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JPH0351179B2 - - Google Patents
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JPH0351179B2 - - Google Patents

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Publication number
JPH0351179B2
JPH0351179B2 JP61245140A JP24514086A JPH0351179B2 JP H0351179 B2 JPH0351179 B2 JP H0351179B2 JP 61245140 A JP61245140 A JP 61245140A JP 24514086 A JP24514086 A JP 24514086A JP H0351179 B2 JPH0351179 B2 JP H0351179B2
Authority
JP
Japan
Prior art keywords
layer
temperature
ferromagnetic material
magnetic
ferromagnetic
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 - Lifetime
Application number
JP61245140A
Other languages
Japanese (ja)
Other versions
JPS62129048A (en
Inventor
Furanshisu Shoo Robaato
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Publication of JPS62129048A publication Critical patent/JPS62129048A/en
Publication of JPH0351179B2 publication Critical patent/JPH0351179B2/ja
Granted legal-status Critical Current

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Classifications

    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B18/00Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body
    • A61B18/04Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body by heating
    • A61B18/08Surgical instruments, devices or methods for transferring non-mechanical forms of energy to or from the body by heating by means of electrically-heated probes

Landscapes

  • Health & Medical Sciences (AREA)
  • Surgery (AREA)
  • Engineering & Computer Science (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Medical Informatics (AREA)
  • Molecular Biology (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Plasma & Fusion (AREA)
  • Biomedical Technology (AREA)
  • Heart & Thoracic Surgery (AREA)
  • Physics & Mathematics (AREA)
  • Otolaryngology (AREA)
  • Animal Behavior & Ethology (AREA)
  • General Health & Medical Sciences (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Surgical Instruments (AREA)
  • General Induction Heating (AREA)
  • Laser Surgery Devices (AREA)
  • Control Of High-Frequency Heating Circuits (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は改良された電気加熱切断刃およびそ
の加熱温度自動調整方法に関し、さらに詳細には
強磁性体のキユリー温度を利用して加熱温度を自
動調整しうる電気加熱切断刃およびその加熱温度
自動調整方法に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an improved electrically heated cutting blade and a method for automatically adjusting the heating temperature thereof, and more specifically, to an improved method for adjusting the heating temperature using the Curie temperature of a ferromagnetic material. The present invention relates to an automatically adjustable electrically heated cutting blade and a method for automatically adjusting its heating temperature.

〔従来の技術〕[Conventional technology]

従来、強磁性体のキユリー温度を利用して電流
のジユール熱による発熱を自動的にコントロール
する方式が、たとえば実公昭48−35676号、特開
昭49−76058号或いは特開昭51−122983号に見ら
れるように、電気加熱切断刃として外科手術用具
などの分野で利用されている。
Conventionally, methods for automatically controlling heat generation due to Joule heat of current using the Curie temperature of ferromagnetic materials have been proposed, for example, in Japanese Utility Model Publication No. 48-35676, Japanese Patent Application Laid-Open No. 49-76058, or Japanese Patent Application Laid-open No. 122983-1983. As seen in , it is used as an electrically heated cutting blade in fields such as surgical tools.

本発明に利用される基本原理は、上記特開昭51
−122983号公報にも記載されているように従来公
知である。すなわち、強磁性導体における高周波
電流は、導体外周部に集中する傾向がある。その
電流密度は導体表面で最大となり、表面から内部
への距離が大きくなるにつれて減少する。この電
流密度が表面の最大電流密度の37%となる深さ
(表面から内部への距離)を、一般に「表層深さ」
と称している。この表層深さは強磁性導体の透磁
率の関数であつて、次式により示される: 〔式中、dは表層深さ、ρは強磁性材料の抵抗
値、fは電流周波数、μは強磁性材料の透磁率で
ある。〕 この関係は古くから知られており、たとえばボ
ゾース、「フエロマグネチズム」(1951)に記載さ
れている。
The basic principle utilized in the present invention is the above-mentioned Japanese Patent Application Laid-open No. 51
It is conventionally known as described in Japanese Patent No.-122983. That is, high frequency current in a ferromagnetic conductor tends to concentrate on the outer periphery of the conductor. The current density is maximum at the conductor surface and decreases as the distance from the surface to the interior increases. The depth at which this current density is 37% of the maximum current density at the surface (distance from the surface to the inside) is generally called the "surface depth".
It is called. This surface depth is a function of the magnetic permeability of the ferromagnetic conductor and is given by: [In the formula, d is the surface depth, ρ is the resistance value of the ferromagnetic material, f is the current frequency, and μ is the magnetic permeability of the ferromagnetic material. ] This relationship has been known for a long time, and is described, for example, in Bozos's ``Feromagnetism'' (1951).

一般に、強磁性材料はそのキユリー点温度(以
下、単に「キユリー点」と云う)より低い温度に
て100、200もしくはそね以上の透磁率を有する一
方、キユリー点より高い温度では透磁性材料の透
磁率は約1となる。上記式から判るように、強磁
性材料の表層深さはキユリー点より高い温度の場
合にはキユリー点より低い場合よりも10倍以上大
きくなりうる。
In general, ferromagnetic materials have a magnetic permeability of 100, 200, or more at temperatures below their Curie point temperature (hereinafter simply referred to as the "Curie point"); The magnetic permeability is approximately 1. As can be seen from the above equation, the surface depth of a ferromagnetic material can be more than 10 times greater at temperatures above the Curie point than at temperatures below the Curie point.

他方、加熱体に供給される電力量およびその結
果加熱体内に生ずるジユール熱は、加熱体を流過
する電流と加熱体の抵抗値との関数である。この
関数は、式 P=I2R 〔式中、Pはジユール熱、Iは電流、Rは加熱
体の抵抗値である。〕 によつて表わされる。加熱体における電流の大き
さは使用に際し一定で変化しないので、この式か
ら判るように、加熱体内に発生するジユール熱の
量は加熱体の抵抗値の関数となる。
On the other hand, the amount of electrical power supplied to the heating element and the resulting Joule heat generated within the heating element is a function of the current passing through the heating element and the resistance of the heating element. This function is expressed by the formula P=I 2 R [where P is Joule's heat, I is electric current, and R is the resistance value of the heating element. ] is represented by. Since the magnitude of the current in the heating element is constant and does not change during use, as can be seen from this equation, the amount of Joule heat generated within the heating element is a function of the resistance value of the heating element.

