JPS6238179A - Method and apparatus for forming heat point in electromagnetic induction type hyperthermia - Google Patents

Method and apparatus for forming heat point in electromagnetic induction type hyperthermia

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Publication number
JPS6238179A
JPS6238179A JP17819185A JP17819185A JPS6238179A JP S6238179 A JPS6238179 A JP S6238179A JP 17819185 A JP17819185 A JP 17819185A JP 17819185 A JP17819185 A JP 17819185A JP S6238179 A JPS6238179 A JP S6238179A
Authority
JP
Japan
Prior art keywords
frequency alternating
magnetic pole
magnetic field
alternating magnetic
polarity
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.)
Granted
Application number
JP17819185A
Other languages
Japanese (ja)
Other versions
JPH0463710B2 (en
Inventor
照剛 上野
原田 耕介
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.)
Iwatsu Electric Co Ltd
Original Assignee
Iwatsu Electric Co Ltd
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 Iwatsu Electric Co Ltd filed Critical Iwatsu Electric Co Ltd
Priority to JP17819185A priority Critical patent/JPS6238179A/en
Publication of JPS6238179A publication Critical patent/JPS6238179A/en
Publication of JPH0463710B2 publication Critical patent/JPH0463710B2/ja
Granted legal-status Critical Current

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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】 〔産業上の利用分野〕 本発明は、導電性物体内の局所をi磁誘導で加熱する方
法及び装置に関し、更に詳細には1人体内のガン病巣部
分の温度を上昇させてガンを加熱治療するために好適な
方法及び装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method and apparatus for heating a local area within a conductive object using i-magnetic induction, and more specifically to a method and apparatus for heating a local area within a conductive object using i-magnetic induction. The present invention relates to a method and apparatus suitable for elevating and thermally treating cancer.

〔従来の技術〕[Conventional technology]

正常なm織に比べて、ガン細胞や豚腸は熱に弱い。この
特徴を利用したガンの治療法、即ち、ハイパサーミア(
hyperthermia )の研究が近年注目されて
いる。これは病巣部の温度を42℃〜45℃柳度に上昇
させて、ガン細胞を壊死、若しくはその増殖を阻止させ
ようとするものである。
Cancer cells and pig intestines are more sensitive to heat than normal tissue. A cancer treatment method that utilizes this characteristic is hyperthermia (
hyperthermia) has been attracting attention in recent years. This is intended to increase the temperature of the lesion to 42°C to 45°C to cause necrosis of cancer cells or to prevent their proliferation.

〔発明が解決しようとする間萌点〕[The problem that the invention attempts to solve]

しかし病巣部の入に熱点を集中さぜることは極めて困難
なため、このハイパサーミア技術は未だ実用化されてい
ない。即ち、これfで組成の奥深くに病巣がある場合、
そこにのみ熱刷を形成することは困難であった。
However, this hyperthermia technology has not yet been put to practical use because it is extremely difficult to concentrate the heat spot on the lesion. That is, if there is a foci deep within the composition,
It was difficult to form a hot printing only there.

そこで1本発明の目的は、ガンの加熱治療、又はこれ対
外の医療や工業等に適用可能な導電性物体内の局所加熱
方法及びその装置を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a method and apparatus for locally heating a conductive object, which can be applied to heat treatment of cancer, or to other medical and industrial applications.

Ct8jg虜をM決するための手段〕 上紀問題虐を解決し、上記目的を達成するための本発明
に係わる導電性物体内の局所の加熱方法は、導電性物体
内の局所を加熱する方法であり。
A method for heating a local area within a conductive object according to the present invention for solving the above-mentioned problems and achieving the above object is a method for heating a local area within a conductive object. can be.

その中心が前記局所の中心に対して一方の側にあり且つ
前記物体を貫通するように設定されている第1の高周波
交番磁界を発生させると同時に、その中心が前記局所の
中心に対して他方の側にあり且つ前記物体を貫通するよ
うに設定され且つ#配出1の高周波交番磁界に対して位
相差を有している第2の高周波交番磁界を発生させ、こ
t”LKよって前記物体内に渦電流を発生させること、
前記第1及び第2の高周波交番磁界の相互関係と実質的
に同一の相互関係を有する第3及び第4の高周波交番磁
界を、 l]記局所に対する角度位置関係が前記第1及
び第2の高周波交番磁界と岩なるように発生させ、これ
によって前記物体内に渦電流を発生させることを含む 
−−、ことを 特徴とするものである。
generating a first high-frequency alternating magnetic field whose center is on one side with respect to the center of the local area and set to penetrate the object; A second high-frequency alternating magnetic field is generated, which is located on the side of generating eddy currents within the body;
third and fourth high frequency alternating magnetic fields having substantially the same mutual relationship as the mutual relationship of the first and second high frequency alternating magnetic fields; generating a high frequency alternating magnetic field, thereby generating eddy currents within said object;
--, it is characterized by.

本発明に係わる導電性物体内の局所加熱装置は。A local heating device within a conductive object according to the present invention is as follows.

第1及び第2の高周波交番磁界を発生させるための第1
.第2.第3及び第4の磁極の他に、第1及び第2の高
周波交番磁界の広がりを■止するための第5.第6.第
7.第8の磁極を有する。
A first for generating first and second high frequency alternating magnetic fields.
.. Second. In addition to the third and fourth magnetic poles, there is also a fifth magnetic pole for stopping the spread of the first and second high frequency alternating magnetic fields. 6th. 7th. It has an eighth magnetic pole.

