JP2009290977A - Method for converting magnetic field of stationary permanent magnet into magnetic field of magnetic flux vibration, and taking out mechanical energy and electric energy - Google Patents
Method for converting magnetic field of stationary permanent magnet into magnetic field of magnetic flux vibration, and taking out mechanical energy and electric energy Download PDFInfo
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Description
本発明は、静止した永久磁石の磁場を時間変化の磁場に変換することにより磁束振動を発生させ、永久磁石の磁場エネルギーを外に仕事を与えるエネルギーに変換することに関する。特に、永久磁石の磁場エネルギーを力学的エネルギー、電気エネルギーに変換することに関するものである。 The present invention relates to converting a magnetic field of a stationary permanent magnet into a time-varying magnetic field to generate magnetic flux vibration and converting the magnetic field energy of the permanent magnet into energy that gives work to the outside. In particular, it relates to converting the magnetic field energy of a permanent magnet into mechanical energy and electrical energy.
従来、電気磁気学では、静止した永久磁石の磁場エネルギーを外に仕事を与えるエネルギーとして利用することは、不可能であるとされてきた。永久磁石を運動させることにより、外に仕事を与えるとされてきた。
また、特開平9−271163号(特許文献1)は装置に関するものである。
Japanese Patent Laid-Open No. 9-271163 (Patent Document 1) relates to an apparatus.
従来、静止した永久磁石の磁場エネルギーは外に仕事を与えないエネルギーとされてきた。この磁場エネルギーを外に仕事を与えるエネルギーに変換するには、磁場の時間変化つまり磁束の振動を存在させることが必要である。
この発明が解決しようとする課題は、静止した永久磁石の磁場が磁束振動をともなう磁場に変換可能であるという、原理的解明、そしてその方法である。
また上記特許文献1は、複数の永久磁石の同極を点、線、面で接触、又は近接させ配設した永久磁石の磁場は、時間変化の磁場、つまり磁束振動の存在する磁場であることを考慮していないため、回転軸の振動自在の構造の必要性を記述していない問題点があった。
Conventionally, the magnetic field energy of a stationary permanent magnet has been regarded as energy that does not give work to the outside. In order to convert this magnetic field energy into energy that gives work to the outside, it is necessary to cause a time change of the magnetic field, that is, a vibration of the magnetic flux.
The problem to be solved by the present invention is the principle elucidation and the method that the magnetic field of a stationary permanent magnet can be converted into a magnetic field with magnetic flux oscillation.
Further, in
本出願人は、原理的な解明を実施するにあたり、数学上の素数に関する数論式(数式1)と永久磁石を用いた化学的実験の等価性に注目した。
素数に関する数論式を吟味すると、数論式の意味する幾何学的構造、つまりトーラス球面とかトーラス球面上での運動方程式(数式2)そして力の作用表示(数式3)が求まる。 そして、複数の永久磁石の同極を点で接触させて配設した磁場内での水溶液中のイオン (水銀イオンとよう素イオン)の分布状態、運動軌道は数論式の意味する内容と一致することを見出した。
In carrying out the principle clarification, the present applicant paid attention to the equivalence between a mathematical theory (Mathematical Expression 1) relating to a mathematical prime number and a chemical experiment using a permanent magnet.
Examining the number theorem related to prime numbers, we can find the geometric structure that the number theorem means, that is, the torus sphere, the equation of motion on the torus sphere (Equation 2) and the action display of the force (Equation 3). The distribution state and motion trajectory of ions (mercury ions and iodine ions) in an aqueous solution in a magnetic field arranged with the same poles of a plurality of permanent magnets in contact with each other agree with the meaning of the number formula. I found out.
このことより、純数学上の素数に関する数論式は、複数の永久磁石の同極接触、又は近接させて配設したときの磁場の幾何学的構造と等価な関係となる。つまり数論式から導かれる幾何学的構造、トーラス球面は複数の永久磁石の同極を点、線、面で接触、又は近接させて配設したときの磁場の幾何学的構造を与える。 Thus, the mathematical formula relating to prime numbers in pure mathematics has a relation equivalent to the geometric structure of the magnetic field when the permanent magnets are arranged in the same-polarity contact or close to each other. That is, the geometrical structure derived from the mathematical formula, the torus spherical surface, gives the geometrical structure of the magnetic field when the same poles of a plurality of permanent magnets are arranged in contact with or close to each other by points, lines or surfaces.
