GB2151025A - Transducer - Google Patents
Transducer Download PDFInfo
- Publication number
- GB2151025A GB2151025A GB08414282A GB8414282A GB2151025A GB 2151025 A GB2151025 A GB 2151025A GB 08414282 A GB08414282 A GB 08414282A GB 8414282 A GB8414282 A GB 8414282A GB 2151025 A GB2151025 A GB 2151025A
- Authority
- GB
- United Kingdom
- Prior art keywords
- transducer
- electrode elements
- sheet
- lamina
- array
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01H—MEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
- G01H11/00—Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by detecting changes in electric or magnetic properties
- G01H11/06—Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by detecting changes in electric or magnetic properties by electric means
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B06—GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
- B06B—METHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
- B06B1/00—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
- B06B1/02—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy
- B06B1/08—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with magnetostriction
- B06B1/085—Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with magnetostriction using multiple elements, e.g. arrays
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Ultra Sonic Daignosis Equipment (AREA)
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
- Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
- Geophysics And Detection Of Objects (AREA)
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Abstract
A transducer for effecting conversion between acoustic stress wave energy and electrical energy comprises a plurality of individual electrically conductive electrode elements (10) presenting a one or two dimensional array of coplanar electrode element faces, an overlying sheet (16) of dielectric material e.g. MYLAR (R.T.M.) carrying an electrically conductive film or coating on its side remote from the individual electrode elements (10) and which is common to the individual electrode elements, means (14, 19) for supporting the sheet peripherally to lie freely on, but in tension over, the coplanar faces (11) of the individual electrode elements (10), adjacent areas of which are spaced from each other by gaps (17, 18) which are sufficiently large compared with the thickness of the sheet (16) to avoid or minimise shear stress transmission between adjacent areas of the sheet overlying respective adjacent individual electrode elements (10). By imposing a phase or time delay on signals fed to or from the individual electrode elements (10) the beam produced by the array or its response beam may be angularly scanned or focussed. <IMAGE>
Description
SPECIFICATION
Improvements relating to transducers
This invention relates to a transducer for effecting conversion between stress wave and
electrical energy and to a method of making
such a transducer.
The invention has been developed in relation to transducers required for certain forms
of apparatus (hereinafter referred to as being
of the kind specified) but is capable of appli
cation generally to stress wave-electrical transducers.
Apparatus of the kind specified is intended to provide data relating to an object (includ
ing, for example, data as to the existence or position of the object or one or more characteristics of the object) otherwise than by direct vision, and the object data may be ascertained or read either by human perception (as by visual display or by audible or tactile display) or by machine vision.
In a specific form of apparatus of the kind specified the apparatus comprises a combination of
(a) transmitting means for transmitting stress wave energy (hereinafter called the transmitted signal) to a field of view to illuminate the object with such energy,
(b) receiving means for receiving at least part of the energy (herein called the received signal) reflected from the object when in the field of view and effectively forming an image in respect of the illumination of the object by the transmitted signal,
(c) means for imposing predetermined characteristics upon at least part of the signals giving rise to the image in respect of at least one of the parameters pertaining thereto and selected to establish that the image shall contain the required object data,
(d) means for analysing the image derived from the stress wave energy.
The term "image" used herein is to be deemed to include a plurality of signals (readable by human perception or by machine, as appropriate) whether presented serially in time or in spacial juxtaposition or separation and collectively representing the existence, position or attitude of the object, or one or more dimensions thereof, or the configuration or area of the object viewed from any direction.
In a particular form of apparatus of the kind specified the means for imposing predetermined characteristics upon the signals giving rise to the image may differ widely in accordance with the particular data concerning the object which the received signal is required to carry. Thus, if one of the characteristics which the image is required to present is the range or distance of the object or some part thereof from a predetermined point, e.g. the station at which the transmitting means is situated, then the means for imposing the predetermined characteristic may comprise a means for frequency modulating the stress wave transmitted signal in a mode such that the frequency difference between the transmitted signal and the received signal, due to the elapse of transit time between initial radiation of the signal and receipt of the reflection, is representative of the range or distance.In such a case the means for imposing the predetermined characteristic would appropriately impose a frequency sweep on the transmitted signal which may be linear or nonlinear but preferably of saw-tooth form.