〔作 用〕[For production]

上記発明において、第1の高周波交番G作と第2の高周
波交番S界と42互いに逆相関係である。
In the above invention, the first high frequency alternating G field and the second high frequency alternating S field 42 are in an antiphase relationship with each other.

従って、第1の高周波交番S界と第2の高周波交番S界
で秋ず7また領域に大きな渦電流が電碍誘導で発生する
。】対の第1及び第2の高周波交番磁界のみであれば、
加熱領域が第1及び第2の高周波交番S界に沿って柱状
に生じるが、異なる角度位償で第3及び第4の高周波交
番B界を発生させると、各高周波交番磁界の交差点部分
即ち所望局所の温度が最も高くなる。従って1局P9T
以外の温ルの上昇を抑えて局所を所望温度にすることが
できる。
Therefore, a large eddy current is generated in the first high frequency alternating S field and the second high frequency alternating S field in the fall area 7 due to electrical insulation. ] If only the first and second high-frequency alternating magnetic fields of the pair are used,
The heating region is generated in a columnar manner along the first and second high-frequency alternating S fields, but when the third and fourth high-frequency alternating B fields are generated with different angular position compensation, the heating region is generated at the intersection point of each high-frequency alternating magnetic field, that is, the desired Local temperature is highest. Therefore, 1 station P9T
It is possible to suppress the rise in temperature other than that and bring the local temperature to the desired temperature.

本発明の装置においては、第5.第6.第7及び第8の
磁極の効果によって第1及び第2の高周波交番S界の広
が9が抑制さt、微小部分の加熱が可籠になる。
In the apparatus of the present invention, the fifth. 6th. The effect of the seventh and eighth magnetic poles suppresses the spread 9 of the first and second high-frequency alternating S fields, making it possible to heat minute portions.

〔実施例〕〔Example〕

次に1図面を参照して本発明の]実施例に係わる人体の
病巣部を加熱する方法及び装置を説明する、第1図及び
第2図は、*純化して示されて例えば頭部等の人体山内
のガン病巣部(2声を加熱治療する装置な示す。ガン病
巣部(2)は1円柱状に示さTしている人体(11の中
心に位置している。この病巣部(2)を加熱する時には
、ここを通る複数本の仮想直線+31(41+51 +
61を設定し、各頂線+31 (41+51 +61に
沿って4つの磁界発生装置(7+ f8+ (9+ (
101を配置する。
Next, a method and apparatus for heating a lesion of a human body according to an embodiment of the present invention will be explained with reference to FIGS. 1 and 2. The cancer focus area (2) in the human body is shown as a heat treatment device. ), when heating multiple virtual straight lines +31 (41+51 +
61, and four magnetic field generators (7+ f8+ (9+ (
Place 101.

今、]つの侮磁界発生装置7)を例にとって説明丁、b
と、 第1.i2. 第3.&び第4 f) コ(# 
011[12Ia:10市を有し、ここに高周波交@M
z源(+51がスイッチS。
Now, an explanation will be given using the two magnetic field generators 7) as an example.
And, 1st. i2. Third. & 4th f) Ko(#
011[12Ia: Has 10 cities and has high frequency exchange @M
z source (+51 is switch S.

を弁して接続されている。第1のコイル(111は直線
(3)に沿って人体(1)の一方の倶1に配置され、第
2のコイルQ21は@線(3)に沿って人体(1)の他
方の側に配置さf+でいる。第3のフィル031はp線
(3)に沿って人体(1)の他方の側に配置さね、第4
のコイル[+41はih !(34fc沿って人体(1
1の一方の側に配置されている。第1のコイルQllと
第4のコイルα41.及び第2のコイル0Zと第3のフ
ィル(]31は、ガン病巣部(2)の大きさに対応して
決定された間隔を有して平行配置されている、第1、第
2.第3及び第4のフィルσυq力u:x +141は
1人体(1)に向う方向を基準にして第1の極性、第2
の極性、第1の極性、第2の極性となるように、順次に
直列に接続されている。こ九等のコイル(II+−(1
41にスイッチS1を弁して例えは]O以上の高周波電
流が側1シによって流されると、ある瞬時において矢印
!161で示す第1の高周波交番S界と、矢印αnで示
す第2の高周波交番磁界とが発生する。この時、第1の
フィル011の人体側に生じる第1の磁極はへ極となり
、第2のコイルQ2+の人体側に生じる第2の磁極は磁
極となり、第3のコイル030人体側に生じる第3のa
極はN極となり、第4のフィルt141の人体側に生じ
る第4の磁極は磁極となる。
It is connected with a valve. The first coil (111 is placed on one side of the human body (1) along the straight line (3), and the second coil Q21 is placed on the other side of the human body (1) along the @ line (3). The third filter 031 is located on the other side of the human body (1) along the p-line (3), and the fourth
The coil [+41 is ih! (Human body along 34fc (1
1 on one side. The first coil Qll and the fourth coil α41. The second coil 0Z and the third fill ( ) 31 are arranged in parallel with an interval determined according to the size of the cancer lesion (2). The third and fourth fill συq forces u: x +141 have the first polarity and the second polarity with respect to the direction toward the human body (1).
They are connected in series in order so that the polarity becomes , the first polarity, and the second polarity. This ninth class coil (II+-(1
For example, when the switch S1 is turned on at 41 and a high frequency current of 0 or more is caused to flow through the side 1, at a certain instant the arrow ! A first high frequency alternating S field indicated by 161 and a second high frequency alternating magnetic field indicated by arrow αn are generated. At this time, the first magnetic pole generated on the human body side of the first fill 011 becomes a polarity, the second magnetic pole generated on the human body side of the second coil Q2+ becomes a magnetic pole, and the third magnetic pole generated on the human body side of the third coil 030 becomes a magnetic pole. 3 a
The pole becomes a north pole, and the fourth magnetic pole generated on the human body side of the fourth filter t141 becomes a magnetic pole.