そこで、強磁性材料で作成された加熱体におい
ては、温度がキユリー点を越えて上昇すると表層
厚さが増大し、その結果電流が流れる断面積が増
大して抵抗値を減少させる。かくして、温度がキ
ユリー点より高い場合にはキユリー点より低い場
合に比べ、加熱体に供給される電力が少なくなつ
て発生するジユール熱を減少させる。このジユー
ル熱の減少は、加熱体の温度がキユリー点より低
くなつて加熱体における表層深さがキユリー点よ
り低い際の強磁性材料における透磁率の増大によ
り減少するまで持続する。
Therefore, in a heating body made of a ferromagnetic material, when the temperature rises above the Curie point, the surface layer thickness increases, and as a result, the cross-sectional area through which the current flows increases and the resistance value decreases. Thus, when the temperature is higher than the Curie point, less electric power is supplied to the heating element than when the temperature is lower than the Curie point, thereby reducing the generated Joule heat. This reduction in Joule heat continues until the temperature of the heating element falls below the Curie point and is reduced due to the increase in magnetic permeability in the ferromagnetic material when the surface depth in the heating element is below the Curie point.

さらに、加熱体を流れる電流は所定の大きさに
設定できる。従つて、上記の基本原理に基づき、
強磁性材料の加熱体は、そのキユリー点を境とし
て所定の温度範囲内で自動温度調整することがで
きる。
Furthermore, the current flowing through the heating element can be set to a predetermined magnitude. Therefore, based on the above basic principle,
A heating element made of ferromagnetic material can automatically adjust its temperature within a predetermined temperature range around its Curie point.

このような原本原理に従つて構成された外科手
術用メスが特開昭51−122983号公報に開示された
技術である。すなわち、切断刃と熱結合した強磁
性材料のキユリー点を境とする透磁率の変化によ
り、切断刃の温度をキユリー点近くの或る範囲内
で自動温度調整するものである。
A surgical scalpel constructed according to the original principle is disclosed in Japanese Patent Application Laid-Open No. 122983/1983. That is, the temperature of the cutting blade is automatically adjusted within a certain range near the Curie point by changing the magnetic permeability of the ferromagnetic material thermally coupled to the cutting blade, with the Curie point as the boundary.

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

しかしながら、これら従来の強磁性材料におい
ては、その自動温度調整能力はキユリー点より高
い際の電流抵抗値(その結果、発生するジユール
熱の量)が依然として強磁性材料の比較的高い抵
抗値によつて左右されるので限界を有し、このこ
とは極く微少範囲内で温度をより鋭敏に自動調整
する際の欠点を意味する。
However, in these conventional ferromagnetic materials, their self-temperature regulating ability is limited by the relatively high resistance of the ferromagnetic materials, where the current resistance (and therefore the amount of Joule heat generated) above the Curie point remains This means that there is a drawback in automatically adjusting the temperature more sensitively within a very small range.

従つて、本発明の目的は、加熱切断刃の種々の
領域に予知不能な状態で接する冷却体の変化に呼
応して、上記基本原理に基づく自動温度調整効率
をより鋭敏に高めることにある。
Therefore, it is an object of the present invention to sharply increase the efficiency of automatic temperature adjustment based on the above basic principle in response to changes in the cooling body that contacts various regions of the heated cutting blade in an unpredictable manner.

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

この目的は、本発明によれば、強磁性構造体を
高透磁率の強磁性材料と実効透磁率が低くかつ高
い導電性および熱伝導性を有する材料の層とから
なる複合積層体によつて達成される。
This object, according to the invention, is achieved by forming a ferromagnetic structure by a composite laminate consisting of a ferromagnetic material with high permeability and a layer of material with low effective permeability and high electrical and thermal conductivity. achieved.

従つて、本発明は、被加熱部の温度を所定範囲
に自動調整する積層電気加熱切断刃において、 前記所定範囲の上限温度近くに透磁率のキユリ
ー転移点を有する強磁性材料の層と、この強磁性
材料層に電気接触すると共にこの強磁性材料より
も高い導電率と高い熱伝導率とを有する導電性材
料の層と、前記2つの層からなる積層体に連結さ
れた高周波電流源とを備え、 前記積層体が、キユリー点以下の温度では強磁
性材料層を流れる電流の表層深さが強磁性材料層
の厚さより小さくなり、キユリー点以上の温度で
は強磁性材料層を流れる電流の表層深さが強磁性
材料層の厚さより大きくなるような厚さを有する
強磁性材料および導電性材料の層で構成されるこ
とを特徴とする積層電気加熱切断刃を提供する。
Therefore, the present invention provides a laminated electrically heated cutting blade that automatically adjusts the temperature of a heated part within a predetermined range, which comprises: a layer of a ferromagnetic material having a Curie transition point of magnetic permeability near the upper limit temperature of the predetermined range; a layer of conductive material in electrical contact with the layer of ferromagnetic material and having higher electrical conductivity and higher thermal conductivity than the ferromagnetic material; and a high frequency current source coupled to the stack of the two layers. In the laminate, the surface depth of the current flowing through the ferromagnetic material layer is smaller than the thickness of the ferromagnetic material layer at a temperature below the Curie point, and the surface depth of the current flowing through the ferromagnetic material layer at a temperature above the Curie point. A laminated electrically heated cutting blade is provided, characterized in that it is composed of a layer of ferromagnetic material and an electrically conductive material having a thickness such that the depth is greater than the thickness of the ferromagnetic material layer.

