EP0133665B1 - Appareils pour détruire les calculs à distance - Google Patents
Appareils pour détruire les calculs à distance Download PDFInfo
- Publication number
- EP0133665B1 EP0133665B1 EP84108750A EP84108750A EP0133665B1 EP 0133665 B1 EP0133665 B1 EP 0133665B1 EP 84108750 A EP84108750 A EP 84108750A EP 84108750 A EP84108750 A EP 84108750A EP 0133665 B1 EP0133665 B1 EP 0133665B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- shock wave
- shock
- lens
- tube
- wave
- 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
Links
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Classifications
-
- G—PHYSICS
- G10—MUSICAL INSTRUMENTS; ACOUSTICS
- G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
- G10K9/00—Devices in which sound is produced by vibrating a diaphragm or analogous element, e.g. fog horns, vehicle hooters or buzzers
- G10K9/12—Devices in which sound is produced by vibrating a diaphragm or analogous element, e.g. fog horns, vehicle hooters or buzzers electrically operated
-
- G—PHYSICS
- G10—MUSICAL INSTRUMENTS; ACOUSTICS
- G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
- G10K11/00—Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
- G10K11/18—Methods or devices for transmitting, conducting or directing sound
- G10K11/26—Sound-focusing or directing, e.g. scanning
- G10K11/30—Sound-focusing or directing, e.g. scanning using refraction, e.g. acoustic lenses
Definitions
- the invention relates to a device for the contactless smashing of a concrement located in the body of a living being with a shock wave generator which can be aligned with a target area in the body.
- Devices of this type are used in medicine, e.g. to destroy stones in the kidney of humans. They are particularly beneficial because they avoid any intervention in the body. It is not necessary to operate surgically. There is also no need to bring probes and devices to the concrement. A risk from infection or injury, e.g. when inserting the probe or operations, can not occur in contactless smashing.
- a device for crushing concrements is described in DE-AS 2351 247.
- a spark discharge is brought about between two electrodes in a first focal point.
- This causes a shock wave, the wavefront of which extends on all sides, i.e. spreads spherically.
- the waves are reflected on the wall of the ellipsoid of revolution. They collect in the second focal point of the ellipsoid of revolution.
- the reflected waves arrive simultaneously in this second focal point, in which the concrement is placed.
- the concrement is destroyed under the collision of the shock waves.
- the coupling between the ellipsoid of revolution and the body in which the concrement is located takes place via a thin film that lies against the body without an air gap.
- the focus chamber is filled with water.
- This device has the disadvantage that changes in the shock wave energy are possible only within small limits and only with considerable expenditure on equipment by changing the distance between the underwater electrodes.
- a further disadvantage is that the mutual distance between the electrodes for generating high-intensity shock waves generally has to be a few millimeters, as a result of which the shock wave source has no punctiform geometry and imaging errors can occur during focusing.
- the underwater electrodes wear heavily with each discharge, so that their lifespan is limited, which necessitates regular maintenance of the device.
- the device according to DE-AS 2351247 also entails the fact that the patient's body is separated from the high-voltage spark gap only by the coupling film which is in contact with the body and by the water. Damage to the coupling foil carries a certain risk for the patient.
- DE-OS 2 902 331 describes a device for transcutaneous, bloodless obliteration of small reticular and spider vein varices.
- controllable ultrasound elements are used as the wave generator, which are arranged parabolically so that their sound energies meet at a focal point in which the varice to be destroyed is placed.
- the entire arrangement of the ultrasonic elements is longitudinally displaceable by means of a worm drive and an adjusting screw. This allows different distances of the focal point from the applicator end to be set.
- the power of the ultrasound crystals is not sufficient to crush stones in the deep interior of a human body.
- the exact setting of the individual ultrasonic vibrators with regard to both the location and the energy is therefore not critical. Switching off individual ultrasonic crystals for the purpose of adjusting the ultrasonic energy in the focal point is not provided.
- DE-OS 3119 295 describes a device for destroying concrements in body cavities with the aid of a large-area ultrasound transducer as a vibration generator.
- a focusing ultrasonic transducer with a pulse peak power of at least 100 kW is used.