第1及び第2の高周波交番S界叫α力の中心は。The centers of the first and second high-frequency alternating S-field forces are:

仮想直線(3)に沿ってはいるが一致はしておらず。Although they are along the virtual straight line (3), they do not match.

病巣部(2)を挾み込むように延びている、第1の高山
沖亦禾庸界日−シ爪ワの宜困姑か舌mW師ふけ】80度
の位相差即ち逆相関係になっている。従って、第1及び
第2の高周波交番磁界tlbI(+77で挾1れた柱状
部分における渦電流は他の部分に比べて強く生じる。な
お、人体及びガン病巣部f21は導電性を有しているの
で、高周波磁界に基つ〈電磁誘導によって渦1FIL流
が発生する。上述の如く渦電流が発生すると、ジュール
熱が発生し、温度が上昇する。
The first Takayama-Oki-Yi-Yu-Yu-Kai-hi-Shin-tsume-wa-Yi-Kou-A-Tongue mW-shi-duke] which extends so as to sandwich the lesion (2) has a phase difference of 80 degrees, that is, an inverse phase relationship. ing. Therefore, the eddy current in the columnar part sandwiched by the first and second high-frequency alternating magnetic fields tlbI (+77) is generated more strongly than in other parts.The human body and the cancer focus part f21 have electrical conductivity. Therefore, an eddy current is generated due to electromagnetic induction based on a high frequency magnetic field. When an eddy current is generated as described above, Joule heat is generated and the temperature rises.

ここで重要なことは、単一の磁界発生装置17+による
温度上昇では人体(1)の正常部分の破壊が生じない様
に高周波電流の太ぎさ、コイルQll〜σ市の巻き数を
決定することである。従って、単一の磁界発生装置(7
)で病巣部(2)を要求される温度(42℃−45℃)
葉で上昇させることは困難である。そこで、病巣部(2
)に交差する別の直線+41 +51 +61における
磁界発生装置(81(9+ (II) vcよっても高
周波交番磁界を発生させる。これにより、各高周波交番
磁界の交差点領域即ち遁巣部(2)の温I!tを他に比
べて大幅に高くすることが出来る。
What is important here is to determine the thickness of the high-frequency current and the number of turns of the coils Qll to σ so that the temperature rise caused by the single magnetic field generator 17+ will not destroy the normal parts of the human body (1). It is. Therefore, a single magnetic field generator (7
), the temperature required for the lesion (2) (42℃-45℃)
It is difficult to raise with leaves. Therefore, the lesion area (2
A high frequency alternating magnetic field is also generated by the magnetic field generating device (81 (9+ (II) vc) at another straight line +41 +51 +61 intersecting with I!t can be made significantly higher than others.

039α特噛QDは第5.第6.第7及び第8のコイル
であり、第1及び第2の7rFJ周波交番研界σtil
Q71の広がりを1lIII限するために設けらjてい
る。第1図テは配線が省略されているが、具体的には第
3図に示す如く、第1〜第4のコイルqυ〜041と向
−の摂のu5IVC接続さtでいる。そして、第5.第
6.第7及び第8のコイルQ8i (191(2tJl
(211の人体(1)に対向する側を基準にして第1の
極性、第2の極性、第2の極性、第3の極性になるよう
に各コイルα■〜Zllの杼性が決定されている。従っ
て、ある瞬時においては、第3図に示す如く、第5.第
6.第7及び第8のコイルO浅α!JIG?υ2DはN
極、磁極、磁極、N極になる。この第5〜第8のコイル
賭〜Ullの磁極の強さは、第1及び第2の高周波交番
磁界+161 flηの広がりを11]限するように設
定されている。ff1Jち、第1の磁極PIと第4の磁
極P6とが接近した時に両者間に磁束の流れが生じるこ
とを制限するたぬに。
039α special bite QD is the 5th. 6th. The seventh and eighth coils are the first and second 7rFJ frequency alternating field σtil
It is provided to limit the spread of Q71 by 1lIII. Although the wiring is omitted in FIG. 1, specifically, as shown in FIG. 3, it is connected to the U5IVC in the opposite direction to the first to fourth coils qυ~041. And the fifth. 6th. 7th and 8th coil Q8i (191 (2tJl
(The shuttle characteristics of each coil α■ to Zll are determined so that the polarity is the first polarity, the second polarity, the second polarity, and the third polarity based on the side facing the human body (1) of 211. Therefore, at a certain instant, as shown in Fig. 3, the 5th, 6th, 7th, and 8th coils O shallow α!JIG?υ2D are N
It becomes a pole, a magnetic pole, a magnetic pole, a north pole. The strength of the magnetic poles of the fifth to eighth coils is set so as to limit the spread of the first and second high-frequency alternating magnetic fields +161flη. ff1J A tongue that restricts the flow of magnetic flux between the first magnetic pole PI and the fourth magnetic pole P6 when they approach each other.

同極性で互いに隣接された第1の磁極P1と第5の磁極
lノ、との反発作用、及び第4のEB極P4と第6の仏
(侃P6との反発作用をオII用している。右側の第7
及び第8の磁極P?、P、も同様に利用されている。
By using the repulsive action between the first magnetic pole P1 and the fifth magnetic pole lno, which are adjacent to each other with the same polarity, and the repulsive action between the fourth EB pole P4 and the sixth pole P6, No. 7 on the right.
and the eighth magnetic pole P? ,P are also used in the same way.