この積層電気加熱切断刃において、温度変化を
より鋭敏に自動調整するべく、導電性材料の層を
強磁性材料層よりも高い熱伝導率を有する特に銅
または銀で構成すれば好適である。
In this laminated electrically heated cutting blade, in order to automatically adjust temperature changes more sensitively, it is preferable that the conductive material layer is made of copper or silver, which has a higher thermal conductivity than the ferromagnetic material layer.

この積層電気加熱切断刃は、一縁部を鋭利にし
て殊に外科手術用メスとして使用することができ
る。
This laminated electrically heated cutting blade has one edge sharpened so that it can be used, in particular, as a surgical scalpel.

なお、強磁性材料層の外側表面に配置された電
気絶縁材の層と、前記強磁性材料層の長さの少な
くとも一部に沿つて前記絶縁材上に配置された導
電性材料の層とをさらに設け、この導電性材料の
層を強磁性材料層へその一端部近くでのみ接続し
て導電性材料の層から強磁性材料層への導電路を
形成すれば、自動温度調整の効果を高める上で一
層好適である。
A layer of electrically insulating material disposed on the outer surface of the layer of ferromagnetic material and a layer of electrically conductive material disposed on the insulating material along at least a portion of the length of the layer of ferromagnetic material. Further, if this layer of conductive material is connected to the layer of ferromagnetic material only near one end thereof to form a conductive path from the layer of conductive material to the layer of ferromagnetic material, the effectiveness of automatic temperature regulation is enhanced. The above is more suitable.

また、本発明は、高周波電流源に電気接続され
た交流電気抵抗加熱用部材において、前記加熱用
部材は少なくとも所定温度範囲にわたり温度上昇
と共に低下する電気抵抗を有し、さらに高熱伝導
性かつ高導電性の材料よりなる導電性の非磁性支
持部材を備え、この支持部材はその表面の少なく
とも一部にわたり磁性材料の薄層を有し、この磁
性材料はそのキユリー点より低い温度にて1より
大きい最大比透磁率を有すると共にキユリー点よ
り高い温度にてほぼ1の最小比透磁率を有し、前
記加熱用部材が前記高周波電流源に電気接続され
た際高周波数にて交流電流が流れて前記加熱用部
材にジユール熱を生ぜしめ、前記交流電流は前記
最大の透磁率により前記磁性材料層のキユリー点
より低い温度での作用に従い前記磁性材料の薄層
に制限される一方、前記交流電流は前記温度が上
昇してキユリー点に接近しかつ前記透磁率が低下
する際前記非磁性支持部材に拡散するよう構成し
たことを特徴とする交流電気抵抗加熱用部材を提
供する。
The present invention also provides an AC electrical resistance heating member electrically connected to a high frequency current source, wherein the heating member has an electrical resistance that decreases as the temperature rises over at least a predetermined temperature range, and further has high thermal conductivity and high conductivity. an electrically conductive non-magnetic support member made of a magnetic material, the support member having a thin layer of magnetic material over at least a portion of its surface, the magnetic material having an electrically conductive non-magnetic support member having an electrically conductive non-magnetic support member having an electrically conductive non-magnetic support member having an electrically conductive non-magnetic support member having a thin layer of magnetic material over at least a portion of its surface; It has a maximum relative magnetic permeability and a minimum relative magnetic permeability of approximately 1 at temperatures above the Curie point, and when the heating member is electrically connected to the high frequency current source, an alternating current flows at a high frequency to generating Joule heat in the heating element, the alternating current is limited to the thin layer of the magnetic material in accordance with the effect of the maximum magnetic permeability at temperatures below the Curie temperature of the layer of magnetic material, while the alternating current is Provided is an alternating current electrical resistance heating member, characterized in that it is configured to diffuse into the non-magnetic support member when the temperature rises and approaches the Curie point and the magnetic permeability decreases.

かくして、本発明の他の面によれば、高周波電
流の供給に応じて上限および下限が狭い範囲内で
多層構造体の温度上昇を自動調整する方法におい
て、前記多層構造体は一対の材料層からなり、多
層構造体のそれぞれの領域において変化する冷却
負荷を受けるよう設定され、 狭い温度範囲の上限に近い温度で、透磁率のキ
ユリー転移点を有する第1の導電路を特定する前
記一方の層に高周波電流の一部を流すステツプ
と、 前記一方の層より低い磁気透磁率の実効値と高
い導電性および熱伝導性を有する第2の導電路と
して特定される層であつて、前記一方の層と積層
を形成する前記他方の層に前記高周波電流の他の
部分を流すステツプと、 狭い範囲内の温度で前記多層構造体を維持する
ための多層材料の冷却負荷と温度との関数とし
て、それぞれの層に流れる高周波電流の相対的割
合を変化させることにより、より少ない冷却負荷
を受ける領域に比べて、より大きな冷却負荷を受
ける多層構造体の領域に対しより多く加熱するス
テツプと、 からなることを特徴とする多層構造体の温度上昇
を自動調整する方法も提供される。
Thus, according to another aspect of the invention, in a method for automatically adjusting the temperature rise of a multilayer structure within a narrow range of upper and lower limits in response to the supply of high-frequency current, the multilayer structure comprises a pair of material layers. said one layer being configured to undergo a varying cooling load in each region of the multilayer structure and identifying a first conductive path having a Curie transition point of magnetic permeability at a temperature near the upper limit of a narrow temperature range; a layer specified as a second conductive path having a lower effective value of magnetic permeability and higher electrical conductivity and thermal conductivity than the one layer; passing another portion of said high frequency current through said other layer forming a laminate with a layer; as a function of the cooling load and temperature of the multilayer material to maintain said multilayer structure within a narrow range of temperatures; heating regions of the multilayer structure that receive a greater cooling load more than regions that receive a lower cooling load by varying the relative proportions of high-frequency current flowing through each layer; There is also provided a method for automatically adjusting the temperature rise of a multilayer structure, characterized in that:

さらに、複合積層体のその他の材料を注意深く
選定すれば、切断刃のいろいろの領域間の熱の分
路を増すことによりさらに自動調整作用を高める
ことができる。また複合体のその他の材料を注意
深く選定すると切断刃の鋭さと耐久性を増すこと
もできる。
Additionally, careful selection of the other materials in the composite laminate can further enhance the self-adjusting action by increasing the shunting of heat between the various regions of the cutting blade. Careful selection of other materials in the composite can also increase the sharpness and durability of the cutting blade.

