CN1756955A - Device having matched accoustical impedance and method - Google Patents
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Abstract
The invention, in its several embodiments, includes a method of making (100, 300) a plurality of impedance-matched layers (215, 220, 225) interposed between a target media (230) and an acoustical source (210), the interposed impedance-matched layers (215, 220, 225) thereby providing optimal transmission of energy from the acoustical source (210) or a transducer (110) to the target media (230).
Description
Technical field
Relate generally to sound source of the present invention and ultrasonic transducer are specifically related to have the ultrasonic transducer of optimum sound impedance matching, and make this type of device reach the method for optimum sound impedance matching.
Background technology
When a sound source is conveyed into target material with signal,, will lose many acoustic energy if acoustic impedance does not match between sound source and target material.For example, during medical ultrasound was learned, what be used as transducer was approximately 34 * 10 such as its acoustic impedance of typical piezoelectric supersonic source
6Kg/m
2S, and be analogous to the acoustic impedance of water under the medical treatment situation as the acoustic impedance of the human body of target, be 1.5 * 10
6Kg/m
2S.Well-known in the present technique field, the difference that the energy reflection coefficient equals two acoustic impedances divided by these two acoustic impedance sums, again get resultant numerical value square.To cause on the interface between skin tissue and the transducer about 84% acoustic energy to be reflected when so, acoustic impedance does not match.For top example, sound energy reflection coefficient is about 0.84, this means, roughly 84% incident acoustic energy is reflected.The solution of this kind serious problems is to settle " quarter-wave matching layer " between skin tissue and transducer knownly.Be placed in lip-deep its acoustic impedance of this kind matching layer of piezoelectric crystal and should be the geometrical mean of sound source acoustic impedance and target skin acoustic impedance, its thickness should equal the quarter-wave odd-multiple of sound wave in the matching layer.During with mathematical symbolism, make Z
0Represent the acoustic impedance of piezoelectric crystal, Z
2Represent the acoustic impedance of target skin, then the acoustic impedance Z of matching layer
1Provide by following formula:
Z
1＝(Z
0 Z
2)
1/2 [1]
Matching layer thickness L
1Provide by following formula:
L
1＝(2n-1)λ
1/4 [2]
In the formula, λ
1Be the wavelength of sound in the medium 1, n is an integer.
In the present technique field, the theoretical foundation of quarter-wave matching layer is known, in acoustics document, the relevant document of the relevant document of ultrasonic engineering, sufficient explanation is arranged, a kind of solving method of the classical boundary value problem in acoustic theory aspect when its reflection planes ripple enters another kind of medium from a kind of medium by a middle layer with medical imaging.Finding the solution of this boundary value problem is such, if the condition of formula (1) and formula (2) is satisfied in the middle layer, then the acoustic energy of propagating in first medium is conveyed into 100% ground in second medium.Although this analysis result is only effective to single-frequency strictly speaking, the experimental result report in this area shows, even concerning the wide device of the wideband with broad frequency spectrum, also can benefit greatly from use this kind matching layer.
Be not too big if impedance matches, the quarter-wave matching layer can provide feasible solution.For example, in the described in the above medical ultrasound occasion, the matching layer impedance that is drawn by formula (1) is approximately 7 * 10
6Kg/m
2S.This impedance accomplishes known in the art, it be in suitably can acoustic impedance range as some rubber of matching layer and plastic material in.Today, in the applications of ultrasound of medical profession and industry member, the single matching layer of this kind is used widely.
On the other hand, degree is not big if the impedance between two kinds of materials matches, and then the quarter-wave matching layer no longer can constitute actual solution.For example, wish that making acoustic impedance is 34 * 10
6Kg/m
2The typical piezoelectric transducer of s and acoustic impedance are 415kg/m
2The air of s mates, and then shows bright relational expression according to formula (1), is 0.12 * 10 with the acoustic impedance that requires single matching layer
6Kg/m
2S., known in the art do not have suitable material to have this required resistance value, therefore, requires to have certain other method.
Though, having proposed certain methods and improved the acoustics coupling that realizes state-of-the-art at two kinds of storerooms with complete different acoustic impedances with reality, they all are proved to be in the acoustic energy transmission is the not high with efficient of specificity.In the state-of-the-art, people adopt meagre to thick, the aeriferous tight plastic foil of tundish of about 10 μ m, have the 100kHz transducer of flat dry face in order to covering.Claim in the report of this method, do not sacrifice the gain that 10dB is arranged under the responsive bandwidth.A kind of diverse ways is to add imperceptible epoxy resin spherolite, makes the Low ESR matching materials and is applied to transducer front face.It is reported that the improvement situation of this kind occasion can make frequency high to 1MHz.In the method for state-of-the-art, typically comprise a kind of special elastomeric material, can solve the impedance mismatch problem between transducer and air when making quarter-wave to a certain extent.And can make two matching layers, wherein, when ground floor is not the best, can find the optimum second layer.Typically, ground floor is made of the rubber (for example, GE RTV 615) that wherein comprises 50 μ m diameter bubbles.In a kind of like this method, two matching layers have one to optimize criterion, and the acoustic impedance between promptly from the sound source to the destination media should be dull alternation.Though it still is not an optimum matching, the preceding method that this method compares shows as the bandwidth performance that can provide broad.Another suggestion proposes a kind of nonmonotonic multilayer matching layer, has proved that it only to the arrowband coupling effectively.In another method, increase gradually or many thin layers of reducing form matching layer by the meaning of combination by acoustic impedance.In this method, constitute total matching layer by each layer that is thinned to 1/30 wavelength.It is to constitute the multilayer matching layer with the material that obtains easily that a kind of method is arranged, and can make the transducer and air coupling of about 450kHz, is applied to during steel contactless, non-damage type test.At last, be presented to the U.S. Pat Pat.No.6 of Mahesh Bhardwaj November 6 calendar year 2001, a kind of matching layer be described in 311,573, it is made of several layers, wherein, the piezoelectric transducer of standard can with the air approximate match.In the exemplary, coated with aluminum and hard epoxy resin on piezoelectricity lead zirconates-lead titanates (PZT) member, and add the paper that coats clay at last.People are with the representative of Bhardwaj as state-of-the-art, and Bhardwaj provides several special examples, make piezoelectric crystal and air coupling such as PZT.Bhardwaj illustrates (the 4th be listed as 38-57 capable) in the example 1 that he provides:
" transducer of 1MHz can constitute as follows:
Piezoelectric: PZT, Z
0=34 * 10
6Kg/m
2S;
First transmission layer: aluminium, V=6325m/s, Z1=17 * 10
6Kg/m
2S, P/8@1MHz=1000/8=125ns, in the formula, 1000ns is an one-period, P is that unit is the frequency of MHz.
