JPS59105464A - Electromagnetic wave generator for heat treatment - Google Patents
Electromagnetic wave generator for heat treatmentInfo
- Publication number
- JPS59105464A JPS59105464A JP21630882A JP21630882A JPS59105464A JP S59105464 A JPS59105464 A JP S59105464A JP 21630882 A JP21630882 A JP 21630882A JP 21630882 A JP21630882 A JP 21630882A JP S59105464 A JPS59105464 A JP S59105464A
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- JP
- Japan
- Prior art keywords
- antenna
- dielectric
- electromagnetic wave
- wave generator
- excitation
- 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.)
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- Thermotherapy And Cooling Therapy Devices (AREA)
- Radiation-Therapy Devices (AREA)
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、人体の癌組織に電磁波を照射して所定温度に
加熱することで癌細胞の再生機能を停止させて致死に至
らせる温熱療法に用いられる電磁波発生器に関す、る。Detailed Description of the Invention The present invention relates to an electromagnetic wave generator used in thermotherapy, which irradiates cancerous tissue in the human body with electromagnetic waves and heats it to a predetermined temperature, thereby stopping the regenerative function of cancer cells and causing death. Related, Ru.
近年、′#:の治療に−′)いて温熱処理が極めて有効
的であることが注目され、悪性腫瘍を約43℃付近の温
度に必要な時間だけ加熱覆る温熱療法の開発が進められ
ている。In recent years, heat treatment has attracted attention as being extremely effective in the treatment of ``#:-''), and efforts are being made to develop heat therapy that heats malignant tumors to a temperature around 43°C for the necessary time. .
このような温熱処理については、一般1こ一対の電極板
で人体を挾んで加温する電界加熱方式、電磁−コイル内
に人体を入れて加温するM L9加加熱式、更に電[<
k波を人体に放射して加温する電磁波加熱方式が71F
+ ?)、7[界及び誘導加熱方式にあっては、体内の
癌1mのみを集中的に加熱するスポット的加熱が困テU
であることから人体のかなりの広範囲を加温づるのに用
いられ、一方、電磁波方式にあっては、電磁波をビーム
集束させることが可能であることから癌組織の掻く近傍
のみを加温する局所加温への利用が考えられている。For such thermal treatment, there are generally electric field heating methods that heat the human body by sandwiching it between a pair of electrode plates, M L9 heating methods that heat the human body by placing it in an electromagnetic coil, and electric field heating methods that heat the human body by placing it in an electromagnetic coil.
71F is an electromagnetic wave heating method that radiates K-waves to the human body to heat it.
+? ), 7 [With field and induction heating methods, spot heating that intensively heats only 1 m of cancer within the body is difficult.
Because of this, it is used to heat a fairly wide area of the human body.On the other hand, with electromagnetic waves, it is possible to focus the electromagnetic waves, so it is possible to heat only the area near the cancerous tissue. It is being considered for use in heating.
ところで、電磁波方式により温熱療法を行なう!問合、
一番手型な構成機器はマイクロ波のLネルギを生体に加
えるための素子としての電磁波発生器であり、こtlも
一般にアプリケータど呼ばれている。By the way, heat therapy is performed using electromagnetic waves! Inquiry,
The most basic type of component is an electromagnetic wave generator as an element for applying microwave L energy to a living body, and this TL is also generally called an applicator.
この電磁波発生器としては従来第1図に示す電磁ホーン
が使用されている。第1図において、電磁ホーン1 t
;L >9波管コネクク4を設けた給電部3とマイクロ
波エネルギを放射するホーン2とで構成され、ホーン2
の内部には第2図に示すように人体との整合をとるため
に高誘電体5を装荷している。As this electromagnetic wave generator, an electromagnetic horn shown in FIG. 1 has conventionally been used. In Fig. 1, an electromagnetic horn 1 t
; L > 9 Consists of a power feeding unit 3 provided with a wave tube connector 4 and a horn 2 that radiates microwave energy, the horn 2
As shown in FIG. 2, a high dielectric material 5 is loaded inside the device to ensure matching with the human body.