〔作 用〕[Effect]

本発明の積層加熱切断刃においては、キユリー
点より低い温度での表層深さが強磁性材料層の厚
さよりも小さくなる一方、キユリー点より高い温
度では表層深さが強磁性材料層の厚さよりも大き
くなる。従つて、キユリー点より高くなつた際、
電流が流れる表層深さは強磁性材料層だけではな
く導電性層をも含むことになり、この層は強磁性
材料層よりも抵抗値がずつと低い。その結果、キ
ユリー点よりも高い温度にて積層加熱切断刃にお
ける電流抵抗値は従来のこの種の切断刃における
よりもずつと低くなり、それに比例して発生ジユ
ール熱もずつと少なくなる。かくして、本発明に
よれば、従来の切断刃よりも自動温度調整能力が
ずつと向上する。
In the laminated heated cutting blade of the present invention, the surface layer depth is smaller than the thickness of the ferromagnetic material layer at temperatures lower than the Curie point, while the surface layer depth is smaller than the thickness of the ferromagnetic material layer at temperatures higher than the Curie point. also becomes larger. Therefore, when the temperature rises above the Kyrie point,
The surface depth through which the current flows includes not only the ferromagnetic material layer but also the conductive layer, and this layer has a lower resistance value than the ferromagnetic material layer. As a result, at temperatures higher than the Curie point, the current resistance value of the laminated heating cutting blade becomes gradually lower than that of conventional cutting blades of this type, and the generated Joule heat decreases proportionally. Thus, according to the present invention, the automatic temperature adjustment ability is gradually improved over conventional cutting blades.

上記したように、本発明によれば、高導電性か
つ高熱伝導性の層と強磁性材料の層との連携によ
り、表層深さが強磁性材料層よりも厚くなるキユ
リー点より高い温度において、高導電性層(たと
えば銅の層)を流れる高周波電流の比率が増大
し、その結果積層電気加熱切断刃の発生ジユール
熱が顕著に減少する。この作用効果は加熱される
べき部分とは無関係に得られる。
As described above, according to the present invention, due to the cooperation between the highly electrically conductive and highly thermally conductive layer and the ferromagnetic material layer, at temperatures above the Curie point where the surface layer depth becomes thicker than the ferromagnetic material layer, The proportion of high frequency current flowing through the highly conductive layer (eg copper layer) is increased, resulting in a significant reduction in the Joule heat generated by the laminated electrically heated cutting blade. This effect is obtained independently of the part to be heated.

〔実施例〕〔Example〕

以下、添付第1図および第2図を参照して、本
発明を切断刃としての実施例につき詳細に説明す
る。
Hereinafter, with reference to the attached FIGS. 1 and 2, the present invention will be described in detail with respect to an embodiment as a cutting blade.

第1図および第2図において、刃の支持部9は
適当なプラスチツク材料で作成され、手術器具の
把手部11に取付けられる。器具の切断刃15を
形成する構造体13は刃の支持部9に取付けられ
て、把手部11に近い始端17から把手部11に
遠い末端19まで延在している。この積層構造体
13は、第2図の断面で示すように、鋭い切断刃
15を確保し得るような硬度を有しかつ非磁性鋼
又は焼入れ炭素鋼のような好ましくは低い透磁率
を有する中央層21を備える。
1 and 2, the blade support 9 is made of a suitable plastic material and attached to the handle 11 of the surgical instrument. A structure 13 forming the cutting blade 15 of the instrument is attached to the blade support 9 and extends from a starting end 17 near the handle 11 to an end 19 distal to the handle 11. This laminated structure 13 is made of a central material having a hardness to ensure a sharp cutting edge 15 and preferably of low magnetic permeability, such as non-magnetic steel or hardened carbon steel, as shown in cross-section in FIG. A layer 21 is provided.

中央層21の両側に配置した隣接層23はたと
えば銅または銀のような低い透磁率と高い熱的・
電気的伝導度とを有する材料であつて、切断刃1
5に沿つて温度変化を減ずるように切断刃の長さ
に沿い高温領域から低温領域まで優れた熱伝導を
行う。更にこれら層23は、後述するように、高
周波電流で発生するジユール熱を減ずるような高
い導電路を形成する。このように組合せた層21
と23とは、複合積層体の有効な低透磁率及び高
い電気的・熱的伝導部分を形成する。
Adjacent layers 23 arranged on either side of the central layer 21 are made of a material with low magnetic permeability and high thermal resistance, such as copper or silver.
The cutting blade 1 is made of a material having electrical conductivity.
Provides excellent heat transfer from hot to cold areas along the length of the cutting blade to reduce temperature variations along the length of the cutting blade. Additionally, these layers 23 form highly conductive paths that reduce Joule heating generated by high frequency currents, as will be discussed below. Layer 21 combined in this way
and 23 form an effective low permeability and high electrical and thermal conductivity portion of the composite laminate.

高い透磁率及び所望の動作温度範囲の上限近く
にキユリー点を有するたとえば鉄ニツケル合金の
ような強磁性材料の薄い層25が層21,23に
隣接配置される。低い導電率及び高い磁気飽和値
も、層25の材料の望ましい特性である。
A thin layer 25 of a ferromagnetic material, such as an iron-nickel alloy, having high magnetic permeability and a Curie point near the upper limit of the desired operating temperature range is disposed adjacent layers 21,23. Low electrical conductivity and high magnetic saturation values are also desirable properties for the material of layer 25.

