CN106228971A - Broadband sound focusing lens based on fractal acoustic metamaterial and preparation method thereof - Google Patents

Broadband sound focusing lens based on fractal acoustic metamaterial and preparation method thereof Download PDF

Info

Publication number
CN106228971A
CN106228971A CN201610589500.2A CN201610589500A CN106228971A CN 106228971 A CN106228971 A CN 106228971A CN 201610589500 A CN201610589500 A CN 201610589500A CN 106228971 A CN106228971 A CN 106228971A
Authority
CN
China
Prior art keywords
fractal
unit
focusing lens
refractive index
acoustic
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201610589500.2A
Other languages
Chinese (zh)
Other versions
CN106228971B (en
Inventor
程强
宋刚永
黄蓓
董慧媛
崔铁军
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Southeast University
Original Assignee
Southeast University
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Southeast University filed Critical Southeast University
Priority to CN201610589500.2A priority Critical patent/CN106228971B/en
Publication of CN106228971A publication Critical patent/CN106228971A/en
Application granted granted Critical
Publication of CN106228971B publication Critical patent/CN106228971B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00Methods 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
    • G10K11/18Methods or devices for transmitting, conducting or directing sound
    • G10K11/26Sound-focusing or directing, e.g. scanning
    • G10K11/30Sound-focusing or directing, e.g. scanning using refraction, e.g. acoustic lenses

Abstract

The present invention discloses a kind of broadband sound focusing lens based on fractal acoustic metamaterial and preparation method thereof, these broadband sound focusing lens include base material and the fractal structure cell array being positioned on this base material, this fractal structure cell array is arranged to make up by multiple fractal periodic units, and each fractal periodic unit is corresponding to a refraction point of condenser lens;Fractal periodic unit includes fractal unit and air two parts, and the refractive index of fractal unit that arbitrary refraction point is corresponding is consistent with the theoretical refractive index of this refraction point.The present invention uses fractal unit to form Acoustic focusing lens first, provides the new paragon of design new material for acoustic engineering, increases the actual path length that sound wave is propagated in cellular construction, improve the refractive index of cellular construction by the way of fractal;These Acoustic focusing lens have broadband character, can realize the well focussed effect of sound wave in broad frequency range.

Description

Broadband sound focusing lens based on fractal acoustic metamaterial and preparation method thereof
Technical field
The present invention relates to a kind of condenser lens and preparation method thereof, particularly to a kind of width based on fractal acoustic metamaterial Band sound focusing lens and preparation method thereof.
Background technology
Along with Novel manual electromagnetic material theoretical research and application and development are goed deep into by people, Meta Materials is at acoustic direction Application also result in the interest of numerous research worker.Meta Materials at acoustics with the similar corresponding relation on electromagnetism front Being confirmed in the middle of the research of people, the probability that the concept of Meta Materials expands to sound wave section is also being ground by the expert in this field Study carefully.Non-natural parameter characteristic can also be obtained at sound wave wave band at research acoustically, cellular construction based on Meta Materials before, Such as DNG feature (negative density and negative elastic modelling quantity), zero refractive index, even negative index, acoustic imaging, stealthy, conversion sound Learn, and acoustic surface.The design of acoustic elements mainly has two kinds of strategies: resonant element and effective medium theory composite.Closely Coming, the feasibility of the design of the disresonance unit based on folding space structure proposes the most in theory and is also tested Confirm.These structures can be used to design some specific parameters, such as low absorption and wide bandwidth of operation, but in unit design There is also the challenge of impedance matching.
Fractal structure is common in the fractal geomorphic feature in nature landform, is usually applied to architectural design, antenna, microwave Device designs.Fractal acoustic metamaterial is the space folding structure of a kind of self similarity, also in that this self-similarity, fractal sound Learn Meta Materials and have excellent characteristics.Fractal structure looks the most complicated, but it can pass through computer program design, and leads to Cross 3D printer printing speed molding, have and have good application prospect.
