JPH0463710B2 - - Google Patents

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Publication number
JPH0463710B2
JPH0463710B2 JP17819185A JP17819185A JPH0463710B2 JP H0463710 B2 JPH0463710 B2 JP H0463710B2 JP 17819185 A JP17819185 A JP 17819185A JP 17819185 A JP17819185 A JP 17819185A JP H0463710 B2 JPH0463710 B2 JP H0463710B2
Authority
JP
Japan
Prior art keywords
magnetic pole
magnetic
frequency alternating
magnetic field
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.)
Expired
Application number
JP17819185A
Other languages
Japanese (ja)
Other versions
JPS6238179A (en
Inventor
Terutake Ueno
Kosuke Harada
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.)
Iwasaki Tsushinki KK
Original Assignee
Iwasaki Tsushinki KK
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 Iwasaki Tsushinki KK filed Critical Iwasaki Tsushinki KK
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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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電磁誘導で加
熱する装置に関し、更に詳細には、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
ために好適な装置に関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a device that heats a local area within a conductive object by electromagnetic induction, and more specifically, the present invention relates to a device that heats a local area within a conductive object by electromagnetic induction. The present invention relates to a device suitable for heat treating cancer.

〔従来の技術〕[Conventional technology]

正常な組織に比べて、ガン細胞や腫瘍は熱に弱
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℃
程度に上昇させて、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 tumors are more sensitive to heat than normal tissues. Research on hyperthermia, a cancer treatment method that utilizes this feature, has been attracting attention in recent years. This reduces the temperature of the lesion to 42°C to 45°C.
The aim is to increase the level of cancer cells to cause necrosis or to prevent their proliferation.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかし病巣部のみに熱点を集中させることは極
めて困難なため、このイパサーミア技術は未だ実
用化されていない。即ち、これまで組成の奥深く
に病巣がある場合、そこにのみ熱点を形成するこ
とは困難であつた。
However, because it is extremely difficult to concentrate the heat spot only on the lesion, this ipathermia technology has not yet been put into practical use. That is, until now, when there are foci deep within the composition, it has been difficult to form hot spots only there.

そこで、本発明の目的は、ガンの加熱治療、又
はこれ以外の医療や工業等に適用可能な導電性物
体内の局所加熱装置を提供することにある。
SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a local heating device within a conductive object that can be applied to heat treatment of cancer, or to other medical and industrial applications.

〔問題点を解決するための手段〕[Means for solving problems]

上記目的を達成するための本発明は、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
内の局所加熱装置に係わるものである。
To achieve the above object, the present invention is a device for heating a local area within a conductive object, which comprises 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 generator is configured to generate a high frequency alternating magnetic field for causing an eddy current to flow within the object,
Further, the high frequency alternating magnetic field generator has a first magnetic pole of the first polarity, a second magnetic pole of the second polarity, a third magnetic pole of the first polarity, and a fourth magnetic pole of the second polarity. a magnetic pole, a fifth magnetic pole of the first polarity, a sixth magnetic pole of the second polarity, a seventh magnetic pole of the second polarity, and a first magnetic pole.
and an eighth magnetic pole with a polarity of , the first magnetic pole is arranged along the straight line on one side of the object, and the second magnetic pole is arranged on the other side of the object with The third magnetic pole is arranged along a straight line and is arranged opposite to the first magnetic pole to generate a first high-frequency alternating magnetic field between the third magnetic pole and the third magnetic pole on the other side of the object. The fourth magnetic pole is arranged along the straight line on one side of the object and generates a second high-frequency alternating magnetic field between it and the third magnetic pole. The fifth and sixth magnetic poles are arranged opposite to the third magnetic pole for
The magnetic pole is disposed between the first magnetic pole and the fourth 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, Seventh and eighth magnetic poles are disposed between the second magnetic pole and the third magnetic pole, and are configured to generate a high frequency alternating magnetic field for limiting the spread of the first and second high frequency alternating magnetic fields. and is configured to heat the local area corresponding to the intersection of the plurality of virtual straight lines by sequentially operating the plurality of high frequency alternating magnetic field generators. This relates to local heating devices.

本発明の装置においては、第5,第6,第7及
び第8の磁極の効果によつて第1及び第2の高周
交番磁界の広がりが抑制され、微小部分の加熱が
可能になる。
In the device of the present invention, the spread of the first and second high-frequency alternating magnetic fields is suppressed by the effects of the fifth, sixth, seventh, and eighth magnetic poles, making it possible to heat a minute portion.