If the required object data includes information concerning the lateral or angular position of the object, or a part thereof, or the angular width subtended by the object at a predetermined point, e.g. that at which the transmitting means is situated, then the means for imposing a predetermined characteristic may include means to establish that the transmitted signal and/or the received signal is radiated and/or received respectively by way of a beam represented conveniently as a polar diagram with the radius vector centered on a predetermined point and having a maximum value in the central region of said beam and a minimum value at each of two opposite boundaries thereof in a reference plane. The reference plane may be horizontal, vertical, or in some intermediate angular position.
In some cases it may be advantageous to provide transmitting and/or receiving means in which the beam is convergent to a focus or a focal region spaced longitudinally of the transmitting and/or receiving means along an axis extending outwardly into the field of view.
The means for imposing predetermined characteristics on the transmitted and/or received stress wave signals may further include means for scanning the beam angularly through the field of view between boundaries thereof, e.g. in an asimothal plane or in an elevational plane, or both, or in some intermediate plane.
Transducers for effecting conversion between stress wave energy and electrical energy are required for incorporation in the transmitting means and the receiving means.
Possibly a transducer common to both the transmitting means and the receiving means may be used.
The speed or frequency of which such mode of operation is required to be carried out often precludes the use of mounting means for the transducers permitting the transducers to be moved physically to the different angular positions required.
It is known that such beams may be moved angularly or scanned by the use of a transducer which comprises an array of transducer elements connected to the power amplifier or output element of the transmitting means or to the input element of the receiving means through respective channels which include means for imposing a phase difference or time difference between the signals fed to the transducer elements or received therefrom as the case may be, thereby electronically effecting angular deflection of the beam.
The performance of such an array is adversely affected by the need to provide individual transducer elements to form such array and one of the principal objects of the present invention is to avoid or reduce this disadvantage as well as to provide for reduction in the cost of manufacturing such a transducer array.
Further, in cases where it is required to provide a beam either for the transmitting or receiving means of a form which is convergent to a focus or focal region spaced longitudinally from the transducer means along said axis, the need to provide individual transducer elements imposes considerable complications and contributes to the cost of providing an appropriate array, and imposes considerable limitations on the extent to which the size of the array can be reduced.
According to the invention there is provided a transducer for effecting conversion between stress wave energy and electrical energy comprising a plurality of transducer elements collectively forming an array and each of which includes opposing conductive electrode means and an intervening dielectric element wherein at least the dielectric element comprises a lamina (the first lamina) common to the transducer elements.
Advantageously, one of the opposing electrode means may also comprise a further lamina (the second lamina) which is common to the transducer elements.
The transducer may be combined with time delay means connected to each of, or selected, channels or conductors connected to respective electrode elements of the array, the time delay means imposing respective time delays of such magnitude as to establish a convergent or focused beam.
Further, the transducer may be combined with variable time delay means connected to each of, or selected, channels or conductors connected to respective electrode elements of the array, and means for varying the magnitudes of the respective time delays to establish scanning of a beam provided by the array.
The first lamina may be in the form of a sheet of dielectric material and the second lamina may comprise an electrically conductive film or coating on the sheet.
From a further aspect the invention resides in a method of making a multi-channel transducer for effecting conversion between stress wave energy and electrical energy, such method comprising laying a dielectric lamina over coplanar faces of an array of spaced apart, electrically conductive, electrode elements, securing the lamina peripherally around the array, and providing a further conductive electrode means on the side of the lamina opposite to the array.
The further conductive electrode means may conveniently comprise a further lamina (the second lamina) formed as a film or coating on the first lamina.
The invention will now be described, by way of example, with reference to the accompanying drawings wherein:
Figure 1 is a view in cross-section on the line A-A' of Fig. 2 through one embodiment of transducer in accordance with the invention and made by the method thereof;
Figure 2 is a view in cross-section on the line B-B' of Fig. 1.
Echo location systems (being one form of apparatus of the kind specified) operating in air as aids for the blind commonly use solid dielectric transducers for both radiating and receiving ultrasonic waves. One such system is described by KAY in the Radio and Electronic Engineer, Volume 44, No.11, pp.
605-627 and dated November, 1 974. On page 610 is described the transducer design used in the system. The radiation and receiving field of the transducer is fixed in space relative to the active face and can be moved only by physically moving the transducer.
A line array of transducers of the type described can be used to form a radiation field by suitably coupling them together through an electrical network. When all the signals at the transducer terminals are in phase coincidence a narrower beam is formed which is perpendicular to the active face of the array. Applying a phase delay between each element causes the beam to be deflected from the perpendicular direction by an amount determined by the phase delay. Alternatively, a time delay can be used between each element to produce a deflection of the beam from the perpendicular. Both of these methods of beam deflection or beam scanning are now well known principles used in radar, sonar and ultrasonic testing in solids or body tissue.
