JPS6389152A - Ultrasonic stone crushing apparatus - Google Patents

Ultrasonic stone crushing apparatus

Info

Publication number
JPS6389152A
JPS6389152A JP61234360A JP23436086A JPS6389152A JP S6389152 A JPS6389152 A JP S6389152A JP 61234360 A JP61234360 A JP 61234360A JP 23436086 A JP23436086 A JP 23436086A JP S6389152 A JPS6389152 A JP S6389152A
Authority
JP
Japan
Prior art keywords
ultrasonic
radiator
stone
stone crushing
transducers
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP61234360A
Other languages
Japanese (ja)
Inventor
一郎 小倉
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP61234360A priority Critical patent/JPS6389152A/en
Publication of JPS6389152A publication Critical patent/JPS6389152A/en
Pending legal-status Critical Current

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Abstract

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

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野 この発明は超音波を用いて結石を破砕する装置に係り、
特に超音波パルス波を発生する放射器が結石を破砕する
必要な十分なエネルギーを与えることと.その破砕が可
能な位置を局在することができる結石破砕装置に関する
[Detailed Description of the Invention] [Object of the Invention] (Industrial Field of Application) This invention relates to a device for crushing stones using ultrasonic waves.
In particular, a radiator that generates ultrasonic pulse waves must provide sufficient energy to fragment the stone. The present invention relates to a stone crushing device that can localize the location where stone crushing is possible.

(従来の技術) 超音波を利用して結石の破砕に応用できる装置の公知例
として,例えば特開昭60−145131号公報に示さ
れる結石破砕用超音波パルス発生装置がある。、この装
置では、焦点領域lこ集束される衝撃波を発生するため
に球形の圧電変換器が使用されている。この場合,この
球形の曲率の中心点が焦点領域となり,超音波パルス波
の集中により結石破砕がなされることになる。従って、
曲率中心点に破砕しようとする結石を位置させることが
必要で.そのため、球形の開口部より前方に曲率中心点
が存在するよう構成することになる。一方、球形の表面
積すなわち超音波パルスの放射面積は大きい程、破砕す
るエネルギーの高い超音波パルスが放射できるので効率
がよい。前述の条件で効率よい超音波パルスを放射する
ために最大の効率で行なう形状はM3図に示すように半
球にしたとき開口面33が同一での条件で放射面31が
最大となる。しか−し、この場合その曲率中心層2力f
−MO面33の面内にあるので、この場所に破砕しよう
とする結石を位置させることは実用上困難となり。
(Prior Art) As a known example of a device that can be applied to crushing stones using ultrasonic waves, there is an ultrasonic pulse generator for crushing stones, which is disclosed in, for example, Japanese Patent Laid-Open No. 145131/1983. In this device, a spherical piezoelectric transducer is used to generate a shock wave that is focused on a focal region. In this case, the center point of this spherical curvature becomes the focal region, and the stone is crushed by the concentration of the ultrasonic pulse waves. Therefore,
It is necessary to position the stone to be fragmented at the center of curvature. Therefore, the structure is such that the center of curvature exists in front of the spherical opening. On the other hand, the larger the spherical surface area, that is, the radiation area of the ultrasonic pulse, the more efficient the ultrasonic pulse can be emitted with high crushing energy. In order to radiate efficient ultrasonic pulses under the above-mentioned conditions, the shape that can be achieved with maximum efficiency is a hemispherical shape as shown in Fig. M3, and the radiation surface 31 is maximized under the condition that the aperture surface 33 is the same. However, in this case, the curvature center layer 2 force f
- Since it is within the plane of the MO plane 33, it is practically difficult to position the stone to be crushed at this location.

通常、第4図に示すような曲率中心点35が設定される
。この時の放射面34は開口面36が第2図に示す開口
面33と等しいとすれば、放射面31よりは/トさい面
積となり超音波パルスのエネルギーが小さくなる。超音
波パルスのエネルギーが同等のものを得ようとするため
には、超音波放射器の駆動電力を増大させるか又は、放
射器の面積を面積を増大させ同等とすることになるが、
駆動回路の高電圧化又は、開口面積の増大は装置の大型
化になり、技術的困難がともなうとともに、生体に使用
するときの実用上の大きさにも制限があり好ましくない
Usually, a curvature center point 35 as shown in FIG. 4 is set. At this time, if the aperture surface 36 of the radiation surface 34 is equal to the aperture surface 33 shown in FIG. 2, the area of the radiation surface 34 will be smaller than that of the radiation surface 31, and the energy of the ultrasonic pulse will be smaller. In order to obtain the same ultrasonic pulse energy, the drive power of the ultrasonic radiator must be increased, or the area of the radiator must be increased to make it equivalent.
Increasing the voltage of the drive circuit or increasing the aperture area increases the size of the device, which is accompanied by technical difficulties, and also limits the practical size when used in a living body, which is undesirable.