数論式から導かれる運動方式はエネルギー方程式ともみなされるので数2よりΦの2乗が全エネルギーに対応する。全エネルギーは数論式より、lnλ(k)×(lnλ(k)+c)×ω(ωは振動を表示)と対応し、そしてlnλ(k)×(lnλ(k)+c)は解析の結果、磁束の分布に対応する。
よって複数の永久磁石の同極を点、線、面で接触、又は近接させ配設したときの磁場エネルギーは磁束の時間変化、つまり磁束振動のエネルギーに変換する。静止した永久磁石の磁場は複数の永久磁石の同極を点、線、面で接触、又は近接させ配設することにより、時間変化の磁場に変換する。
Since the motion method derived from the number theory formula is also regarded as an energy equation, the square of Φ corresponds to the total energy from
Therefore, the magnetic field energy when the same poles of a plurality of permanent magnets are arranged in contact with or close to each other by points, lines, or surfaces is converted into time-varying magnetic flux, that is, energy of magnetic flux vibration. The magnetic field of a stationary permanent magnet is converted into a time-varying magnetic field by arranging the same poles of a plurality of permanent magnets in contact with or close to each other with dots, lines, or surfaces.
従って静止した永久磁石の磁場も時間変化の磁場に変換する方法は、複数の永久磁石の同極(N極とN極、又はS極とS極)を点、線、面で接触、又は近接させて配設すればよい。このように永久磁石が配設された磁場内では実験より、磁性体、磁石は回転運動(自転公転)を行なうし、又銅板を回転させなくても単極誘動現象が発生する。そして、複数の永久磁石の同極を点、線、面で接触、又は近接させ配設したものを銅板とアルミニウム板で包んだとき、銅板とアルミニウムの間に電圧の時間変化(数式4)が発生する。 Therefore, the method of converting the magnetic field of a stationary permanent magnet into a time-varying magnetic field is that the same polarity (N pole and N pole, or S pole and S pole) of a plurality of permanent magnets is in contact with, or close to, a point, line, or surface. What is necessary is just to arrange | position. Thus, in the magnetic field in which the permanent magnet is disposed, the magnetic body and the magnet are rotated (rotation and revolution) by experiments, and a unipolar induction phenomenon occurs without rotating the copper plate. Then, when the same poles of a plurality of permanent magnets are contacted or arranged close to each other by dots, lines, or surfaces, the voltage changes with time between the copper plate and aluminum (Formula 4). appear.
磁束振動の磁場は、磁性体、磁石を運動させることは公知である。
複数の永久磁石の同極を点、線、面で接触、又は近接させ配設したときの磁場は磁束振動の磁場であるから、その磁場内に磁性体、磁石をおけば運動する。特に磁石は磁束振動をする磁場との相互作用により安定した大きな運動エネルギー又は回転エネルギーを発生する。
It is well known that the magnetic field of magnetic flux oscillation moves a magnetic material and a magnet.
Since the magnetic field when the same poles of a plurality of permanent magnets are arranged in contact with or close to each other by points, lines, or surfaces is a magnetic field of magnetic flux oscillation, the magnetic body and the magnet move if placed in the magnetic field. In particular, a magnet generates stable large kinetic energy or rotational energy by interaction with a magnetic field that vibrates magnetic flux.
磁束振動をする磁場は、電気エネルギーを発生させることは公知である。
複数の永久磁石の同極を点、線、面で接触、又は近接させ配設したものを銅板とそして銅板とイオン化傾向が異なる金属板、例えばアルミニウム板で包んだ構造物を複数個組み合わせれば磁束振動にともなう共振現象を利用して電気エネルギーを得られる。
It is well known that a magnetic field that vibrates magnetic flux generates electrical energy.
Combining a plurality of structures in which the same poles of a plurality of permanent magnets are contacted or placed close to each other by dots, lines, or surfaces, and are wrapped with a copper plate and a metal plate having a different ionization tendency from the copper plate, such as an aluminum plate Electrical energy can be obtained by utilizing the resonance phenomenon associated with magnetic flux vibration.
磁束振動のエネルギーを力学的エネルギーに変換するとき、磁場内に設置されている回転体としての磁性体、磁石、そして回転体に結合している回転軸は、磁束振動と同調することにより力学的エネルギーを生ずる。従って、回転体としての磁性体、磁石、そして回転軸は回転自在、振動自在に支持されることが力学的エネルギーに変換するときの必要条件となる。 When converting the energy of magnetic flux vibration into mechanical energy, the magnetic body as a rotating body, a magnet, and the rotating shaft connected to the rotating body installed in the magnetic field are mechanically synchronized with the magnetic flux vibration. Produce energy. Therefore, it is a necessary condition for converting the magnetic body, the magnet, and the rotating shaft as the rotating body to be able to rotate and vibrate so as to be converted into mechanical energy.