- An embodiment is also shown in which individual ring-shaped ultrasonic elements, which form the transducer, are arranged on a spherical surface. None is said about a change in performance according to the type and depth of the concretion.
- the effort for such a device, in particular with regard to the formation of the ring-shaped ultrasound elements should be considerable.
- shock tube As it is used in principle in the present invention, is described.
- a copper membrane is located in front of a flat coil, separated by an insulating film.
- a tube filled with water connects to this copper membrane.
- a voltage in the range of 2-20 kV to the flat coil, a magnetic field is induced in the copper membrane, which causes repulsive forces that suddenly push the membrane away from the coil.
- Such a shock wave tube is used e.g. for substance studies in chemistry.
- a device according to the preamble of claim 1 is known from JP-B 5 540 257.
- the object of the present invention is to increase the operational reliability of such a device, to obtain an image on a target area with the smallest possible imaging error and to reduce maintenance work.
- this object is achieved in that a shock wave generator, known per se and producing the flat shock wave, with an electrical coil and a membrane arranged in front of it is provided as the shock wave generator.
- this device uses a shock wave generator that generates plane waves, the shock waves coming from only one direction have to be bundled and focused.
- imaging errors are less likely than if spherical waves proceeding from a spark gap and traveling in all directions have to be focused.
- the temporal and spatial reproducibility of the shock wave is significantly improved when generated with a shock wave tube compared to the generation with a spark gap.
- there is no maintenance work due to wear and tear of the electrodes in a spark gap. Because a shock wave tube generates the shock waves with the help of electromagnetic forces and does not require a spark gap.
- a shock wave tube is constructed in such a way that it contains a copper membrane at one end of a tube filled with liquid, preferably with water, which is arranged in front of a flat coil, separated by an insulating film. Due to a current pulse in the flat coil, the copper membrane is repelled by it and thereby generates the shock wave in the liquid.
- the copper membrane itself and the pipe section adjoining it are usually connected to a common reference potential, i.e. they are grounded. There is therefore no high voltage at the coupling medium that conducts the shock wave, which increases the electrical safety of patient and staff.
- FIG. 1 shows a shock wave tube 1 known per se, consisting of a jacket 2, a flat coil 3 with two electrical connections 5 and 7, an insulating film 9, a copper membrane 11 and a metallic tube piece 13, in front of an acoustic converging lens 15 , which has a focal point F, placed.
- the pipe section 13 is filled with a liquid 14, e.g. filled with water.
- the shock wave tube 1 is coupled to a body 19 via a coupling medium 17 with water-like acoustic properties.
- the body 19, e.g. a patient has a concretion 23, e.g. a kidney stone.
- the converging lens 15 can be displaced relative to the jacket 2 of the shock tube 1 via a fine adjustment 24 with a bolt 24a and a locking edge 24b in the direction of a double arrow 25.
- the bolt 24a is guided in a slot-shaped recess 24c in the casing 2.
- the shock wave tube 1, the converging lens 15 and the fine adjustment 24 are mounted on a common frame, tripod or a mounting plate 26.
- This mounting plate 26 is mounted on a bearing 26a which can be pivoted on all sides and is displaceable in all spatial directions. As a result, the shock wave tube 1 can be aligned with the concretion 23 such that the focal point F lies in the concretion 23.
- the copper membrane 11 and the pipe section 13 are electrically connected to a protective potential such as earth 27, as is the one connection 7 of the flat coil 3.
- the other connection 5 of the flat coil 3 is connected to a supply and via a switch 29, which includes an auxiliary contact 31 Control unit 33 out.
- a high voltage U is generated in the supply and control unit 33 via a capacitor / resistance circuit (not shown). This can be several kilovolts, for example 20 kV. The voltage U can be adjustable.
- a control signal which is supplied from the supply and control unit 33 to the auxiliary contact 31 via a control line 35, causes the switch 29 to close.
- a part of the energy stored in the (not shown) capacitor of the supply and control unit 33 is discharged abruptly into the flat coil 3, which builds up a magnetic field very quickly.