〔実施例〕〔Example〕

次に、図面を参照して本発明の1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、単純化して示されて例
えば頭部等の人体1内のガン病巣部2を加熱治療
する装置を示す。ガン病巣部2は、円柱状に示さ
れている人体1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3,4,5,6を設定し、各直線3,4,
5,6に沿つて4つの磁界発生装置7,8,9,
10を配置する。
Next, a method and apparatus for heating a lesion in a human body according to an embodiment of the present invention will be described with reference to the drawings. FIGS. 1 and 2 show, in a simplified manner, an apparatus for thermally treating a cancerous lesion 2 in a human body 1, for example the head. The cancer focus 2 is located at the center of the human body 1, which is shown in a cylindrical shape. When heating this lesion area 2, a plurality of virtual straight lines 3, 4, 5, 6 passing through this area are set, and each straight line 3, 4,
5, 6 along four magnetic field generators 7, 8, 9,
Place 10.

今、1つの磁界発生装置7を例にとつて説明す
ると、第1,第2,第3及び第4のコイル11,
12,13,14を有し、ここに高周波交流電源
15がスイツチS1を介して接続されている。第1
のコイル11は直線3に沿つて人体1の一方の側
に配置され、第2のコイル12は直線3に沿つて
人体1の他方の側に配置されている。第3のコイ
ル13は直線3に沿つて人体1の他方の側に配置
され、第4のコイル14は直線3に沿つて人体1
の一方の側に配置されている。第1のコイル11
と第4のコイル14、及び第2のコイル12と第
3のコイル13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のコイル11,1
2,13,14は、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。これ等のコイル11〜14にスイツチS1を介
して例えば105以上の高周波電流が電源15によ
つて流されると、ある瞬時において矢印16で示
す第1の高周波交番磁界と、矢印17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
コイル11の人体側に生じる第1の磁極はN極と
なり、第2のコイル12の人体側に生じる第2の
磁極はS極となり、第3のコイル13の人体側に
生じる第3の磁極はN極となり、第4のコイル1
4の人体側に生じる第4の磁極はS極となる。
Now, to explain one magnetic field generator 7 as an example, the first, second, third and fourth coils 11,
12, 13, and 14, to which a high frequency AC power source 15 is connected via a switch S1 . 1st
The second coil 11 is placed on one side of the human body 1 along the straight line 3, and the second coil 12 is placed on the other side of the human body 1 along the straight line 3. The third coil 13 is placed on the other side of the human body 1 along the straight line 3, and the fourth coil 14 is placed on the other side of the human body 1 along the straight line 3.
is placed on one side of the first coil 11
and the fourth coil 14, and the second coil 12 and the third coil 13 are arranged in parallel with an interval determined according to the size of the cancerous lesion 2. First, second, third and fourth coils 11, 1
2, 13, and 14 are sequentially connected in series so as to have a first polarity, a second polarity, a first polarity, and a second polarity based on the direction toward the human body 1. When a high frequency current of, for example, 10 5 or more is applied to these coils 11 to 14 by the power supply 15 via the switch S 1 , at a certain instant a first high frequency alternating magnetic field as shown by the arrow 16 and a first high frequency alternating magnetic field as shown by the arrow 17 are generated. Second
A high frequency alternating magnetic field is generated. At this time, the first magnetic pole generated on the human body side of the first coil 11 becomes the north pole, the second magnetic pole generated on the human body side of the second coil 12 becomes the south pole, and the third magnetic pole generated on the human body side of the third coil 13 becomes the north pole. The resulting third magnetic pole becomes the N pole, and the fourth coil 1
The fourth magnetic pole generated on the human body side of No. 4 is the S pole.

