EP0031614B1 - Curved array of sequenced ultrasound transducers - Google Patents
Curved array of sequenced ultrasound transducers Download PDFInfo
- Publication number
- EP0031614B1 EP0031614B1 EP19800201181 EP80201181A EP0031614B1 EP 0031614 B1 EP0031614 B1 EP 0031614B1 EP 19800201181 EP19800201181 EP 19800201181 EP 80201181 A EP80201181 A EP 80201181A EP 0031614 B1 EP0031614 B1 EP 0031614B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- elements
- array
- transducer elements
- active group
- ultrasound
- 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
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
- G10K11/02—Mechanical acoustic impedances; Impedance matching, e.g. by horns; Acoustic resonators
-
- 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
- G10K11/34—Sound-focusing or directing, e.g. scanning using electrical steering of transducer arrays, e.g. beam steering
- G10K11/341—Circuits therefor
- G10K11/345—Circuits therefor using energy switching from one active element to another
Definitions
- the invention relates to an apparatus for producing and/or receiving a scanned beam of ultrasound energy comprising:
- Internal body organs may be imaged and otherwise characterized by apparatus which. directs pulses of ultrasound energy into the body and subsequently detects echos which originate when the energy is reflected from tissue interfaces or other discontinuities within the body.
- apparatus which. directs pulses of ultrasound energy into the body and subsequently detects echos which originate when the energy is reflected from tissue interfaces or other discontinuities within the body.
- the ultrasound energy is directed into the body in a relatively narrow beam.
- Electric signals which describe the position and direction of the beam with respect to the body, as well as the relative arrival time and amplitude of the echos, are utilized to generate a visual display and/or mapping of the internal body structures.
- the direction of the ultrasound beam is manually controlled by a technician (generally by physical motion of a probe head) to build up a display pattern.
- Ultrasound systems for generating real time displays of rapidly moving body organs generally utilize electromechanical or electronic means to change the position and direction of one or more beams of ultrasound energy with respect to the body.
- Motion of a beam of ultrasound energy with respect to the body may be provided by sequentially activating transducer elements in a flat linear array to effectively scan an area of the body with a sequence of substantially parallel ultrasound beams.
- a device of this type is described in US-A-3,013,170.
- a beam of ultrasound energy may, alternately, be scanned around a single origin point to produce a so- called "sector-scan".
- Sector-scan geometries are particularly useful since ultrasound energy may be directed between the ribs to scan the interior of the chest cavity.
- Sector scanning has been achieved in the prior art by rapidly rotating one or more transducers about an axis, by steering energy from a fixed transducer with a rotating ultrasound reflector, or by sequencing individual transducer elements in a linear curved array.
- DE-A-2,818,915 describes a curved transducer array with individual transducers which are individually activated to produce a sector-scan.
- the transverse spatial resolution which may be obtained from a sequence array of ultrasound transducers is related to dimensions of the individual transducer elements in the array. Small transducer elements are desirable for obtaining fine resolution.
- the amount of ultrasound energy produced by an individual transducer element is, however, limited by its size.
- the signal-to-noise ratio of the returned ultrasound echos necessarily depends on the amount of ultrasound energy introduced into the body. Thus, the signal to noise ratio suffers if small transducer elements are individually activated to achieve a scanning action. Diffraction effects will furthermore, cause spreading of an ultrasound beam which originates from a single, small ultrasound transducer element.
- the ultrasonic beam is directed through a small window in order to decrease its lateral dimensions, thereby decreasing the amount of energy in the beam even further.
- the apparatus according to the invention is characterized in that it further comprises:
- the invention also relates to a method for manufacturing a curved array of ultrasound transducer elements for such an apparatus, comprising the steps of:
- Figure 1 is a linear array of ultrasound transducers 110 which is known in the prior art.
- a series of individual transducers elements 100 are disposed along a line 101.
- Separate electrodes 102 are provided for each transducer in the array and are connected to electronic circuits (not shown) which permit sequential activation of the elements to, in effect, move the source of an ultrasound beam along the line 101.
- Figure 2 illustrates an application of the array 110 of Figure 1.
- a group of adjacent transducers 111 are simultaneously activated to produce a beam of ultrasound energy 112 which is inwardly projected into a body 113.
- the array 110 is disposed on the surface of a probe assembly 114 which includes switching circuits 115.
- the switching circuits act to incrementally shift the group of active transducers 111 along the array to generate a linear scan of the beam 112 with respect to the body.
- the operation of prior art imaging systems with incrementally shifted arrays is described in the articles Ultrasonic Imaging Using Arrays, Albert Macovski and Methods and Terminology for Diagnostic Ultrasound Imaging Systems, Maxwell G. Maginness in the Proceedings of the IEEE, Vol. 67, No. 4, April 1979 at page 484 and 641 respectively.
