JPS59218164A - Apparatus for increasing piercing amount of magnetic force line pulse - Google Patents

Apparatus for increasing piercing amount of magnetic force line pulse

Info

Publication number
JPS59218164A
JPS59218164A JP58090579A JP9057983A JPS59218164A JP S59218164 A JPS59218164 A JP S59218164A JP 58090579 A JP58090579 A JP 58090579A JP 9057983 A JP9057983 A JP 9057983A JP S59218164 A JPS59218164 A JP S59218164A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic force
lines
generating
coils
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP58090579A
Other languages
Japanese (ja)
Inventor
政木 和三
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to JP58090579A priority Critical patent/JPS59218164A/en
Publication of JPS59218164A publication Critical patent/JPS59218164A/en
Pending legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明は、磁力線によって磁気治療を行うに当り、磁力
線発生用コイルから距離の離れた場所においても強い磁
束密度を得るだめの磁力線パルスの貫通量増大装置に関
するものであシ、磁力線発生用コイルを同一方向に対し
縦列に配置して、各磁力線発生用コイルを磁力線が貫通
するようにし、磁力線発生用コイル外部への漏減磁束を
少なくすると共に、磁力線発生用コイルにおける内径方
向の発生磁力線を増加するだめのものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for increasing the penetration amount of magnetic field line pulses in order to obtain a strong magnetic flux density even at a distance from a magnetic field line generation coil when performing magnetic therapy using magnetic field lines. B. The coils for generating lines of magnetic force are arranged in tandem in the same direction so that the lines of magnetic force pass through each coil for generating lines of magnetic force, thereby reducing leakage and demagnetization flux to the outside of the coil for generating lines of magnetic force, and The purpose is to increase the lines of magnetic force generated in the inner diameter direction.

即ち、本発明は、複数個の磁力線発生用コイルを磁力線
発生用パルス発信装置に対して直列まだは並列に結線し
、それらの磁力線発生用コイルを発生する磁力線が同一
方向に貫通するように配設したことを特徴とする磁力線
パルスの貫通量増大装置の構造を要旨とするものである
That is, the present invention connects a plurality of magnetic force line generation coils in series or in parallel to a magnetic force line generation pulse transmitter, and arranges the magnetic force line generation coils so that the magnetic force lines generated pass through them in the same direction. The gist of the present invention is the structure of a device for increasing the amount of penetration of magnetic field pulses.

磁力線発生用コイルに電流を通ずるときには、第1図に
示すように、磁力線Fは磁力線発生用コイルLの中心線
を通るもの以外は殆んど円形の漏洩磁束となり、磁力線
発生用コイルLから離れるに従って磁力線は著しく減少
してゆくものである。
When a current is passed through the coil for generating lines of magnetic force, as shown in Fig. 1, the lines of magnetic force F become almost circular leakage magnetic flux except those that pass through the center line of the coil for generating lines of magnetic force L, and leave the coil L for generating lines of magnetic force. Accordingly, the lines of magnetic force decrease significantly.

即ち、第2図に示すように、縦軸に磁気強度をとり、横
軸に磁力−発生用コイル面からの距離を半径rを基準と
して表わせば、磁力線発生用コイル面から半径だけ離れ
た点における磁気強度は約1/2となシ、直径だけ離れ
た点におけ、b磁気強度は1/8以下となる。
In other words, as shown in Figure 2, if the vertical axis represents the magnetic intensity and the horizontal axis represents the distance from the magnetic force-generating coil surface with radius r as a reference, then the point is a point that is the radius away from the magnetic field line generating coil surface. The magnetic strength at point b is about 1/2, and at a point a diameter away, the magnetic strength at b is less than 1/8.