- a current is induced in the copper membrane 11, which is opposite to the current in the flat coil 3 and a magnetic opposing field testifies. The copper membrane 11 is knocked away from the flat coil 3 by the force of the opposing field.
- This knocking away of the copper membrane 11 creates a flat shock wave, ie an abrupt compression in the liquid 14 upstream of the membrane 11.
- This shock wave shows a steep pressure increase, for example to 200 bar.
- the pressure wave gains steepness in its course through the pipe section 13, the converging lens 15 and the patient's body 19.
- the shock wave After passing through the converging lens 15, the shock wave is shaped such that it converges at the focal point F.
- the concrement 23 is placed there, and the focused shock wave releases part of its energy content to the concrement 23, which is brittle compared to the environment, by means of tensile or compressive forces. These forces break up the concrement 23 into several parts and thus cause it to be broken up.
- This explained crushing device offers the considerable advantage that the grounded copper membrane 11 and the grounded pipe section 13 do not represent a source of danger for the patient 19 or the operating personnel.
- the electrical safety of the device can be improved for the operating personnel by an additional insulating sheath (not shown), e.g. in the form of a plastic coating of the outer surface of the jacket 2, can be increased.
- an additional insulating sheath e.g. in the form of a plastic coating of the outer surface of the jacket 2
- a sack 37 filled with the coupling medium 17 is used at the point of entry of the shock wave in the patient 19, there is a double security for the patient 19 from the high electrical voltage. This security is determined on the one hand by the insulating bag wall and on the other hand by the insulating film 9 in front of the flat coil 3.
- the switch 29 can also be integrated in the supply and control unit 33. It can also be located away from the shock tube assembly. Since a spark gap does not necessarily have to be used for triggering, namely e.g. Vacuum or, more recently, SF6 switches are also out of the question, eliminating the need for complex maintenance and operating work that would be associated with the spark gap.
- FIG. 2 shows a shock wave tube 1 known per se, to which a system 40 of acoustic lenses for imaging a flat shock wave onto a concrement 23 in the body of a patient 19 is assigned.
- the acoustic lens system 40 consists of a diverging lens 42, a condenser 44 and a converging lens 46 and has a focal point F.
- the preferred material for the acoustic lens system 40 is acrylic glass or polystyrene.
- the plane shock wave generated in the shock wave tube 1 is widened in its cross section by the diverging lens 42. The shock wave is then directed in parallel by the capacitor 44 and then focused on the focal point F by the converging lens 46.
- the configurations of the shock wave tube 1 and the holding device described for FIG. 1 also apply to this embodiment of the imaging system.
- the entire system 40 of acoustic lenses can be displaced relative to the shock wave tube 1 in the axial direction of the double arrow 25.
- the advantage of this exemplary embodiment is that the shock wave enters the patient's body 19 over a larger cross section of the body surface. This makes it possible to keep the energy density in the patient's tissue, in particular on the body surface 48, low.
Claims (8)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE19833328051 DE3328051A1 (de) | 1983-08-03 | 1983-08-03 | Einrichtung zum beruehrungslosen zertruemmern von konkrementen |
DE3328051 | 1983-08-03 |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0133665A2 EP0133665A2 (fr) | 1985-03-06 |
EP0133665A3 EP0133665A3 (en) | 1985-04-03 |
EP0133665B1 true EP0133665B1 (fr) | 1988-06-22 |
Family
ID=6205689