第1及び第2の高周波交番磁界16,17の中
心は、仮想直線3に沿つてはいるが一致はしてお
らず、病巣部2を挾み込むように延びている。第
1の高周波交番磁界16と第2の高周波交番磁界
17とは180度の位相差即ち逆相関係になつてい
る。従つて、第1及び第2の高周波交番磁界1
6,17で挾ま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2は導電性を有しているので、高周波磁界
に基づく電磁誘導によつて渦電流が発生する。上
述の如く渦電流が発生すると、ジユール熱が発生
し、温度が上昇する。
The centers of the first and second high-frequency alternating magnetic fields 16 and 17 are along the virtual straight line 3 but do not coincide, and extend so as to sandwich the lesion 2 . The first high-frequency alternating magnetic field 16 and the second high-frequency alternating magnetic field 17 have a phase difference of 180 degrees, that is, have an antiphase relationship. Therefore, the first and second high frequency alternating magnetic fields 1
The eddy current in the columnar part sandwiched between 6 and 17 is stronger than in other parts. Note that since the human body and the cancerous lesion 2 are electrically conductive, eddy currents are generated by electromagnetic induction based on the high-frequency magnetic field. When eddy currents are 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7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大きさ、コイル11〜14
の巻き数を決定することである。従つて、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℃)ま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4,5,6に
おける磁界発生装置8,9,10によつても高周
波交番磁界を発生させる。これにより、各高周交
番磁界の交差点領域即ち遁巣部2の温度を他に比
べて大幅に高することが出来る。
What is important here is that the magnitude of the high-frequency current and the coils 11 to 14 should be adjusted so that normal parts of the human body 1 will not be destroyed due to temperature rise caused by a single magnetic field generator 7.
The first step is to determine the number of turns. Therefore, a single magnetic field generator 7 can reach the required temperature (42
It is difficult to raise the temperature to 45°C. Therefore, high-frequency alternating magnetic fields are also generated by magnetic field generators 8, 9, and 10 on other straight lines 4, 5, and 6 that intersect the lesion 2. As a result, the temperature of the intersection region of each high-frequency alternating magnetic field, that is, the temperature of the escape nest portion 2 can be made significantly higher than that of the other regions.

18,19,20,21は第5,第6,第7及
び第8のコイルであり、第1及び第2の高周波交
番磁界16,17の広がりを制限するために設け
られている。第1図で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11〜14と同一の電源15に接続されて
いる。そして、第5,第6,第7及び第8のコイ
ル18,19,20,21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18〜21
の極性が決定されている。従つて、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18,19,20,21はN極、
S極、S極、N極になる。この第5〜第8のコイ
ル18〜21の磁極の強さは、第1及び第2の高
周波交番磁界16,17の広がりを制限するよう
に設定されている。即ち、第1の磁極P1と第4
の磁極P4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めに、同極性で互いに
隣接された第1の磁極P1と第5の磁極P5との反
発作用、及び第4の磁極P4と第6の磁極P6との
反発作用を利用している。右側の第7及び第8の
磁極P7,P8も同様に利用されている。なお、第
5及び第6の磁極P5,P6の強さは、これ等の相
互間に磁束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P7,P8の強さも同様に
設定されている。
18, 19, 20, and 21 are fifth, sixth, seventh, and eighth coils, which are provided to limit the spread of the first and second high-frequency alternating magnetic fields 16, 17. Although wiring is omitted in FIG. 1, specifically, as shown in FIG. 3, the coils are connected to the same power source 15 as the first to fourth coils 11 to 14. The fifth, sixth, seventh, and eighth coils 18, 19, 20, and 21 have a first polarity, a second polarity, a second polarity, and a third polarity based on the side facing the human body 1. Connect each coil 18 to 21 so that the polarity is
The polarity of is determined. Therefore, at a certain moment, as shown in FIG. 3, the fifth, sixth, seventh and eighth coils 18, 19, 20, 21 have N poles
It becomes S pole, S pole, N pole. The strength of the magnetic poles of the fifth to eighth coils 18 to 21 is set so as to limit the spread of the first and second high frequency alternating magnetic fields 16 and 17. That is, the first magnetic pole P 1 and the fourth
In order to limit the flow of magnetic flux between the two magnetic poles P4 when they approach each other, repulsion between the first magnetic pole P1 and the fifth magnetic pole P5 , which are adjacent to each other and have the same polarity, and The repulsion between the fourth magnetic pole P 4 and the sixth magnetic pole P 6 is utilized. The seventh and eighth magnetic poles P 7 and P 8 on the right are also utilized in the same way. Note that the strengths of the fifth and sixth magnetic poles P 5 and P 6 are set so that a flow of magnetic flux occurs between them. The strengths of the seventh and eighth magnetic poles P 7 and P 8 are similarly set.