Summary of the invention
Goal of the invention: the first object of the present invention is to provide a kind of broadband based on fractal acoustic metamaterial sound focusing saturating Mirror, the second object of the present invention is to provide the preparation method of these broadband sound focusing lens.
Technical scheme: a kind of broadband sound focusing lens based on fractal acoustic metamaterial of the present invention, this broadband sound Condenser lens includes base material and the fractal structure cell array being positioned on this base material, this fractal structure cell array Being arranged to make up by multiple fractal periodic units, each fractal periodic unit is corresponding to a refraction point of condenser lens;Fractal week Phase unit includes fractal unit and air two parts, the refractive index of the fractal unit that arbitrary refraction point is corresponding and the reason of this refraction point Opinion refractive index is consistent.
Concrete, the fractal unit that arbitrary refraction point is corresponding is selected from the one in the fractal unit of single order~N rank, and wherein, N is Integer, and N >=2.
Further, the fractal unit in every rank is that this fractal unit of rank standard carries out shape after opening part reason on acoustic propagation direction The deformation unit become, the structure of the fractal unit of standard and size by Computer Fractal program according to the cycle chi of fractal periodic unit Very little automatically generate.
Further, this periodic dimensions operating frequency range based on equivalent medium theory, according to condenser lens determines.
Preferably, base material and fractal unit are formed through 3D printing by photosensitive resin material.
Further, fractal unit is the fractal unit of Hilbert.
The preparation method of broadband sound focusing lens based on fractal acoustic metamaterial of the present invention, including walking as follows Rapid:
Step 1, determines the theoretical refractive index value of each refraction point of condenser lens to be prepared;
Step 2, realizes the theoretical refractive index of each refraction point by fractal periodic unit, determines that each refraction point is corresponding The structure of fractal unit and size in typing periodic unit;
Step 3, the fractal unit that each refraction point of step 2 being obtained is corresponding requires to arrange shape according to sound focusing lens theory Become fractal building block array, and be fixed on base material, form the structural model of broadband sound focusing lens, pass through 3D Print this structural model and obtain broadband sound focusing lens.
In above-mentioned steps 1, according to hyperbolic secant function n (y)=n0Sech (α y) determines each refraction point of condenser lens Theoretical refractive index value, wherein,n0For the refractive index value of condenser lens center, h is half condenser lens Height, nhRefractive index value for condenser lens edge.
Concrete, in step 2, structure and the size of fractal unit determine by the following method:
Step 21, according to refractive index of the centre value n of condenser lens to be prepared0, determine dividing for analog focus lens The top step number N, N≤n of shape unit0≤ N+1, N are integer;
Step 22, according to the working band of condenser lens to be prepared, determines the periodic dimensions of fractal periodic unit;By week The phase fractal program of size input computer, by this programming automatic generation single order~the structure of the N rank fractal unit of standard and size;
Step 23, extracts single order~the performance parameter of the N rank fractal unit of standard, respectively with the folding of condenser lens to be prepared The rate Gradient distribution of penetrating is compared, according to comparison result respectively on acoustic propagation direction to single order~the N rank fractal unit of standard Structure carries out opening process, obtains structure and the size of the fractal unit of single order~N rank for analog focus lens;
Step 24, extracts single order~the performance parameter of the fractal unit in N rank, obtains the refraction of the fractal unit in each rank by sweeping ginseng Rate, compares the theoretical refractive index of each refraction point of condenser lens to be prepared, determines the fractal unit that each refraction point is corresponding.
Further, in step 3, fractal unit is formed fractal structure cell array according to periodic dimensions arrangement, and will It is fixed on base material, obtains the structural model of broadband sound focusing lens, uses photosensitive resin material to print this structure mould Type, obtains broadband sound focusing lens.