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP84108750A Expired EP0133665B1 (fr) | 1983-08-03 | 1984-07-24 | Appareils pour détruire les calculs à distance |
Country Status (3)
Country | Link |
---|---|
US (1) | US4674505A (fr) |
EP (1) | EP0133665B1 (fr) |
DE (2) | DE3328051A1 (fr) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE19916891C1 (de) * | 1999-04-14 | 2000-08-31 | Siemens Ag | Einrichtung zur Erzeugung akustischer Wellen und Verwendung einer derartigen Einrichtung |
DE10207737C1 (de) * | 2002-02-22 | 2003-04-17 | Siemens Ag | Schaltkreis für eine elektromagnetische Quelle zur Erzeugung akustischer Wellen |
Families Citing this family (131)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
USRE33590E (en) * | 1983-12-14 | 1991-05-21 | Edap International, S.A. | Method for examining, localizing and treating with ultrasound |
US5143073A (en) * | 1983-12-14 | 1992-09-01 | Edap International, S.A. | Wave apparatus system |
FR2578081B1 (fr) * | 1985-02-28 | 1987-05-07 | Centre Nat Rech Scient | Dispositif acoustique multi-lentilles a grandissement et focale variables |
EP0205878B1 (fr) * | 1985-05-28 | 1989-04-26 | Siemens Aktiengesellschaft | Appareil pour la destruction à distance de concrétions |
JPS62336A (ja) * | 1985-06-26 | 1987-01-06 | 八千代田工業株式会社 | 液中衝撃波による体外よりの結石破砕装置 |
DE3669203D1 (de) * | 1985-12-20 | 1990-04-05 | Siemens Ag | Verfahren zur kontrolle der eigenschaften des fokus eines ultraschallfeldes und vorrichtung zur durchfuehrung des verfahrens. |
DE3545381C2 (de) * | 1985-12-20 | 1994-02-24 | Siemens Ag | Ultraschallwandler zur Messung der Schalleistung eines fokussierten Ultraschallfeldes |
US4813402A (en) * | 1986-02-19 | 1989-03-21 | Siemens Aktiengesellschaft | Coupling member for a shock wave therapy device |
DE8608200U1 (fr) * | 1986-03-25 | 1987-07-23 | Siemens Ag, 1000 Berlin Und 8000 Muenchen, De | |
EP0240797B1 (fr) * | 1986-04-01 | 1990-07-11 | Siemens Aktiengesellschaft | Générateur d'ondes de choc à rendement amélioré |
EP0243650B1 (fr) * | 1986-04-01 | 1990-06-06 | Siemens Aktiengesellschaft | Générateur d'ondes de choc à focalisation améliorée |
US4796608A (en) * | 1986-06-16 | 1989-01-10 | Siemens Aktiengesellschaft | Shock wave generator for an apparatus for non-contacting disintegration of calculi in the body of a life form |
EP0258561A1 (fr) * | 1986-07-08 | 1988-03-09 | Siemens Aktiengesellschaft | Générateur d'ondes de choc, utilisé en particulier pour la lithotripsie |
US5095891A (en) * | 1986-07-10 | 1992-03-17 | Siemens Aktiengesellschaft | Connecting cable for use with a pulse generator and a shock wave generator |
US4782821A (en) * | 1986-07-14 | 1988-11-08 | Siemens Aktiengesellschaft | Shock wave generator for an installation for non-contacting disintegration of calculi in the body of a life form |
EP0253053B1 (fr) * | 1986-07-14 | 1994-04-27 | Siemens Aktiengesellschaft | Générateur d'ondes de choc pour un dispositif de désintégration à distance des concrétions dans un organisme vivant |
EP0254104B1 (fr) * | 1986-07-16 | 1990-10-03 | Siemens Aktiengesellschaft | Générateur d'ondes de choc pour la production d'une onde de choc acoustique impulsionnelle |
EP0255636B1 (fr) * | 1986-07-30 | 1990-04-25 | Siemens Aktiengesellschaft | Capteur pour des ondes de chocs acoustiques |
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- 1984-07-24 US US06/634,021 patent/US4674505A/en not_active Expired - Lifetime
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DE19916891C1 (de) * | 1999-04-14 | 2000-08-31 | Siemens Ag | Einrichtung zur Erzeugung akustischer Wellen und Verwendung einer derartigen Einrichtung |
DE10207737C1 (de) * | 2002-02-22 | 2003-04-17 | Siemens Ag | Schaltkreis für eine elektromagnetische Quelle zur Erzeugung akustischer Wellen |
Also Published As
Publication number | Publication date |
---|---|
EP0133665A3 (en) | 1985-04-03 |
DE3328051A1 (de) | 1985-02-14 |
EP0133665A2 (fr) | 1985-03-06 |
US4674505A (en) | 1987-06-23 |
DE3472209D1 (en) | 1988-07-28 |
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