この高誘電体5は人体の比誘電率とほぼ同稈酊の比誘電
率をもった高誘電物質で作られており、給電部3に設け
た導波管との整合は高誘電体5を図示のテーパ形状とす
ることで実現している。This high-permittivity material 5 is made of a high-permittivity material with a relative permittivity that is almost the same as that of the human body, and matching with the waveguide provided in the power feeding section 3 is achieved by using the high-permittivity material 5. This is achieved by creating the tapered shape shown in the figure.
第3図は従来の電磁ホーン1を用いた温熱療法の説明図
であり、電磁ホーン1と人体6との間に冷却用の水膜7
を介在して癌11#1li8に向けてマイクロ波を照射
し、癌相8Bを必要な時間だけ43℃付近に加温すると
、癌細胞の再生機能が失われ、細胞致死効果が得られる
。FIG. 3 is an explanatory diagram of thermotherapy using a conventional electromagnetic horn 1, in which a cooling water film 7 is provided between the electromagnetic horn 1 and the human body 6.
By irradiating the cancer 11#1li8 with microwaves and heating the cancer phase 8B to around 43° C. for the necessary time, the cancer cell regeneration function is lost and a cell killing effect is obtained.
ところが、従来の電磁ホーンを用いた電磁波発生器にあ
っては、使用周波数を2Gl−tz以上にしないと電磁
ホーンが人体に電磁波を人11)j g−せるには不都
合な程大型化する欠点があるため、従来は医療用として
使用が許されている2、45Gl−1zの周波数イ・使
用することでホキ1化を実現している。However, the disadvantage of conventional electromagnetic wave generators using electromagnetic horns is that unless the operating frequency is set to 2Gl-tz or higher, the size of the electromagnetic horn becomes inconvenient for transmitting electromagnetic waves to the human body. Therefore, by using the frequency of 2,45Gl-1z, which has been allowed to be used for medical purposes, it is possible to achieve the standardization.
しかし、人体に対する電磁波の浸透度は周波数が高い稈
浅くなり、2’、 、45 G H7では人体表面層で
の滅駒が大ぎく約2CIHの深さまでしか加温できない
という状況にある。However, the penetration of electromagnetic waves into the human body becomes shallower when the frequency is higher, and in 2', , 45 GH7, the surface layer of the human body is severely damaged and heating is only possible to a depth of about 2 CIH.
勿論、使用周波数を低くすれば、例えば434M l−
l zで約5cmというように加温できる深さを焉める
ごどができるが、前述したようにメガヘルツオーダで(
ユ電磁ホーンが極めて大型化し、側底人体に電磁波を入
射さける@蒸装置としての実用化は内勤であった。Of course, if the frequency used is lowered, e.g. 434M l-
It is possible to limit the depth that can be heated, such as about 5 cm in lz, but as mentioned above, in the megahertz order (
The electromagnetic horn became extremely large, and it was an office job to put it to practical use as a steaming device that prevents electromagnetic waves from entering the human body.
本発明(,15、このような従来の問題点に鑑みてなさ
れたもので、人体に電磁波が充分に浸透できるメガl\
ルツΔ−グの周波数で使用でき月つド療用として充分に
小型化された温熱療法用電磁波発生器を提供することを
目的とする。The present invention (15) was made in view of these conventional problems, and is a mega l\\ that allows electromagnetic waves to sufficiently penetrate the human body.
It is an object of the present invention to provide an electromagnetic wave generator for thermotherapy that can be used at a frequency of 100 Hz and is sufficiently miniaturized for medical treatment.
この目的を達成するため本発明は、通信用に用いられて
いる誘電体アンテナの逆の使用法、すなわち、電磁波の
外部に対する放躬効室を通信用とは逆に極力下げて放射
エネルギを誘電体の内部に封じ込める手法を基本とし、
一端に敢躬面を形成した人体の比誘電率に略等しい比誘
電率をもった柱状誘電体の内部に励振アンテナを114
じ込め、41状誘電体の外部に引出された給電線により
500MHz以下の周波数で励振して人体に電磁]ネル
ギを集中して放射づ′るように(ッlJものである。To achieve this objective, the present invention proposes the reverse use of the dielectric antenna used for communication, that is, the radiation effect chamber for external electromagnetic waves is reduced as much as possible to reduce the radiated energy to the dielectric antenna. Based on the method of sealing it inside the body,
An excitation antenna 114 is installed inside a columnar dielectric material having a dielectric constant approximately equal to that of the human body and having a dielectric constant formed on one end.