Beneficial effect: compared with prior art, it is an advantage of the current invention that: (1) present invention uses fractal unit to use first In forming Acoustic focusing lens, provide the new paragon of design new material for acoustic engineering, by the way of fractal, increase sound wave The actual path length propagated in cellular construction, improves the refractive index of cellular construction;And, along with the exponent number of fractal unit Raising, be also easier to obtain high index of refraction, fractal unit the lens formed or wave absorbing device have more excellent performance;(2) The Acoustic focusing lens of the present invention have broadband character, can realize the well focussed effect of sound wave in broad frequency range;(3) The Acoustic focusing lens preparation method simple and fast of the present invention, and raw material uses photosensitive resin, and prepared Acoustic focusing is saturating Mirror has the feature of lightweight and low cost, is suitable to popularization and application.
Accompanying drawing explanation
Fig. 1 is the structural representation of the broadband sound focusing lens of the present invention;
Fig. 2 a is the structural representation of the fractal unit of single order in embodiment;
Fig. 2 b is the structural representation of the fractal unit of second order in embodiment;
Fig. 2 c is the structural representation of the three fractal unit in rank in embodiment;
Fig. 3 a be single order fractal unit equivalent refractive index in 2kHz~5kHz frequency range in embodiment, equiva lent impedance, etc. Effect density and the change curve of concrete moduli;
Fig. 3 b be second order fractal unit equivalent refractive index in 2kHz~5kHz frequency range in embodiment, equiva lent impedance, etc. Effect density and the change curve of concrete moduli.
Fig. 3 c be the three fractal unit in rank equivalent refractive index in 2kHz~5kHz frequency range in embodiment, equiva lent impedance, etc. Effect density and the change curve of concrete moduli.
Fig. 4 is that single order in embodiment, second order, the three fractal unit in the rank variations in refractive index in 2kHz~5kHz frequency range is bent Line;
Fig. 5 be Acoustic focusing lens to be prepared in embodiment ideal refractive rate distribution and fractal unit attainable from Dissipate index distribution;
Fig. 6 is the structural representation of the condenser lens prepared in embodiment;
Fig. 7 a be the actual test acoustic lens that records under 2kHz and 5kHz operating frequency and emulation acoustic lens in the x-direction Output acoustic pressure amplitude scattergram;
Fig. 7 b is the actual test acoustic lens that records under 2kHz and 5kHz operating frequency and emulation acoustic lens in the y-direction defeated Go out acoustic pressure amplitude scattergram;
The acoustic pressure distribution that acoustic pressure distribution and the actual test lens of lens emulation when Fig. 8 a is 2kHz obtains;
The acoustic pressure distribution that acoustic pressure distribution and the actual test lens of lens emulation when Fig. 8 b is 3kHz obtains;
The acoustic pressure distribution that acoustic pressure distribution and the actual test lens of lens emulation when Fig. 8 c is 4kHz obtains;
The acoustic pressure distribution that acoustic pressure distribution and the actual test lens of lens emulation when Fig. 8 d is 5kHz obtains.
Detailed description of the invention
Below in conjunction with the accompanying drawings technical scheme is described further.
The broadband sound focusing lens based on fractal acoustic metamaterial of the present invention, such as Fig. 1, these broadband sound focusing lens include Fractal structure cell array 2 and base material 1, fractal structure cell array 2 is positioned on this base material 1, for simulated sound Learning the refractive index of each refraction point of condenser lens, base material 1 is used for supporting fractal structure cell array 2.
Fractal structure cell array 2 is arranged to make up by multiple fractal periodic units, and each fractal periodic unit is corresponding to poly- One refraction point of focus lens.Each fractal periodic unit has identical periodic dimensions U, and periodic dimensions U uses effective medium Theoretical method, operating frequency range according to condenser lens determine.