So the thickness of this transmission layer is 125 * 10
-9* 6,325,000=0.79mm.
Second transmission layer: hard epoxy resin, V=2600m/s, Z
2=3 * 10
6Kg/m
2S, P/16@1MHz=1000/16=62.5ns.
So the thickness of this transmission layer is 62.5 * 10
-9* 2,600,000=0.16mm.
Surface layer: coat the paper of clay, V=500m/s, Z
3=0.6 * 10
6Kg/m
2S, P/16@1MHz=1000/16=62.5ns.
So the thickness of this layer is 62.5 * 10
-9* 500,000=0.03mm.”
In this instantiation, use three matching layers and make PZT and air coupling.Following table 1 is briefly listed the acoustic impedance of this method.Here, be conveyed into the acoustic energy of air less than 20% from PZT.
Table 1
| Acoustic impedance (kg/m 2·s) | |
| Sound source: Z 0(PZT) | 34×10 6 |
| Ground floor: Z 1 | 17×10 6 |
| The second layer: Z 2 | 3×10 6 |
| The 3rd layer: Z 3 | 0.6×10 6 |
| Target medium: Z 5(air) | 415 |
Explanation (the 5th be listed as 1-16 capable) in the example 2 of Bhardwaj:
" can constitute by many parts transmission layer according to transducer of the present invention, as following listed:
Piezoelectric layer (PZT), Z
0=34 * 10
6Kg/m
2S
Aluminium lamination: Z
1=17 * 10
6Kg/m
2S
Aluminium composite bed: Z
2=7 * 10
6Kg/m
2S
Epoxy resin layer: Z
3=3 * 10
6Kg/m
2S
Papery surface layer: Z
4=0.3 * 10
6Kg/m
2S "
Here, use four matching layers, make PZT and air coupling.Following table 2 is briefly listed the acoustic impedance of Bhardwaj second example, and its acoustic energy transfer efficiency is less than 20%.
Table 2
| Acoustic impedance (kg/m 2·s) | |
| Sound source: Z 0(PZT) | 34×10 6 |
| Ground floor: Z 1 | 17×10 6 |
| The second layer: Z 2 | 7×10 6 |
| The 3rd layer: Z 3 | 3×10 6 |
| The 4th layer: Z 4 | 0.3×10 6 |
| Destination media: Z 5(air) | 415 |
Top method is to be drawn by experiment fully under special state, without any original basis and analytical framework.Making the theoretical solution that still needs to have massively the best on transducer and other sound sources, making the acoustic impedance coupling between sound source and the target medium.
Summary of the invention
In some embodiment of the present invention, comprise the method for making transducer with a plurality of impedance matchings, it comprises step: provide to have the sound source impedance Z
0Piezoelectric unit; Selection has target impedance Z
(n+1)Target medium; Determine the matching layer number N, wherein, N be one greater than 1 integer; And, be 1, make following processing for increment: determine required impedance according to the method that N matching layer is solved boundary value problem until each matching layer J of the matching layer number N of stipulating; For having determined required impedance Z in fact
JMatching layer J, select its material, wherein, the material selected to matching layer J has velocity of sound V
JAnd with matching layer J in the related wavelength X of the velocity of sound
JFor matching layer J, determine a positive integer n of selected material
JWith material thickness L
J, with thickness L
JMatching layer J be applied on the transducer.
Manufacturing has in the method for transducer of a plurality of impedance matching layers and also comprises: produce acoustic pressure by a sound source in having first medium of an acoustic impedance value; Utilize a receiving transducer to measure the acoustic pressure that in first medium, produces by this sound source; In having second medium of an acoustic impedance value, produce acoustic pressure by this sound source; Utilize this receiving transducer to measure the acoustic pressure that in second medium, produces by this sound source; And according to the acoustic impedance of first medium, the acoustic impedance of second medium, the acoustic pressure that acoustic pressure that is recorded in first medium by receiving transducer and receiving transducer record in second medium is determined the effective sound source impedance that obtains.
Description of drawings
For further understanding characteristic of the present invention and purpose, can consult following detailed description in conjunction with the accompanying drawings.In each accompanying drawing, give same or similar reference number for alike unit, wherein:
The flow process of Fig. 1 illustrates bright the preferred method of the present invention embodiment;
Fig. 2 shows bright example according to many matching layers transducing head embodiment of the present invention; And
The flow process of Fig. 3 illustrates the method for optimizing of determining effective sound source impedance among bright the present invention.