It is designed to concentrate and radiate electromagnetic energy to the human body by exciting it at a frequency of 500 MHz or less using a power supply line drawn out to the outside of the 41-shaped dielectric.
以下、本発明の実施例を図面に基づい°C説明する。Hereinafter, embodiments of the present invention will be explained based on the drawings.
第4図は本発明の一実施例を示した斜視図である。FIG. 4 is a perspective view showing an embodiment of the present invention.
まず、構成を説明1゛ると、10は円形断面を有する柱
状誘電体であり、一端に人体に電磁波エネルギを放射す
るための放射面12を形成しており、放射面12に相対
した反対側にはループアンテナ14が励振アンテナとし
て柱状誘電体10内に封じ込められでおり、ループアン
テナ14よりは一対の給電線16が外部に引き出されて
いる。 ここて11状誘電体10は人体組織とほぼ同程
度の比誘電率εrをもった誘電物質で作られており、人
捧絹tr&の実効的な比誘電率は非常に高く、ε−80
−ヘ・100稈mであることから、この人体組織の比誘
電二↑゛に13Lぽ等しい例えばεr =80とkる誘
電物質をもって卆1状誘電体10は作られている。First, to explain the configuration, 10 is a columnar dielectric body with a circular cross section, and one end forms a radiation surface 12 for radiating electromagnetic wave energy to the human body, and the opposite side to the radiation surface 12 A loop antenna 14 is enclosed within the columnar dielectric 10 as an excitation antenna, and a pair of feed lines 16 are drawn out from the loop antenna 14. Here, the 11-shaped dielectric body 10 is made of a dielectric material having a dielectric constant εr that is approximately the same as that of human tissue, and the effective dielectric constant of human silk tr& is extremely high, ε-80.
Since the diameter is 100 m, the rectangular dielectric 10 is made of a dielectric material with a dielectric material of εr = 80, for example, which is equal to 13L to the dielectric constant of this human tissue.
勿論、(1状誘電体10は人体組織とほぼ等しい稈rσ
の圧管IIを右回ると共に誘電損失の少ない誘電体シイ
刊を用いているしのである。Of course, (the one-shaped dielectric 10 has a culm rσ almost equal to human tissue)
The pressure tube II is rotated clockwise and a dielectric material with low dielectric loss is used.
−八、柱状誘電体10に封じ込められたループアシ1′
)14は500Ml−1zJx下の電磁波を効率よく(
1状誘電体10を誘電体導波器として人体に電磁波を伝
110させる励振特性をhし、ループアンテナ14の大
きさは500 M ’l−I Z以下の周波数帯で使用
されている人気中に設置されている通信用のループアン
テナの大きさに対し、柱状誘電体10の比誘電率εrで
定まる1/J″TF、即ちεr−80とMるど約1./
9の大きざで実現できる。-8. Loop reed 1' enclosed in columnar dielectric 10
)14 efficiently transmits electromagnetic waves under 500Ml-1zJx (
The mono-shaped dielectric 10 is used as a dielectric waveguide to transmit electromagnetic waves to the human body with excitation characteristics 110, and the size of the loop antenna 14 is a popular antenna used in a frequency band of 500 M'l-IZ or less. For the size of a communication loop antenna installed in
This can be achieved with a size of 9.
又ループアンテナ14に対〜η−る給電線16による励
振信号の供給は使用周波数が500 M t−1z以下
であることから、同軸/7−プルを整合回路を介して給
電線。1Gに接続することで行なう。Furthermore, since the frequency used is less than 500 Mt-1z, the excitation signal is supplied to the loop antenna 14 by the feeder line 16 through a matching circuit using a coaxial/7-pull feeder. This is done by connecting to 1G.
次に本発明の詳細な説明する。Next, the present invention will be explained in detail.
柱状誘電体10に封じ込められたループアンテナ14の
励振でhり則された電磁波は、t11状誘電10内を伝
搬して人体に入射する電磁波エネルギと、誘電体10J
、り外部に放射される電磁波エネルギとなり、両名の関
係を説明すると、第5図の特性グラフに示ザ関係になる
。The electromagnetic waves harmonized by the excitation of the loop antenna 14 enclosed in the columnar dielectric 10 are divided into electromagnetic wave energy that propagates inside the T11-shaped dielectric 10 and enters the human body, and the dielectric 10J.