Fractal periodic unit includes fractal unit 3 and air two parts, the refraction of the fractal unit 3 that arbitrary refraction point is corresponding Rate is consistent with the theoretical refractive index of this refraction point.The fractal unit 3 that arbitrary refraction point is corresponding is all selected from the fractal list of single order~N rank One in unit, wherein, N is integer, and N >=2;Can first according to the periodic dimensions U of fractal periodic unit by Computer Fractal journey Sequence generates structure and the size of each rank fractal unit of standard, then opens each rank fractal unit of standard on acoustic propagation direction Mouth processes, and obtains structure and the size of the final fractal unit in each rank;Processed by opening, make corresponding fractal of each refraction point The refractive index of unit 3 is consistent with theoretical refractive index, makes Acoustic focusing lens realize wide working band.
Fractal unit 3 can be Hilbert fractal structure, and it can effectively improve the refractive index of cellular construction, it is achieved thin The design of lens.
Base material 1 and fractal unit 3 can be formed through 3D printing by photosensitive resin material.
The Acoustic focusing lens of the present invention have broadband character, can realize the well focussed of sound wave in broad frequency range Effect.Compared with prior art, fractal unit 3 is used for forming Acoustic focusing lens by the present invention first, these Acoustic focusing lens Be equivalent to a kind of acoustic metamaterial, including the fractal structure list formed by periodic dimensions U periodic arrangement by a series of fractal unit 3 Element array 2, increases the actual path length that sound wave is propagated in cellular construction by the way of fractal, improves cellular construction Refractive index;And, along with the raising of the exponent number of fractal unit, be also easier to obtain high index of refraction, by fractal unit 3 formed saturating Mirror or wave absorbing device have more excellent performance;Meanwhile, by the cellular construction of its fractal unit of engineer, material can be controlled Effective dielectric constant, pcrmeability, refractive index, the electromagnetic parameter such as natural impedance, it is achieved the material that nature exists does not has Character.
The preparation method of the broadband sound focusing lens based on fractal acoustic metamaterial of the present invention, comprises the steps:
(1) the theoretical refractive index value of each refraction point of condenser lens to be prepared is determined;
Changing owing to the refractive index of the every bit of condenser lens is as longitudinal position, therefore, design acoustics gathers During focus lens (hereinafter referred to as " condenser lens "), the distribution of its refractive index is it suffices that hyperbolic secant function: n (y)=n0sech (α y), α is by formulaDefinition obtains;Wherein, n0Being the refractive index value of condenser lens center, h is half The height of individual condenser lens, nhIt it is the refractive index value of condenser lens edge.
(2) simulated the theoretical refractive index of each refraction point by fractal periodic unit, determine corresponding the dividing of each refraction point The structure of fractal unit 3 and size in type periodic unit;
First, according to refractive index of the centre value n of condenser lens to be prepared0, determine for analog focus lens is fractal The top step number N, N≤n of unit 30≤ N+1, N are integer;In embodiments of the invention, 3 < n0< 4, therefore, fractal unit 3 Top step number is N=3, i.e. uses single order, the fractal unit of second order and three rank to carry out analog focus lens.
Secondly, according to the working band (i.e. operating frequency range) of condenser lens to be prepared, fractal periodic unit is determined Periodic dimensions U, by the periodic dimensions fractal program of U input computer, by this programming automatic generation single order~the N rank fractal list of standard The structure of unit and size.In the present embodiment, the working band of Acoustic focusing lens to be prepared is 2kHz to 5kHz, by equivalence matchmaker Matter theory understands, and each fractal unit 3 suffers from identical periodic dimensions, in the working band that this example is selected, and its periodic dimensions U =0.94cm;By Computer Fractal Program Generating standard single order, the fractal unit of standard second order and standard three rank, this fractal unit 3 For the fractal unit of Hilbert.
Again, single order~the performance parameter of the N rank fractal unit of standard are extracted respectively, with the refraction of condenser lens to be prepared Rate Gradient distribution is compared, and is finely adjusted structure and the size of the 1~N fractal unit of rank standard according to comparison result, respectively Acoustic propagation direction carries out opening process to the structure of single order~the N rank fractal unit of standard, obtains for analog focus lens The structure of the fractal unit of single order~N rank and size, the performance parameter of the fractal unit of this single order~N rank and condenser lens folding Penetrate rate Gradient distribution closest.