Embodiment
In some embodiment of the present invention, comprise the transducer that has matching layer and acoustic impedance optimum matching, and the method that reaches optimum matching.In the following Example each, what no matter illustrate is the interpolation medium that are made of one deck or which floor, shows that all the interpolation medium between transducing sound source and target medium have best impedance matching.In the practice, the scope and the numerical value of required impedance on concrete enforcement is depended in the selection of matching layer number.When establishing best many matching layers method for optimizing, in fact rely on the original boundaries value equation of typically using in single matching layer, its method is promoted.Following public method and gained result belong to many matching layers, and the boundary value problem that it solves can provide best solution to intercalation in two or more, and this method may extend to N matching layer.Resistance value to each layer generation all is best, uses them when coming guiding material to select, and can provide maximum transmitted efficient for the acoustic energy from the transducer sound source.
In the example 1, has impedance Z
0The sound source layer with have an impedance Z
2Target medium between the single matching layer of interpolation.The required impedance Z of this matching layer
1Be decided by the sound source impedance Z
0Square root and target medium impedance Z
2Square root both are long-pending, promptly
Z
1＝(Z
0Z
2)
1/2 [3]
In the example 2, has impedance Z
0The sound source layer with have an impedance Z
3Target medium between two matching layers of interpolation.The required impedance Z of first matching layer
1Be decided by the sound source impedance Z
0Cubic root square with the target medium impedance Z
3Cubic root both are long-pending, promptly
Z
1＝Z
0 2/3 Z
3 1/3 [4]
Similarly, the required impedance Z of second matching layer
2Be decided by the sound source impedance Z
0Cubic root and target medium impedance Z
3Cubic root square both are long-pending, promptly
Z
2＝Z
0 1/3 Z
3 2/3 [5]
In the example 3, has impedance Z
0The sound source layer with have an impedance Z
4Target medium between three matching layers of interpolation.The required impedance Z of first matching layer
1Be decided by the sound source impedance Z
03/4 power and target medium impedance Z
41/4 power both are long-pending, promptly
Z
1＝Z
0 3/4 Z
4 1/4 [6]
Similarly, the required impedance Z of second matching layer
2Be decided by the sound source impedance Z
0Square root and target medium impedance Z
4Square root two long-pending, promptly
Z
2＝Z
0 1/2 Z
4 1/2 [7]
Similarly, the required impedance Z of the 3rd matching layer
3Be decided by the sound source impedance Z
01/4 power and target medium impedance Z
43/4 power both are long-pending, promptly
Z
3＝Z
0 1/4 Z
4 3/4 [8]
In the example 4, has impedance Z
0The sound source layer with have an impedance Z
5Target medium between four matching layers of interpolation.The required impedance Z of first matching layer
1Be decided by the sound source impedance Z
04/5 power and target medium impedance Z
51/5 power both are long-pending, promptly
Z
1＝Z
0 4/5 Z
5 1/5 [9]
Similarly, the required impedance Z of second matching layer
2Be decided by the sound source impedance Z
03/5 power and target medium impedance Z
52/5 power both are long-pending, promptly
Z
2＝Z
0 3/5 Z
5 2/5 [10]
Similarly, the required impedance Z of the 3rd matching layer
3Be decided by the sound source impedance Z
02/5 power and target medium impedance Z
53/5 power both are long-pending, promptly
Z
3＝Z
0 2/5 Z
5 3/5 [11]
At last, the required impedance Z of the 4th matching layer
4Be decided by the sound source impedance Z
01/5 power and target medium impedance Z
54/5 power both are long-pending, promptly
Z
4＝Z
0 1/5 Z
5 4/5 [12]
Usually, for the transducer of N matching layer (N is a positive integer), to having impedance Z
0The sound source layer with have an impedance Z
(n+1)Target medium between in each in the method for intercalation computing impedance value, the required impedance Z of each interior intercalation J (J is an integer in 1 to N scope) in succession
JCalculate as follows:
Z
J＝Z
0 [(N+1-J)/(N+1)] Z
(N+1) (J/N+1) [13]
Be similar in the another set of calculation procedure to single matching layer computing impedance, can determine the thickness of matching layer, maximum acoustic energy transmission is arranged when guaranteeing to see through matching layer.If the thickness of matching layer J is L
J, the wavelength of sound in the J layer is λ
J, then
L
J＝(2n
J-1)λ
J/4 [14]
In the formula, n
JBe a positive integer, in the weighing apparatus of between the structural requirement of material and ghost effect, making even, n
JPreferably elect 1,2 or 3 as.The THICKNESS CALCULATION of single matching layer meets fully shows bright single matching layer formula in the formula (2).The exemplary method 100 that shows bright manufacturing electro-acoustic transducer or acoustic resonance source on Fig. 1, its calculation procedure above the applied in any combination is to dispose best impedance matching layer.On step 115, make initial selection and determine that selection has transducing type or the acoustic resonance type sound source material of impedance Z (0) and resonance frequency f (0), determines the impedance Z (N+1) of target medium together with it, determines the matching layer number N.On step 125, carry out interative computation, for this reason, on step 120, the sound source material is defined as the 0th layer of J=0.For each matching layer J, on step 135, determine the impedance of matching layer J by following formula:
Z
J＝Z
0 [(N+1-J)/(N+1)] Z
(N+1) (J/N+1) [15]
On next step step 140, select to have definite impedance Z
JAnd wavelength X
JMaterial, here, wavelength X
JDraw the velocity of sound that can be in material and the resonance frequency f (0) of sound source work.On step 145,, determine the thickness Integer n according to the structure and the quality of material of selecting and known it
JThen, on step 150, determine the thickness of specific matching layer J.Along with, will be applied to for the computing method of matching layer J on the layer after this, and piezoelectric unit is as 0 layer.Insert this exemplary method of stating on can be applicable to ultrasonic transducer, also can be applicable on the sound source.In those are used, determine effective sound source impedance according to following public step, and on step 190, be substituted in the transducer impedance Z (0) that learns on the step 115 with the effective sound source impedance that obtains.