, is the electromagnetic wave energy radiated to the outside, and the relationship between the two is shown in the characteristic graph of FIG.
即15、第5図は誘電体の比誘電率εrに対する誘電体
内部の放射電力Wiと、誘電体外部に放射される放射電
力WOどの比を柱状誘電体直径を横軸にとって示したも
ので、通信用の誘電体アンテナにあっては使用する誘電
体の比誘電率εrを小さくすることにより放射電力比W
r/WOを1以下としているが、本発明においては柱状
M電体10の比誘電5(εrはεr =80と極めて高
いため、+1状誘電体の直径が同じでも放射電力比Wi
/WO°、10・−20程庶が1qられ、t↑状誘電
体10内を伝搬ηる放射電力Wiに対し柱状誘電体10
より人気中に放射される放射電力WOは1/10〜1
/ 20稈lqの極く僅かな放射電力に抑えられ、ルー
プアン7す14よりのb’l躬エネルギの大部分が柱状
誘電体10内を伝搬し−(放射面12より人体に入q・
1される。In other words, Fig. 5 shows the ratio of the radiated power Wi inside the dielectric to the dielectric constant εr and the radiated power WO radiated to the outside of the dielectric with the diameter of the columnar dielectric as the horizontal axis. In dielectric antennas for communication, the radiation power ratio W can be reduced by reducing the relative dielectric constant εr of the dielectric used.
Although r/WO is set to be less than 1, in the present invention, the relative dielectricity of the columnar M electric body 10 is 5 (εr = 80, which is extremely high, so even if the diameter of the +1-shaped dielectric body is the same, the radiation power ratio Wi
/WO°, 1q is increased by 10·-20, and the radiation power Wi propagating in the t↑-shaped dielectric 10 is
The radiated power WO during the more popular period is 1/10~1
The radiation power is suppressed to an extremely small amount of 20 lq, and most of the energy from the loop ann 7 and 14 propagates within the columnar dielectric 10 and enters the human body from the radiation surface 12.
1 will be given.
更にhY■Iに説明するならば、+1状誘電体10に月
じ込めらねたループアンテナ14より柱状誘電体10と
空気どの境界面に垂直に入削りる電磁波の入131力を
Pl、柱状誘電体10より大気中に成用される透過電力
をPL、界面で反則されて柱状誘電体10内に戻−)で
くる反o1電力をPrとした場合、次の関係式が成り)
’7つ、1(但し、εaは空気の比誘電イ゛(ε・1)
即ち、柱状誘電体10の比誘電率εI゛=80とすると
、
P i / P t −0、7988
となり、ループアンテナ14にす(1状誘電体10と空
気との界面に!1′!白に電磁波が入口J L、でも約
2割しか外部に放射されず、残りの8割はれ状誘電体1
0の内部に反6・1され、しかもループアンテナ14よ
りの電磁波が柱状誘電体10と空気との界面に垂直に入
射する部分μ極く僅かであり、他の部分は90度以下と
なる入剣角をもって入射していることから、(1状誘電
体10の外部に対する放射電力は更に小さなものとなり
、ループアンテナ171から放射され1.?電磁波エネ
ルギの約9割以上を柱状誘電体10内に封じ込めること
が出来る。Furthermore, to explain hY■I, the input 131 force of electromagnetic waves perpendicular to the interface between the columnar dielectric 10 and the air from the loop antenna 14 inserted into the +1-shaped dielectric 10 is Pl, the columnar dielectric 10 If the transmitted power transmitted from the dielectric 10 into the atmosphere is PL, and the inverse o1 power reflected at the interface and returned to the columnar dielectric 10 is Pr, the following relational expression holds.
'7, 1 (where εa is the dielectric constant of air (ε・1)
That is, if the dielectric constant εI'' of the columnar dielectric 10 is 80, then P i / P t -0, 7988, and the loop antenna 14 (at the interface between the 1-shaped dielectric 10 and air!1'! White) However, only about 20% of the electromagnetic waves are radiated to the outside at the entrance JL, and the remaining 80% is emitted from the flaky dielectric 1.