強磁性層25と導電体29との間には始端17
から末端19まで実質的に強磁性体層25の全長
にわたつて電気絶縁層27を配置し、この導電体
29は強磁性体層25に接続する。このようにし
て、信号源23から積層構造体13に加えられた
高周波信号は導電体29に沿つて末端19へ、次
いで帰路層21,23及び25を介して信号源3
2に導かれる。信号源32によつて供給される高
周波電流の周波数または振幅は、切断刃15の動
作温度を調整するように変化させることができ
る。
There is a starting end 17 between the ferromagnetic layer 25 and the conductor 29.
An electrically insulating layer 27 is disposed over substantially the entire length of the ferromagnetic layer 25 from the end 19 to the end 19, and this electrical conductor 29 is connected to the ferromagnetic layer 25. In this way, the high frequency signal applied to the laminated structure 13 from the signal source 23 is transmitted along the conductor 29 to the terminal end 19 and then via the return layers 21, 23 and 25 to the signal source 23.
2. The frequency or amplitude of the high frequency current provided by signal source 32 can be varied to adjust the operating temperature of cutting blade 15.

第1図の積層構造は中心線30に対し導電体2
9を片側に設けて対称的に構成し、末端19で強
磁性体の複合構造体に接続すると共に始端17の
近くで信号源の1つの導電体29に共通接続して
もよいことに注目すべきである。
The laminated structure in FIG.
9 may be arranged symmetrically on one side, connected to the ferromagnetic composite structure at the end 19 and commonly connected to one conductor 29 of the signal source near the starting end 17. Should.

強磁性体層25の動作温度範囲における高周波
透磁率は、複合積層体21及び23の実効透磁率
よりもずつと大きくなるよう、たとえば200乃至
1000程度になるよう容易に選択することができ
る。他方、複合積層体21,23の実効導電率
は、強磁性体層25におけるよりも遥かに大きい
値(たとえば10乃至20倍程度)となるよう容易に
選択し得る。高周波電流の流れる表層の深さは、
電流が流れる材料の導電率と透磁率および加えら
れる高周波電流の周波数とに逆比例する。強磁性
体層25の寸法及びその透磁率は、充分高い周波
数の電流で付勢されたとき表層効果が電流を実質
的に強磁性体層25に集中するよう選択すること
ができる。温度がキユリー点に向かつて上昇する
につれ、強磁性体層25の材料の透磁率は1に向
かつて減少し、高周波電流の流れる深さが増大す
る。これは強磁性体層25を流れる高周波電流の
割合をより小さくする一方、複合積層体21,2
3を流れる高周波電流の割合をより大きくする結
果となる。温度がキユリー点に向かつて上昇する
ときに起る強磁性体層25から複合積層体21,
23への電流の再分布、及び温度がキユーリ点か
ら低下する際に起る逆の再分布は、強磁性体層2
5より充分大きい複合積層体21,23の導電率
によつて更に助成される。
The high-frequency magnetic permeability of the ferromagnetic layer 25 in the operating temperature range is, for example, 200 to 200, so that it becomes gradually larger than the effective magnetic permeability of the composite laminates 21 and 23.
It can be easily selected to be around 1000. On the other hand, the effective conductivity of the composite laminates 21, 23 can be easily selected to be much larger (for example, on the order of 10 to 20 times) than in the ferromagnetic layer 25. The depth of the surface layer through which high-frequency current flows is
It is inversely proportional to the electrical conductivity and magnetic permeability of the material through which the current flows and the frequency of the applied high-frequency current. The dimensions of the ferromagnetic layer 25 and its magnetic permeability can be selected such that when energized with a current of sufficiently high frequency, surface effects substantially concentrate the current in the ferromagnetic layer 25. As the temperature increases toward the Curie point, the magnetic permeability of the material of the ferromagnetic layer 25 decreases toward 1, increasing the depth through which the high-frequency current flows. This makes the proportion of high frequency current flowing through the ferromagnetic layer 25 smaller, while the composite laminates 21, 2
This results in a larger proportion of the high frequency current flowing through 3. from the ferromagnetic layer 25 to the composite laminate 21, which occurs as the temperature increases towards the Curie point.
The redistribution of current into the ferromagnetic layer 2 and the opposite redistribution that occurs as the temperature decreases from the Curie point
This is further aided by the electrical conductivity of the composite laminates 21, 23 which is significantly greater than 5.

積層体の各々で発生するジユール熱は、その層
の電気抵抗及びその層を流れる高周波電流の強さ
の関数である。強磁性体層25の電気抵抗値は複
合積層体21,23の実効電気抵抗より実質的に
高い。従つて、温度変化の関数として起る各層2
1,23及び25間の高周波電流の分布変化は、
高周波電流により発生するジユール熱の対応変化
をもたらし、低い温度では加熱の増加を、また高
い温度では加熱の減少を起す。
The Joule heat generated in each stack is a function of the electrical resistance of that layer and the strength of the high frequency current flowing through that layer. The electrical resistance value of the ferromagnetic layer 25 is substantially higher than the effective electrical resistance of the composite laminates 21 and 23. Therefore, each layer 2 occurs as a function of temperature change.
The distribution change of high frequency current between 1, 23 and 25 is
A corresponding change in the Joule heat generated by the high frequency current results in increased heating at lower temperatures and decreased heating at higher temperatures.

よつて、本発明の複合積層体21,23,25
の第1の利点は、全てが強磁性材料から成る構造
を利用した従来の切断刃で得られる自動温度調整
よりも優れた自動温度調整を与えることである。
Therefore, the composite laminates 21, 23, 25 of the present invention
The first advantage is that it provides automatic temperature regulation that is superior to that obtained with conventional cutting blades that utilize structures made of all ferromagnetic materials.

強磁性合金のみを利用した従来の切断刃よりも
優れた本発明の複合積層体の第2の利点は、複合
積層体21,23の実効熱伝導率を強磁性体層2
5におけるよりもずつて高く選択し得ることであ
る。
The second advantage of the composite laminate of the present invention over conventional cutting blades that utilize only ferromagnetic alloys is that the effective thermal conductivity of the composite laminates 21 and 23 is lower than that of the ferromagnetic layer 2.
It is possible to select higher values than in 5.