第1図において、第2の磁界発生装置8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の磁界発生装置7の第1〜第8のコ
イル11,12,13,14,18,19,2
0,21に対応して、第9〜第16のコイル11
a,12a13a,14a,18a,19a,2
0a,21aを有する。この第2の磁界発生装置
8は、第1及び第2の高周波交番磁界16,17
に直交する方向に第3及び第4の高周波交番磁界
16a,17aを発生させる点を除いては、第1
の磁界発生装置7と同一である。従つて、その詳
しい説明を省略する。
In FIG. 1, the second magnetic field generator 8 is arranged at an angular position perpendicular to the first magnetic field generator 7, and the first to eighth coils 11, 12 of the first magnetic field generator 7 ,13,14,18,19,2
0, 21, the 9th to 16th coils 11
a, 12a 13a, 14a, 18a, 19a, 2
It has 0a and 21a. This second magnetic field generator 8 generates first and second high frequency alternating magnetic fields 16, 17.
Except for generating third and fourth high-frequency alternating magnetic fields 16a and 17a in a direction perpendicular to the first
This is the same as the magnetic field generating device 7 of . Therefore, detailed explanation thereof will be omitted.

第3及び第4の磁界発生装置9,10は、第1
及び第2の磁界発生装置7,8の相互間に配置さ
れている。そして、病巣部2の立体的加熱を強め
るために、第3及び第4の磁界発生装置9,10
の各コイルは垂直軸(Z軸)方向に並置されてい
る。従つて、第1図には上側になるコイルのみが
示されている。第2図は第1図の−線から見
た第3の磁界発生装置9と人体1との関係を示
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11〜14、及び第5〜第8のコ
イル18〜21に対応して第17〜第20のコイル1
1b,12b,13b,14b及び第21〜第24の
コイル18b,19b,20b,21bが夫々設
けられている。これにより、矢印16a,17a
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
16b,17b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図でコイル11
c,12cのみで示す第4の磁界発生装置10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。
The third and fourth magnetic field generators 9 and 10 are
and second magnetic field generators 7 and 8. In order to intensify the three-dimensional heating of the lesion 2, third and fourth magnetic field generators 9 and 10 are installed.
The coils are arranged in parallel in the vertical axis (Z-axis) direction. Therefore, only the upper coil is shown in FIG. FIG. 2 shows the relationship between the third magnetic field generator 9 and the human body 1 as seen from the - line in FIG. The 17th to 20th coils 1 correspond to the first, second, third, and fourth coils 11 to 14 and the fifth to eighth coils 18 to 21 of the first magnetic field generator 7.
1b, 12b, 13b, 14b and 21st to 24th coils 18b, 19b, 20b, 21b are provided, respectively. As a result, arrows 16a and 17a
As shown in FIG. 2, fifth and sixth high frequency alternating magnetic fields are generated. The configuration and operation of the third magnetic field generator 9 are the same as the first magnetic field generator 7 except that the fifth and sixth high frequency alternating magnetic fields 16b, 17b are generated at different angles. Coil 11 in Figure 1
The fourth magnetic field generating device 10, indicated only by c and 12c, is also configured essentially the same as the first magnetic field generating device 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のスイツチS1,S2,S3
び図示されていない第4のスイツチの切り替えに
よつて、第1〜第4の磁界発生装置7〜10に時
間差を有して順次に高周波電流を流す。これによ
り、電磁誘導で渦電流が発生し、ジユール熱でガ
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7〜10のいずれに電流を流しても
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、周辺を冷却するよ
うにしてもよい。
When heating the cancer lesion 2 with the apparatus shown in FIGS. 1 to 3, by switching the first to third switches S 1 , S 2 , S 3 and a fourth switch (not shown), A high frequency current is sequentially applied to the first to fourth magnetic field generators 7 to 10 with a time difference. As a result, an eddy current is generated due to electromagnetic induction, and the cancer focus portion 2 is heated by Joule heat. At this time, no matter which of the first to fourth magnetic field generators 7 to 10 is supplied with current, an eddy current flows through the cancer focus area 2, so that the temperature of the cancer focus area 2 becomes the highest. At this time, cancer focus area 2
In addition, eddy currents flow and the temperature rises, but since the heating caused by the eddy currents is not superimposed, the temperature does not become very high. Note that the heating area is the cancer lesion area 2.
If it protrudes significantly from the surface, the surrounding area may be cooled.