0, the electromagnetic wave from the loop antenna 14 is incident perpendicularly to the interface between the columnar dielectric 10 and the air in a very small part μ, and in other parts the angle of incidence is less than 90 degrees. Since it is incident at a sword angle, the radiated power to the outside of the columnar dielectric 10 becomes even smaller, and approximately 90% or more of the electromagnetic wave energy radiated from the loop antenna 171 is transmitted into the columnar dielectric 10. It can be contained.
一方、第4図に示した本発明の電磁波発りに器による人
体の温熱治療に際しては第3図に示したと同様に柱状誘
電体10の放射面12と人体どの問に冷7.II用の水
膜を介在させて電磁波を人体に入則さ1!るようになる
が、水の誘電率εWはεw=80.7とほぼ+1状誘電
体10の比誘電fεrに等しいことから、水膜を介在さ
せたことにJ:る反qi11(′1失t、口;[どんど
無く、人体の内部にループアンテナ’LIJ、り放射し
た電磁波エネルギを集中して入射ざぜることが出来、且
つ励振周波数を500 Ml−17以下の周波数にしで
いることから人体内部の充分な深さに電磁波エネルギが
浸透して癌組織をtIn rmすることが出来、加えて
人体に入射する電磁波:「ネルギTJ1.1状誘電体1
0の放射面12の形状て定まるビーム特性をもつことか
ら加温を必要どづ−るWt絹織をスポット的に加)晶す
ることが出来る。On the other hand, when performing thermal treatment on a human body using the electromagnetic wave emitting device of the present invention shown in FIG. 4, a cold 7. Electromagnetic waves enter the human body through a water film for II! However, since the dielectric constant εW of water is εw = 80.7, which is approximately equal to the dielectric permittivity fεr of the +1-like dielectric 10, the interposition of the water film has a t, Mouth: [The loop antenna 'LIJ' inside the human body can concentrate the radiated electromagnetic wave energy and dissipate it, and the excitation frequency can be kept below 500 Ml-17, so it can be used as a loop antenna inside the human body. The electromagnetic wave energy can penetrate to a sufficient depth inside the body to tIn rm the cancer tissue, and in addition, the electromagnetic wave that enters the human body:
Since the beam characteristics are determined by the shape of the radiation surface 12 of zero, it is possible to spot-crystallize Wt silk fabric, which requires heating.
第6.7及び8図のそれぞれは本発明の電磁波発生器に
用いる!11状誘電10の他の実施例を示した断面図(
゛あり、第4図の円形断面をもった柱状m電1木10に
あってはル−プアンテナ14より放射された電磁波が多
重モードで伝搬されてモード損失を生じやすいことがら
、+1状m 7[1体1oを伝搬する電磁波の伝搬モー
ドを少なくするため、第6図に示J艮円形の断面形状を
もった柱状誘電体10、又第7図に示す楕円形の断面形
状をもった柱状誘電体10、若I・< tel:第8図
に示’J−7r:八角形のような多角形断面をもった柱
状誘電体1oどすることが望ましい。Each of Figures 6.7 and 8 is used in the electromagnetic wave generator of the present invention! A cross-sectional view showing another example of the 11-shaped dielectric 10 (
In the case of the columnar electric tree 10 having a circular cross section as shown in FIG. [In order to reduce the propagation mode of electromagnetic waves propagating through one body 1o, a columnar dielectric body 10 with a circular cross-sectional shape as shown in FIG. The dielectric material 10 is preferably a columnar dielectric material 10 having a polygonal cross section such as an octagon as shown in FIG.
又、柱状誘電体1oに月じ込める励振アンテナとしては
、第4図に示したループ77ンテ士14の他に第9図に
示すグイボールアンテラづ8、第10図に示す一対の電
極板2oを封じ込めた板状アンテナ、第11図に示す平
面反射板を二つに折り曲げた形のコ□−ナリフレクタ2
2とグイボールアンテナ18を相合ぜたコーナリフ1ノ
クタアンテナ、第12図に示づ折返しアンテナ24、更
に第13図に示すヘリカルアンテナ2Gのいずれかを使
用するようにし−てb良く、これらの各)7ンアナ(よ
第4図のループ)7ンfブ14ど同様に空気中におi−
する人さざの1/【汀の大きさをもって柱状誘電体10
の内部に封じ込められる。In addition to the loop 77 antenna 14 shown in FIG. 4, the excitation antenna that can be inserted into the columnar dielectric 1o includes the guibor antenna 8 shown in FIG. 9, and the pair of electrode plates 2o shown in FIG. A plate-shaped antenna that encapsulates the antenna, and a corner reflector 2 in the form of a flat reflector bent in two as shown in Fig. 11.