The opening purpose of fractal unit is the theoretical refractive index value obtaining this point, and therefore whether opening number is can be somebody's turn to do The refractive index of point is as the criterion, and opening number is generally 1~3;The opening number of the fractal unit in every rank may be identical, it is also possible to no With.
In the present embodiment, respectively extract standard single order, the equivalent refractive index of the fractal unit of standard second order and standard three rank, etc. The parameters such as effect impedance, equivalent density and concrete moduli, to standard single order, the structure of the fractal unit of standard second order and standard three rank It is finely adjusted, obtains single order, the fractal unit of second order and three rank, the height H=13mm of the fractal unit in every rank, thickness D=0.5mm; Concrete, such as Fig. 2 a, the fractal unit of single order 31 is that unit fractal to standard single order has carried out deformation process, i.e. in acoustic propagation direction On it carried out opening processed, length and width size W of the fractal unit of single order 311=4.5mm, opening size S1=1.5mm, Its parameter characteristic in the working band of Acoustic focusing lens 2kHz~5kHz such as Fig. 3 a;Such as Fig. 2 b, the fractal unit of second order 32 It is that unit fractal to standard second order has carried out deformation process, i.e. on acoustic propagation direction, it has been carried out an opening and processed, two Length and width size W of the fractal unit in rank 322=6.5mm, minor matters length L=2.5mm stretched into inside it, opening size S2= 1.5mm, outward opening size J=1.5mm, its parameter characteristic in the working band of 2kHz~5kHz such as Fig. 3 b;Such as Fig. 2 c, three The fractal unit in rank 33 is that the fractal unit in standard three rank has been carried out deformation process, i.e. on acoustic propagation direction, it has been carried out two Opening processes, length and width size W of the three fractal unit in rank 333=8.4mm, acoustic wave inlet size K=0.5mm, opening size S3= 1.5mm, its parameter characteristic in the working band of 2kHz~5kHz such as Fig. 3 c.
Finally, extract single order~the performance parameter of the fractal unit in N rank, obtain the refractive index of the fractal unit in each rank by sweeping ginseng Distribution, compares the theoretical refractive index of each refraction point of condenser lens to be prepared, determines the fractal list that each refraction point is corresponding Unit 3.In the present embodiment, single order, second order, the three fractal unit in rank index distribution such as Fig. 4 in working band, wherein, single order Fractal unit is for realizing the refraction point that refractive index value in condenser lens is close to 1, and the fractal unit of second order is used for realizing condenser lens The middle refractive index value refraction point close to 2, the three fractal unit in rank are for realizing the refraction point that refractive index value is close to 3.
(3) after the structure analyzing the fractal unit 3 determining that each refraction point is corresponding and size, according to sound focusing lens theory Requirement, forms fractal structure unit by corresponding fractal unit 3 according to periodic dimensions arrangement according to the distribution situation of each refraction point Array 2, and be fixed on base material 1, obtain the structural model of broadband sound focusing lens, use photosensitive resin material 3D Print this structural model, obtain broadband sound focusing lens.
