15) from (Formula 14). Since the complex function on the right side of (Formula 15) is expressed by a complex variable of a trigonometric function, G has the concept of a loop distribution, that is, an alignment distribution.
Ｇと同じように考えて微細構造定数は（数式１６）で表わされる。従って微細構造定数も整列分布という概念を有している。 Considering the same as G, the fine structure constant is expressed by (Formula 16). Therefore, the fine structure constant also has the concept of aligned distribution.
Ｇとか微細構造定数の整列分布の概念は、万有引力とかク−ロン力、反ク−ロン力による電荷の運動はル−プ軌道をとることを示唆する。従って電荷はト−ラス、球面上に整列分布している素数磁束に沿って円運動とか対数スパイラル運動という整列運動を行う。 The concept of an ordered distribution of G or fine structure constants suggests that the movement of electric charges due to universal gravitation, cron force, or anti-cron force takes a loop orbit. Accordingly, the charges undergo an alignment motion such as a circular motion or a logarithmic spiral motion along the prime magnetic flux that is aligned and distributed on the torus and the spherical surface.
以上の記述により素数磁場内の金属の伝導電子はト−ラス、球面上で整列運動を行いそして素数磁場に垂直方向にスパイラル状で整列分布している素数磁束に沿って金属表面に配位しようとする。 According to the above description, the conduction electrons of the metal in the prime magnetic field are aligned on the metal surface along the prime magnetic flux that is aligned and distributed in the spiral and perpendicular direction to the prime magnetic field. And
金属の表面をホ−ルとフラットに形成することによりホ−ル底部では伝導電子の整列運動による磁気モ−メントの整列が乱れることにより伝導電子はホ−ル底部に集積する。 By forming the metal surface flat with the hole, the alignment of the magnetic moment due to the alignment movement of the conduction electrons is disturbed at the bottom of the hole, so that the conduction electrons are accumulated at the bottom of the hole.
ホ−ル底部に集積した伝導電子はエントロピ−力によりフラットに流れる。従ってホ−ル底部はアノ−ド極、フラットはカソ−ド極としての電池機能を保有する。電流はフラットからホ−ル底部へ流れる。 The conduction electrons accumulated at the bottom of the hole flow flat due to entropy force. Therefore, the bottom of the hole has a battery function as an anode and the flat as a cathode. Current flows from the flat to the bottom of the hole.
従って、素数磁場内に、多数のホ−ルとフラットを格子状に配置した金属を配設し、多数のホ−ル底部とフラットを導体で結線することにより電解質を用いない永続的な電池を得ることができる。 Therefore, a permanent battery that does not use an electrolyte can be obtained by arranging a large number of holes and flats in a lattice shape in a prime magnetic field, and connecting the bottoms and flats of the holes with a conductor. Obtainable.
永続的な電池は発電、動力源などの種々の用途に用いることができる。 The permanent battery can be used for various applications such as power generation and power source.
１ ト−ラス
２ 球面
３ ト−ラス上で整列分布している素数磁束
４ 球面上で整列分布している素数磁束
５ 垂直方向に整列分布している素数磁束
６ 立体角π ／３
７ 金属表面のホ−ル
８ 金属表面のフラット
９ 金属 例えばアルミニウム板とか銅板
１０ 永久磁石
１１ ホ−ル底部を結線する導体
１２ フラットを結線する導体
１３ 電流
1 Torus
2 Spherical surface
3 Prime magnetic flux lined up on the torus
4 Prime magnetic flux lined up on the spherical surface
5 Prime magnetic flux aligned and distributed in the vertical direction
6 Solid angle π / 3
7 Hole on metal surface
8 Metal surface flat
9 Metal For example, aluminum plate or copper plate
10 Permanent magnet
11 Conductor connecting the hole bottom
12 Conductor connecting flats
13 Current
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| JP2015015841A (en) * | 2013-07-05 | 2015-01-22 | 加藤 哲雄 | Method for obtaining hydrogen by decomposing water by action of permanent magnet |
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| JPH0610924Y2 (en) * | 1988-08-05 | 1994-03-23 | 東芝ホームテクノ株式会社 | Electric water heater |
| JP2002136417A (en) * | 2000-11-02 | 2002-05-14 | Azuma Sugata Kk | Hanger for japanese-style clothing |
| JP2004166779A (en) * | 2002-11-18 | 2004-06-17 | Haruhiko Kameda | Hanger for clothes |
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| JPS60105480A (en) * | 1983-11-14 | 1985-06-10 | Toray Ind Inc | Cooling of belt of belt-cast apparatus |
| JPH0610924Y2 (en) * | 1988-08-05 | 1994-03-23 | 東芝ホームテクノ株式会社 | Electric water heater |
| JP2002136417A (en) * | 2000-11-02 | 2002-05-14 | Azuma Sugata Kk | Hanger for japanese-style clothing |
| JP2004166779A (en) * | 2002-11-18 | 2004-06-17 | Haruhiko Kameda | Hanger for clothes |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| JP2015015841A (en) * | 2013-07-05 | 2015-01-22 | 加藤 哲雄 | Method for obtaining hydrogen by decomposing water by action of permanent magnet |
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