このように、複合された積層体21,23は、
組織との接触によつて冷却されていない切断刃領
域から冷却されつつある領域への熱伝導を著しく
増大させることができ、これにより自動温度調整
作用を向上させる。たとえば銅、非磁性鋼と銅な
どの低透磁率の積層体は典型的な鉄ニツケル強磁
性合金よりも約30倍も高い熱伝導率を有するの
で、この「熱分流」効果による温度調整の改善は
全てが強磁性体材料で作成された従来の同様な構
造よりも著しく大きい。
In this way, the composite laminates 21 and 23 are
Heat transfer from the area of the cutting blade that is not cooled by contact with tissue to the area that is being cooled can be significantly increased, thereby improving self-temperature regulation. For example, low permeability laminates such as copper, non-magnetic steel and copper have thermal conductivities approximately 30 times higher than typical iron-nickel ferromagnetic alloys, resulting in improved temperature regulation due to this "thermal shunting" effect. is significantly larger than conventional similar structures made entirely of ferromagnetic materials.

切断部材自体がそこに流れる高周波電流により
電気加熱される第1図及び第2図に示した実施例
において、複合積層体の他の利点は、中央層より
鋭利かつ、より耐久性の切断刃を設けられるよう
な硬度に選択し得ることである。たとえば、もし
中央層21を#302ステンレス鋼で作成するとす
れば、これは切断刃自体が電流を流して直接にジ
ユール熱を発生する従来の切断刃におけるように
切断刃全体を典型的な鉄ニツケル強磁性合金で構
成したロツクウエルC硬度約10のものと比較し、
ロツクウエルC硬度30を有するであろう。
In the embodiment shown in Figures 1 and 2, where the cutting member itself is electrically heated by a high frequency current flowing through it, another advantage of the composite laminate is that it provides a sharper and more durable cutting edge than the central layer. The hardness can be selected as required. For example, if the center layer 21 is made of #302 stainless steel, this means that the entire cutting blade is made of typical iron-nickel steel, as in conventional cutting blades where the cutting blade itself conducts electrical current and directly generates heat. Compared to Rockwell C hardness of about 10 made of ferromagnetic alloy,
It will have a Rockwell C hardness of 30.

また、第3図の断面で示したような、切断刃の
周囲にこの種の複合積層体の高周波電流用導電体
を配置した本発明の他の実施例によれば、複合積
層体の同様な利点が得られることにも注目すべき
である。この実施例において、導電体36は2つ
の積層39と37とから成つており、その1つは
鉄ニツケル合金のような低い導電率と、高い磁気
飽和と所定温度のキユリー点とを有する高い透磁
率の強磁性材料より成り、他方は銅もしくは銀の
ような低い透磁率と高い電気的・熱的伝導度とを
有する材料より成つている。導電体36は層38
によつて切断部材40から電気絶縁され、切断部
材40は切断刃15を有し(又は切断部材はセラ
ミツクもしくはガラスなどの非導電性材料で加工
される)かつこれに熱結合されている。すべて高
周波電流は、熱伝導によつて切断部材を加熱する
よう積層導電体36を通して流れる。導電性複合
積層体におけるジユール熱の自動調整の改良は、
上述のメカニズムによつて達成される。
In addition, according to another embodiment of the present invention, as shown in the cross section of FIG. It should also be noted that advantages are obtained. In this embodiment, the conductor 36 consists of two laminated layers 39 and 37, one of which has a low conductivity, such as an iron-nickel alloy, and a high permeability with high magnetic saturation and a Curie point at a given temperature. The other is made of a ferromagnetic material with low magnetic permeability and high electrical and thermal conductivity, such as copper or silver. Conductor 36 is layer 38
The cutting member 40 has a cutting blade 15 (or the cutting member is fabricated from a non-conductive material such as ceramic or glass) and is thermally coupled thereto. All high frequency currents flow through the laminated conductor 36 to heat the cutting member by thermal conduction. Improvements in automatic regulation of Joule heat in conductive composite laminates
This is achieved by the mechanism described above.

〔発明の効果〕〔Effect of the invention〕

上記した自動調整式加熱切断刃は、止血と同時
に手術を行う外科手術用に有益である。自動調整
すべき温度は、その温度近くにキユリー点を有す
るたとえば鉄ニツケル合金のような強磁性材料を
複合積層体における強磁性材料層として選定する
ことにより達成される。
The self-adjusting heated cutting blade described above is useful for surgical operations that simultaneously perform hemostasis. The self-adjusting temperature is achieved by selecting a ferromagnetic material, such as an iron-nickel alloy, having a Curie point near that temperature, as the ferromagnetic material layer in the composite stack.

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

第1図は本発明の実施例による切断刃の平面
図、第2図は第1図の切断刃の2−2線断面図、
第3図は本発明の他の実施例の断面図である。 11…把手部、13…積層構造体、15…切断
刃、17…始端、19…末端、21,23…複合
積層体、25…強磁性体層、27…電気絶縁層、
29…導電体、30…中心線、36…導電体、3
7…積層、38…層、39…積層、40…切断部
材。
FIG. 1 is a plan view of a cutting blade according to an embodiment of the present invention, FIG. 2 is a sectional view taken along line 2-2 of the cutting blade in FIG.
FIG. 3 is a sectional view of another embodiment of the invention. DESCRIPTION OF SYMBOLS 11... Handle part, 13... Laminated structure, 15... Cutting blade, 17... Starting end, 19... End, 21, 23... Composite laminate, 25... Ferromagnetic layer, 27... Electrical insulation layer,
29... Conductor, 30... Center line, 36... Electric conductor, 3
7... Lamination, 38... Layer, 39... Lamination, 40... Cutting member.