In the present embodiment, using photosensitive resin material printed substrates material 1 and fractal unit 3, the Acoustic focusing prepared is saturating The structural representation of mirror sample such as Fig. 6, it is made up of the fractal cell array of two-layer 2, and the total length of this sample is Lf= 19.74cm, the cycle is U=0.94cm, and gross thickness is Wf=1.73cm, two minimum ranges arranged between fractal unit are Ws= 0.5mm.Such as Fig. 5, it can be seen that the attainable discrete index distribution of Acoustic focusing lens formed by the arrangement of fractal unit It is distributed with the ideal refractive rate of Acoustic focusing lens and complies fully with.The Acoustic focusing lens of prepared in accordance with the method for the present invention are original Sample is a layer unit structure, can realize the well focussed effect of sound wave, for further enhancing its sound in broad frequency range Focusing performance, highlights the advantage of this method further, uses the fractal cell array of two-layer 2, such as " the Measured in Fig. 8 d Field " shown in figure, when 5kHz, experiment records its output sound focusing energy and reaches 5:1 with input acoustic energy ratio, and sound wave gathers Burnt effect is notable;If continuing to increase the number of plies, then its thickness will substantially increase, and this will cause acoustic lens materials cost to improve, Also result in acoustic lens impedance to increase further simultaneously, in turn result in acoustic reflection loss and sound focusing energy reduces, affect sound wave The shortcomings such as focusing effect, therefore, use two-layer cellular construction in the present embodiment.
In order to verify the correctness of this method, the performance of prepared sample is tested.
Concrete method of testing is: prepared Acoustic focusing lens are placed in test zone, total by sweep test region Sonic pressure field, obtains the scattergram of acoustic pressure, concrete, is placed in by sample in two-dimensional acoustic field near-field scan platform, and sample is positioned at raises one's voice Between device array and mike, lucite is slightly compressed on sample, obtains plane wave by loudspeaker array, and comes with mike Near scanning sample, the acoustic pressure of test zone, obtains its output acoustic pressure amplitude scattergram (Fig. 7 a~7b) in x direction and y direction And acoustic pressure distribution situation (Fig. 8 a~8d).Meanwhile, it is simulated emulating to Expected Results to these Acoustic focusing lens, sound will be emulated The acoustic pressure distribution of lens compares with the actual test result of the acoustic lens prepared.
Fig. 7 a~7b is the actual test acoustic lens recorded under 2kHz and 5kHz operating frequency and emulates the defeated of acoustic lens Go out acoustic pressure amplitude scattergram, Fig. 7 a represents in the x-direction along acoustic propagation direction, Fig. 7 b represents in the y-direction in focal spot Vertical direction along acoustic propagation direction.In Fig. 7 a and Fig. 7 b, two curves in top are the simulation figure under 5kHz working band and reality Border test image, it can be seen that two curve distribution are almost consistent, illustrates that the experiment of 5kHz acoustic lens coincide very with simulation architecture Good, and, obtaining sound field amplitude gain at distance acoustic lens about 120mm is the focusing effect of 11.3dB;Under in Fig. 7 a~7b Two, side curve is the emulating image under 2kHz working band and actual test image, it can be seen that experiment during 2kHz is with imitative True result is the most identical, and to record its focusing effect be 8dB, and actual test herein is owing to during 2kHz, sound is real with the error of emulation Test what slit source acoustic conductance in platform caused, i.e. the upper poly (methyl methacrylate) plate of experiment porch and sample room has less space, in low frequency work Owing to its wavelength is long, there is certain sound diffraction ability when making, in turn result in certain sound capacity loss, have impact on low Frequently focusing effect time.
The acoustic pressure distribution feelings of the actual test lens recorded under Fig. 8 a~8b respectively different operating frequency and emulation lens Condition, wherein, the acoustic pressure distribution that acoustic pressure distribution and the actual test lens of lens emulation when Fig. 8 a is 2000Hz obtains, Fig. 8 b is The acoustic pressure distribution that acoustic pressure distribution and the actual test lens of lens emulation during 3000Hz obtains, lens emulation when Fig. 8 c is 4000Hz The acoustic pressure distribution that obtains with actual test lens of acoustic pressure distribution, the acoustic pressure distribution of lens emulation when Fig. 8 d is 5000Hz and reality The acoustic pressure distribution that test lens obtains.In experimental result picture, for the sound-filed simulation figure of lens emulation in white dashed line frame, white is empty It is the sound-filed simulation figure of actual test lens on the left of wire frame, by contrast it can be seen that actual test case is kissed with simulation scenarios Close.