具体的には、複数の永久磁石の同極を点、線、面で接触、又は近接させ配設された永久磁石群が円盤状の形状をなすとき、円盤の中心点から永久磁石群の上平面に垂直に回転軸を設け回転軸に回転体としての磁石を配設すればよい。回転体としての磁石は単構造の永久磁石でもよいし、複数の永久磁石の同極を点、線、面で接触又は近接させ配設した構造でもよい。ただ、単構造の永久磁石は磁極の減衰が考えられ後者の方が有利である。 Specifically, when a group of permanent magnets arranged such that the same poles of a plurality of permanent magnets are in contact with or close to each other with dots, lines, or surfaces form a disk shape, the upper side of the permanent magnet group is A rotating shaft may be provided perpendicular to the plane, and a magnet as a rotating body may be disposed on the rotating shaft. The magnet as the rotating body may be a single structure permanent magnet, or may be a structure in which the same poles of a plurality of permanent magnets are arranged in contact with or close to each other by dots, lines, or surfaces. However, in the case of a single-structure permanent magnet, it is possible to attenuate the magnetic pole, and the latter is more advantageous.
本発明の最大の効果は、永久磁石の磁場エネルギーを外に仕事を与えるエネルギーとして利用できることである。
永久磁石のエネルギーを力学的エネルギー、電気エネルギーとして取り出すことにより エネルギー供給源として利用できることである。従来は、磁石を動かすことによりエネルギーを得ていたが、本発明は磁石を動かすことなくエネルギーを得られる。
The greatest effect of the present invention is that the magnetic field energy of the permanent magnet can be used as energy for giving work to the outside.
Permanent magnet energy can be used as an energy supply source by taking it out as mechanical energy or electrical energy. Conventionally, energy is obtained by moving a magnet, but the present invention can obtain energy without moving a magnet.
磁束振動のエネルギーを電気エネルギーとして取り出すとき、電気分解反応のエネルギーとして利用できる。例えば、水電解反応(化1)に必要なエネルギーとして利用できる。 化1より水素を得ることが出来る。 When the energy of magnetic flux vibration is taken out as electric energy, it can be used as the energy of electrolysis reaction. For example, it can be used as energy required for the water electrolysis reaction (Chemical Formula 1). Hydrogen can be obtained from Chemical Formula 1.
図1は4個の永久磁石を加工、切断等により成形したものを、同極を点で接触させて配設した図である。1は成形した永久磁石、2はプラスチック等の非磁性材料で永久磁石とは接着剤等で固定されている。3は垂直線と永久磁石との傾斜角で0〜150度の範囲が望ましい。図1のように永久磁石を配設したときに生じる磁場は、時間変化の磁場である。つまり磁束振動の磁場である。 FIG. 1 is a diagram in which four permanent magnets formed by machining, cutting or the like are arranged with their same poles in contact with dots. 1 is a molded permanent magnet, 2 is a non-magnetic material such as plastic, and is fixed to the permanent magnet with an adhesive or the like. 3 is an inclination angle between the vertical line and the permanent magnet, and is preferably in the range of 0 to 150 degrees. The magnetic field generated when the permanent magnet is disposed as shown in FIG. 1 is a time-varying magnetic field. That is, it is a magnetic field of magnetic flux oscillation.
磁束振動によるエネルギーを力学的エネルギーに変換するには、図2のような回転体を作製する。図2は4の永久磁石を加工、切断等により成形したものを、同極を点で接触させて配設した図である。4は成形した永久磁石、2はプラスチック等の非磁性材料で、永久磁石とは接着剤等で固定されている。3は垂直線と永久磁石との傾斜角で0〜150度の範囲が望ましい。 In order to convert energy generated by magnetic flux vibration into mechanical energy, a rotating body as shown in FIG. 2 is produced. FIG. 2 is a diagram in which four permanent magnets formed by machining, cutting, or the like are disposed with the same poles in contact with dots. 4 is a molded permanent magnet, 2 is a non-magnetic material such as plastic, and is fixed to the permanent magnet with an adhesive or the like. 3 is an inclination angle between the vertical line and the permanent magnet, and is preferably in the range of 0 to 150 degrees.
注意すべきことは図1の1の永久磁石は上下方向に磁化された永久磁石、図2の4の永久磁石は左右方向に磁化された永久磁石を用いることである。つまりベースとなる永久磁石群の磁化方向と回転体としての永久磁石群の磁化方向は直交しなければならない。この理由は、電気磁気学上のローレンツ力と関係し、直交構造にしないと回転力が得られない為である。
It should be noted that the
図3は回転体を回転軸に結合し、そして回転軸は回転自在、振動自在な構造にした図である。5は回転軸でプラクチックとかステンレススチールのような非磁性材料を用いる。6は例えばベアリングのような構造で、回転軸は回転自在であり、かつ上下左右に振動自在な構造である。回転軸と回転体はネジのような構造で固定されていてもよい。回転軸の上端はベアリングのような構造物に支持されている。 FIG. 3 is a diagram in which a rotating body is coupled to a rotating shaft, and the rotating shaft is configured to be rotatable and oscillating. 5 uses a non-magnetic material such as practic or stainless steel on the rotating shaft. Reference numeral 6 denotes a structure such as a bearing, which has a structure in which the rotation shaft is rotatable and can vibrate vertically and horizontally. The rotating shaft and the rotating body may be fixed with a screw-like structure. The upper end of the rotating shaft is supported by a structure such as a bearing.