Claims (1)

【特許請求の範囲】 1 被加熱部の温度を所定範囲に自動調整する積
層電気加熱切断刃において、 前記所定範囲の上限温度近くに透磁率のキユリ
ー転移点を有する強磁性材料の層と、この強磁性
材料層に電気接触すると共にこの強磁性材料より
も高い導電率と高い熱伝導率とを有する導電性材
料の層と、前記2つの層からなる積層体に連結さ
れた高周波電流源とを備え、 前記積層体が、キユリー点以下の温度では強磁
性材料層を流れる電流の表層深さが強磁性材料層
の厚さより小さくなり、キユリー点以上の温度で
は強磁性材料層を流れる電流の表層深さが強磁性
材料層の厚さより大きくなるような厚さを有する
強磁性材料および導電性材料の層で構成されるこ
とを特徴とする積層電気加熱切断刃。 2 強磁性材料層の外側表面に配置された電気絶
縁材の層と、前記強磁性材料層の長さの少なくと
も一部に沿つて前記絶縁材上に配置された導電性
材料の層とをさらに備え、この導電性材料の層を
強磁性材料層へその一端部近くでのみ接続して導
電性材料の層から強磁性材料層への導電路を形成
してなる特許請求の範囲第1項記載の積層電気加
熱切断刃。 3 導電性材料の層が銅および銀よりなる群から
選択される特許請求の範囲第1項記載の積層電気
加熱切断刃。 4 高周波電流源に電気接続された交流電気抵抗
加熱用部材において、 前記加熱用部材は少なくとも所定温度範囲にわ
たり温度上昇と共に低下する電気抵抗を有し、さ
らに高熱伝導性かつ高導電性の材料よりなる導電
性の非磁性支持部材を備え、 この支持部材はその表面の少なくとも一部にわ
たり磁性材料の薄層を有し、 この磁性材料はそのキユリー点より低い温度に
て1より大きい最大比透磁率を有すると共にキユ
リー点より高い温度にてほぼ1の最小比透磁率を
有し、 前記加熱用部材が前記高周波電流源に電気接続
された際高周波数にて交流電流が流れて前記加熱
用部材にジユール熱を生ぜしめ、 前記交流電流は前記最大の透磁率により前記磁
性材料層のキユリー点より低い温度での作用に従
い前記磁性材料の薄層に制限される一方、 前記交流電流は前記温度が上昇してキユリー点
に接近しかつ前記透磁率が低下する際前記非磁性
支持部材に拡散するよう構成したことを特徴とす
る交流電気抵抗加熱用部材。 5 高周波電流の供給に応じて上限および下限が
狭い範囲内で多層構造体の温度上昇を自動調整す
る方法において、前記多層構造体は一対の材料層
からなり、多層構造体のそれぞれの領域において
変化する冷却負荷を受けるよう設定され、 狭い温度範囲の上限に近い温度で、透磁率のキ
ユリー転移点を有する第1の導電路を特定する前
記一方の層に高周波電流の一部を流すステツプ
と、 前記一方の層より低い磁気透磁率の実効値と高
い導電性および熱伝導性を有する第2の導電路と
して特定される層であつて、前記一方の層と積層
を形成する前記他方の層に前記高周波電流の他の
部分を流すステツプと、 狭い範囲内の温度で前記多層構造体を維持する
ための多層材料の冷却負荷と温度との関数とし
て、それぞれの層に流れる高周波電流の相対的割
合を変化させることにより、より少ない冷却負荷
を受ける領域に比べて、より大きな冷却負荷を受
ける多層構造体の領域に対しより多く加熱するス
テツプと、 からなることを特徴とする多層構造体の温度上昇
を自動調整する方法。
[Claims] 1. A laminated electrically heated cutting blade that automatically adjusts the temperature of a heated part within a predetermined range, comprising: a layer of a ferromagnetic material having a Curie transition point of magnetic permeability near the upper limit temperature of the predetermined range; a layer of conductive material in electrical contact with the layer of ferromagnetic material and having higher electrical conductivity and higher thermal conductivity than the ferromagnetic material; and a high frequency current source coupled to the stack of the two layers. In the laminate, the surface depth of the current flowing through the ferromagnetic material layer is smaller than the thickness of the ferromagnetic material layer at a temperature below the Curie point, and the surface depth of the current flowing through the ferromagnetic material layer at a temperature above the Curie point. A laminated electrically heated cutting blade characterized in that it is composed of a layer of ferromagnetic material and an electrically conductive material having a thickness such that the depth is greater than the thickness of the ferromagnetic material layer. 2 a layer of electrically insulating material disposed on an outer surface of the layer of ferromagnetic material; and a layer of electrically conductive material disposed on the insulating material along at least a portion of the length of the layer of ferromagnetic material. and the layer of conductive material is connected to the layer of ferromagnetic material only near one end thereof to form a conductive path from the layer of conductive material to the layer of ferromagnetic material. Laminated electric heating cutting blade. 3. The laminated electrically heated cutting blade of claim 1, wherein the layer of conductive material is selected from the group consisting of copper and silver. 4. In an AC electrical resistance heating member electrically connected to a high frequency current source, the heating member has an electrical resistance that decreases as the temperature rises over at least a predetermined temperature range, and is further made of a material with high thermal conductivity and high electrical conductivity. an electrically conductive non-magnetic support member having a thin layer of magnetic material over at least a portion of its surface, the magnetic material having a maximum relative permeability greater than 1 at a temperature below its Curie temperature; and has a minimum relative magnetic permeability of approximately 1 at a temperature higher than the Curie point, and when the heating member is electrically connected to the high frequency current source, an alternating current at a high frequency flows through the heating member to generating heat, the alternating current being confined to the thin layer of the magnetic material in accordance with the effect of the maximum magnetic permeability at a temperature below the Curie point of the layer of magnetic material, while the alternating current is flowing as the temperature increases. An alternating current electrical resistance heating member characterized in that it is configured to diffuse into the non-magnetic support member when the magnetic permeability decreases as the magnetic permeability approaches the Curie point. 5. A method for automatically adjusting the temperature rise of a multilayer structure within a narrow range of upper and lower limits according to the supply of high-frequency current, wherein the multilayer structure is composed of a pair of material layers, and the temperature rise in each region of the multilayer structure is passing a portion of a high frequency current through said one layer identifying a first conductive path that is configured to receive a cooling load of at least one layer and has a Curie transition point of magnetic permeability at a temperature near the upper limit of a narrow temperature range; A layer specified as a second conductive path having a lower effective value of magnetic permeability and higher electrical conductivity and thermal conductivity than the one layer, the other layer forming a lamination with the one layer. passing another portion of said high frequency current; and the relative proportion of high frequency current flowing through each layer as a function of temperature and cooling load of the multilayer material to maintain said multilayer structure within a narrow range of temperatures. heating a region of the multilayer structure receiving a larger cooling load more than a region receiving a smaller cooling load by changing the temperature of the multilayer structure. How to automatically adjust.
JP61245140A 1978-04-20 1986-10-15 Improved electric heating cutter blade and automatic temperature control method Granted JPS62129048A (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US89838878A 1978-04-20 1978-04-20
US898388 1978-04-20