It is possible to use any one of the corner riff 1 nocta antenna which is a combination of the 2 and the Gui ball antenna 18, the folded antenna 24 shown in Fig. 12, and the helical antenna 2G shown in Fig. 13. ) 7 nana (loop in Figure 4) 7 n f b 14 Similarly, the i-
Ripples 1/[Columnar dielectric material 10 with the size of the shore
is sealed inside.
マ、励振アンアナどしては第9・〜・13図に示したア
ンテナに限定されず、100〜1000Ml−17とな
る\111「及び又1;i LJ 111=帯で使用す
ることの出来る適宜のアンテナを使用することが出来る
。The excitation antenna is not limited to the antennas shown in Figures 9 to 13, but can be any suitable antenna that can be used in the 100 to 1000 Ml-17 range. antenna can be used.
又、11状誘電体10に封じ込める励振アンテナとしη
−は柱状誘電体10が高誘電物質でなることか1)争方
向1’lのアンテラであっても放射電磁波を充分に柱状
誘電体10内に封じ込めることが可能であるが、9上し
くは所定の方向に電磁波を集中的に放口・1?Iる指向
性をもった励振アンテナを用いる。In addition, as an excitation antenna confined in an 11-shaped dielectric 10, η
- means that the columnar dielectric 10 is made of a high dielectric material. 1) It is possible to sufficiently confine the radiated electromagnetic waves within the columnar dielectric 10 even if the antenna is in the opposite direction 1'l. Emit electromagnetic waves intensively in a predetermined direction ・1? An excitation antenna with directivity is used.
次に本発明の詳細な説明すると、500 M l−17
以下の周波数をもつ電磁波を敢口・jするため、人体内
に存在する深部の癌[l織に対しても電磁波を浸透さ1
!て加温することが出来る。Next, to explain the present invention in detail, 500 M l-17
Because it uses electromagnetic waves with the following frequencies, electromagnetic waves can penetrate even deep cancer tissues within the human body.
! It can be heated by
叉、電磁波導波管としての人体の比誘電率にほぼ等しい
比誘電率をもつ+1状誘電体の内部に励振アンテナを封
じ込めていることから、励振アンテナのサイズは人気中
におけるサイズの1/r7c′Tの大きさとづることが
出来、使用周波数を500M Hz以下に下げても励振
アンテナを充分に小型化出来るため、励振アンテナの大
ぎさで決まる柱状誘電体のt3−イズも充分に小さく出
来、医療用の電磁波導波管として取り扱いが(イめて容
易(,7小ヘリの電磁波発生器を実現している。Furthermore, since the excitation antenna is sealed inside a +1-shaped dielectric material that has a dielectric constant almost equal to that of the human body as an electromagnetic waveguide, the size of the excitation antenna is 1/r7c of the popular size. 'T can be expressed as the size of T, and even if the operating frequency is lowered to 500 MHz or less, the excitation antenna can be made sufficiently small, so the t3-ise of the columnar dielectric, which is determined by the size of the excitation antenna, can also be made sufficiently small. It is extremely easy to handle as a medical electromagnetic waveguide, and has been used as an electromagnetic wave generator for 7 small helicopters.
更に励振アンテナよりの電磁波が伝搬する柱状誘電体は
人体組織の比誘電率の(沫ぼ等しい誘電率をもった誘電
物質で作られているため、人体どの接解部にお(ブる反
射損は極く僅かであり、励振アンテナJ:りの故割−r
−ネルギの大部分を人体の内部に向けてビーム状に入射
させることが出来、極めて高い放射効率を実現している
。Furthermore, the columnar dielectric material through which the electromagnetic waves from the excitation antenna propagate is made of a dielectric material with a relative permittivity that is exactly the same as that of human tissue, so there is no reflection loss at any contact point in the human body. is extremely small, and the excitation antenna J:
- Most of the energy can be directed into the human body in the form of a beam, achieving extremely high radiation efficiency.