- British patent Specification 1,546,445 describes a curved linear array of transducers which are individually activated to generate a sector-scanned ultrasound beam.
- a positive (converging) lens is utilized with the transducer array to focus the beam through the spaces between the ribs. Because only one transducer element is active at a time, the array of British patent 1,546,445 suffers from relatively low spatial resolution and signal-to-noise ratio. The performance of the array cannot, however, be improved by directly applying the incrementally shifted active group geometry of Figure 2 to the curved array configuration.
- the simultaneous activation of a group of adjacent elements on a curved array necessarily produces a sharply focussed beam which diverges in the far field and is unsuitable for medical imaging.
- FIG. 3 schematically illustrates a transducer array of the present invention.
- a plurality of electro-acoustic transducer elements 200 are disposed along an arc and are oriented to project and receive ultrasound energy in the direction of the center of the arc.
- the individual elements 200 in the array are provided with separate electrodes and are connected, via wires 202, and a sequencing circuit to pulse generator and receiver circuits (not shown).
- the array is contained in a housing 204 which includes an ultrasound transmissive window 206.
- the housing may be filled with an ultrasound transmissive fluid 208, for example, castor oil, which is matched to the ultrasound transmissive properties of the human body. Alternately the housing may be filled with a solid material. In general the filling should have an acoustic attenuation between those of water and human tissue and should have an acoustic impedance which is matched to the impedance of human tissue.
- a group of adjacent transducer elements (for example 220) within the array is activated for the transmission and reception of each ultrasound pulse.
- the active group of transducers is incrementally shifted along the array, one transducer at a time, on a pulse to pulse basis to provide a sector scan of ultrasound energy.
- Defocussing means are included to compensate for the strong inherent focussing of the curved array.
- the curved array, with an incrementally shifted group of active detectors, in combination with the defocussing means, produces a finer spatial resolution and higher signal to noise ratio than curved sequenced arrays of the prior art.
- FIG. 4 illustrates a preferred embodiment of the defocussing means.
- a group 220 of adjacent transducers A-K within the array is activated by sequencing switches (not shown for the sake for clarity).
- the central transducer F within the zone is connected directly to ultrasound pulse generator 240 and receiver 250 circuits via a transmit-receive (TR) switch 260.
- TR transmit-receive
- the transducer pair E and G immediately adjacent the central transducer is connected to the TR switch 260 via a first delay 270.
- the next adjacent pair of transducers D and H are connected to the TR switch through a second delay circuit 280 which provides a longer delay than the delay circuit 270.
- Each next adjacent pair of transducers within the group i.e.
- C and I, B and J, A and K are connected to the TR switch via delay circuits (290, 300, 310) which provide increasing delays in proportion to the distance from the center of the active group to the associated transducers.
- the magnitude of the delays are chosen, using techniques which are well known in the art and which are described, for example, in the above referenced Macovski article, to compensate for the physical focussing effects of the curved array and thus provide a more parallel beam of ultrasound energy. Alternately the beam may thus be focussed at a point deep within the body of a patient.
- Figure 5 illustrates a system for incrementally shifting the active group along the transducer array.
- Pulsers 400, receiver amplifiers 410, and associated TR isolators 420 are connected in a conventional fashion to first ends of a bank of bidirectional delay lines 430.
- the bank of delay lines 430 includes delay lines of varying time delay which are calculated to provide the defocussing compensation for the active group as described above with respect to the Figure 4.
- the opposite end of each delay line in the bank 430 is connected to a row of switches in an analog switch matrix 440.
- Each column of switches in the switch matrix 440 is connected to a separate element 200 in the transducer array 450.
- a separate switch (which may be a MOS transistor) is provided at each cross point (that is the intersection of each row with each column) in the switch matrix.
- the switching elements are individually activated by the output lines of a read-only memory (ROM) 460.
- Input lines of the read-only memory 460 are addressed by the output of a sequencer circuit which may be a sequential counter 470 driven by a clock 480.
- the sequencer circuit addresses consecutive words in the read-only memory which establish the connection patterns between the individual transducer elements in the array and corresponding delay lines to effect incremental shifting of a defocussed, active group along the array.
- Table I illustrates the first three words of a read-only memory which shifts an active group of nine transducer elements along an array by establishing connections to four delay lines I through IV.
- bit patterns of Table I are shortened for the sake of clarity of illustration; the principles illustrated therein may be extended to active groups and arrays which include larger or smaller numbers of transducer elements.
- Figure 6 is an alternate embodiment of a transducer array wherein the defocussing means comprise a negative lens 500.