第3図は、2個の磁力線発生用コイルL1■、2をその
直径だけの距離を離して配置したときの磁力線Fの状態
を示したものである。この場合には、磁力線Fは磁力線
発生用コイルLI L2間のコイル直径内では殆んど平
行となり、外部への漏洩磁束は極めて少なくなっている
。このときにおける磁気強度・は、第4図に示すように
、一方の磁力線発生用コイルLlに近い距離Oのときに
最大の値を示し、距離が半径だけ離れたときにおいて僅
かに減少するだけで、他方の磁力線発生用コイルL2に
接近すれば再び最大の値となる。
FIG. 3 shows the state of the lines of magnetic force F when the two coils L1 and 2 for generating lines of magnetic force are arranged with a distance equal to their diameters apart. In this case, the lines of magnetic force F are almost parallel within the coil diameter between the coils LI L2 for generating lines of magnetic force, and the leakage magnetic flux to the outside is extremely small. As shown in Fig. 4, the magnetic intensity at this time reaches its maximum value when the distance O is close to one of the magnetic field line generating coils Ll, and decreases only slightly when the distance is away by the radius. , when it approaches the other magnetic field line generating coil L2, it becomes the maximum value again.

このように、中心線に沿って2個の磁力線発生用コイル
を配置して、それらの磁力線発生用コイル間に物体を置
く場合には、磁力線はその物体の内部を殆んど平行磁力
線の形で貫通することになり、目的物に対して強力な磁
束密度を供給することが可能となる。
In this way, when two coils for generating magnetic lines of force are arranged along the center line and an object is placed between the coils for generating lines of magnetic force, the lines of magnetic force are formed inside the object in the form of almost parallel magnetic lines of force. This makes it possible to supply a strong magnetic flux density to the target object.

第5図は、3個の磁力線発生用コイルLI L2 La
を並列に配置したものであって、その磁力線Fは図示の
ように磁力線発生用コイル内では殆んど平行線として貫
通する。
Figure 5 shows three magnetic field line generation coils LI L2 La
are arranged in parallel, and the lines of magnetic force F pass through the coil for generating lines of magnetic force as almost parallel lines as shown in the figure.

第3図の磁力線発生用コイルを2個用いたものは、磁気
治療用電流を2個の磁力線発生用コイルに対し同時に同
一方向の磁束が発生するように流し、これら2個の磁力
線発生用コイルの間に身体を置くことによって、身体の
内部に殆んど平行線的な磁力線が貫通ずることになる。
In the case of using two coils for generating magnetic lines of force as shown in Fig. 3, a current for magnetic therapy is passed through the two coils for generating lines of magnetic force so that magnetic flux is generated in the same direction at the same time. By placing your body between them, almost parallel lines of magnetic force will penetrate inside your body.

第5図のように、3個の磁力線発生用コイルを中心線方
向に配設したものは、身体における両手とか、両足を各
磁力線発生用コイルの間に置くことによって同時に治療
を行うことができる。
As shown in Figure 5, when three coils for generating magnetic lines of force are arranged in the direction of the center line, treatment can be performed simultaneously by placing both hands or both feet between the coils for generating lines of magnetic force. .

第6図の配線図は、2個の磁力線発生用コイルLIL2
を磁力線発生用パルス発信装置Aに対して直列に接続し
た状態を示し、第7図の配線図は、3個の磁力線発生用
コイルL+ L2 Laを磁力線発生用パルス発信装置
Aに対して並列に接続した状態を示しており、磁力線発
生用パルス発信装置Aとして適宜なものを採用すること
ができ、その電源の電圧および電流の容量によって適当
な接続を採用し得る。
The wiring diagram in Figure 6 shows two magnetic field line generation coils LIL2.
The wiring diagram in Fig. 7 shows a state in which three magnetic field line generating coils L+ L2 La are connected in parallel to the magnetic field line generating pulse transmitting device A. The connected state is shown, and an appropriate device can be adopted as the pulse transmitter A for generating magnetic lines of force, and an appropriate connection can be adopted depending on the voltage and current capacity of the power source.

第8〜10図は、磁力線発生用コイルに流れる電流の波
形を示してたり、第8図に示すような片極パルス状の電
流、または第9図に示すような二相性活動電位波形のパ
ルス電流、さらには第10図に示すような短形波の電流
などを任意に採用し得る。
Figures 8 to 10 show the waveforms of the current flowing through the magnetic field line generating coil, unipolar pulse current as shown in Figure 8, or biphasic action potential waveform pulses as shown in Figure 9. Any current, or even rectangular wave current as shown in FIG. 10, may be arbitrarily employed.