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

このように従来の技術では、結石を破砕するための超音
波パルスの放射器において、被治療の生体に対し装着可
能な小さな開口面の放射器では、その放射面積が小さく
なるため、破砕に十分なエネルギーが困難であり、駆動
電力を増大する必要があるが、生体に対する高電圧の危
険性や放射器の振動子特性にも影響を与える。また、高
電圧駆動回路はコストパーフォーマンスが悪いので、こ
れらによらないエネルギー増大の方法が必要である。
In this way, with conventional technology, when using an ultrasonic pulse radiator for crushing stones, a radiator with a small aperture that can be attached to a living body to be treated has a small radiation area, so it is not sufficient to crush stones. However, it is difficult to obtain high energy, and it is necessary to increase the driving power, but it also affects the danger of high voltage to living organisms and the oscillator characteristics of the radiator. Furthermore, since high voltage drive circuits have poor cost performance, there is a need for a method of increasing energy that does not rely on these.

本発明は、開口面積および開口面と焦点の位置関係を変
えることなく、放射される超音波パルスのエネルギーを
増強させることができる装置を提供することを目的とす
る。
An object of the present invention is to provide a device that can increase the energy of emitted ultrasonic pulses without changing the aperture area and the positional relationship between the aperture surface and the focal point.

〔発明の構成〕[Structure of the invention]

(問題点を解決するための手段) 本発明は、集束させた超音波パルス波によって結石の破
砕を行なう装置において、回転体の内面に小区分された
振動子を環状の群をなすように配置して超音波放射器を
構成すると共に前記振動子群のそれぞれから放射される
超音波パルスが、該回転体の外部にある軸上の所定位置
lこ同時に到達するよう前記各振動子間で移相量を与え
て駆動するごとを特徴とする超音波結石破砕装置を提供
する。
(Means for Solving the Problems) The present invention provides an apparatus for crushing stones using focused ultrasonic pulse waves, in which subdivided vibrators are arranged in an annular group on the inner surface of a rotating body. to constitute an ultrasonic radiator, and the ultrasonic pulses emitted from each of the transducers are moved between the transducers so that they simultaneously reach a predetermined position on an axis outside the rotating body. An ultrasonic stone crushing device is provided, which is characterized in that it is driven by applying a phase amount.

(作用) このような本発明では、従来のように幾何学的に等距離
を要せず、すなわち放射器は球形に限定されるものでは
なく、超音波パルスを集中させる位置すなわち破砕しよ
うとする結石を位置させる実質上の焦点を含む軸を回転
軸とする回転体の内面を放射面とする放射器により、さ
らにその放射器は小区画に区分された超音波振動子で構
成されその各区分の振動子の駆動タイミングが少しずつ
異なり、各区分からの超音波パルスが実質上の焦点へ到
達する時間がすべて等しくなるように駆動タイミングが
調整される。この球に構成・調整される本発明では、放
射器の形状を球形より奥行の深い回転体とすることによ
り1球形のものより大きな放射面積が実現できるので、
焦点に集中される超音波エネルギーを増大させることが
可能になる。
(Function) In the present invention, geometrically equidistant distances are not required as in the conventional case, that is, the radiator is not limited to a spherical shape, and the radiator is not limited to a spherical shape, but the position where the ultrasonic pulse is concentrated, that is, the radiator is intended to be crushed. The radiator is composed of an ultrasonic transducer divided into small sections, and the radiator is composed of an ultrasonic transducer divided into small sections. The drive timings of the transducers are slightly different, and the drive timings are adjusted so that the time it takes for the ultrasonic pulses from each section to reach the actual focal point is all equal. In the present invention configured and adjusted as a sphere, by making the shape of the radiator a rotating body with a deeper depth than that of a sphere, a radiation area larger than that of a single sphere can be realized.
It becomes possible to increase the ultrasound energy concentrated in the focal point.

放射面の振動子の区分は、軸対称となっており駆動タイ
ミングが同じになる環状に小区分される。
The sections of the vibrator on the radiation surface are axially symmetrical and are subdivided into annular sections having the same drive timing.

