EP0108190B1 - Stosswellenreflektor - Google Patents
Stosswellenreflektor Download PDFInfo
- Publication number
- EP0108190B1 EP0108190B1 EP83106090A EP83106090A EP0108190B1 EP 0108190 B1 EP0108190 B1 EP 0108190B1 EP 83106090 A EP83106090 A EP 83106090A EP 83106090 A EP83106090 A EP 83106090A EP 0108190 B1 EP0108190 B1 EP 0108190B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- reflector
- angle
- wave
- die
- max
- 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
- 230000035939 shock Effects 0.000 title description 10
- 239000000463 material Substances 0.000 claims description 12
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 9
- 239000007788 liquid Substances 0.000 claims description 7
- 230000008878 coupling Effects 0.000 claims description 4
- 238000010168 coupling process Methods 0.000 claims description 4
- 238000005859 coupling reaction Methods 0.000 claims description 4
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 claims description 2
- 229910052715 tantalum Inorganic materials 0.000 claims 1
- GUVRBAGPIYLISA-UHFFFAOYSA-N tantalum atom Chemical compound [Ta] GUVRBAGPIYLISA-UHFFFAOYSA-N 0.000 claims 1
- 206010029148 Nephrolithiasis Diseases 0.000 description 9
- 208000000913 Kidney Calculi Diseases 0.000 description 5
- 229910001369 Brass Inorganic materials 0.000 description 3
- 239000010951 brass Substances 0.000 description 3
- 241001136792 Alle Species 0.000 description 1
- 206010013710 Drug interaction Diseases 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000018109 developmental process Effects 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000001902 propagating effect Effects 0.000 description 1
- 230000000284 resting effect Effects 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 239000004575 stone Substances 0.000 description 1
Images
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
- 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
- G10K11/28—Sound-focusing or directing, e.g. scanning using reflection, e.g. parabolic reflectors
Definitions
- the invention relates to a reflector for focusing shock waves for the contact-free comminution of concrements in bodies of living beings according to DE-A-23 51247.
- the reflector has the shape of an ellipsoid and has the task of absorbing shock waves that are generated at a spark gap in the first focal point and spread through a liquid in the reflector to the second focal point, in which the concrement to be destroyed e.g. a kidney stone is in focus.
- the reflector should transmit as high a proportion of the wave energy generated in the first focal point as possible in phase to the second focal point.
- Reflectors made of brass are known with an enclosure angle of approximately 250 °, whereby the full solid angle (4n) is used to approximately 90% and an axis ratio a: b of approximately 2: 1 (E. Schmiedt: Contributions to Urology, Vol. 2 , Pages 8-13, Kunststoff 1980).
- the other constraints such as stability and easy workability have led to the use of brass.
- the invention has for its object to provide a reflector that focuses shock waves with a higher efficiency than the reflectors known from the prior art.
- the invention is based on the knowledge that it is not the jump in sound wave resistance ⁇ ⁇ c that alone is the decisive variable for good focusing, but that the speeds of the sound wave in the reflector material and in the liquid must be coordinated with one another.
- the waves hitting the surface of the reflector stimulate it, among other things. to transversal vibrations that propagate with characteristic propagation velocities in the reflector material and on its surface.
- the reflected wavefront is disturbed if, due to time differences, the reflection surface already swings in the direction of the surface normal when the primary wavefront arrives.
- In-phase focusing in the second focal point is achieved when the wave propagates faster in the liquid than in the reflector.
- the wavefront then always hits a stationary reflector surface.
- materials can also be used whose transverse surface speed is greater than the speed of sound in the coupling medium, e.g. Water is when only the leading of the surface wave is prevented by the geometry of the reflector by complying with the condition mentioned in claim 1.
- the reflected useful wave itself remains undisturbed and retains the original steepness of the primary wave. All other faults - e.g. are generated by the lagging surface wave - follow the useful wave with a time delay and cannot impair the focusing process.
- Reflectors according to the invention realize a much better focusing than before, since all wave components overlap in phase.
- the slope of the pressure rise which is essential for comminution, remains high.
- the shredding performance increases, fewer applications than before are necessary, which relieves the patient and increases the service life of the spark gap.
- the condition c To ⁇ c s is met if lead is used as the reflector material and water is used as the coupling liquid. Since the transverse speed of sound in lead at 710 m / sec is lower than the speed of sound in water at 1480 m / sec, the propagating primary wave 7 is always faster than the surface wave 10. The condition is therefore always fulfilled regardless of the reflector geometry. A critical angle ⁇ k does not occur. It is not necessary for the entire reflector body to be made of lead. It is sufficient if the inner surface of the reflector consists of a layer of lead.
- the condition according to the invention can also be met by reflectors made of a material whose c To > c s .
- the focus can be improved for the same material by choosing the axial ratio of the ellipsoid closer to 1 or by dispensing with edge zones (smaller angle of coverage).
- the edge zones are extremely important for the transmission and should not be left out.