Publications (2)

Publication Number Publication Date
JPS62129048A JPS62129048A (en) 1987-06-11
JPH0351179B2 true JPH0351179B2 (en) 1991-08-06

Family

ID=25409375

Family Applications (2)

Application Number Title Priority Date Filing Date
JP4887079A Granted JPS54164389A (en) 1978-04-20 1979-04-20 Improvement type electric heater and its method and its structure
JP61245140A Granted JPS62129048A (en) 1978-04-20 1986-10-15 Improved electric heating cutter blade and automatic temperature control method

Family Applications Before (1)

Application Number Title Priority Date Filing Date
JP4887079A Granted JPS54164389A (en) 1978-04-20 1979-04-20 Improvement type electric heater and its method and its structure

Country Status (6)

Country Link
JP (2) JPS54164389A (en)
BR (1) BR7902444A (en)
DE (1) DE2914401A1 (en)
FR (1) FR2428279A1 (en)
GB (1) GB2022974A (en)
NL (1) NL7903018A (en)

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JP2012523923A (en) * 2009-04-17 2012-10-11 ドメイン・サージカル,インコーポレーテッド Inductive thermal surgical tool
US8932279B2 (en) 2011-04-08 2015-01-13 Domain Surgical, Inc. System and method for cooling of a heated surgical instrument and/or surgical site and treating tissue
US9078655B2 (en) 2009-04-17 2015-07-14 Domain Surgical, Inc. Heated balloon catheter
US9131977B2 (en) 2009-04-17 2015-09-15 Domain Surgical, Inc. Layered ferromagnetic coated conductor thermal surgical tool
US10357306B2 (en) 2014-05-14 2019-07-23 Domain Surgical, Inc. Planar ferromagnetic coated surgical tip and method for making
US11123127B2 (en) 2009-04-17 2021-09-21 Domain Surgical, Inc. System and method of controlling power delivery to a surgical instrument
US11266459B2 (en) 2011-09-13 2022-03-08 Domain Surgical, Inc. Sealing and/or cutting instrument

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4481057A (en) * 1980-10-28 1984-11-06 Oximetrix, Inc. Cutting device and method of manufacture
JPH0320664U (en) * 1989-07-06 1991-02-28
JP2558584B2 (en) * 1991-04-05 1996-11-27 メトカル・インコーポレーテッド Instruments for cutting, coagulating and removing body tissue
US6230603B1 (en) * 1996-04-29 2001-05-15 Zbigniew Kubala Cutting blade for resistance-heated elastomer cutters
US9265556B2 (en) 2009-04-17 2016-02-23 Domain Surgical, Inc. Thermally adjustable surgical tool, balloon catheters and sculpting of biologic materials
US9107666B2 (en) 2009-04-17 2015-08-18 Domain Surgical, Inc. Thermal resecting loop
WO2013106036A2 (en) 2011-04-08 2013-07-18 Preston Manwaring Impedance matching circuit
WO2012158722A2 (en) 2011-05-16 2012-11-22 Mcnally, David, J. Surgical instrument guide

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4091813A (en) * 1975-03-14 1978-05-30 Robert F. Shaw Surgical instrument having self-regulated electrical proximity heating of its cutting edge and method of using the same
ZA761133B (en) * 1975-03-14 1977-02-23 R Shaw Surgical instrument having self-regulated electrical skin-depth heating of its cutting edge and method of using the same

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012523923A (en) * 2009-04-17 2012-10-11 ドメイン・サージカル,インコーポレーテッド Inductive thermal surgical tool
US9078655B2 (en) 2009-04-17 2015-07-14 Domain Surgical, Inc. Heated balloon catheter
US9131977B2 (en) 2009-04-17 2015-09-15 Domain Surgical, Inc. Layered ferromagnetic coated conductor thermal surgical tool
US9220557B2 (en) 2009-04-17 2015-12-29 Domain Surgical, Inc. Thermal surgical tool
US11123127B2 (en) 2009-04-17 2021-09-21 Domain Surgical, Inc. System and method of controlling power delivery to a surgical instrument
US8932279B2 (en) 2011-04-08 2015-01-13 Domain Surgical, Inc. System and method for cooling of a heated surgical instrument and/or surgical site and treating tissue
US11266459B2 (en) 2011-09-13 2022-03-08 Domain Surgical, Inc. Sealing and/or cutting instrument
US10357306B2 (en) 2014-05-14 2019-07-23 Domain Surgical, Inc. Planar ferromagnetic coated surgical tip and method for making
US11701160B2 (en) 2014-05-14 2023-07-18 Domain Surgical, Inc. Planar ferromagnetic coated surgical tip and method for making

Also Published As

Publication number Publication date
GB2022974A (en) 1979-12-19
JPS62129048A (en) 1987-06-11
JPS54164389A (en) 1979-12-27
NL7903018A (en) 1979-10-23
DE2914401A1 (en) 1979-10-31
BR7902444A (en) 1979-10-23
FR2428279A1 (en) 1980-01-04
JPS6232938B2 (en) 1987-07-17

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