区分の段数は焦点の集中範囲の大きさにより決定され、
小区分数の多いものほど小さな焦点が構成される。
The number of division stages is determined by the size of the focal concentration range,
The larger the number of subdivisions, the smaller the focus.

(実施例) 本発明の実施の1例を第1図に示す。(Example) An example of implementation of the present invention is shown in FIG.

生体11の内部にある結石°12が軸上にある様な中心
軸7を回転軸とするn次関数(但しn≠2)曲線、又は
複数の関数の組み合せ関数曲線の回転体6の内面に環状
の撮動子1a・・・1gが固定された放射器を備えてい
る。この放射器と生体との間には超音波伝搬様管を介在
させることは、従来技術と同様の方法で行なわれる。振
動子1a・・・1gにはそれぞれ移相器2a・・・2g
が接続され、超音波駆動パルス発生器4からの振動子駆
動パルスは、各移相器2a・・・2gを通じて、それぞ
れ位相差を与えて振動子1a・・・Igが駆動され超音
波パルスを発生する。本実施例では開口面13に近い振
動子1aが最大の移相量で、順次底面方向の振動子1b
へ行くに従って移相量が小さくなり振動子1gが最少と
なる。この移相量は、移相量制御回路3で与えられ1だ
こ宅は回軸体6の形状と結石位置によりあらかじめ決定
される。かくして結石に対し、より遠方にある振動子1
gから次順駆動され、それぞれ発せられた超音波パルス
が同時刻に結石にすなわち実質上の焦点に到達するので
結石を破砕が行なわれる。
On the inner surface of the rotating body 6, an n-dimensional function (however, n≠2) curve whose rotational axis is the central axis 7 such that the calculus 12 inside the living body 11 is on the axis, or a combination function curve of a plurality of functions. It is equipped with a radiator to which annular imagers 1a...1g are fixed. Interposing the ultrasonic wave propagation tube between the radiator and the living body is performed in the same manner as in the prior art. The vibrators 1a...1g each have a phase shifter 2a...2g.
are connected, and the transducer drive pulse from the ultrasonic drive pulse generator 4 passes through each phase shifter 2a...2g, giving a phase difference to each of the transducers 1a...Ig to drive the ultrasonic pulse. Occur. In this embodiment, the vibrator 1a close to the opening surface 13 has the largest phase shift, and the vibrator 1b toward the bottom surface sequentially
The amount of phase shift decreases as the distance increases, and the amount of phase shift becomes smaller at the vibrator 1g. This amount of phase shift is given by a phase shift amount control circuit 3, and is determined in advance based on the shape of the rotating shaft 6 and the position of the stone. Thus, the oscillator 1 located further away from the stone
The ultrasonic pulses are sequentially driven starting from g, and the emitted ultrasonic pulses reach the stone, that is, the virtual focus, at the same time, so that the stone is crushed.

第2図は1本発明の他の実施例で各区分の振動子1a・
・・1gがそれぞれ超音波駆動パルス発生器4a・・・
4gによって駆動される。駆動タイミング発生回路5は
、小区分の環状撮動子1a・・・1gに与える駆動タイ
ミングの時間遅れを発生して、それぞれの摂動子1a・
・・1gからの超音波パルスが結石に同時刻に到達する
ように制御している。
FIG. 2 shows another embodiment of the present invention, with vibrators 1a and 1a in each section.
...1g is each ultrasonic drive pulse generator 4a...
Powered by 4g. The drive timing generation circuit 5 generates a time delay in the drive timing given to the annular sensors 1a, .
...The ultrasonic pulses from 1g are controlled so that they reach the stone at the same time.

いずれの実施例においても移相量制御回路3の移相量を
変化すること、又は駆動タイミング発生回路5の時間遅
れを変化することにより軸7上のいかなる位置の結石に
焦点を合せることが可能で結石と放射器との距離も制限
を受けないようにすることも可能である。
In either embodiment, it is possible to focus on a stone at any position on the shaft 7 by changing the phase shift amount of the phase shift amount control circuit 3 or by changing the time delay of the drive timing generation circuit 5. It is also possible to avoid restrictions on the distance between the stone and the radiator.

な右、環状振動子は必ずしも一体の振動子でなくても分
割された振動子でも同−位相才たは同−多イミングで駆
動されるなら本発明の目的とすることを可能にする。
Note that the annular vibrator is not necessarily an integral vibrator, but even divided vibrators can achieve the object of the present invention if they are driven with the same phase or multiple timings.