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Multimedia (AREA)
- Surgical Instruments (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE3241026 | 1982-11-06 | ||
DE3241026A DE3241026C2 (de) | 1982-11-06 | 1982-11-06 | Reflektor zur Fokussierung von Stoßwellen |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0108190A2 EP0108190A2 (de) | 1984-05-16 |
EP0108190A3 EP0108190A3 (en) | 1984-07-25 |
EP0108190B1 true EP0108190B1 (de) | 1986-09-24 |
Family
ID=6177450
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP83106090A Expired EP0108190B1 (de) | 1982-11-06 | 1983-06-22 | Stosswellenreflektor |
Country Status (4)
Country | Link |
---|---|
US (1) | US4570634A (enrdf_load_stackoverflow) |
EP (1) | EP0108190B1 (enrdf_load_stackoverflow) |
JP (1) | JPS5988146A (enrdf_load_stackoverflow) |
DE (2) | DE3241026C2 (enrdf_load_stackoverflow) |
Families Citing this family (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5150712A (en) * | 1983-12-14 | 1992-09-29 | Edap International, S.A. | Apparatus for examining and localizing tumors using ultra sounds, comprising a device for localized hyperthermia treatment |
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 |
NL8400504A (nl) * | 1984-02-16 | 1985-09-16 | Optische Ind De Oude Delft Nv | Inrichting voor het aanrakingsloos vergruizen van zich in een lichaam bevindende concrementen. |
DE3617032C2 (de) * | 1985-05-24 | 1997-06-05 | Elscint Ltd | Lithotripsiegerät mit extrakorporalem Stoßwellengenerator |
DE3544344A1 (de) * | 1985-12-14 | 1987-06-19 | Dornier Medizintechnik | Vorrichtung zur thromboisierung mittels stosswellen |
FR2600520B1 (fr) * | 1986-06-30 | 1990-09-21 | Technomed Int Sa | Appareil de generation d'ondes de choc de frequence elevee dans un liquide pour la destruction a distance de cibles, telles que des concretions dont la connectique d'alimentation en courant electrique est disposee a l'interieur d'un element tubulaire limitant ou empechant les fuites electromagnetiques |
CS261485B1 (en) * | 1986-10-29 | 1989-02-10 | Jiri Mudr Rndr Benes | Device for clinic out-of-body lithotripsy of gall stones |
FR2623080A1 (fr) * | 1987-11-16 | 1989-05-19 | Technomed Int Sa | Procede de fabrication d'un dispositif generateur d'ondes de choc indolores et dispositif et appareil ainsi fabriques |
DE3835318C1 (enrdf_load_stackoverflow) * | 1988-10-17 | 1990-06-28 | Storz Medical Ag, Kreuzlingen, Ch | |
DE3900433A1 (de) * | 1989-01-10 | 1990-07-12 | Schubert Werner | Verfahren und vorrichtung fuer die behandlung von erkrankungen mit ultraschallwellen |
SE465552B (sv) * | 1989-03-21 | 1991-09-30 | Hans Wiksell | Anordning foer soenderdelning av konkrement i kroppen paa en patient |
US4945898A (en) * | 1989-07-12 | 1990-08-07 | Diasonics, Inc. | Power supply |
US5065761A (en) * | 1989-07-12 | 1991-11-19 | Diasonics, Inc. | Lithotripsy system |
US6755796B2 (en) | 1999-02-07 | 2004-06-29 | Medispec Ltd. | Pressure-pulse therapy apparatus |
IL128404A0 (en) * | 1999-02-07 | 2000-01-31 | Spector Avner | Device for transmission of shock waves on to large surfaces of human tissue |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE1264681B (de) * | 1961-07-05 | 1968-03-28 | Siemens Ag | Fuer die medizinische Ultraschalldiagnose nach dem Impuls-Echoverfahren bestimmtes ultraschall-spiegeloptisches System zum Senden und Empfangen von Ultraschallwellen |
US3302163A (en) * | 1965-08-31 | 1967-01-31 | Jr Daniel E Andrews | Broad band acoustic transducer |
CH574734A5 (enrdf_load_stackoverflow) * | 1973-10-12 | 1976-04-30 | Dornier System Gmbh | |
DE2508494A1 (de) * | 1975-02-27 | 1976-09-02 | Hansrichard Dipl Phys D Schulz | Anordnung zum fokussieren von elektromagnetischen oder mechanischen wellen |
DE2538960C2 (de) * | 1975-09-02 | 1985-04-11 | Dornier System Gmbh, 7990 Friedrichshafen | Vorrichtung zum berührungslosen Zertrümmern von in einem Lebewesen befindlichen Konkrementen |
US4311147A (en) * | 1979-05-26 | 1982-01-19 | Richard Wolf Gmbh | Apparatus for contact-free disintegration of kidney stones or other calculi |
-
1982
- 1982-11-06 DE DE3241026A patent/DE3241026C2/de not_active Expired
-
1983
- 1983-06-22 DE DE8383106090T patent/DE3366440D1/de not_active Expired
- 1983-06-22 EP EP83106090A patent/EP0108190B1/de not_active Expired
- 1983-07-28 JP JP58136897A patent/JPS5988146A/ja active Granted
- 1983-10-25 US US06/545,203 patent/US4570634A/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
DE3366440D1 (en) | 1986-10-30 |
JPH0417660B2 (enrdf_load_stackoverflow) | 1992-03-26 |
EP0108190A3 (en) | 1984-07-25 |
EP0108190A2 (de) | 1984-05-16 |
JPS5988146A (ja) | 1984-05-22 |
DE3241026C2 (de) | 1986-12-04 |
DE3241026A1 (de) | 1984-05-10 |
US4570634A (en) | 1986-02-18 |
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