EP0337062A2 - Transducteur acousto-électrique - Google Patents
Transducteur acousto-électrique Download PDFInfo
- Publication number
- EP0337062A2 EP0337062A2 EP89101963A EP89101963A EP0337062A2 EP 0337062 A2 EP0337062 A2 EP 0337062A2 EP 89101963 A EP89101963 A EP 89101963A EP 89101963 A EP89101963 A EP 89101963A EP 0337062 A2 EP0337062 A2 EP 0337062A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- corrugated
- support body
- band
- coil
- tape
- 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.)
- Withdrawn
Links
Images
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; ELECTRIC HEARING AIDS; PUBLIC ADDRESS SYSTEMS
- H04R15/00—Magnetostrictive transducers
Definitions
- the invention relates to an acoustoelectric transducer with a support body carrying coil turns, in particular an oscillating hollow body with a curved surface, such as a magnetostrictive ball.
- a generic acoustic transducer is known from EP-A-0 177 383, to which reference is made in full.
- the document shows an omnidirectional, that is to say emitting in all directions, electroacoustic transducer with a spherical in a preferred embodiment
- Body made of magnetostrictive material that can contract and expand in a magnetic field and thus generate air vibrations by its movement in a suitable modulated field and can thus serve as a loudspeaker.
- the magnetostrictive is used as a support body for a coil winding generating the modulated magnetic field in the form of windings made of round copper wire which are tightly wound on the support body.
- the invention is therefore based on the object to further develop the known transducer while avoiding the advantages mentioned in that, with simple application of the coil turns, a uniform distribution of the modulation energy is achieved without impairing the vibration behavior of the magnetostrictive body, in particular transducers of large dimensions, and therefore suitable for deep ones Frequencies are available.
- the above object is achieved in an acoustoelectric transducer of the type mentioned at the outset in that the coil is placed on the support body as a strip of flat material which is corrugated transversely to the direction of travel.
- the band corrugated to the direction of travel it is initially meant that the waves and valleys of the corrugated band extend transversely to the direction of travel thereof and alternate with one another in the direction of travel.
- the invention achieves an optimally uniform distribution of the modulation energy.
- the conductive ribbon can easily swing with the support body.
- the corrugated tape lies only with its troughs on the support body, while it extends freely between the corresponding support lines.
- the band is made of copper material, which on the one hand has the suitable desired elastomechanical properties - namely flexibly deformable but without its own strong elastic restoring forces - and is also the suitable material due to a low specific resistance in electrical terms.
- Aluminum has a somewhat lower but still very good conductivity compared to copper, but it has a lower mass and a ribbon made of this material and therefore has less influence on the oscillation of the magnetostrictive sphere than a copper ribbon.
- the ribbon can be easily applied. It has been found that, particularly in the case of larger transducers with diameters in the range of a few decimeters, the flat material is the suitable material, inter alia because it does not twist. Due to its transverse corrugation, the corrugated flat band adapts optimally to the double-curved support body, such as, in particular, a sphere, but also a rotational ellipsoid with a curved generator. In the corrugated form, it can be conveniently applied to larger bodies with a curved surface, such as, in particular, a sphere, since it can adapt to the curved shape due to the transverse waves. With such larger vibrating bodies with dimensions in the range of several decimeters and more, it contains the only practicable solution.
- corrugated conductor tracks are also on the supporting body, In particular, a ball can only be wound or possibly held in any way, so a preferred embodiment provides that the tape is glued to the support body.
- the corrugated tape is glued to the support body only in the area of its troughs, while the crests of the waves rise freely from the support body, so that they can easily be subject to the above-mentioned deformation. There are various options for sticking.
- the corrugated tape itself is provided on the back with an adhesive layer, for example in the form of a double-sided adhesive tape, that is to say an adhesive tape which is coated on both sides with adhesive.
- the support body is provided with adhesive, if necessary.
- the corrugated conduction band and / or the support body could also be provided with a thermoplastic layer, whereupon the corrugated conduction band is applied to the support body with heating, so that it is firmly connected to the support body after cooling and thus solidification of the thermoplastic layer.
- the width of the corrugated conduction band can in principle be selected in a wide range and depends on the winding length, the desired impedance and the desired number of turns for a given thickness of the material. It is preferably provided that the width of the corrugated band is between 0.5 to 2.0 percent of the diameter of the support body, typical widths being between 5 and 10 mm.
- the distance between the turns should be chosen to be as small as possible without mutual contact in order to avoid or largely reduce electromagnetic coupling losses. In practice, depending on the size of the sphere, distances of the order of a millimeter and less can be achieved.