高周波交番磁界の周数を高くすれば、渦電流に
よる発熱効果も上る。この時、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。即
ち、病巣部が人体の奥深くある場合、高周磁界を
印加すると、病巣部に熱点を形成することができ
ない場合がある。しかし、100MHzに満たない周
波数においては表皮効果を殆んど無視することが
できる。
If the frequency of the high-frequency alternating magnetic field is increased, the heat generation effect due to eddy currents will also increase. At this time, it is thought that eddy currents concentrate near the conductor surface due to the skin effect. That is, when a lesion is located deep within the human body, applying a high frequency magnetic field may fail to form a hot spot at the lesion. However, at frequencies below 100MHz, the skin effect can be almost ignored.

生体内の温度上昇を妨げる要因として血流によ
る冷却効果があるが、これを無視して表皮からの
深さが0.05mの点の病巣部の温度を5℃上昇させ
るために要する時間を、外部磁界B0=1mT、比
熱C=4.19×103J・K-1・g-1、密度D=1.01gcm
-3、周波数50MHzの条件で求めると、約770msと
なる。従つて、血流による冷却効果があつても、
熱点形成は十分可能である。また病巣部の場所と
病状が許される場合には一時的な止血またはレー
ザ光線または温湯等との併用もできる。
The cooling effect of blood flow is a factor that prevents temperature rise in the body, but ignoring this, the time required to raise the temperature of the lesion at a depth of 0.05 m from the epidermis by 5°C is calculated as Magnetic field B 0 = 1 mT, specific heat C = 4.19×10 3 J・K -1・g -1 , density D = 1.01 gcm
-3 , it is approximately 770ms when calculated under the condition of a frequency of 50MHz. Therefore, even though there is a cooling effect due to blood flow,
Hot spot formation is fully possible. In addition, if the location of the lesion and the medical condition permit, temporary hemostasis can be achieved, and laser beams, hot water, etc. can be used in combination.

上述から明らかな如く、本治療法では、放射線
や薬剤を使用しないので、副作用が極めて少な
い。従つて、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。
As is clear from the above, this treatment method does not use radiation or drugs, so there are very few side effects. Therefore, great effects can be expected for cancer heating 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16と第2の高周
波交番磁界17とで挾まれた領域の渦電流密度が
大になることを、第4図〜第6図によつて説明す
る。第4図及び第5図はx軸方向及びy軸方向に
±8の目盛が付された正方形の導体板22の中心
x=y=0の近傍の電流密度を上昇させる方法を
示す。導体板22として導電率及び透磁率が共に
均一の2次元の導体板を用意し、全体に均一な磁
界H0を印加しておく。また第4図及び第5図に
斜線で示す二つの小領域23,24には均一磁界
H0に加えて、更に局所磁界HA,HBをそれぞれ第
5図の矢印の向きに印加する。即ち、一方には
H0と同位相の局所磁界HAを、他方にはH0と反位
相の局所磁界HBを印加する。この局所磁界HA
HBの発生は、いずれも例えば空芯コイル(図示
せず)を導体板22の上下に置き、これを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22のy軸上の渦電流密度を計算により求めた
結果である。ここで局所磁界HA,HBを|HA|=
|HB|=a|H0|としてa=1とa=10の場合
の渦電流密度を夫々求め、特性線25によりa=
10の場合の結果を示し、特性線26によりa=1
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,HBの振幅が小さい場合(即ちa=
1)には局所磁界HA,HBの影響は小さく、中心
y=0近傍の電流密度は増加しないが、局所磁界
HA,HBの振幅が大きい場合(即ちa=10)には
局所磁界の影響が大きく、中心y=0近傍で二つ
の電流ループが集合して大きな電流密度を得るこ
とができることが判る。
Next, the fact that the eddy current density in the region sandwiched between the first high-frequency alternating magnetic field 16 and the second high-frequency alternating magnetic field 17 becomes large will be explained with reference to FIGS. 4 to 6. FIGS. 4 and 5 show a method of increasing the current density near the center x=y=0 of a square conductor plate 22 with scales of ±8 in the x-axis and y-axis directions. A two-dimensional conductor plate having uniform conductivity and magnetic permeability is prepared as the conductor plate 22, and a uniform magnetic field H 0 is applied to the entire conductor plate. In addition, there is a uniform magnetic field in the two small areas 23 and 24 indicated by diagonal lines in FIGS. 4 and 5.
In addition to H 0 , local magnetic fields H A and H B are applied in the directions of the arrows in FIG. 5, respectively. That is, on the one hand
A local magnetic field H A having the same phase as H 0 is applied to the other, and a local magnetic field H B having the opposite phase to H 0 is applied to the other. This local magnetic field H A ,
To generate H B , for example, air-core coils (not shown) are placed above and below the conductor plate 22 and used as a pair. FIG. 6 shows the result of calculating the eddy current density on the y-axis of the two-dimensional conductor plate 22 shown in FIG. Here, the local magnetic fields H A , H B are |H A |=
|H B |=a|H 0 |, calculate the eddy current density for a=1 and a=10, and use the characteristic line 25 to find a=
The results are shown for the case of 10, and a=1 according to the characteristic line 26.
The results are shown for the case. As is clear from Fig. 6, when the amplitudes of the local magnetic fields H A and H B are small (i.e. a=
In 1), the influence of local magnetic fields H A and H B is small, and the current density near the center y = 0 does not increase, but the local magnetic fields
It can be seen that when the amplitudes of H A and H B are large (ie, a=10), the influence of the local magnetic field is large, and two current loops gather near the center y=0, making it possible to obtain a large current density.