- a group of transducers is sequentially shifted across the array as in the embodiment of Figure 3 to produce a sector scan. All of the transducers in the group 200 may be simultaneously pulsed.
- the delay line defocussing means of Figure 4 may be utilized in conjunction with the lens 500.
- the lens may be constructed from metal or plastic and may advantageously comprise two negative lens elements separated by a fluid-filled cavity 510.
- FIG. 7 illustrates first steps in a preferred method for manufacturing the transducer array.
- the array is advantageously formed from a single rectangular bar 600 of piezo-electric ceramic (which may comprise Type PZT-5). Copper electrodes 605 and 610 are bonded to the front 601 and rear 602 major surfaces of the bar with a silver bearing epoxy resin.
- a flexible matching window 615 is then cast directly on the front electrode.
- the matching window may be advantageously cast from a mixture of two parts of a Stycast 1264 resin binder and one part tungsten powder. The window is cast by pouring the mixture directly onto the surface of the front electrode and allowing the tungsten powder to settle. After the resin is cured, the window is machined to a thickness of one quarter acoustic wavelength at the operating frequency of the array. For example, a window designed for operation at 3.5 MHz is machined to approximately 0.09 mm thickness.
- a series of parallel grooves 620 are then cut through the rear electrode 610 and into the upper surface of the bar to segregate individual transducer elements 630 with their associated rear electrodes.
- the grooves are approximately 0.13 mm wide and penetrate to 75% of the thickness of the ceramic bar.
- the ceramic bar is approximately 80.5 millimeters long, 12.5 millimeters wide, and 2.0 millimeters thick.
- the bar is divided by 71 saw cuts to form 72 transducer elements.
- the rear electrodes on the endmost transducer elements are grounded to the front electrode so that the array comprises 70 functional transducer elements.
- Figures 8 and 9 illustrate the further construction of the array.
- the grooved ceramic bar 600 with attached electrodes 605 and 610 and window 615 is formed around a semicylindrical mandrel 650, the grooves in the bar being parallel to the axis of the cylinder.
- the bar cracks under each groove 620 to produce a curved array of separate, electroded transducer elements 630 which are retained in place by the front electrode 605 and window 615.
- a supporting foam air cell 660 is then cast between the elements 630 and around the rear surface of the curved transducer array.
- the air cell retains the transducer elements in place and further provides a low acoustic impedance backing for the individual elements.
- the air cell may typically comprise glass micro-balloons in an epoxy resin binder.
- the upper electrodes 610 are wider than the ceramic bar and are folded back along the edges of the air cell to provide electrical connections to the individual elements.
Description
- The invention relates to an apparatus for producing and/or receiving a scanned beam of ultrasound energy comprising:
- an array, including a plurality of ultrasound transducer elements disposed along a curved line, each element being oriented to direct ultrasound energy towards and to receive ultrasound energy from the center of the curve; and
- means for transmitting electrical pulses to and for receiving electrical pulses from the transducer elements.
- Internal body organs may be imaged and otherwise characterized by apparatus which. directs pulses of ultrasound energy into the body and subsequently detects echos which originate when the energy is reflected from tissue interfaces or other discontinuities within the body. In typical apparatus the ultrasound energy is directed into the body in a relatively narrow beam. Electric signals which describe the position and direction of the beam with respect to the body, as well as the relative arrival time and amplitude of the echos, are utilized to generate a visual display and/or mapping of the internal body structures. In many applications the direction of the ultrasound beam is manually controlled by a technician (generally by physical motion of a probe head) to build up a display pattern. While these methods are adequate for imaging stationary body structures, the time required for physical motion of a probe is generally much too long to image rapidly moving body structures (for example the valves in a beating heart) in real time. Ultrasound systems for generating real time displays of rapidly moving body organs generally utilize electromechanical or electronic means to change the position and direction of one or more beams of ultrasound energy with respect to the body.
- Motion of a beam of ultrasound energy with respect to the body may be provided by sequentially activating transducer elements in a flat linear array to effectively scan an area of the body with a sequence of substantially parallel ultrasound beams. A device of this type is described in US-A-3,013,170. A beam of ultrasound energy may, alternately, be scanned around a single origin point to produce a so- called "sector-scan". Sector-scan geometries are particularly useful since ultrasound energy may be directed between the ribs to scan the interior of the chest cavity. Sector scanning has been achieved in the prior art by rapidly rotating one or more transducers about an axis, by steering energy from a fixed transducer with a rotating ultrasound reflector, or by sequencing individual transducer elements in a linear curved array. DE-A-2,818,915 describes a curved transducer array with individual transducers which are individually activated to produce a sector-scan.