- the invention ensures that both the inductive magnetic coupling between the ball and this module lationsbändchen is maximum and can be distributed evenly over the entire surface and that the inductive coupling losses at the lower frequencies are largely avoided as well as that the impedance can be brought to a desired value, for example 4 ohms. These goals would not be achievable with a round wire that would either have too high an impedance or, in the case of a strong version, because of its strength, would result in poor coupling and losses.
- the tape is applied to the magnetostrictive ball via an insulating layer (adhesive, etc.) and vibrates with it, without affecting its vibration behavior in any way. If a higher resistance of the coil band is desired, a conductive material other than the copper which is suitable per se, for example in particular nickel, can also be used.
- the acoustic transducer 1 has a spherical support body 2, which consists of magnetostrictive material, such as a nickel-cobalt alloy with a high nickel content, or else has a layer of such material on an insulating elastic carrier.
- a spherical support body 2 which consists of magnetostrictive material, such as a nickel-cobalt alloy with a high nickel content, or else has a layer of such material on an insulating elastic carrier.
- an electrically insulated conductor in the form of a transversely corrugated conductive tape 3 applied.
- FIG. 1 shows a schematic representation of the guidance and corrugation of the ribbon, which as such is shown in part in FIG.
- the insulation can be formed by an attachment layer 4 applied to the back of the corrugated conductive tape 3.
- the layer 4 can be an adhesive layer, for example in the form of a double-sided adhesive tape. It can also be a thermoplastic layer, by means of which the corrugated band 3 is attached to the support
- the support body 2 can also directly with an insulating layer, also in the form of a thermoplastic layer or an adhesive layer, if necessary. be provided in the form of a coiled adhesive tape on both sides, whereupon a corrugated conduction tape 3 is applied without its own rear attachment layer and fixed in this way.
- the conduction band 3 is preferably made of copper. The conduction band 3 is wound onto the support body 2 in the manner shown in FIG. 1, and because of its corrugated configuration it adapts easily and simply to the contour of the support body 2, which can in principle be of any type.
- the corrugated band 3 is flexible, so that it flexibly adapts to the vibrations of the support body 2, which consist of an increase or decrease in radius, so that no stresses occur and in particular the vibration behavior of the body 2 due to the electrical conductor 3 formed coil is not affected in any way.
- the ends 6, 7 of the corrugated band 3 are connected to a voltage source 8 which supplies the suitable modulated voltage, if necessary. via impedance converters and with the provision of other suitable electronic components, as are discussed in EP-A-0 177 383.
- the corrugated band has such a width that it can be applied to the carrier 2 with a sufficient number of mutually electrically separated, that is, spaced turns. Accordingly, the width of the band is preferably in the range of 0.5 to 2 percent of the diameter of a rotating body, preferably a sphere, for example in the case of a supporting body for a loudspeaker covering the usual frequency range from low to high tones with a supporting body diameter of the order of magnitude of a few Decimeters in the range of 5 to 10 mm.
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
- Electrostatic, Electromagnetic, Magneto- Strictive, And Variable-Resistance Transducers (AREA)
- Transducers For Ultrasonic Waves (AREA)
- Apparatuses For Generation Of Mechanical Vibrations (AREA)
- Diaphragms For Electromechanical Transducers (AREA)
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE8803776U | 1988-03-19 | ||
| DE8803776U DE8803776U1 (de) | 1988-03-19 | 1988-03-19 | Akustoelektrischer Wandler |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| EP0337062A2 true EP0337062A2 (fr) | 1989-10-18 |
| EP0337062A3 EP0337062A3 (fr) | 1991-12-27 |
Family
ID=6822092
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP19890101963 Withdrawn EP0337062A3 (fr) | 1988-03-19 | 1989-02-04 | Transducteur acousto-électrique |
Country Status (3)
| Country | Link |
|---|---|
| US (1) | US4924503A (fr) |
| EP (1) | EP0337062A3 (fr) |