The embodiment of the present invention now illustrated and described in effect provides a transducer array as a single unit but with individual channel access to elements of the array. It is not only more convenient to incorporate in apparatus of the kind specified and other forms of apparatus than would be the case were individual transducer elements utilised to form they array, but can also be manufactured more economically and provide improved performance as regards beam deflection or scanning whilst avoiding the necessity to move the array physically.
In the embodiment illustrated a plurality of electrically conductive electrode elements 10 are provided. These may be of electrically conductive metal or of a plastics material (an insulator) coated with electrically conductive metal.
The elements may conveniently be of cubic form, although the height dimension as seen in Fig. 1 and the width dimensions as seen in
Fig. 2 need not necessarily be equal.
The elements 10 are mounted in an array with their top faces 11, as seen in Fig. 2, coplanar and their bottom faces supported by a base plate 1 2 through the intermediary of an intervening plate 1 3 of insulating material.
The plate 1 2 may be formed integrally with an outer frame 14, the top face of which is coplanar with the top faces 11 of the elements 10. The frame 14 and the base plate 1 2 may be formed of metal or a plastics (insulating) material as desired.
The base plate has openings in alignment with respective elements 10 to provide for passage of conductors 1 5 for connection to respective electrode elements 10. The latter may be made of metal or may be made of insulating material with an electrically conductive coating on at least their top faces to which, in this case, the conductors 1 5 would be connected.
On the top faces 11 of the electrode elements 10 is laid a sheet of dielectric material such as "Mylar" (RTM) (the first lamina hereinbefore referred to) and which is coated on its top surface remote from the electrode elements 10 with a film of conducting material, for example aluminium or gold (the second lamina hereinbefore mentioned).
Because of the scale of the drawings these two laminae are not shown separately and a single reference 1 6 designates them collectively.
Conveniently the sheet 1 6 is secured to the top surface of the frame 1 4 adhesively. For this purpose the top surface of the frame 1 4 is preferably roughened on a suitable flat scratching material. The top surfaces of the electrode elements 10 may be roughened as indicated at 21 (shown in two instances only).
This establishes the existence of an air film between the sheet 1 6 and the top surfaces of the electrodes and determines the frequency response of the transducer. Conveniently the roughening of these surfaces of the electrode elements along the top surface of the frame 1 4 may be carried out at the same time in a single operation, although this is not essential.
A typical grit size of 60-280 may be used for effecting the roughening, for example, according to the frequency response required from the transducer. Alternatively the top surface of the elements may be appropriately machined, e.g. to produce grooves as seen at 20 controlling the frequency response. Likewise the top surface of the frame may be machined either separately or at the same time.
The thickness of the sheet 1 6 may typically be 5.0 microns and the film or coating of conductive material 0.05 microns. Preparatory to coating the top surface of the frame 14 with glue and laying the sheet 1 6 thereover, the sheet may be tensioned in its own plane by an amount depending upon the frequency response required. In some circumstances the tension need be sufficient only to remove any wrinkles from the sheet. Clamps 1 9 may be provided to embrace and protect the peripheral margin of the sheet 1 6 and the frame 1 4 and left in position permanently.
The electrode elements 10 are insulated electrically from each other by the provision of lateral gaps 1 7 and 1 8 between them. These may be air gaps but could contain solid state insulating material if required.
The sheet 1 6 is not fixed to the top surfaces of the electrode elements 10, nor is the sheet 1 6 clamped or similarly constrained over those areas which lie above the gaps 1 7 and 1 8 between individual electrode elements 10 whether the gaps are air-filled or contain solid state insulating material.
The gaps 1 7 and 1 8 extending in mutually perpendicular directions of the array may be equal and are preferably substantially greater than the thickness of the sheet 1 6. A typical value for the thickness of the sheet would be, as mentioned, 5 microns whereas each of the gaps 1 7 and 1 8 would typically be 500 microns. This provides for satisfactory operation of the transducer in the frequency range 100 kHz to 200 kHz.