- The transverse spatial resolution which may be obtained from a sequence array of ultrasound transducers is related to dimensions of the individual transducer elements in the array. Small transducer elements are desirable for obtaining fine resolution. The amount of ultrasound energy produced by an individual transducer element is, however, limited by its size. The signal-to-noise ratio of the returned ultrasound echos necessarily depends on the amount of ultrasound energy introduced into the body. Thus, the signal to noise ratio suffers if small transducer elements are individually activated to achieve a scanning action. Diffraction effects will furthermore, cause spreading of an ultrasound beam which originates from a single, small ultrasound transducer element. In the apparatus described in DEA2,B1B,915 the ultrasonic beam is directed through a small window in order to decrease its lateral dimensions, thereby decreasing the amount of energy in the beam even further.
- In the prior art the amount of energy in a beam produced by a flat linear array has been increased by simultaneously activating a group of adjacent transducers. Means were provided for incrementally shifting the active group along the array to provide fine spatial resolution and high signal-to-noise ratios. While this technique is appropriate for use with flat transducer arrays, which produce a parallel beam scanning geometry, the simultaneous activation of a group of adjacent transducers in a curved array inherently generates a focussed ultrasound beam. Sequenced group arrays have not, therefore, found application for the generation of high resolution sector-scans.
- It is an object of the invention to provide an apparatus of the kind described, in which simultaneous activation of a group of adjacent transducers is possible without a focussed ultrasound beam being generated. To this end the apparatus according to the invention is characterized in that it further comprises:
- means for connecting a group of active transducer elements to the means for transmitting electrical pulses and for receiving electrical pulses, the group of active elements comprising a preselected number of adjacent transducer elements in the array, said preselected number being greater than one and less than the total number of transducer elements in the array;
- means for sequentially changing the elements in the active group to incrementally shift the active group along the curve; and
- means for defocussing ultrasound energy produced and received by the transducer elements in the active group which means function to cause said ultrasound energy to be directed in a substantially parallel beam.
- The invention also relates to a method for manufacturing a curved array of ultrasound transducer elements for such an apparatus, comprising the steps of:
- attaching front and rear conductive electrodes to front and rear surfaces respectively of a substantially flat bar of piezo-electric ceramic;
- cutting a plurality of parallel grooves through the rear electrode and partially through the thickness of the bar;
- placing the front surface of the grooved bar on a semicylindrical mandrel, the grooves being parallel to the axis of the mandrel, and bending the bar around the mandrel so that portions of the bar under the grooves are fractured to separate individual transducer elements, the front electrode remaining intact during the fracturing of the bar, the individual elements being retained against the mandrel by at least the front electrode; and
- filling the spaces between the individual transducer elements with a resin binder which retains the elements on an arc conforming to the surface of the mandrel.
- It is pointed out that GB-A-1,437,486 describes a curved transducer array comprising straight linear arrays that consist of slabs of piezo-electric material that have been provided with slots.
- The invention will now be explained more in detail with reference to the attached drawings in which:
- Figures 1 and 2 show a prior art sequenced flat array of ultrasound transducers;
- Figure 3 is a curved transducer array of the present invention;
- Figure 4 illustrates the principle of time delay defocussing for the array of Fig. 3;
- Figure 5 schematically illustrates a system for operating the array of Figure 3;
- Figure 6 is an alternate embodiment of the invention which includes a defocussing lens;
- Figure 7 illustrates a stage in the production of the array of Figure 3;
- Figure 8 illustrates a completed array; and
- Figure 9 is a detail of Figure 8.
- Figure 1 is a linear array of
ultrasound transducers 110 which is known in the prior art. A series ofindividual transducers elements 100 are disposed along aline 101.Separate electrodes 102 are provided for each transducer in the array and are connected to electronic circuits (not shown) which permit sequential activation of the elements to, in effect, move the source of an ultrasound beam along theline 101. - Figure 2 illustrates an application of the
array 110 of Figure 1. A group ofadjacent transducers 111 are simultaneously activated to produce a beam ofultrasound energy 112 which is inwardly projected into abody 113. Thearray 110 is disposed on the surface of aprobe assembly 114 which includesswitching circuits 115. The switching circuits act to incrementally shift the group ofactive transducers 111 along the array to generate a linear scan of thebeam 112 with respect to the body. The operation of prior art imaging systems with incrementally shifted arrays is described in the articles Ultrasonic Imaging Using Arrays, Albert Macovski and Methods and Terminology for Diagnostic Ultrasound Imaging Systems, Maxwell G. Maginness in the Proceedings of the IEEE, Vol. 67, No. 4, April 1979 at page 484 and 641 respectively. Those articles are incorporated herein, by reference, as background material. As indicated in those articles, the incremental shifting of a group of transducers within the array improves spatial resolution and provides a higher signal to noise ratio than could be achieved by the sequential activation of individual transducer elements. - British patent Specification 1,546,445 describes a curved linear array of transducers which are individually activated to generate a sector-scanned ultrasound beam. A positive (converging) lens is utilized with the transducer array to focus the beam through the spaces between the ribs. Because only one transducer element is active at a time, the array of British patent 1,546,445 suffers from relatively low spatial resolution and signal-to-noise ratio. The performance of the array cannot, however, be improved by directly applying the incrementally shifted active group geometry of Figure 2 to the curved array configuration. The simultaneous activation of a group of adjacent elements on a curved array necessarily produces a sharply focussed beam which diverges in the far field and is unsuitable for medical imaging.