In the following Example, with the application of the bright top disclosed method of some enforcement illustrations of making ultrasonic transducer, show the bright transducer of making by example on Fig. 2, it has the acoustic impedance of optimum matching.Comprise the PZT sound source layer that constitutes by preferred embodiment 210 in the transducer 200, first matching layer 215 and second matching layer 220 are arranged in the above, if desired, can be according to each matching layer that is applied with again above them in succession that is set forth in of the present invention, until the N layer.Because each interpolation matching layer has best matched impedance, thereby will be transferred to efficiently on the target medium 230 at the acoustic energy that produces on the sound source 210.
At first, in the application under general occasion, make typical piezoelectric unit such as PZT and air coupling, the example impedance that piezoelectric unit has is 34 * 10
6Kg/m
2S, target medium is that the impedance of air is 415kg/m in this example
2S.When application formula (1) is made the transducer of single matching layer, require matching layer to have unpractical impedance 0.12 * 10
6Kg/m
2S.So, when the elaboration manufacturing of using disclosed method for optimizing has the transducer of two matching layers, can calculate, the impedance of first matching layer should be 0.78 * 10
6Kg/m
2S, the impedance of second matching layer should be 0.018 * 10
6Kg/m
2S.The selected matching layer material that satisfies these standards can guarantee best configuration, the acoustic energy of maximum can be conveyed in the target medium.
Professional in this area is clear from top example to be known, increases the range of choice that the matching layer number can increase material, can make best transducer whereby.For example, when using single matching layer and making PZT and air coupling, the impedance that requires matching layer is 0.12 * 10
6Kg/m
2S., it seems that the material with this suitable acoustic impedance is a cork, and its absorptivity is very big, therefore, is inappropriate for most of practical applications.Yet, making when having the transducer of two matching layers, it is 0.78 * 10 that people can select impedance
6Kg/m
2S and 0.018 * 10
6Kg/m
2The material of s, such as can selecting from various types of elastomeric materials, in addition, their attenuation coefficient is little.Therefore, this type of material can provide the practical methods that makes PZT and air coupling.
In another example, use three couplings according to the present invention and make PZT and air coupling.Following table 3 is briefly listed the result of this exemplary method, and here, the acoustic energy transfer efficiency is close to 100%.
Table 3
| Acoustic impedance (kg/m 2·s) | |
| Sound source: Z 0(PZT) | 34×10 6 |
| Ground floor: | 2×10 6 |
| The second layer: Z 2 | 0.12×10 6 |
| The 3rd layer: Z 3 | 0.007×10 6 |
| Destination media: Z 5(air) | 415 |
In the example then, use four matching layers and make PZT and air coupling.Below table 4 briefly list the result of the preferred method of the present invention, here, can have to be close to 100% acoustic energy and outwards to transmit.
Table 4
| Acoustic impedance (kg/m 2·s) | |
| Sound source: Z 0(PZT) | 34×10 6 |
| Ground floor: Z 1 | 3.5×10 6 |
| The second layer: Z 2 | 0.37×10 6 |
| The 3rd layer: Z 3 | 0.038×10 6 |
| The 4th layer: Z 4 | 0.004×10 6 |
| Destination media: Z 5(air) | 415 |
Method described above provides feasible and effective measures make and reach acoustic impedance coupling between two kinds of materials, whereby, can make the ultrasonic transducer with optimum sound impedance matching.Ultrasonic transducer according to the elaboration in this explanation is made can provide maximum acoustic energy transmission from the transducing sound source to target medium.Though, here can be between any two kinds of materials provide the optimum sound impedance matching with the method for its some embodiment explanation by the matching layer of defined amount, but described in the example that provides above, it will guide people to consider the coupling of typical piezoelectric unit such as PZT and between air.The conventional method of some concrete performances is disclosed here.As described above, the acoustic impedance of PZT is 34 * 10
6Kg/m
2S, the acoustic impedance of air is 415kg/m
2S.If use single matching layer, then show bright known typical consequence in this method simplification accepted way of doing sth (1) and the formula (2).As shown above under this kind occasion, the impedance of matching layer will be 0.12 * 10
6Kg/m
2S.As top specified, vegetable cork is one of only a few material that has this kind impedance.Yet, because the absorptivity height of this material also is about to lose a large amount of acoustic energy, so this is a kind of inferior matching layer alternative materials.
Commentaries on classics is shown two bright matching layers above seeing, the impedance that obtains is 0.78 * 10
6Kg/m
2S and 0.018 * 10
6Kg/m
2S.Know have various types of rubber to manufacture and have this type of resistance value.For example, can make rubberite be configured to impedance and be approximately 0.78 * 10
6Kg/m
2S, the about 2400m/s of the velocity of sound, the ultrasonic wavelength of 1MHz frequency is 2.4mm.Matching layer with this made can be thinned to quarter-wave, also is n
J=1 o'clock thickness 0.6mm.In addition, can make soft rubber be configured to impedance about 0.018 * 10
6Kg/m
2S, the about 1050m/s of the velocity of sound, the ultrasound wave of 1MHz frequency about 1mm that grows up.Its thickness of matching layer with this made can be thinned to quarter-wave or 0.25mm.
Commentaries on classics is seen and is shown four bright matching layers in the top table 4, can use following material: for ground floor, and various types of Plexiglas's and TEFLON
Can supply usefulness, for example can obtain 3.5 * 10
6Kg/m
2The impedance of s; For the second layer, soft rubber can provide 0.37 * 10
6Kg/m
2The impedance of s; For the 3rd layer, the soft rubber of some types has 0.038 * 10
6Kg/m
2The impedance of s; And for the 4th layer, the soft rubber of paper and some types has 0.004 * 10
6Kg/m
2The impedance of s.