なお、第5及び第6の磁極P、 、 P、の強さは、こ
れ等の相互間に礎東の流れが生じるように設定されてい
る。第7及び第8の磁極P?、Psの強さも同様に設定
されている。
Note that the strengths of the fifth and sixth magnetic poles P, P, P, are set so that a flow of the foundation occurs between them. Seventh and eighth magnetic poles P? , Ps are similarly set.

第1図において、第2の磁界発生装置 (81は、第1
の磁界発生装置(7)に対して直角の角度位置に配置さ
れ、第1の磁界発生装fl (71の第1〜第8のコ(
ルt111G21u:N(1410&clIclII 
K対応して、第9〜第16のコイル+1la)(12a
月138)(142月11’1a)119aJ(2+l
a)+21a)を有てる。この第2の磁界発生装置 (
81は。
In FIG. 1, the second magnetic field generator (81 is the first
The first magnetic field generating device fl (71, first to eighth co(
t111G21u:N(1410&clIclII
Corresponding to K, the 9th to 16th coils + 1la) (12a
month 138) (142 month 11'1a) 119aJ (2+l
a) +21a). This second magnetic field generator (
81 is.

第1及び第2の高周波交番磁界a61(17に直交する
方向に第3及び第4の高周波交番磁界+1fta)11
7a)’p光発生せる虜を除いては、第1の磁界発生装
置(7)と向−である。従って、その詳しい説明を省略
する。
First and second high frequency alternating magnetic fields a61 (third and fourth high frequency alternating magnetic fields +1fta in the direction perpendicular to 17) 11
7a)'P Except for the device that generates light, it is in the same direction as the first magnetic field generator (7). Therefore, detailed explanation thereof will be omitted.

第3及び第4の磁界発生装置+91001は、第1及び
第2の磁界発生装置 +71 +81の相互間に配tさ
9ている。そして、病巣部(2)の立体的加熱を強ぬる
ために、第3及び第4の磁界発生装置+91 QOIの
各コイルは垂直軸(Z#)方向に並置されている。従っ
て。
The third and fourth magnetic field generators +91001 are arranged between the first and second magnetic field generators +71 and +81. In order to strongly heat the lesion (2) three-dimensionally, the coils of the third and fourth magnetic field generators +91 QOI are arranged in parallel in the vertical axis (Z#) direction. Therefore.

1g1図には上側になるコイルのλが示されている。1g1 diagram shows λ of the upper coil.

第2図は第1図のローnINから見た第3の磁界発生装
置(91と入体山との関係な示す。第1の磁界発生装置
(7)の第1、第2.第3及び第4のコイル(l])〜
04;、及び第5〜第8のコイルtta〜21)に対応
して第17〜第20のフィル(11b月12b月13b
)(14b)及び第21〜第24の) イル118bJ
lISlbH20bH21bJが夫々設けられている。
FIG. 2 shows the relationship between the third magnetic field generator (91) and the inlet peak as seen from the low nIN in FIG. 1. The first, second, third, and Fourth coil (l])~
04; and the 17th to 20th fills (11b month 12b month 13b) corresponding to the 5th to 8th coils tta to 21)
) (14b) and 21st to 24th) Ile 118bJ
lISlbH20bH21bJ are provided respectively.

こt(により、矢印(16B)117a)に示す如く、
第5及び第6の高周波交番磁界が生じる。この第3の磁
界発生装置(9)の構成及び動作は、異なる角度で第5
及び第6の高周波交番磁界+1fibN17b)を発生
させる点を除いて第1の磁界発生装置(7)と同一であ
る。第1図でフィル(1icJ(12cJのみで示す第
4の磁界発生装置αQも第1の磁界発生装置(7)と本
質的に同一に構成されている。
As shown in the arrow (16B) 117a,
Fifth and sixth high frequency alternating magnetic fields are generated. The configuration and operation of this third magnetic field generator (9) are as follows:
This device is the same as the first magnetic field generator (7) except that it generates a sixth high-frequency alternating magnetic field +1fibN17b). In FIG. 1, the fourth magnetic field generator αQ, indicated only by 1icJ (12cJ), has essentially the same configuration as the first magnetic field generator (7).

第1図〜第3図の装置で、ガン病巣部(2)を加熱する
時には、第1〜第3のスイッチS、、S、、 S、及び
図示されていない第4のスイッチの切り替えによって・
、第1〜第4の磁界発生装置(7)〜Qlに時間差を有
して順次に高周波X流を流丁。これにより。
When heating the cancerous lesion (2) using the apparatus shown in FIGS. 1 to 3, the following steps are performed:
, the high frequency X current is sequentially applied to the first to fourth magnetic field generators (7) to Ql with a time difference. Due to this.

1!磁誘導で渦電流が発生し、ジュール熱でガン病巣部
(2)が加熱される。この時、第1〜第4の磁界発生装
置 (71〜QOIのいずれに電流Z流してもガン病巣
部(2)に渦電流が流れるので、ガン病巣部(2)の温
度が最も高くなる。この時、ガン病巣部(2)以外にも
渦電流が流れ、温度が上昇するが、渦電流による加熱が
重畳されないため、さほど高い温度にはならない。なお
、加熱領域がガン病巣部(2)から大幅にはみ出る場合
には、8辺乞冷却するようにしてもよい。
1! Eddy currents are generated by magnetic induction, and the cancerous lesion (2) is heated by Joule heat. At this time, no matter which of the first to fourth magnetic field generators (71 to QOI) an eddy current flows through the cancer focus part (2), the temperature of the cancer focus part (2) becomes the highest. At this time, eddy currents flow in areas other than the cancer focus area (2), and the temperature rises, but the heating by the eddy currents is not superimposed, so the temperature does not become very high.Please note that the heated area is the cancer focus area (2). If it protrudes significantly from the surface, cooling may be performed on all eight sides.