従つて、局所磁界HA,HBが高周波電流の印加
によつて、その電流の向きに対応して変化するた
め、導体板22の端に比べてy=0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
て渦電流の増加によるいわゆる熱点が形成され
る。ここで均一磁界H0は局所磁界HA,HBの振幅
の大小による渦電流の発生効率を理論検討するた
めに導入したものであるから、実際の場合には不
要である。
Therefore, as the local magnetic fields H A and H B change depending on the direction of the current due to the application of the high-frequency current, a large change in the magnetic field occurs near y=0 compared to the end of the conductor plate 22. As a result, so-called hot spots are formed due to an increase in eddy currents. Here, the uniform magnetic field H 0 is introduced to theoretically study the efficiency of eddy current generation depending on the magnitude of the amplitude of the local magnetic fields H A and H B , so it is not necessary in an actual case.

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16,17に対応するので、第1
及び第2の高周波交番磁界16,17に挾まれた
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1内の病巣部2を加熱する必
要があるので、第4図及び第5図をそのまま適用
しても病巣部2のみ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。
The local magnetic fields H A and H B correspond to the first and second high-frequency alternating magnetic fields 16 and 17 in FIG.
It is clear that the eddy current density in the region sandwiched by the second high-frequency alternating magnetic fields 16 and 17 increases. In FIG. 1, it is necessary to heat the lesion 2 within the human body 1, so even if FIGS. 4 and 5 are applied as they are, it is impossible to heat only 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、例えば次の変形例が可能なものである。
The present invention is not limited to the embodiments described above, and the following modifications are possible, for example.

(a) 第7図に示す如く、磁心27,28,29,
30を設け、ここにコイル31,32,33,
34を巻き回し、スイツチS1を介して電源15
から高周波電流を流し、第3図の場合と同様に
第1〜第8の磁極P1〜P8を形成してもよい。
(a) As shown in Figure 7, magnetic cores 27, 28, 29,
30 is provided, and coils 31, 32, 33,
Wind up 34 and connect power supply 15 via switch S1.
The first to eighth magnetic poles P 1 to P 8 may be formed by flowing a high frequency current through the magnetic poles as in the case of FIG. 3.

(b) 第1図に示す、複数の磁界発生装置7〜10
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、異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
周波交番磁界を発生させた後に、第3及び第4
の高周波交番磁界、更に、第5及び第6の高周
波交番磁界を発生するようにしてもよい。
(b) A plurality of magnetic field generators 7 to 10 shown in FIG.
Instead of providing a magnetic field generating device 7, one magnetic field generating device 7 may be rotated around the lesion 2 to apply a high frequency alternating magnetic field from different angular positions. That is, after generating the first and second high frequency alternating magnetic fields with a single magnetic field generating device, the third and fourth high frequency alternating magnetic fields are generated.
A fifth and a sixth high frequency alternating magnetic field may be generated.

(c) 第3図において第5〜第8の磁極P5〜P8
強さを更に強め、磁束(磁力線)が病巣部2の
近傍までU字状にくい込むようにしてもよい。
(c) In FIG. 3, the strength of the fifth to eighth magnetic poles P 5 to P 8 may be further strengthened so that the magnetic flux (lines of magnetic force) penetrates into the vicinity of the lesion 2 in a U-shape.