The thickness of each matching layer is decided by formula (14), wherein, can select matching layer thickness Integer n to each matching layer J
J, resulting benefit comprises that the high and manufacturing process of acoustic energy transfer efficiency can improve.
In the transducer example of the present invention, the PZT device preferably has a crest frequency or resonance frequency, have one or more soft rubber layers and/or one or more rubberite layer in a preferred embodiment, they or be coated on transducer face, or be coated on in succession the matching layer.The coating of rubber proceeds to until satisfying required quarter-wave thickness.Here, wavelength is defined as the resonance frequency of the interior velocity of sound of rubber divided by piezoelectric unit.THICKNESS CALCULATION is referring to formula (14).Except applying rubberite, in the additional embodiments, being bonded with each other of many matching layers relies on common epoxy resin, clay and self-adhesive tape, or other high-viscosity epoxy resins, cementing agent or clay.
Because structural requirement, when becoming quarter-wave unrealistic the matching layer made, or when not wishing to become quarter-wave thin like that the made, must get matching layer thickness Integer n
JValue is greater than 1.For example, n
JGot 2 o'clock, matching layer thickness will be four/three-wavelength.By disclosure file, the skilled person in the present technique field knows, people can do the target gross thickness of each matching layer of making to the end and can represent with roughly the same wavelength unit roughly, but each matching layer needn't be required to be identical materials.Just, work as λ
1Be substantially equal to λ
2The time, two combinable target thicknesses that reach 1/2nd wavelength of quarter-wave matching layer.When doing like this, it is 1/2nd wavelength X that people can roughly obtain combination thickness
1/ 2.This method that reaches target thickness can expand to bigger target thickness again.For example, can wish that target thickness is 3 λ
2/ 2, wherein, first thickness is 5 λ
1/ 4, second thickness is λ
2/ 4, whereby, work as λ
1Be substantially equal to λ
2The time, obtain combination thickness 3 λ
1/ 2.
Though, also be that lead zirconates-lead titanates is used for ultrasonic transducer or sound source as preferred material with PZT, but some embodiment of this method also can be applicable on any piezoelectric as the sound source material.Other material comprises quartz crystal, barium titanate, lithium sulfate, lithium niobate, lead meta-columbute and other suitable machine-electrical coupling agent.As for target medium, prevailing target medium expection is air and other gas medium; But, target medium also can be to comprise water and like the liquid of water object and comprise biological tissue and the solid of class biological tissue material.
Though what the example that provides was above represented is the piezo-electric device that works in megahertz (MHz) frequency range, the skilled person in the present technique field knows that this method can be applicable to be operated on the interior any piezoelectric transducer of any frequency range.This respect, can comprise working in kilo hertz (kHz) frequency range even the piezoelectric transducer on the low frequency more, and use manufacturings such as semiconductor technology, deposition process and/or nanometer technology method, work in the piezoelectric transducer on megahertz (MHz), gigahertz (GHZ) (GHz) and terahertz (THz) frequency range.
Although the method by example explanation is at piezo-electric device, but the skilled person in the present technique field knows, some embodiment of this method can be applicable to any sound source or ultrasonic transducer, and no matter it adopts any technology to produce sound wave, only need accomplish, as following defined, measure its effective acoustic impedance Z for the sound source of being considered
EFF, and with Z
EFFSound source acoustic impedance Z in resolving above replacing
0About sound source being determined its effective acoustic impedance Z
EFFThe measuring method of being implemented has detailed description in the above by example.And by the example explanation, it both can be applicable to piezoelectric sound sources, also can be applicable to any sound source.Therefore, can make the target medium of any sound source and any medium or care reach best impedance matching.Especially, this measuring method can be applicable to capacitive device and magnetoelectricity device.Can be applied to loudspeaker, osophone, alarm, whistle and musical instrument etc., just, can be applicable to produce any object of sound wave.
Below, in Fig. 3, showing bright a series of experiment measuring, people can determine effective acoustic impedance of any sound source by it, then, this effective acoustic impedance can be applicable in the method for the present invention.At first, on step 310, relevant sound source is acted on the medium of first medium or care, also be target medium A or have on the medium A ' of similar acoustic characteristic with target medium A.For example, sound source is acted on the medium A, its acoustic impedance is defined as Z
A, and the acoustic impedance Z of supposition medium A
ACan measure independently, and sound source is not mated with this target medium as yet best.On step 315, use an independent receiving transducer and have impedance Z
AMedium A in the optional position on, measure the acoustic pressure P that produces by relevant sound source
RAReceiving transducer must be not identical with sound source, and even essential not similar, it can be to work in well on the sound generating principle very inequality.Certainly, it should be able to be adapted to be operated in the frequency and sound intensity scope of sound source.Because it is enough to measure the relative size of acoustic pressure, so, do not need receiving transducer is calibrated to the absolute acoustic pressure of energy measurement.Though, receiving transducer does not need accurate decision with respect to the position of sound source, but this type of measurement should be followed gratifying acoustic measurement practice, should on enough big spacing distance, measure, so that the known near field puppet of professional resembles effect and do not form interference problem to measuring in this area.
The acoustic pressure P that in medium A, records by receiving transducer
RABe shown below:
P
RA＝p
0τ
0A＝P
0[2Z
A/(Z
EFF+Z
A)] [16]
In the formula, p
0Be the acoustic pressure at sound source place, τ
0ABe the transmission coefficient between sound source and the medium A, Z
EFFIt is effective acoustic impedance of sound source.