- Figure 3 schematically illustrates a transducer array of the present invention. A plurality of electro-
acoustic transducer elements 200 are disposed along an arc and are oriented to project and receive ultrasound energy in the direction of the center of the arc. Theindividual elements 200 in the array are provided with separate electrodes and are connected, viawires 202, and a sequencing circuit to pulse generator and receiver circuits (not shown). The array is contained in ahousing 204 which includes anultrasound transmissive window 206. The housing may be filled with anultrasound transmissive fluid 208, for example, castor oil, which is matched to the ultrasound transmissive properties of the human body. Alternately the housing may be filled with a solid material. In general the filling should have an acoustic attenuation between those of water and human tissue and should have an acoustic impedance which is matched to the impedance of human tissue. - A group of adjacent transducer elements (for example 220) within the array is activated for the transmission and reception of each ultrasound pulse. The active group of transducers is incrementally shifted along the array, one transducer at a time, on a pulse to pulse basis to provide a sector scan of ultrasound energy. Defocussing means are included to compensate for the strong inherent focussing of the curved array. The curved array, with an incrementally shifted group of active detectors, in combination with the defocussing means, produces a finer spatial resolution and higher signal to noise ratio than curved sequenced arrays of the prior art.
- Figure 4 illustrates a preferred embodiment of the defocussing means. At a given instant, a
group 220 of adjacent transducers A-K within the array is activated by sequencing switches (not shown for the sake for clarity). The central transducer F within the zone is connected directly toultrasound pulse generator 240 andreceiver 250 circuits via a transmit-receive (TR)switch 260. The transducer pair E and G immediately adjacent the central transducer is connected to theTR switch 260 via afirst delay 270. The next adjacent pair of transducers D and H are connected to the TR switch through asecond delay circuit 280 which provides a longer delay than thedelay circuit 270. Each next adjacent pair of transducers within the group (i.e. C and I, B and J, A and K) are connected to the TR switch via delay circuits (290, 300, 310) which provide increasing delays in proportion to the distance from the center of the active group to the associated transducers. The magnitude of the delays are chosen, using techniques which are well known in the art and which are described, for example, in the above referenced Macovski article, to compensate for the physical focussing effects of the curved array and thus provide a more parallel beam of ultrasound energy. Alternately the beam may thus be focussed at a point deep within the body of a patient. - Figure 5 illustrates a system for incrementally shifting the active group along the transducer array.
Pulsers 400,receiver amplifiers 410, and associated TR isolators 420 are connected in a conventional fashion to first ends of a bank ofbidirectional delay lines 430. The bank ofdelay lines 430 includes delay lines of varying time delay which are calculated to provide the defocussing compensation for the active group as described above with respect to the Figure 4. The opposite end of each delay line in thebank 430 is connected to a row of switches in ananalog switch matrix 440. Each column of switches in theswitch matrix 440 is connected to aseparate element 200 in thetransducer array 450. A separate switch (which may be a MOS transistor) is provided at each cross point (that is the intersection of each row with each column) in the switch matrix. The switching elements are individually activated by the output lines of a read-only memory (ROM) 460. Input lines of the read-only memory 460 are addressed by the output of a sequencer circuit which may be asequential counter 470 driven by aclock 480. The sequencer circuit addresses consecutive words in the read-only memory which establish the connection patterns between the individual transducer elements in the array and corresponding delay lines to effect incremental shifting of a defocussed, active group along the array. As an example, Table I illustrates the first three words of a read-only memory which shifts an active group of nine transducer elements along an array by establishing connections to four delay lines I through IV. -
- The bit patterns of Table I are shortened for the sake of clarity of illustration; the principles illustrated therein may be extended to active groups and arrays which include larger or smaller numbers of transducer elements.