【図面の簡単な説明】[Brief explanation of drawings]

図は本発明の実施例を示し、第1図は1個の磁力線発生
用コイルの場合における磁力線図、第2図は第1図の場
合における磁束強度図、第3図は2個のm力線発生用コ
イル間における磁力線図、第4図は第1図の場合におけ
る磁束強度図、第5゜図は:つ飼の磁力線発生用コイル
を用いた場合の磁力線図、第6図は2個の磁力線発生用
コイルを直列に接続した場合の配線図、第7図は3個の
磁力線発生用コイルを並列に接続した場合の配ml’f
A、第8〜10図に、(”]れも磁力線発生用コイルに
流す電流の波形図である。 図中の符号を説明すれば、次の通りである。 Lは磁力1線発生用コイル  Fは磁力線Aは磁力線発
生用パルス発信装置 特許出願人 林  原 、? 1 図 才3図 t2図 4wJ r    ?r v!、屯鯉 才 5 図 3 才 8 図
The figures show an embodiment of the present invention, in which Figure 1 is a magnetic field line diagram in the case of one magnetic field line generating coil, Figure 2 is a magnetic flux intensity diagram in the case of Figure 1, and Figure 3 is a magnetic flux intensity diagram in the case of two m-forces. Figure 4 is a magnetic flux intensity diagram between the line generation coils, Figure 4 is a magnetic flux intensity diagram in the case of Figure 1, Figure 5 is a magnetic force line diagram when two coils are used, Figure 6 is a diagram of magnetic force lines when two coils are used. Figure 7 shows the wiring diagram when three magnetic field line generating coils are connected in series, and Figure 7 shows the wiring diagram when three magnetic field line generating coils are connected in parallel.
A. Figures 8 to 10 are waveform diagrams of the current flowing through the coil for generating lines of magnetic force. The symbols in the figures are as follows. L is the coil for generating one line of magnetic force. F is a line of magnetic force A is a pulse transmitter for generating magnetic lines of force Patent applicant Hayashi Hara, ?1 Figure 3 Figure t2 Figure 4 wJ r ?r v!

Claims (1)

【特許請求の範囲】[Claims] 複数個の磁力線発生用コイルを磁力線発生用パルス発信
装置に対して直列まだは並列に結線し、それらの磁力線
発生用コイルを発生する磁力線が同一方向に貫通するよ
うに配設したことを特徴とする磁力線パルスの貫通量増
大装置。
A plurality of coils for generating magnetic lines of force are connected in series or in parallel to a pulse transmitter for generating lines of magnetic force, and the coils for generating lines of magnetic force are arranged so that the lines of magnetic force that generate them penetrate in the same direction. A device for increasing the amount of penetration of magnetic field pulses.
JP58090579A 1983-05-25 1983-05-25 Apparatus for increasing piercing amount of magnetic force line pulse Pending JPS59218164A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58090579A JPS59218164A (en) 1983-05-25 1983-05-25 Apparatus for increasing piercing amount of magnetic force line pulse

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58090579A JPS59218164A (en) 1983-05-25 1983-05-25 Apparatus for increasing piercing amount of magnetic force line pulse

Publications (1)

Publication Number Publication Date
JPS59218164A true JPS59218164A (en) 1984-12-08

Family

ID=14002341

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58090579A Pending JPS59218164A (en) 1983-05-25 1983-05-25 Apparatus for increasing piercing amount of magnetic force line pulse

Country Status (1)

Country Link
JP (1) JPS59218164A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009539511A (en) * 2006-06-14 2009-11-19 エンジョイ スポレチノスト エス ルチェニム オメゼニム A device that attenuates cellular metabolism

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55160720A (en) * 1979-05-29 1980-12-13 Mochida Pharmaceut Co Ltd Remedial composition for cancer and its remedial device
JPS5731873A (en) * 1980-08-05 1982-02-20 Electro Biology Inc Electromagnetic treatment device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55160720A (en) * 1979-05-29 1980-12-13 Mochida Pharmaceut Co Ltd Remedial composition for cancer and its remedial device
JPS5731873A (en) * 1980-08-05 1982-02-20 Electro Biology Inc Electromagnetic treatment device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009539511A (en) * 2006-06-14 2009-11-19 エンジョイ スポレチノスト エス ルチェニム オメゼニム A device that attenuates cellular metabolism

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