Because each electrode element 10 is required to radiate or receive signals independently, or nearly independently, of each other, and since radiation action is one of movement or deformation of the dielectric lamina either towards or away from the top face of the electrode element 10, it would seem natural to clamp the dielectric sheet in the gaps 1 7 and 1 8 between the elements. It is one of the primary features of the invention that the dielectric is not clamped opposite these gaps and this materially contributes to reducing the difficulty of cost of manufacture.
By adoption of a gap width for the gaps 1 7 and 1 8 which is wide compared with the thickness of the dielectric, shear forces which could propogate through the dielectric across the gaps 1 7 and 1 8 are attenuated sufficiently to make them negligible and avoid or reduce stress coupling between the transducer elements each constituted by an electrode element 10, the portion of the dielectric sheet lying on top of such element, and the further electrode means comprising the film or coating of conductive material (the second lamina) on top of the sheet.
Although the specific embodiment described and illustrated shows the top surfaces of the electrode elements as lying in a single flat plane, it will be understood that it would be within the scope of the invention for these surfaces (collectively) to present some other shape consistent with ability to stress a sheet such as 1 6 over the exposed surfaces of these elements in contact therewith or separated by air gap due to roughening or grooving as previously described. Thus, the upper surfaces of the elements 10 could collectively present a convex cylindrical shape should this be desired.
An application of the invention to a transducer required to provide a convergent or focus beam would include time delay means connected in series with each of, or a selected number of, the conductors 1 5 to impose increments of time delay in radiation (or reception) of wave energy from the electrode elements 10 systematically over the array.
To effect scanning further variable time delay means may be provided in each of the conductors or selected conductors 1 5. Such variable time delay means is preferably activated electronically to achieve rapid cyclic scanning movements of the beam to establish scanning of the field of view.
Claims (14)
1. A transducer for effecting conversion between stress wave energy and electrical energy comprising a plurality of transducer elements collectively forming an array and each of which includes opposed conductive electrode means and an intervening dielectric element, wherein at least the dielectric element comprises a lamina (the first lamina) common to the transducer elements.
2. A transducer according to claim 1 wherein one of the electrode means comprises a further lamina (the second lamina) common to the transducer elements.
3. A transducer according to claim 2 wherein the first lamina comprises a sheet of dielectric material and the second lamina comprises an electrically conductive film or coating on the sheet.
4. A transducer according to claim 3 wherein the other electrode means of each transducer comprises an individual, electrically conductive, electrode element, these electrode elements being spaced apart from each other in a direction parallel to the plane of the sheet to provide gaps between each element.
5. A transducer according to claim 4 wherein those areas of the sheet which are in alignment with the gaps between the electrode elements are free from clamping or constraint in a direction perpendicular to the sheet.
6. A transducer according to either of claims 4 and 5 wherein the width of the gaps between adjacent electrode elements is large compared with the thickness of the sheet.
7. A transducer according to any one of claims 4 to 6 wherein a frame is provided surrounding the electrode elements and the sheet of dielectric material is secured to the frame.
8. A transducer according to claim 7 wherein the sheet is unsecured with respect to the immediately adjacent faces of the electrode elements so as to be free to move towards and away from these.
9. A transducer according to any one of claims 4 to 8 wherein the electrode elements are connected to respective conductors providing for multi-channel connections to or from the transducer.
10. A transducer according to any one of claims 4 to 9 in combination with time delay means connected in each of, or selected, channels or conductors connected to respective electrode elements of the array, the time delay means imposing respective time delays of such magnitude as to establish a convergent or focusing beam.
11. A transducer according to any one of claims 4 to 10 in combination with variable time delay means connected in each of, or selected, channels or conductors connected to respective electrode elements of the array, and means for varying the magnitudes of the respective time delays to establish scanning of a beam provided by the array.
1 2. A method of making a multi-channel transducer for effecting conversion between stress wave energy and electrical energy comprising laying a dielectric lamina over coplanar faces of an array of spaced apart electrically conductive electrode elements, securing the lamina peripherally around the array, and providing further conductive electrode means on the side of the lamina remote from the electrode elements.
1 3. A method according to claim 10 wherein securement of the lamina peripherally is effected by providing a frame surrounding the array of electrode elements and adhesively attaching a margin of the lamina to the frame.