〔発明の効果〕〔Effect of the invention〕

従来球面の放射器では、超音波エネルギーを増大させる
ために開口面を大きくしたり、駆動電力の増大が必要で
実用的1こは困難があるが1本発明によれば生体への装
着に適した開口面で、放射器の表面積を増大させること
が可能で、より強力な結石破砕の超音波エネルギーを得
ることができ放射器小形化が可能となる。
Conventional spherical radiators require a larger aperture and an increase in driving power to increase ultrasonic energy, making them difficult to put into practical use; however, the present invention is suitable for mounting on living organisms. The surface area of the radiator can be increased by the opening surface, which allows more powerful ultrasonic energy for stone crushing to be obtained, and the radiator can be made smaller.

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

第1図はこの発明の実施例を示す図、第2図はこの発明
の他の実施例を示す図、第3図は従来技術による最大の
効果を得るための構成を示す図、第4図は従来技術によ
る実用的な構成を示す図である。 1a・・・1g・・・小区分された振動子、  2a・
・・2g・・・移相器、3・・・移相量制御回路、4,
4a・・・4g・・・超音波駆動パルス発生器、5・・
・駆動タイミング発生回路、6・・・回転体、7・・・
回転軸、11・・・生体、12・・・結石、13・・・
開口面、31・・・生球の球面、32・・・焦点、33
・・・開口面、34・・・球面、35・・・焦点。 36・・開口面。
Fig. 1 is a diagram showing an embodiment of the present invention, Fig. 2 is a diagram showing another embodiment of the invention, Fig. 3 is a diagram showing a configuration for obtaining the maximum effect according to the prior art, and Fig. 4 is a diagram showing an embodiment of the present invention. 1 is a diagram showing a practical configuration according to the prior art. 1a...1g...Subdivided vibrator, 2a...
...2g...phase shifter, 3...phase shift amount control circuit, 4,
4a...4g...Ultrasonic drive pulse generator, 5...
・Drive timing generation circuit, 6...Rotating body, 7...
Rotation axis, 11... Living body, 12... Stone, 13...
Aperture surface, 31... Spherical surface of living sphere, 32... Focus, 33
...Aperture surface, 34...Spherical surface, 35...Focal point. 36... Opening surface.

Claims (2)

【特許請求の範囲】[Claims] (1)集束された超音波パルス波によって結石の破砕を
行なう装置において、回転体の内面に小区分された振動
子を環状の群をなすように配置して超音波放射器を構成
すると共に前記振動子群のそれぞれから放射される超音
波パルスが、前記回転体の外部にある軸上の所定位置に
同時に到達するよう、前記各振動子間で移相量を与えて
駆動することを特徴とする超音波結石破砕装置。
(1) In a device for crushing stones using focused ultrasonic pulse waves, an ultrasonic radiator is constructed by arranging subdivided vibrators in an annular group on the inner surface of a rotating body. The transducer is driven by giving a phase shift amount between each of the transducers so that the ultrasonic pulses emitted from each of the transducers reach a predetermined position on a shaft outside the rotary body at the same time. Ultrasonic stone crushing device.
(2)軸上の所定位置までの到達時刻が一致するように
、振動子群の駆動タイミングを変えて駆動することを特
徴とする特許請求の範囲第1項記載の超音波結石破砕装
置。
(2) The ultrasonic stone crushing device according to claim 1, characterized in that the drive timing of the vibrator group is changed so that the arrival times to a predetermined position on the shaft coincide with each other.
JP61234360A 1986-10-03 1986-10-03 Ultrasonic stone crushing apparatus Pending JPS6389152A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61234360A JPS6389152A (en) 1986-10-03 1986-10-03 Ultrasonic stone crushing apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61234360A JPS6389152A (en) 1986-10-03 1986-10-03 Ultrasonic stone crushing apparatus

Publications (1)

Publication Number Publication Date
JPS6389152A true JPS6389152A (en) 1988-04-20

Family

ID=16969782

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61234360A Pending JPS6389152A (en) 1986-10-03 1986-10-03 Ultrasonic stone crushing apparatus

Country Status (1)

Country Link
JP (1) JPS6389152A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0257244A (en) * 1988-08-24 1990-02-27 Shimadzu Corp Lithotrite
JP2012115585A (en) * 2010-12-03 2012-06-21 Tohoku Univ Array type ultrasonic transmitter

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0257244A (en) * 1988-08-24 1990-02-27 Shimadzu Corp Lithotrite
JP2012115585A (en) * 2010-12-03 2012-06-21 Tohoku Univ Array type ultrasonic transmitter

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