図4は回転構造の側面図である。この回転構造図が、磁束振動のエネルギーを回転エネルギーとして取り出す最良の形態である。永久磁石の残留磁束密度、保持力ともに大きくすれば回転エネルギーも大きくなる。 FIG. 4 is a side view of the rotating structure. This rotational structure diagram is the best mode for extracting magnetic flux vibration energy as rotational energy. Increasing the residual magnetic flux density and holding force of the permanent magnet increases the rotational energy.
図5は、磁束振動のエネルギーを電気エネルギーに変換する図である。複数の永久磁石の同極を点、線、面で接触、又は近接させ配設したときの磁場は、時間変化の磁場であるから、電圧が発生する。同極接触、又は近接構造の永久磁石を銅板と銅板とイオン化傾向が異なる金属板、例えばアルミニウム板で包んだ構造物を複数個組み合わせることにより、磁束振動の共振現象を利用して有効な電圧を取り出す。図5は2個組み合わせた図を記す。 FIG. 5 is a diagram for converting magnetic flux vibration energy into electrical energy. Since the magnetic field when the same poles of a plurality of permanent magnets are arranged in contact with or close to each other by points, lines, or surfaces is a time-varying magnetic field, a voltage is generated. By combining a plurality of structures in which permanent magnets with the same polarity contact or proximity structure are wrapped with a copper plate and a metal plate with different ionization tendency, such as an aluminum plate, an effective voltage can be obtained using the resonance phenomenon of magnetic flux vibration. Take out. FIG. 5 shows a combination of two.
磁束振動のエネルギーを回転エネルギー、又は電気エネルギーとして取り出すことにより電力として利用できる。 It can be used as electric power by taking out the energy of magnetic flux vibration as rotational energy or electric energy.
1 上下方向に磁化された永久磁石
2 プラスチック板のような非磁性材料
3 垂直線と磁石との傾斜角
4 左右方向に磁化された永久磁石
5 回転軸
6 ベアリングのような回転自在、振動自在な構造物
7 アルミニウム板
8 銅板
9 電圧
10 上下方向に磁化された永久磁石
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Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012170171A (en) * | 2011-02-10 | 2012-09-06 | Tetsuo Kato | Method for obtaining electrical quantity from permanent magnet |
JP2013081347A (en) * | 2011-10-04 | 2013-05-02 | Fujita Yasohito | Generator of electromagnetic induction application type and electrostatic induction application type |
JP2014103758A (en) * | 2012-11-20 | 2014-06-05 | Tetsuo Kato | Method of converting magnetic field energy of stationary permanent magnet into energy for giving work to the outside |
JP2014204564A (en) * | 2013-04-05 | 2014-10-27 | 加藤 哲雄 | Method for extracting permanent electric energy from stationary permanent magnet |
JP2015213393A (en) * | 2014-05-02 | 2015-11-26 | 加藤 哲雄 | Method for extracting high magnetic field energy from permanent magnet |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
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JPH09271163A (en) * | 1996-03-29 | 1997-10-14 | Tetsuo Kato | Rotating equipment of magnetic substance which uses permanent magnets |
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Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
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JPH09271163A (en) * | 1996-03-29 | 1997-10-14 | Tetsuo Kato | Rotating equipment of magnetic substance which uses permanent magnets |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012170171A (en) * | 2011-02-10 | 2012-09-06 | Tetsuo Kato | Method for obtaining electrical quantity from permanent magnet |
JP2013081347A (en) * | 2011-10-04 | 2013-05-02 | Fujita Yasohito | Generator of electromagnetic induction application type and electrostatic induction application type |
JP2014103758A (en) * | 2012-11-20 | 2014-06-05 | Tetsuo Kato | Method of converting magnetic field energy of stationary permanent magnet into energy for giving work to the outside |
JP2014204564A (en) * | 2013-04-05 | 2014-10-27 | 加藤 哲雄 | Method for extracting permanent electric energy from stationary permanent magnet |
JP2015213393A (en) * | 2014-05-02 | 2015-11-26 | 加藤 哲雄 | Method for extracting high magnetic field energy from permanent magnet |
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