Next step, on step 320, the second medium B that is different from A or A ' with acoustic characteristic replaces medium A or A ', and the acoustic characteristic of medium B still is adapted to the operation of sound source and receiving transducer.Every other variable all preferably remains unchanged, and for example, the sound source transducer is identical with the distance maintenance between the receiving transducer, then, on step 325, measures acoustic pressure P by receiving transducer
RBThe acoustic pressure P that receiving transducer records in medium B
RBBe shown below:
P
RB＝P
0τ
0B＝P
0[2Z
B/(Z
EFF+Z
B)] [17]
In the formula, τ
0BIt is the transmission coefficient between sound source and the medium B.Here,, guaranteed during measurement that sound source works on the same power level no matter for medium A or B, so, can ask for the ratio of top two formulas, obtain
P
RA/P
RB＝[2Z
A/(Z
EFF+Z
A)]/[2Z
B/(Z
EFF+Z
B)] [18]
Formula defining variable Ω below using:
Ω＝[P
RA/P
RB]/[Z
B/Z
A] [19]
So, on step 330, draw Z according to the relational expression that derives
EFFValue:
Z
EFF＝[Z
B-ΩZ
A]/[Ω-1] [20]
In the top example, the impedance of media material A and B is known, and by processing described above, variable Ω is obtained by experiment.At last, can confirm, effectively acoustic impedance Z
EFFBe such sound source acoustic impedance, on step 335, utilize method described above can use its Z
EFFReplace Z
0, promptly
Z
EFF=Z
0[21] use described above and Fig. 1 in show bright method, can make any sound source and target or be that target medium reaches impedance matching.
Below, show brightly how to use effective acoustic impedance that this experimental technique is determined a given sound source with two examples, and how to use some embodiment of the present invention and make sound source and its target material reach optimum matching.
In first example, capacitive transducer is made design, make it to work in ocean particularly in the seawater.Here, adopt identical transducer, measure the acoustic pressure that produces by sound source in the briny environment as working in roughly the same interior receiving transducer and the piezoelectric transducer of frequency range.Then, for example replacing seawater with distilled water repeats to measure.These two kinds of measurements can be determined effective acoustic impedance of capacitive transducer in conjunction with the acoustic characteristic with known seawater and distilled water.At last, use exemplary method or calculate matching layer suitable when making the optimum matching transducer, according to impedance that obtains and the selected a series of coating processing of thickness, just can between transducer and ocean, provide best acoustic matching when being applied to it on the sound source again.As previously described, thus, this optimum matching can make capacitive transducer work on its top efficiency.
In second example, in the 5-10kHz frequency range, loudspeaker design is become to work in the air.Use a suitable microphone to measure the acoustic pressure that produces by the loudspeaker that works in the air.In addition, for example be to measure the acoustic pressure that speaker operation produces in the experiment container of nitrogen being full of again.These experiment measuring values are determined that with top the calculating of effective sound source impedance combines, so as to selecting suitable coating processing, realize best acoustic matching according to the impedance that obtains and thickness.Therefore, have best and speaker performance efficiently.
Claims
(according to the modification of the 19th of treaty)
1. a making has the method for the transducer of three or more impedance matching layers, comprising:
Provide and have the sound source impedance Z
0Piezoelectric element;
The select target medium, it has target impedance Z
(N+1)
Determine the matching layer number N, N is an integer greater than 2; And
For increment be 1, up to each matching layer J of the matching layer number N of regulation,
Determine required impedance Z according to following formula
J:
Z
J＝Z
0 [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)；
Select to have in fact determined required impedance Z
JThe material of matching layer J, wherein, the selected material that is used for matching layer J has a velocity of sound and a wavelength τ related with this velocity of sound of this matching layer J
J
Determine a positive integer value n
J, and the selected material of matching layer J is determined thickness L according to following formula
J:
L
J=(2n
J-1) λ
J/ 4 and,
With thickness L
JMatching layer J be applied on the transducer.
2. a manufacturing has the method for the transducer of a plurality of impedance matching layers, comprising:
Effective sound source impedance Z with derivation is provided
EFFSound source;
The select target medium, it has target impedance Z
(N+1)
Determine the matching layer number N, N is an integer greater than 1; And
For increment is from 1 each matching layer J up to the matching layer number N of stipulating,
Determine required impedance Z according to following formula
J:
Z
J＝Z
EFF [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)；
Select to have in fact determined required impedance Z
JThe material of matching layer J, wherein, the selected material that is used for matching layer J has a velocity of sound J and a wavelength X related with the velocity of sound of this matching layer J
J
Determine a positive integer value n
J, and the selected material of matching layer J is determined thickness L according to following formula
J:
L
J=(2n
J-1) λ
J/ 4 and,
With thickness L
JMatching layer J be applied on the transducer.
3. manufacturing according to claim 2 has the method for the transducer of a plurality of impedance matching layers, further comprises:
In having first medium of an acoustic impedance, produce acoustic pressure by a sound source;
Measure the acoustic pressure that in first medium, produces by this sound source with a receiving transducer;
In having second medium of an acoustic impedance, produce acoustic pressure by this sound source;
Measure the acoustic pressure that in second medium, produces by this sound source with this receiving transducer; And,
Acoustic pressure in the acoustic pressure in first medium that record according to the acoustic impedance of the acoustic impedance of first medium, second medium, by receiving transducer and second medium that recorded by receiving transducer is determined effective sound source impedance of deriving.