更に又、柱状誘電体と空気との境界面に入射した電磁波
は空気の比誘電率に対し柱状誘電体の比M電子が極めて
高いため、空気中に放射されずに(1払誘電体の内部に
電磁波がIJじ込められた状態どくくり、500 M
l−(7以下の周波数帯については医療用とじ−(の#
J、 I■が成されていないが、本発明の電磁波発生器
より外部に漏洩する電磁波エネル1’ F:L極く1早
かであることから電磁波の漏れ出しによる通信坊害を防
ぐためのシールド設備も軽微で済み、医療施設への設備
について電波障害の発生を充分に抑えることが出来る。Furthermore, the electromagnetic waves incident on the interface between the columnar dielectric and the air are not radiated into the air (the inside of the single-layer dielectric When electromagnetic waves are trapped in the IJ, 500 M
l-(For frequency bands below 7, use medical binding (#)
Although J and I■ have not been achieved, since the electromagnetic wave energy 1'F:L leaking to the outside from the electromagnetic wave generator of the present invention is extremely early, it is necessary to prevent communication damage due to leakage of electromagnetic waves. The amount of shielding equipment required is minimal, and it is possible to sufficiently suppress the occurrence of radio wave interference in equipment for medical facilities.
第1.2図は従来の電磁波発生器を示した説明図、第3
図IJ、従来の電磁波発生器ににる温熱治療の説明図、
第4図は本発明の一実施例を示した斜視図、第5図は誘
電体アンブナの放射電力比Wi/ W Oを示したグラ
フ図、第6,7及び8図は本発明にお(Jる柱状誘電体
の他の実施例を示した断面図、第9.10,11.12
及び13図は本発明で用いる励振アンテノの他の実施例
を示した説明図である。
10:柱状誘電体 12′:放側面14:ル
ーブアンテ−]−16:給電線18:ダーイボールアン
7プ 20:電極板22:コーナリフレクタ
24:折返しアンブプ
26:ヘリノJルアンテナ
特π′[出願人 株式会ネ1東314 F:’l器代
理人 弁理士 管内 進
第3図
第4図
第5図
前
第6図
第7図
1o)
第8図Figure 1.2 is an explanatory diagram showing a conventional electromagnetic wave generator, Figure 3
Figure IJ, explanatory diagram of heat treatment using a conventional electromagnetic wave generator,
FIG. 4 is a perspective view showing one embodiment of the present invention, FIG. 5 is a graph showing the radiated power ratio Wi/WO of the dielectric antenna, and FIGS. Cross-sectional views showing other embodiments of columnar dielectrics, Nos. 9.10 and 11.12
13 are explanatory diagrams showing other embodiments of the excitation antenna used in the present invention. 10: Column dielectric 12': Emitting surface 14: Lube antenna]-16: Feed line 18: Daiball amplifier 7 20: Electrode plate 22: Corner reflector 24: Folded amplifier 26: Helino J Le antenna special π' [Applicant Co., Ltd. Ne1 Higashi 314 F:'l Agent Patent Attorney Jurisdiction Susumu Figure 3 Figure 4 Figure 5 Previous Figure 6 Figure 7 Figure 1o) Figure 8
Claims (1)
柱状誘電体の内部に封入された励振アンテナと、前記)
1状誘電体の外部に引き出された前記励振アンテナの給
電線とで成ることを特徴とする温熱療法用電磁波発生器
。 (2)前記柱状誘電体は人体組織の比誘電率に略等しい
比誘電率を右づる特許請求の範囲第1項記載の温熱療法
用電磁波発生器。 (3)航記t1状誘電体は、円形、長円形、楕円形又は
多角形の断面形状を有する特許請求の範囲第1項記載の
温熱療法用電磁波発生器。 (/I)前記励振アンテナは、超短波及び又は極超短波
で励振されるアンテナで成る特許請求の範囲第1項記載
の温熱療法用電磁波発生器、。 (5)前記励振アンテナは500 M 1〜17以下の
周波数で励振されるアンテナで成る特許請求の範囲第1
項記載の温熱療法用電磁波発生器。 (6)前記励振アンテナは、ダイポール、ループ又はヘ
リカル等の線状アンテナもしくは一対の電極を用いた板
状アンテナで成る特許請求の範囲第1項記載の温熱療法
用電磁波発生器。[Scope of Claims] (1) A columnar dielectric having an electromagnetic radiation surface formed at one end, an excitation antenna sealed inside the columnar dielectric;
1. An electromagnetic wave generator for thermotherapy, characterized in that the electromagnetic wave generator comprises a feed line for the excitation antenna drawn out of a single dielectric body. (2) The electromagnetic wave generator for thermotherapy according to claim 1, wherein the columnar dielectric has a relative permittivity approximately equal to the relative permittivity of human tissue. (3) The electromagnetic wave generator for thermotherapy according to claim 1, wherein the T1-shaped dielectric has a circular, oval, elliptical, or polygonal cross-sectional shape. (/I) The electromagnetic wave generator for thermotherapy according to claim 1, wherein the excitation antenna is an antenna excited by ultra-high frequency waves and/or ultra-high frequency waves. (5) The excitation antenna is an antenna excited at a frequency of 500 M 1 to 17 or less.