(d) 病巣部2の大きさに対応させて磁極P1とP4
の間隔、P2とP3の間隔を調整できるようにし
てもよい。また、磁極P1とP2,P3とP4を対向
配置させないで、第1及び第2の高周波交番磁
界を得てもよい。
(d) Magnetic poles P 1 and P 4 corresponding to the size of lesion 2
The interval between P 2 and P 3 may be adjustable. Furthermore, the first and second high-frequency alternating magnetic fields may be obtained without arranging the magnetic poles P 1 and P 2 and P 3 and P 4 facing each other.

〔発明の効果〕〔Effect of the invention〕

上述から明らかな如く、本発明によれば、立体
的物体内部の局所を容易に加熱することができ
る。従つて、ガンの加熱治療等に極めて有益であ
る。
As is clear from the above, according to the present invention, it is possible to easily heat a local area inside a three-dimensional object. Therefore, it is extremely useful for heat treatment of cancer, etc.

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

第1図は本発明の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−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1つを詳しく示す平面図、第4図は2次元の導
体板における渦電流の密度を求めるための導体板
と局所磁界との関係を示す平面図、第5図は第4
図のy軸上の断面図、第6図は第4図の導体板の
y軸上の位置と渦電流密度との関係を示す図、第
7図は変形例の磁界発生装置を示す平面図であ
る。 1…人体、2…ガン病巣部、3,4,5,6…
仮想直線、7,8,9,10…磁界発生装置、1
1…第1のコイル、12…第2のコイル、13…
第3のコイル、14…第4のコイル、15…電
源、16…第1の高周波交番磁界、17…第2の
高周波交番磁界、18…第5のコイル、19…第
6のコイル、20…第7のコイル、21…第8の
コイル。
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 the - line in FIG. Fig. 4 is a plan view showing the relationship between the conductor plate and the local magnetic field for determining the density of eddy current in a two-dimensional conductor plate, and Fig. 5 is a plan view showing the first one in detail.
6 is a diagram showing the relationship between the position of the conductor plate on the y-axis of FIG. 4 and the eddy current density, and FIG. 7 is a plan view showing a modified magnetic field generator. It is. 1...Human body, 2...Cancer lesion, 3, 4, 5, 6...
Virtual straight line, 7, 8, 9, 10...Magnetic field generator, 1
1...first coil, 12...second coil, 13...
Third coil, 14... Fourth coil, 15... Power supply, 16... First high frequency alternating magnetic field, 17... Second high frequency alternating magnetic field, 18... Fifth coil, 19... Sixth coil, 20... 7th coil, 21...8th coil.

Claims (1)

【特許請求の範囲】 1 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の高周波交番磁極を生じさせるた
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。 2 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第1項記載の導
電性物体内の局所加熱装置。
[Scope of Claims] 1. 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, and the high-frequency alternating magnetic field The generator is configured to generate a high frequency alternating magnetic field for causing an eddy current to flow within the object, and the high frequency alternating magnetic field generator has a first magnetic pole of a first polarity and a second magnetic pole of a second polarity. a second magnetic pole;
a third magnetic pole of the first polarity, a fourth magnetic pole of the second polarity, a fifth magnetic pole of the first polarity, a sixth magnetic pole of the second polarity, and a third magnetic pole of the second polarity. 7 magnetic poles and an eighth magnetic pole of a first polarity, the first magnetic pole is arranged along the straight line on one side of the object, and the second magnetic pole is arranged along the straight line on one side of the object. The third magnetic pole is disposed along the straight line on the other side of the object and is disposed opposite to the first magnetic pole in order to generate a first high-frequency alternating magnetic pole between the first magnetic pole and 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 one side of the object, and a second magnetic pole is arranged between the fourth 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. 2. The local heating device in a conductive object according to claim 1, wherein the high frequency alternating magnetic field for preventing the spread 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 JPS6238179A (en) 1987-02-19
JPH0463710B2 true JPH0463710B2 (en) 1992-10-12

Family

ID=16044183

Family Applications (1)

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

Country Status (1)

Country Link
JP (1) JPS6238179A (en)

Families Citing this family (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

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Publication number Publication date
JPS6238179A (en) 1987-02-19

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