4. manufacturing according to claim 3 has the method for the transducer of a plurality of impedance matching layers, wherein, determines the effective sound source impedance Z that derives
EFFStep be based on the acoustic impedance Z of first medium
A, second medium acoustic impedance Z
B, the acoustic pressure P in first medium that record by receiving transducer
RAAnd the acoustic pressure P in second medium that record by receiving transducer
RB, press the relation of plane formula and calculate:
Z
EFF＝[Z
B-{[P
RA/P
RB]/[Z
B/Z
A]}Z
A]/[{[P
RA/P
RB]/[Z
B/Z
A]}-1]。
5. device that acoustic energy is transferred in the target medium with a target impedance, this device comprises:
One has the sound source impedance Z
0Piezoelectric element, and three or more matching layers;
Wherein, each layer J of these three or more matching layers has the required impedance Z that provides according to following formula
J:
Z
J＝Z
0 [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)
And has a wavelength of sound λ
JAnd
Wherein, each layer J of these three or more matching layers has the thickness L that provides according to following formula
J:
L
J＝(2n
J-1)λ
J/4
Wherein, n
JIt is a positive integer; And
Wherein, these three or more matching layers are adhered on the piezoelectric element.
6. one kind is used to make acoustic energy from having impedance Z
0Sound source to having target impedance Z
(N+1)Target medium between realize the goods of coupling, these goods comprise:
Three or more matching layer N, wherein, each layer J of these three or more matching layers has the required impedance Z according to following formula
J:
Z
J＝Z
0 [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)
And has a wavelength of sound λ
J
7. according to the goods of claim 6, wherein, each layer J of these three or more matching layers has the thickness L according to following formula
J:
L
J＝(2n
J-1)λ
J/4
Wherein, n
JIt is a positive integer.
8. according to the goods of claim 6, wherein, target medium is an air.
Claims (8)
1. a manufacturing has the method for the transducer of a plurality of impedance matching layers, comprises step:
Provide and have the sound source impedance Z
0Piezoelectric element;
The select target medium, it has target impedance Z
(N+1)
Determine the matching layer number N, N is an integer greater than 1; And
For increment be 1, up to each matching layer J of the matching layer number N of regulation;
Determine required impedance Z according to following formula
J:
Z
J＝Z
0 [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)
Select to have in fact determined required impedance Z
JThe material of matching layer J, wherein, to having velocity of sound V in the selected material of matching layer J
JAnd with this matching layer J in the related wavelength X of the velocity of sound
J
Determine a positive integer n
J, and the selected material of matching layer J is determined thickness L according to following formula
J:
L
J=(2n
J-1) λ
J/ 4 and,
With thickness L
JMatching layer J be applied on the transducer.
2. a manufacturing has the method for the transducer of a plurality of impedance matching layers, comprises step:
Effective sound source impedance Z with derivation is provided
EFFSound source;
The select target medium, it has target impedance Z
(N+1)
Determine the matching layer number N, N is an integer greater than 1; And
For increment be 1, up to each matching layer J of the matching layer number N of regulation:
Determine required impedance Z according to following formula
J:
Z
J＝Z
EFF [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)
Select to have in fact determined required impedance Z
JThe material of matching layer J, wherein, to having velocity of sound V in the selected material of matching layer J
JAnd with this matching layer J in the related wavelength X of the velocity of sound
J
Determine a positive integer n
J, and the selected material of matching layer J is determined thickness L according to following formula
J:
L
J=(2n
J-1) λ
J/ 4 and,
With thickness L
JMatching layer J be applied on the transducer.
3. manufacturing according to claim 2 has the method for the transducer of a plurality of impedance matching layers, further comprises step:
In having first medium of an acoustic impedance, produce acoustic pressure by a sound source;
Measure the acoustic pressure that in first medium, produces by this sound source with a receiving transducer;
In having second medium of an acoustic impedance, produce acoustic pressure by this sound source;
Measure the acoustic pressure that in second medium, produces by this sound source with this receiving transducer; And,
Acoustic pressure in the acoustic pressure in first medium that record according to the acoustic impedance of the acoustic impedance of first medium, second medium, by receiving transducer and second medium that recorded by receiving transducer is determined effective sound source impedance of deriving.
4. manufacturing according to claim 3 has the method for a plurality of impedance matching layer transducers, wherein, determines the effective sound source impedance Z that derives
EFFMethod be based on the acoustic impedance Z of first medium
A, second medium acoustic impedance Z
B, the acoustic pressure P in first medium that record of receiving transducer
RAAnd the acoustic pressure P in second medium that record of receiving transducer
RB, press the relation of plane formula and calculate:
Z
EFF＝[Z
B-{[P
RA/P
RB]/[Z
B/Z
A]}Z
A]/[{[P
RA/P
RB]/[Z
B/Z
A]}-1]
5. device that acoustic energy is transferred in the target medium with a target impedance, this device comprises:
One has the sound source impedance Z
0Piezoelectric element, and a plurality of matching layer;
Wherein, each layer J of a plurality of matching layers has the required impedance Z that provides according to following formula
J:
Z
J＝Z
0 [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)
And has a wavelength of sound λ
JWherein, each layer J of a plurality of matching layers has the thickness L that provides according to following formula
J:
L
J＝(2n
J-1)λ
J/4
Wherein, n
JIt is a positive integer; And,
Wherein, these a plurality of matching layers are adhered on the piezoelectric element.
6. one kind is used to make acoustic energy from having impedance Z
0 [(N+1-J)/(N+1)]Sound source to having target impedance Z
(N+1) [J/ (N+1)]Target medium between realize the goods of coupling, these goods comprise:
A plurality of matching layer N, wherein, each layer J of a plurality of matching layers has the required impedance Z according to following formula
J:
Z
J＝Z
0 [(N+1-J)/(N+1)]Z
(N+1) (J/N+1)
And has a wavelength of sound λ
J
7. according to the goods of claim 6, wherein, the ground floor J of a plurality of matching layers has the thickness L according to following formula
J:
L
J＝(2n
J-1)λ
J/4
Wherein, n
JIt is a positive integer.