Electromagnetic wave generator for hyperthermia therapy as described in . (6) The electromagnetic wave generator for thermotherapy according to claim 1, wherein the excitation antenna is a linear antenna such as a dipole, loop, or helical antenna, or a plate antenna using a pair of electrodes.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21630882A JPS59105464A (en) | 1982-12-10 | 1982-12-10 | Electromagnetic wave generator for heat treatment |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21630882A JPS59105464A (en) | 1982-12-10 | 1982-12-10 | Electromagnetic wave generator for heat treatment |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59105464A true JPS59105464A (en) | 1984-06-18 |
JPH0151270B2 JPH0151270B2 (en) | 1989-11-02 |
Family
ID=16686484
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21630882A Granted JPS59105464A (en) | 1982-12-10 | 1982-12-10 | Electromagnetic wave generator for heat treatment |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59105464A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60198162A (en) * | 1984-02-24 | 1985-10-07 | 菊地 真 | Applicator for heat treatment |
JPS60198163A (en) * | 1984-02-24 | 1985-10-07 | 菊地 真 | Applicator for heat treatment |
JPS60222069A (en) * | 1984-02-24 | 1985-11-06 | 菊地 眞 | Applicator for heating treatment method |
WO2002072198A1 (en) * | 2001-03-12 | 2002-09-19 | Takano, Yasuki | Method of breaking cancer cell tissue by microelectromagnetic radiation and microelectromagnetic radiator |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5864351U (en) * | 1981-10-23 | 1983-04-30 | ミナト医科学株式会社 | therapeutic antenna device |
-
1982
- 1982-12-10 JP JP21630882A patent/JPS59105464A/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5864351U (en) * | 1981-10-23 | 1983-04-30 | ミナト医科学株式会社 | therapeutic antenna device |
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60198162A (en) * | 1984-02-24 | 1985-10-07 | 菊地 真 | Applicator for heat treatment |
JPS60198163A (en) * | 1984-02-24 | 1985-10-07 | 菊地 真 | Applicator for heat treatment |
JPS60222069A (en) * | 1984-02-24 | 1985-11-06 | 菊地 眞 | Applicator for heating treatment method |
JPS6360676B2 (en) * | 1984-02-24 | 1988-11-25 | ||
JPS6360675B2 (en) * | 1984-02-24 | 1988-11-25 | ||
JPS6360677B2 (en) * | 1984-02-24 | 1988-11-25 | ||
WO2002072198A1 (en) * | 2001-03-12 | 2002-09-19 | Takano, Yasuki | Method of breaking cancer cell tissue by microelectromagnetic radiation and microelectromagnetic radiator |
US7160239B2 (en) | 2001-03-12 | 2007-01-09 | Yasuki Takano | Method of breaking cancer cell tissue by microelectromagnetic radiation and microelectromagnetic radiator |
CN1317045C (en) * | 2001-03-12 | 2007-05-23 | 市川雅英 | Method of breaking cancer cell tissue by microelectromagnetic radiation and microelectromagnetic radiator |
Also Published As
Publication number | Publication date |
---|---|
JPH0151270B2 (en) | 1989-11-02 |
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