高周波交番磁界の周波数を高くすれば、渦電流による発
熱効果も上る。この時1表皮効果で渦電流が導体表面付
近に集中することが考えられる。
Increasing the frequency of the high-frequency alternating magnetic field also increases the heating effect caused by eddy currents. At this time, it is thought that eddy currents are concentrated near the conductor surface due to the skin effect.

即ち、病巣部が人体の奥深くある場合、高尚@礎界を印
加すると、病巣部に熱、IJILン形成することができ
ない場合がある。しかし、100MH2に満たない周波
数においては表皮効四を殆んど無視てることができる。
That is, if the lesion is located deep within the human body, applying a lofty @ foundation may not be able to generate heat or IJIL in the lesion. However, at frequencies below 100 MH2, the skin effect can be almost ignored.

失体内の湛艮土外を妨げる要因として血流による冷却効
果があるが、ζiを無視して表皮からの9さが0.05
mの点の病巣部の湯度を5℃上昇さぜるために要する時
間を、外部磁界Bo=1mT。
The cooling effect of blood flow is a factor that prevents the flow of water inside the body, but ignoring ζi, the 9 from the epidermis is 0.05.
The external magnetic field Bo = 1 mT is the time required to raise the temperature of the hot water in the lesion at point m by 5°C.

比熱0士4.19X] OJ−K −g 、密度D=]
・0】gcm  1周波数50 MHzの条件で求める
と、約770mgとなる。従って、血流による冷却効果
があっても、熱点形成は十分回部である。!た病巣部の
場所と病状が許される場合には一時的な止血fたはレー
ザ光線テたは臨場等との併用側、できる。
Specific heat 4.19X] OJ-K -g, density D=]
・0] gcm When calculated under the condition of 1 frequency of 50 MHz, it is approximately 770 mg. Therefore, even if there is a cooling effect due to blood flow, the formation of hot spots is sufficient. ! If the location of the lesion and the medical condition permit, temporary hemostasis can be used in combination with laser beams, laser beams, etc.

上述から明らかな如く、不治療法では、放射線や薬剤を
使用しないので、副作用が極めて少ない。
As is clear from the above, the non-therapeutic method does not use radiation or drugs, and therefore has extremely few side effects.

従って、レーザーやマイクロ波で治療することができな
い人体内部のガン加熱治療に大きな効果が期待できる。
Therefore, it can be expected to be highly effective in heating cancer treatment inside the human body, which cannot be treated with lasers or microwaves.

次に、第1の高周波交番磁界ubJと第2の高周波交番
al界aηとで挾ま九た領域の渦電流密度が大になるこ
とケ、第4図〜第6図によって説明てる。
Next, it is explained with reference to FIGS. 4 to 6 that the eddy current density in the region sandwiched between the first high frequency alternating magnetic field ubJ and the second high frequency alternating field aη becomes large.

第4図及び第5図はX軸方向及びy一方向に±8の目盛
が付された正方形の導体板のの中心Xミy=0の近傍の
′FiL流q!j度を上昇させる方法を示す。
Figures 4 and 5 show the 'FiL flow q! near the center of the square conductor plate marked with ±8 scales in the X-axis direction and the Y direction. Shows how to increase the j degree.

導体板のとして導電率及び込磁率が共に均一の2次元の
導体glケ用意し、全体に均一な磁界HoY印加してお
く。また第4図及び第5図に斜線で示す二つの小領域の
C!41 ICは均−磁界H0に加えて、更に局所fH
界馬、馬をそれぞれ第5図の矢団の向きに即加する。即
ち、一方にはHoと゛同位相の局所母界HAン、他方に
はHoと反位相の局所団界九を町加する。この局所磁界
HA、HBの発生汀、いずれも例えば空芯コイル(四本
ぜず]を導体板のの上下に置き、これ?1対として用い
る。第6図は第4図に示す二次元の導体板ののy@上の
渦電fN密度を計算により求めた結果である。ここで局
所磁界HA、 HBtr I HAI = IHBl 
= a IHolとしてa=1とa=】0の場合の渦電
流密度を夫々求め、特性線65VC!9a=10の場合
の結果?示し1%性線(ト)によりa = ]の場合の
結果を示す。第6図から明らかな如く局所磁界HA、H
Bの振幅が小さい場合(即ちa=1)には局Pk磁界H
A、HBの影響は小さく、中心y=0近傍の1!流密度
は増加しないか1局所磁界HA ”Bの振幅が大きい場
合(即ちa = 103には局所磁界の影1が太きく、
中心y=O近傍で二つの電流ループが集合して大きな電
#L密度?得ることができることが判も。
A two-dimensional conductor GL with uniform conductivity and magnetic infiltration rate is prepared as a conductor plate, and a uniform magnetic field HoY is applied to the whole. Also, C! of the two small areas indicated by diagonal lines in FIGS. 4 and 5! 41 In addition to the uniform magnetic field H0, IC also has a local fH
Immediately add the Kaima and the horses in the direction of the arrow group in Figure 5. That is, on one side, a local home field HA having the same phase as Ho is added, and on the other hand, a local group world 9 having an antiphase with Ho is added. To generate these local magnetic fields HA and HB, for example, air-core coils (four coils) are placed above and below the conductor plate, and these are used as a pair. This is the result of calculating the eddy electric current fN density on y@ of the conductor plate.Here, the local magnetic field HA, HBtr I HAI = IHBl
= a As IHol, find the eddy current density when a=1 and a=]0, and find the characteristic line 65VC! Result when 9a=10? The results in the case of a = ] are shown using the 1% sex line (g). As is clear from Fig. 6, the local magnetic fields HA, H
When the amplitude of B is small (i.e. a=1), the local Pk magnetic field H
The influence of A and HB is small, with 1! near the center y=0! If the amplitude of the local magnetic field HA ``B is large (i.e., the shadow 1 of the local magnetic field is thick at a = 103,
Two current loops gather near the center y=O, creating a large electric density? It turns out that you can get it too.