- Figure 6 is an alternate embodiment of a transducer array wherein the defocussing means comprise a
negative lens 500. A group of transducers is sequentially shifted across the array as in the embodiment of Figure 3 to produce a sector scan. All of the transducers in thegroup 200 may be simultaneously pulsed. Alternately, the delay line defocussing means of Figure 4 may be utilized in conjunction with thelens 500. The lens may be constructed from metal or plastic and may advantageously comprise two negative lens elements separated by a fluid-filledcavity 510. - Figure 7 illustrates first steps in a preferred method for manufacturing the transducer array. The array is advantageously formed from a single
rectangular bar 600 of piezo-electric ceramic (which may comprise Type PZT-5).Copper electrodes flexible matching window 615 is then cast directly on the front electrode. The matching window may be advantageously cast from a mixture of two parts of a Stycast 1264 resin binder and one part tungsten powder. The window is cast by pouring the mixture directly onto the surface of the front electrode and allowing the tungsten powder to settle. After the resin is cured, the window is machined to a thickness of one quarter acoustic wavelength at the operating frequency of the array. For example, a window designed for operation at 3.5 MHz is machined to approximately 0.09 mm thickness. - A series of
parallel grooves 620 are then cut through therear electrode 610 and into the upper surface of the bar to segregateindividual transducer elements 630 with their associated rear electrodes. Typically the grooves are approximately 0.13 mm wide and penetrate to 75% of the thickness of the ceramic bar. - In a preferred embodiment of the array the ceramic bar is approximately 80.5 millimeters long, 12.5 millimeters wide, and 2.0 millimeters thick. The bar is divided by 71 saw cuts to form 72 transducer elements. The rear electrodes on the endmost transducer elements are grounded to the front electrode so that the array comprises 70 functional transducer elements.
- Figures 8 and 9 illustrate the further construction of the array. The grooved
ceramic bar 600 with attachedelectrodes window 615 is formed around asemicylindrical mandrel 650, the grooves in the bar being parallel to the axis of the cylinder. As illustrated in detail Figure 9 the bar cracks under eachgroove 620 to produce a curved array of separate,electroded transducer elements 630 which are retained in place by thefront electrode 605 andwindow 615. - A supporting
foam air cell 660 is then cast between theelements 630 and around the rear surface of the curved transducer array. The air cell retains the transducer elements in place and further provides a low acoustic impedance backing for the individual elements. The air cell may typically comprise glass micro-balloons in an epoxy resin binder. - In a preferred embodiment of the invention the
upper electrodes 610 are wider than the ceramic bar and are folded back along the edges of the air cell to provide electrical connections to the individual elements.
Claims (10)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US10451679A | 1979-12-17 | 1979-12-17 | |
US104516 | 1979-12-17 |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0031614A1 EP0031614A1 (en) | 1981-07-08 |
EP0031614B1 true EP0031614B1 (en) | 1984-10-24 |
EP0031614B2 EP0031614B2 (en) | 1990-07-18 |
Family
ID=22300906
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP19800201181 Expired EP0031614B2 (en) | 1979-12-17 | 1980-12-09 | Curved array of sequenced ultrasound transducers |
Country Status (5)
Country | Link |
---|---|
EP (1) | EP0031614B2 (en) |
JP (1) | JPS56103598A (en) |
CA (1) | CA1152729A (en) |
DE (1) | DE3069525D1 (en) |
ES (1) | ES497752A0 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9224938B2 (en) | 2011-04-11 | 2015-12-29 | Halliburton Energy Services, Inc. | Piezoelectric element and method to remove extraneous vibration modes |
Families Citing this family (33)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS57113596U (en) * | 1980-12-30 | 1982-07-14 | ||
JPS5887998A (en) * | 1981-11-20 | 1983-05-25 | Hitachi Ltd | Manufacture of ultrasonic wave probe |
JPS5996999U (en) * | 1982-12-21 | 1984-06-30 | 横河電機株式会社 | Ultrasonic array transducer |
US4523122A (en) * | 1983-03-17 | 1985-06-11 | Matsushita Electric Industrial Co., Ltd. | Piezoelectric ultrasonic transducers having acoustic impedance-matching layers |