| DE (1) | DE8803776U1 (fr) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| RU2181231C2 (ru) * | 1997-09-30 | 2002-04-10 | Санкт-Петербургский государственный университет | Магнитострикционный преобразователь |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2648664A1 (fr) * | 1989-06-15 | 1990-12-21 | Commissariat Energie Atomique | Haut-parleur omnidirectionnel a membrane spherique utilisant un ruban magnetostrictif |
| US5307082A (en) * | 1992-10-28 | 1994-04-26 | North Carolina State University | Electrostatically shaped membranes |
| US5458120A (en) * | 1993-12-08 | 1995-10-17 | General Electric Company | Ultrasonic transducer with magnetostrictive lens for dynamically focussing and steering a beam of ultrasound energy |
| US5381068A (en) * | 1993-12-20 | 1995-01-10 | General Electric Company | Ultrasonic transducer with selectable center frequency |
| US20080282812A1 (en) * | 2007-05-15 | 2008-11-20 | Thaddeus Schroeder | Magnetostrictive load sensor and method of manufacture |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2503515B1 (fr) * | 1981-04-01 | 1985-12-27 | Klein Siegfried | Haut-parleur omnidirectionnel pour les frequences aigues du spectre sonore |
| DE3138566A1 (de) * | 1981-09-28 | 1983-04-07 | Siegfried Dr. 75009 Paris Klein | Lautsprecher, insbesondere hochtonlautsprecher |
| US4782471A (en) * | 1984-08-28 | 1988-11-01 | Commissariat A L'energie Atomique | Omnidirectional transducer of elastic waves with a wide pass band and production process |
| FR2573270B1 (fr) * | 1984-11-13 | 1987-01-23 | Commissariat Energie Atomique | Transducteur omnidirectionnel d'ondes elastiques a large bande passante mettant en oeuvre un bobinage spherique magnetostrictif et procede de fabrication |
| FR2619481B1 (fr) * | 1987-08-14 | 1989-11-17 | Commissariat Energie Atomique | Transducteur omnidirectionnel d'ondes elastiques a large bande passante |
-
1988
- 1988-03-19 DE DE8803776U patent/DE8803776U1/de not_active Expired
-
1989
- 1989-02-04 EP EP19890101963 patent/EP0337062A3/fr not_active Withdrawn
- 1989-03-17 US US07/324,722 patent/US4924503A/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| RU2181231C2 (ru) * | 1997-09-30 | 2002-04-10 | Санкт-Петербургский государственный университет | Магнитострикционный преобразователь |
Also Published As
| Publication number | Publication date |
|---|---|
| US4924503A (en) | 1990-05-08 |
| DE8803776U1 (de) | 1988-05-11 |
| EP0337062A3 (fr) | 1991-12-27 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| DE68928871T2 (de) | Dynamischer Lautsprecher | |
| DE69635308T2 (de) | Piezoelektrischer wandler | |
| DE1902849C3 (de) | Mechanisch-elektrisch bzw. elektrisch-mechanischer Wandler | |
| DE1132593B (de) | Akustisch wirksame Platte, insbesondere zur Ankopplung an einen elektroakustischen Wandler | |
| DE60100886T2 (de) | Wandler, insbesondere zum einsatz in akustischen vorrichtungen | |
| DE2828148C2 (de) | Biegeanordnung | |
| DE2922216A1 (de) | Akustischer wandler | |
| DE102004018301A1 (de) | Piezoelektrischer elektroakustischer Wandler | |
| DE3523973A1 (de) | Elektro-schwingungswandler | |
| DE2003950B2 (de) | Akustischer wandler | |
| DE2461278B2 (de) | Elektroakustischer wandler | |
| DE2229239A1 (de) | Elektromagnetische Anordnung fur elektroakustische Wandler u dgl | |
| DE3726496A1 (de) | Gedaempfte magnetkopftraegeranordnung | |
| DE2339433B2 (de) | Elektroakustischer Wandler nach dem elektrostatischen Prinzip | |
| DE3801474C2 (fr) | ||
| DE2434796C3 (de) | Schwingspule für einen elektromechanischen Wandler | |
| US4924858A (en) | Electromagnetic shockwave generator transducer | |
| EP0337062A2 (fr) | Transducteur acousto-électrique | |
| DE2740661C3 (de) | Dynamischer Wandler mit einer Schwingspule in einem mit einer magnetischen Flüssigkeit gefüllten Luftspalt | |
| EP0075911A1 (fr) | Haut-parleur, en particulier haut-parleur d'aigues | |
| DE3110547C2 (fr) | ||
| DE2945739A1 (de) | Elektroakustischer uebertrager | |
| DE1939837A1 (de) | Elektroakustischer Wandler | |
| DE2554150A1 (de) | Schallwandler | |
| DE3143027C2 (de) | Piezoelektrischer Wandler |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
| AK | Designated contracting states |
Kind code of ref document: A2 Designated state(s): AT CH DE ES FR GB IT LI NL SE |
|
| PUAL | Search report despatched |
Free format text: ORIGINAL CODE: 0009013 |
|
| AK | Designated contracting states |
Kind code of ref document: A3 Designated state(s): AT CH DE ES FR GB IT LI NL SE |
|
| STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
|
| 18D | Application deemed to be withdrawn |
Effective date: 19920903 |