従つτ1局所研界HA、HBが高周波1!流の町加によ
って、その11流の向きに対応して変イビするため、導
体板のの端に比べてy=O近傍では大きな磁界の変化を
生じさせることとなり、結果として#l電流の増加によ
るいわゆる熱点が形成さjる。
Accordingly, τ1 local research field HA, HB is high frequency 1! Because the flow changes depending on the direction of the current, it causes a large change in the magnetic field near y=O compared to the edge of the conductor plate, resulting in an increase in #l current. A so-called hot spot is formed.

ここで均一磁界HI、は局F9rfB界曵、九の振幅の
大小による渦電流の発生効率を理論検討てるたぬに導入
したものであるから、実際の場合には不要である。
Here, the uniform magnetic field HI was introduced to theoretically study the efficiency of eddy current generation depending on the magnitude of the amplitude of the F9rfB field, so it is not necessary in actual cases.

局所磁界HA、HBは、第1図の第1及び第2の高周波
交番磁界ルσηに対応するので、第1及び第2の高周波
交番磁界11b1αηに挾テれた領域の渦電流密度が上
昇することは明らかである。第1図では人体山内の病巣
B+21V加熱する必要があるので。
Since the local magnetic fields HA and HB correspond to the first and second high-frequency alternating magnetic fields ση in FIG. 1, the eddy current density in the region sandwiched by the first and second high-frequency alternating magnetic fields 11b1αη increases. That is clear. In Figure 1, it is necessary to heat the lesion B+21V inside the human body.

第4図及び第5図を七の筐ま適用しても病巣部(2)の
入の加熱は不可能である。そこで、複数角度から加熱し
ている。
Even if FIG. 4 and FIG. 5 are applied to seven cases, it is impossible to heat the lesion (2). Therefore, heating is performed from multiple angles.

〔変形例〕[Modified example]

本発明は上述の実施例に限定されるものでなく。 The invention is not limited to the embodiments described above.

例えば次の変形例が可能なものである。For example, the following modifications are possible.

(al  第7図に示す如く、仏心@@21■乞設げ。(al As shown in Figure 7, the Buddha's heart @ @ 21■ Beggar.

、:、1m[:)イルc111c(3((3c(41巻
き回し、スイン4−S+’1介して電源(151から高
周波電Rを流し、第3図の場合と同様に第1〜第8の磁
極P1〜P8ヶ形成してもよい。
, :, 1m [:) Ill c111c (3 8 magnetic poles P1 to P may be formed.

(bl  第1図に示す、複数の磁界発生装置(7)〜
O■を設ける代りに、1台の磁界発生装置(7)を病巣
部(2)を中心に回転させ、朝なる角度位置から高周波
交番磁界を加えるようにしてもよい。即ち、単一の磁界
発生装置で、第1及び第2の高周波交番磁界ン発生させ
た後に、第3及び第4の高周波交番磁界、更に、MIJ
5及び第6の高周波交番磁界ン発生するよりにしてもよ
い。
(bl Multiple magnetic field generators (7) shown in Figure 1
Instead of providing the magnetic field generator (7), one magnetic field generator (7) may be rotated around the lesion (2) and a high frequency alternating magnetic field may be applied from an angular position in the morning. That is, after generating the first and second high-frequency alternating magnetic fields with a single magnetic field generator, the third and fourth high-frequency alternating magnetic fields, and then the MIJ
The fifth and sixth high frequency alternating magnetic fields may be generated.

(cl  第3図において第5〜第8のm 極Ps S
Ps O強さを更に強め、a東【磁力線]が病巣部(2
)の近傍1でU字状にくい込むようにしてもよい。
(cl The 5th to 8th m poles Ps S in Fig. 3
The PsO strength is further strengthened, and the a east [magnetic field line] moves to the lesion area (2
) may be embedded in a U-shape in the vicinity 1.

rdl  病巣部+21の大きさに対応させて母権P、
とP。
rdl matrilineal P, corresponding to the size of the lesion +21;
and P.

の間隔hPtとPlの間隔を調整できるようにしてもよ
い。また、a極P、とP、、PjとP4を対向配置させ
ないで、第1及び菌2の高周波交番磁界を得てもよい。
The interval between hPt and Pl may be adjustable. Alternatively, the high frequency alternating magnetic fields of the first and bacteria 2 may be obtained without arranging the a-poles P, P, and Pj and P4 facing each other.

〔発明の効果〕〔Effect of the invention〕

上述から明らかな如く1本発明によれは、立体的物体内
部の局所を容易に加熱することができる。
As is clear from the above, according to the present invention, a local area inside a three-dimensional object can be easily heated.