JPS59202058A (en) * | 1983-05-02 | 1984-11-15 | Hitachi Medical Corp | Production of probe for ultrasonic inspection apparatus |
DE3483174D1 (en) * | 1983-06-07 | 1990-10-18 | Matsushita Electric Ind Co Ltd | ULTRASONIC TRANSMITTER WITH AN ABSORBING CARRIER. |
JPS60114239A (en) * | 1983-11-28 | 1985-06-20 | 株式会社日立製作所 | Ultrasonic probe |
JPS60192500A (en) * | 1984-03-14 | 1985-09-30 | Nippon Dempa Kogyo Co Ltd | Matrix array type ultrasonic wave probe and its manufacture |
FR2580286B1 (en) * | 1985-04-12 | 1987-05-22 | Sintra | LIGHT ANECHICAL MATERIAL |
FR2614747B1 (en) * | 1987-04-28 | 1989-07-28 | Dory Jacques | ELASTIC PULSE GENERATOR HAVING A PREDETERMINED WAVEFORM AND ITS APPLICATION TO TREATMENT OR MEDICAL DIAGNOSIS |
DK5392A (en) * | 1992-01-17 | 1993-07-18 | Reson System As | SONAR EQUIPMENT FOR MARITIME ENVIRONMENT |
US5423220A (en) * | 1993-01-29 | 1995-06-13 | Parallel Design | Ultrasonic transducer array and manufacturing method thereof |
KR0165516B1 (en) * | 1996-02-26 | 1999-05-01 | 김광호 | Vibration detecting sensor |
US6337465B1 (en) * | 1999-03-09 | 2002-01-08 | Mide Technology Corp. | Laser machining of electroactive ceramics |
US6618620B1 (en) | 2000-11-28 | 2003-09-09 | Txsonics Ltd. | Apparatus for controlling thermal dosing in an thermal treatment system |
US6632179B2 (en) * | 2001-07-31 | 2003-10-14 | Koninklijke Philips Electronics N.V. | Acoustic imaging system with non-focusing lens |
JP3856380B2 (en) * | 2002-04-26 | 2006-12-13 | テイカ株式会社 | Composite piezoelectric vibrator and manufacturing method thereof |
US7611462B2 (en) * | 2003-05-22 | 2009-11-03 | Insightec-Image Guided Treatment Ltd. | Acoustic beam forming in phased arrays including large numbers of transducer elements |
US8409099B2 (en) | 2004-08-26 | 2013-04-02 | Insightec Ltd. | Focused ultrasound system for surrounding a body tissue mass and treatment method |
US20070016039A1 (en) | 2005-06-21 | 2007-01-18 | Insightec-Image Guided Treatment Ltd. | Controlled, non-linear focused ultrasound treatment |
DE102006010009A1 (en) * | 2006-03-04 | 2007-09-13 | Intelligendt Systems & Services Gmbh & Co Kg | A method of manufacturing an ultrasonic probe with an ultrasonic transducer assembly having a curved transmitting and receiving surface |
US8235901B2 (en) | 2006-04-26 | 2012-08-07 | Insightec, Ltd. | Focused ultrasound system with far field tail suppression |
WO2011045669A2 (en) | 2009-10-14 | 2011-04-21 | Insightec Ltd. | Mapping ultrasound transducers |
US9852727B2 (en) | 2010-04-28 | 2017-12-26 | Insightec, Ltd. | Multi-segment ultrasound transducers |
EP2571574B1 (en) * | 2010-05-05 | 2015-04-08 | Technion Research & Development Foundation Ltd. | System of operating a multi focused acoustic wave source |
US9981148B2 (en) | 2010-10-22 | 2018-05-29 | Insightec, Ltd. | Adaptive active cooling during focused ultrasound treatment |
WO2013059358A2 (en) | 2011-10-17 | 2013-04-25 | Butterfly Network, Inc. | Transmissive imaging and related apparatus and methods |
US9667889B2 (en) | 2013-04-03 | 2017-05-30 | Butterfly Network, Inc. | Portable electronic devices with integrated imaging capabilities |
DE102013211627A1 (en) | 2013-06-20 | 2014-12-24 | Robert Bosch Gmbh | Electroacoustic transducer |
FR3027827B1 (en) * | 2014-11-03 | 2020-01-31 | Imasonic | ULTRASONIC TRANSDUCER WITH MICROBALLOON LAYER |
GB2557345B (en) | 2016-12-08 | 2021-10-13 | Bae Systems Plc | MIMO communication system and data link |
GB2565159B (en) * | 2017-07-19 | 2021-12-01 | Bae Systems Plc | Electroacoustic transducer |
CN110646802B (en) * | 2019-09-26 | 2022-08-02 | 哈尔滨工程大学 | Hydrophone mirror symmetry arc array and arrangement method thereof |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS52131676A (en) * | 1976-04-27 | 1977-11-04 | Tokyo Shibaura Electric Co | Probe for ultrasonic diagnostic device |
-
1980
- 1980-12-09 DE DE8080201181T patent/DE3069525D1/en not_active Expired
- 1980-12-09 EP EP19800201181 patent/EP0031614B2/en not_active Expired
- 1980-12-13 JP JP17527380A patent/JPS56103598A/en active Granted
- 1980-12-15 ES ES497752A patent/ES497752A0/en active Granted
- 1980-12-16 CA CA000366878A patent/CA1152729A/en not_active Expired
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9224938B2 (en) | 2011-04-11 | 2015-12-29 | Halliburton Energy Services, Inc. | Piezoelectric element and method to remove extraneous vibration modes |
Also Published As
Publication number | Publication date |
---|---|
ES8107014A1 (en) | 1981-09-16 |
ES497752A0 (en) | 1981-09-16 |