8. according to the goods of claim 6, wherein, target medium is an air.
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US45217303P | 2003-03-04 | 2003-03-04 | |
| US60/452,173 | 2003-03-04 | ||
| US10/793,311 | 2004-03-03 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN1756955A true CN1756955A (en) | 2006-04-05 |
| CN100460871C CN100460871C (en) | 2009-02-11 |
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ID=36689382
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CNB200480005788XA Expired - Lifetime CN100460871C (en) | 2003-03-04 | 2004-03-04 | Device having matched accoustical impedance and method |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN100460871C (en) |
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103220967A (en) * | 2010-08-02 | 2013-07-24 | 莱夫韦弗公司 | Ultra wideband (UWB) baby monitors for detection of infant cardiopulmonary distress |
| CN103540152A (en) * | 2012-07-24 | 2014-01-29 | 常州波速传感器有限公司 | Gradual transition acoustic impedance matching material production method |
| CN104614442A (en) * | 2013-11-05 | 2015-05-13 | 松下知识产权经营株式会社 | Ultrasonic measuring method and device |
| CN107174281A (en) * | 2016-03-09 | 2017-09-19 | 精工爱普生株式会社 | Ultrasonic device, ultrasonic wave module and ultrasonic measurement device |
| CN108882108A (en) * | 2018-07-05 | 2018-11-23 | 湖南大学 | It is applicable in the impedance matching system and its matching process of Yu Haiyang communication electroacoustic transducer |
| CN109246575A (en) * | 2018-08-09 | 2019-01-18 | 广州联声电子科技有限公司 | A kind of preparation method of the progressive acoustic impedance matching layer of high frequency |
| WO2021078291A1 (en) * | 2019-10-25 | 2021-04-29 | 飞依诺科技(苏州)有限公司 | Ultrasonic transducer and method for manufacturing ultrasonic transducer |
| CN112756241A (en) * | 2019-11-06 | 2021-05-07 | 中国石油化工股份有限公司 | Well wall ultrasonic piezoelectric transducer and well wall ultrasonic logging instrument |
| CN114449417A (en) * | 2020-10-30 | 2022-05-06 | 华为技术有限公司 | Speaker and electronic equipment |
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| US4211948A (en) * | 1978-11-08 | 1980-07-08 | General Electric Company | Front surface matched piezoelectric ultrasonic transducer array with wide field of view |
| DE3501808A1 (en) * | 1985-01-21 | 1986-07-24 | Siemens AG, 1000 Berlin und 8000 München | ULTRASONIC CONVERTER |
| JPS62258597A (en) * | 1986-04-25 | 1987-11-11 | Yokogawa Medical Syst Ltd | Ultrasonic transducer |
| ES2301201T3 (en) * | 1997-06-19 | 2008-06-16 | Mahesh C. Bhardwaj | ULTRASONIC TRANSDUCER FOR ELEVATED GAS TRANSDUCTION AND METHOD FOR ULTRASOUND TRANSMISSION IN A NON-CONTACT MODE ON SOLID MATERIALS. |
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|---|---|---|---|---|
| CN103220967A (en) * | 2010-08-02 | 2013-07-24 | 莱夫韦弗公司 | Ultra wideband (UWB) baby monitors for detection of infant cardiopulmonary distress |
| CN103540152A (en) * | 2012-07-24 | 2014-01-29 | 常州波速传感器有限公司 | Gradual transition acoustic impedance matching material production method |
| CN103540152B (en) * | 2012-07-24 | 2016-08-10 | 常州波速传感器有限公司 | Gradual transition acoustic impedance match material compound method |
| CN104614442A (en) * | 2013-11-05 | 2015-05-13 | 松下知识产权经营株式会社 | Ultrasonic measuring method and device |
| CN107174281B (en) * | 2016-03-09 | 2021-07-20 | 精工爱普生株式会社 | Ultrasonic device, ultrasonic module, and ultrasonic measurement device |
| CN107174281A (en) * | 2016-03-09 | 2017-09-19 | 精工爱普生株式会社 | Ultrasonic device, ultrasonic wave module and ultrasonic measurement device |
| CN108882108A (en) * | 2018-07-05 | 2018-11-23 | 湖南大学 | It is applicable in the impedance matching system and its matching process of Yu Haiyang communication electroacoustic transducer |
| CN109246575A (en) * | 2018-08-09 | 2019-01-18 | 广州联声电子科技有限公司 | A kind of preparation method of the progressive acoustic impedance matching layer of high frequency |
| CN109246575B (en) * | 2018-08-09 | 2020-10-16 | 广州联声电子科技有限公司 | Preparation method of high-frequency progressive acoustic impedance matching layer |
| WO2021078291A1 (en) * | 2019-10-25 | 2021-04-29 | 飞依诺科技(苏州)有限公司 | Ultrasonic transducer and method for manufacturing ultrasonic transducer |
| CN112756241A (en) * | 2019-11-06 | 2021-05-07 | 中国石油化工股份有限公司 | Well wall ultrasonic piezoelectric transducer and well wall ultrasonic logging instrument |
| CN112756241B (en) * | 2019-11-06 | 2022-06-03 | 中国石油化工股份有限公司 | Well wall ultrasonic piezoelectric transducer and well wall ultrasonic logging instrument |
| CN114449417A (en) * | 2020-10-30 | 2022-05-06 | 华为技术有限公司 | Speaker and electronic equipment |
| CN114449417B (en) * | 2020-10-30 | 2022-11-25 | 华为技术有限公司 | Speaker and electronic equipment |
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|---|---|
| CN100460871C (en) | 2009-02-11 |
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