従って、ガンの加熱治療等に極めて有益である。Therefore, it is extremely useful for heat treatment of cancer, etc.

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

第1図打本発明の1実施例に係わる局所加熱装置を示す
平面図。 第2図は第1図の11−U線の一部を示す側面図。 第3図は第1図の磁界発生装置の]つ乞詳しく示す平面
図。 第4因は2次元の導体板における渦電流の密度を求ぬる
ための導体板と局P9r侮界との関係乞示す平面図。 第5図は第4図のy軸上のMT面図。 第6図)ゴ第4図の導体板の’l 4’ll止の位置と
#I電流密度との関係を示す図。 第7図は変ノ杉例のl界発生装置Y示す平面図である。 (11・・・人体、(2)・・・ガン病巣部、 (3+
(4115+(61・・・仮想直線、(7)(8)(9
)αQ・・・磁界発生装置、qυ・・・第1のコイル。 じ・・・第2のコイル、αJ・・・第3のフィル、■)
・・・第4のコイル、aシ・・・電源、(IbI・・・
第1の高周波交番磁界。 071・・・第2の高周波交番S界、a81・・・第5
のフィル。 a9・・・第6のフィル、(2I・・・第7のフィル、
 QD・・・第8のコイル。 代  理  人   高  野  則  次第1図 ba tJ2図 第7図 第4図       第5図 第6図 y本口3L イイL置
FIG. 1 is a plan view showing a local heating device according to an embodiment of the present invention. FIG. 2 is a side view showing a part of line 11-U in FIG. 1. FIG. 3 is a plan view showing the magnetic field generator of FIG. 1 in more detail. The fourth factor is a plan view showing the relationship between the conductor plate and the field of station P9r for finding the density of eddy current in the two-dimensional conductor plate. FIG. 5 is an MT plane view on the y-axis of FIG. 4. FIG. 6) A diagram showing the relationship between the 'l 4' ll stop position of the conductor plate in FIG. 4 and the #I current density. FIG. 7 is a plan view showing the l-field generator Y of Hennosugi's example. (11...human body, (2)...cancer lesion, (3+
(4115+(61... virtual straight line, (7) (8) (9
)αQ...magnetic field generator, qυ...first coil. J...Second coil, αJ...Third fill, ■)
...Fourth coil, a...power supply, (IbI...
A first high frequency alternating magnetic field. 071...Second high frequency alternating S field, a81...Fifth
Phil. a9...6th fill, (2I...7th fill,
QD... 8th coil. Agent Nori Takano Figure 1 BA tJ2 Figure 7 Figure 4 Figure 5 Figure 6 y Main entrance 3L Good L placement

Claims (7)