JPS56103598A (en) | 1981-08-18 |
EP0031614B2 (en) | 1990-07-18 |
EP0031614A1 (en) | 1981-07-08 |
CA1152729A (en) | 1983-08-30 |
DE3069525D1 (en) | 1984-11-29 |
JPH0452040B2 (en) | 1992-08-20 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP0031614B1 (en) | Curved array of sequenced ultrasound transducers | |
US4281550A (en) | Curved array of sequenced ultrasound transducers | |
US4550606A (en) | Ultrasonic transducer array with controlled excitation pattern | |
US5651365A (en) | Phased array transducer design and method for manufacture thereof | |
US5678554A (en) | Ultrasound transducer for multiple focusing and method for manufacture thereof | |
US4254661A (en) | Ultrasonic transducer array | |
US5820564A (en) | Method and apparatus for surface ultrasound imaging | |
JP4422718B2 (en) | Micromachined ultrasonic transducer with bias polar beam profile control | |
US4518889A (en) | Piezoelectric apodized ultrasound transducers | |
US6419633B1 (en) | 2D ultrasonic transducer array for two dimensional and three dimensional imaging | |
US6087762A (en) | Ultrasound transceiver and method for producing the same | |
US4542653A (en) | Apparatus and method for beamforming in an ultrasonic transducer array | |
JP2851005B2 (en) | Ultrasonic beam three-dimensional focusing device | |
US4640291A (en) | Bi-plane phased array for ultrasound medical imaging | |
EP0376567A3 (en) | Array of ultrasonic transducer | |
JP5160634B2 (en) | Method and apparatus for forming a microbeam using an adjustable fluid lens | |
US6926671B2 (en) | Ultrasonic imaging apparatus and method | |
CA1133625A (en) | Devices using ultrasounds for forming images, in particular for the internal examination of the human body | |
EP3675742A1 (en) | Dual frequency plane wave ultrasound imaging system | |
CA1201197A (en) | Variable focus transducer | |
US6160340A (en) | Multifrequency ultrasonic transducer for 1.5D imaging | |
KR20030045135A (en) | Method, system and probe for obtaining images | |
US5931785A (en) | Ultrasonic transducer having elements arranged in sections of differing effective pitch | |
US9833219B2 (en) | Angle oriented array for medical ultrasound | |
Payne et al. | Integrated ultrasound transducers |
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 |
Designated state(s): DE FR GB IT SE |
|
17P | Request for examination filed |
Effective date: 19810720 |
|
ITF | It: translation for a ep patent filed |
Owner name: ING. C. GREGORJ S.P.A. |
|
GRAA | (expected) grant |
Free format text: ORIGINAL CODE: 0009210 |
|
AK | Designated contracting states |
Designated state(s): DE FR GB IT SE |
|
REF | Corresponds to: |
Ref document number: 3069525 Country of ref document: DE Date of ref document: 19841129 |
|
ET | Fr: translation filed | ||
PLBI | Opposition filed |
Free format text: ORIGINAL CODE: 0009260 |
|
26 | Opposition filed |
Opponent name: SIEMENS AKTIENGESELLSCHAFT, BERLIN UND MUENCHEN Effective date: 19850710 |
|
PUAH | Patent maintained in amended form |
Free format text: ORIGINAL CODE: 0009272 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: PATENT MAINTAINED AS AMENDED |
|
27A | Patent maintained in amended form |
Effective date: 19900718 |
|
AK | Designated contracting states |
Kind code of ref document: B2 Designated state(s): DE FR GB IT SE |
|
ITF | It: translation for a ep patent filed |
Owner name: ING. C. GREGORJ S.P.A. |
|
ET3 | Fr: translation filed ** decision concerning opposition | ||
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: GB Payment date: 19901130 Year of fee payment: 11 |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: FR Payment date: 19901218 Year of fee payment: 11 |
|
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: SE Payment date: 19901219 Year of fee payment: 11 |
|
ITTA | It: last paid annual fee | ||
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: DE Payment date: 19910225 Year of fee payment: 11 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: GB Effective date: 19911209 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: SE Effective date: 19911210 |
|
GBPC | Gb: european patent ceased through non-payment of renewal fee | ||
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: FR Effective date: 19920831 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: DE Effective date: 19920901 |
|
REG | Reference to a national code |
Ref country code: FR Ref legal event code: ST |
|
EUG | Se: european patent has lapsed |
Ref document number: 80201181.7 Effective date: 19920704 |