14. A transducer substantially as hereinbefore described with reference to and as shown in the accompanying drawings.
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AU36090/84A AU573655B2 (en) | 1983-12-05 | 1984-11-30 | Transducer array |
US06/676,818 US4704556A (en) | 1983-12-05 | 1984-11-30 | Transducers |
DE8484308392T DE3477287D1 (en) | 1983-12-05 | 1984-12-04 | Improvements relating to transducers |
EP84308392A EP0144234B1 (en) | 1983-12-05 | 1984-12-04 | Improvements relating to transducers |
AT84308392T ATE41542T1 (en) | 1983-12-05 | 1984-12-04 | CONVERTER. |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NZ20647583A NZ206475A (en) | 1983-12-05 | 1983-12-05 | Ultrasonic transducer array provides beam steering |
Publications (3)
Publication Number | Publication Date |
---|---|
GB8414282D0 GB8414282D0 (en) | 1984-07-11 |
GB2151025A true GB2151025A (en) | 1985-07-10 |
GB2151025B GB2151025B (en) | 1987-10-07 |
Family
ID=19920605
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB08414282A Expired GB2151025B (en) | 1983-12-05 | 1984-06-05 | Transducer |
Country Status (3)
Country | Link |
---|---|
JP (1) | JPS60157060A (en) |
GB (1) | GB2151025B (en) |
NZ (1) | NZ206475A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
AU573655B2 (en) * | 1983-12-05 | 1988-06-16 | Kay, L. | Transducer array |
US6771785B2 (en) | 2001-10-09 | 2004-08-03 | Frank Joseph Pompei | Ultrasonic transducer for parametric array |
US6775388B1 (en) | 1998-07-16 | 2004-08-10 | Massachusetts Institute Of Technology | Ultrasonic transducers |
US7391872B2 (en) | 1999-04-27 | 2008-06-24 | Frank Joseph Pompei | Parametric audio system |
US8027488B2 (en) | 1998-07-16 | 2011-09-27 | Massachusetts Institute Of Technology | Parametric audio system |
US8538036B2 (en) | 2002-10-30 | 2013-09-17 | Frank Joseph Pompei | Directed acoustic sound system |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2016862A (en) * | 1978-03-13 | 1979-09-26 | Philips Nv | Electret transducers |
GB2092409A (en) * | 1981-01-31 | 1982-08-11 | Deutsche Forsch Luft Raumfahrt | Ultrasonic transducer |
-
1983
- 1983-12-05 NZ NZ20647583A patent/NZ206475A/en unknown
-
1984
- 1984-06-05 GB GB08414282A patent/GB2151025B/en not_active Expired
- 1984-12-05 JP JP59257272A patent/JPS60157060A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2016862A (en) * | 1978-03-13 | 1979-09-26 | Philips Nv | Electret transducers |
GB2092409A (en) * | 1981-01-31 | 1982-08-11 | Deutsche Forsch Luft Raumfahrt | Ultrasonic transducer |
Cited By (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
AU573655B2 (en) * | 1983-12-05 | 1988-06-16 | Kay, L. | Transducer array |
US6775388B1 (en) | 1998-07-16 | 2004-08-10 | Massachusetts Institute Of Technology | Ultrasonic transducers |
US8027488B2 (en) | 1998-07-16 | 2011-09-27 | Massachusetts Institute Of Technology | Parametric audio system |
US9036827B2 (en) | 1998-07-16 | 2015-05-19 | Massachusetts Institute Of Technology | Parametric audio system |
US7391872B2 (en) | 1999-04-27 | 2008-06-24 | Frank Joseph Pompei | Parametric audio system |
US8953821B2 (en) | 2000-01-14 | 2015-02-10 | Frank Joseph Pompei | Parametric audio system |
US6771785B2 (en) | 2001-10-09 | 2004-08-03 | Frank Joseph Pompei | Ultrasonic transducer for parametric array |
US7657044B2 (en) | 2001-10-09 | 2010-02-02 | Frank Joseph Pompei | Ultrasonic transducer for parametric array |
US8369546B2 (en) | 2001-10-09 | 2013-02-05 | Frank Joseph Pompei | Ultrasonic transducer for parametric array |
US8472651B2 (en) | 2001-10-09 | 2013-06-25 | Frank Joseph Pompei | Ultrasonic transducer for parametric array |
US8538036B2 (en) | 2002-10-30 | 2013-09-17 | Frank Joseph Pompei | Directed acoustic sound system |
Also Published As
Publication number | Publication date |
---|---|
JPS60157060A (en) | 1985-08-17 |
GB8414282D0 (en) | 1984-07-11 |
NZ206475A (en) | 1988-09-29 |
GB2151025B (en) | 1987-10-07 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PCNP | Patent ceased through non-payment of renewal fee |