【特許請求の範囲】[Claims] (1)導電性物体内の局所を加熱する方法であり、その
中心が前記局所の中心に対して一方の側にあり且つ前記
物体を貫通するように設定されている第1の高周波交番
磁界を発生させると同時に、その中心が前記局所の中心
に対して他方の側にあり且つ前記物体を貫通するように
設定され且つ前記第1の高周波交番磁界に対して位相差
を有している第2の高周波交番磁界を発生させ、これに
よつて前記物体内に渦電流を発生させること、前記第1
及び第2の高周波交番磁界の相互関係と実質的に同一の
相互関係を有する第3及び第4の高周波交番磁界を、前
記局所に対する角度位置関係が前記第1及び第2の高周
波交番磁界と異なるように発生させ、これによつて前記
物体内に渦電流を発生させること を含むことを特徴とする導 電性物体内の局所加熱方法。
(1) A method of heating a local area within a conductive object, in which a first high-frequency alternating magnetic field whose center is on one side with respect to the center of the local area and is set to penetrate the object is applied. At the same time, a second high-frequency alternating magnetic field is generated, the center of which is located on the other side with respect to the local center, is set to penetrate the object, and has a phase difference with respect to the first high-frequency alternating magnetic field. generating a high frequency alternating magnetic field, thereby generating an eddy current in the object;
and third and fourth high frequency alternating magnetic fields having substantially the same mutual relationship as the second high frequency alternating magnetic field, the angular positional relationship with respect to the local area being different from the first and second high frequency alternating magnetic fields. 1. A method of local heating within a conductive object, the method comprising: generating an eddy current in the object, thereby generating an eddy current within the object.
(2)前記第3及び第4の高周波交番磁界は前記第1及
び第2の高周波交番磁界に対して時間差を有して発生さ
れるものである特許請求の範囲第1項記載の導電性物体
内の局所加熱方法。
(2) The conductive material according to claim 1, wherein the third and fourth high-frequency alternating magnetic fields are generated with a time difference with respect to the first and second high-frequency alternating magnetic fields. Local heating method within the body.
(3)前記位相差は逆相関係になる位相差である特許請
求の範囲第1項記載の導電性物体内の局所加熱方法。
(3) The local heating method within a conductive object according to claim 1, wherein the phase difference is a phase difference that has an inverse phase relationship.
(4)前記第1及び第2の高周波交番磁界は、周波数が
10^5Hz以上の交番磁界である特許請求の範囲第1
項記載の導電性物体内の局所加熱方法。
(4) The first and second high-frequency alternating magnetic fields are alternating magnetic fields having a frequency of 10^5 Hz or more.
Local heating method within a conductive object as described in .
(5)前記導電性物体は人体であり、前記局所はガン病
巣部である特許請求の範囲第1項記載の導電性物体内の
局所加熱方法。
(5) The local heating method within a conductive object according to claim 1, wherein the conductive object is a human body and the local area is a cancer lesion.
(6)導電性物体内の局所を加熱する装置であり、前記
局所を通る複数本の仮想直線に対応して設けられた複数
の高周波交番磁界発生装置から成り、前記高周波交番磁
界発生装置は、前記物体内に渦電流を流すための高周波
交番磁界を発生するように構成され、 且つ前記高周波交番磁界発生装置は、第1の極性の第1
の磁極と、第2の極性の第2の磁極と、第1の極性の第
3の磁極と、第2の極性の第4の磁極と、第1の極性の
第5の磁極と、第2の極性の第6の磁極と、第2の極性
の第7の磁極と、第1の極性の第8の磁極とを有するも
のであり、前記第1の磁極は前記物体の一方の側におい
て前記直線に沿うように配置され、 前記第2の磁極は前記物体の他方の側において前記直線
に沿うように配置され且つ前記第1の磁極との間に第1
の高周波交番磁界を生じさせるために前記第1の磁極に
対向配置され、 前記第3の磁極は前記物体の他方の側において前記直線
に沿うように配置され、 前記第4の磁極は前記物体の一方の側において前記直線
に沿うように配置され且つ前記第3の磁極との間に第2
の高周波交番磁界を生じさせるために前記第3の磁極に
対向配置され、 前記第5及び第6の磁極は前記第1の磁極と前記第4の
磁極との間に配置され且つ前記第1及び第2の高周波交
番磁界の広がりを制限するための高周波交番磁界を発生
するように設定され、前記第7及び第8の磁極は前記第
2の磁極と前記第3の磁極との間に配置され且つ前記第
1及び第2の高周波交番磁界の広がりを制限するための
高周波交番磁界を発生するように設定され、前記複数の
高周波交番磁界発生装置を順次に動作させることにより
前記複数の仮想直線の交差点に対応する前記局所を加熱
するように構成されていることを特徴とする導電性物体
内の局所加熱装置。
(6) A device for heating a local area within a conductive object, comprising a plurality of high frequency alternating magnetic field generating devices provided corresponding to a plurality of virtual straight lines passing through the local area, the high frequency alternating magnetic field generating device: The high-frequency alternating magnetic field generator is configured to generate a high-frequency alternating magnetic field for causing an eddy current to flow in the object, and the high-frequency alternating magnetic field generating device has a first magnetic field of a first polarity.
a second magnetic pole of a second polarity, a third magnetic pole of the first polarity, a fourth magnetic pole of the second polarity, a fifth magnetic pole of the first polarity, and a second magnetic pole of the first polarity. a sixth magnetic pole having a polarity of , a seventh magnetic pole having a second polarity, and an eighth magnetic pole having a first polarity, and the first magnetic pole is located on one side of the object. The second magnetic pole is arranged along the straight line on the other side of the object, and a first magnetic pole is disposed along the straight line on the other side of the object, and a first magnetic pole is disposed along the straight line on the other side of the object.
is arranged opposite to the first magnetic pole to generate a high-frequency alternating magnetic field, the third magnetic pole is arranged along the straight line on the other side of the object, and the fourth magnetic pole is arranged along the straight line on the other side of the object. a second magnetic pole disposed along the straight line on one side and between the third magnetic pole and the third magnetic pole;
are arranged to face the third magnetic pole in order to generate a high-frequency alternating magnetic field, and the fifth and sixth magnetic poles are arranged between the first magnetic pole and the fourth magnetic pole, and the fifth and sixth magnetic poles are arranged between the first and fourth magnetic poles. The seventh and eighth magnetic poles are arranged between the second magnetic pole and the third magnetic pole. and is set to generate a high frequency alternating magnetic field for limiting the spread of the first and second high frequency alternating magnetic fields, and by sequentially operating the plurality of high frequency alternating magnetic field generators, the plurality of virtual straight lines are A local heating device in a conductive object, characterized in that it is configured to heat the local area corresponding to an intersection.
(7)前記広がりを阻止するための高周波交番磁界は、
前記第1及び第2の高周波交番磁界に同期して発生する
ものである特許請求の範囲第6項記載の導電性物体内の
局所加熱装置。
(7) The high frequency alternating magnetic field for preventing the spread is:
7. The local heating device in a conductive object according to claim 6, which is generated in synchronization with the first and second high-frequency alternating magnetic fields.
JP17819185A 1985-08-13 1985-08-13 Method and apparatus for forming heat point in electromagnetic induction type hyperthermia Granted JPS6238179A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17819185A JPS6238179A (en) 1985-08-13 1985-08-13 Method and apparatus for forming heat point in electromagnetic induction type hyperthermia

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17819185A JPS6238179A (en) 1985-08-13 1985-08-13 Method and apparatus for forming heat point in electromagnetic induction type hyperthermia

Publications (2)

Publication Number Publication Date
JPS6238179A true JPS6238179A (en) 1987-02-19
JPH0463710B2 JPH0463710B2 (en) 1992-10-12

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JP17819185A Granted JPS6238179A (en) 1985-08-13 1985-08-13 Method and apparatus for forming heat point in electromagnetic induction type hyperthermia

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01185598A (en) * 1988-01-18 1989-07-25 Yoichi Kobayashi Voice recording and reproducing device for arousing safety driving of automobile

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01185598A (en) * 1988-01-18 1989-07-25 Yoichi Kobayashi Voice recording and reproducing device for arousing safety driving of automobile

Also Published As

Publication number Publication date
JPH0463710B2 (en) 1992-10-12

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