Claims (10)

1. broadband sound focusing lens based on fractal acoustic metamaterial, it is characterised in that described broadband sound focusing lens bag Include base material (1) and the fractal structure cell array (2) being positioned on this base material (1), this fractal structure cell array (2) being arranged to make up by multiple fractal periodic units, each fractal periodic unit is corresponding to a refraction point of condenser lens;Described Fractal periodic unit includes fractal unit (3) and air two parts, the refractive index of the fractal unit (3) that arbitrary refraction point is corresponding with The theoretical refractive index of this refraction point is consistent.
Broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 1, it is characterised in that arbitrary folding The fractal unit (3) that exit point is corresponding is selected from the one in the fractal unit of single order~N rank, and wherein, N is integer, and N >=2.
Broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 2, it is characterised in that every rank are divided Shape unit is the deformation unit formed after this fractal unit of rank standard carries out opening part reason on acoustic propagation direction, the fractal list of standard Structure and the size of unit are automatically generated according to the periodic dimensions of fractal periodic unit by Computer Fractal program.
Broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 3, it is characterised in that this cycle The size operating frequency range based on equivalent medium theory, according to condenser lens determines.
Broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 1, it is characterised in that described base Bottom material (1) and fractal unit (3) are formed through 3D printing by photosensitive resin material.
Broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 1, it is characterised in that described point Shape unit (3) is the fractal unit of Hilbert.
7. a preparation method for the broadband sound focusing lens based on fractal acoustic metamaterial described in claim 1, its feature It is, comprises the steps:
Step 1, determines the theoretical refractive index value of each refraction point of condenser lens to be prepared;
Step 2, realizes the theoretical refractive index of each refraction point by fractal periodic unit, determines corresponding fractal of each refraction point The structure of fractal unit (3) and size in periodic unit;
Step 3, the fractal unit (3) that each refraction point of step 2 being obtained is corresponding requires arrangement shape according to sound focusing lens theory Become fractal building block array (2), and be fixed on base material (1), form the structural model of broadband sound focusing lens, Print this structural model by 3D and obtain broadband sound focusing lens.
The preparation method of broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 7, its feature It is, in step 1, according to hyperbolic secant function n (y)=n0Sech (α y) determines the theoretical refraction of each refraction point of condenser lens Rate value, wherein,n0For the refractive index value of condenser lens center, h is the height of half condenser lens, nhRefractive index value for condenser lens edge.
The preparation method of broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 8, its feature Being, in step 2, structure and the size of described fractal unit (3) determine by the following method:
Step 21, according to refractive index of the centre value n of condenser lens to be prepared0, determine the fractal unit for analog focus lens (3) top step number N, N≤n0≤ N+1, N are integer;
Step 22, according to the working band of condenser lens to be prepared, determines the periodic dimensions of fractal periodic unit, by cycle chi The fractal program of very little input computer, by this programming automatic generation single order~the structure of the N rank fractal unit of standard and size;
Step 23, extracts single order~the performance parameter of the N rank fractal unit of standard, respectively with the refractive index of condenser lens to be prepared Gradient distribution is compared, according to comparison result respectively on acoustic propagation direction to single order~the structure of the N rank fractal unit of standard Carry out opening process, obtain structure and the size of the fractal unit of single order~N rank for analog focus lens;
Step 24, extracts single order~the performance parameter of the fractal unit in N rank, obtains the refractive index of the fractal unit in each rank by sweeping ginseng, Compare the theoretical refractive index of each refraction point of condenser lens to be prepared, determine the fractal unit (3) that each refraction point is corresponding.
The preparation method of broadband sound focusing lens based on fractal acoustic metamaterial the most according to claim 9, its feature It is, in step 3, described fractal unit (3) is formed fractal structure cell array (2) according to periodic dimensions arrangement, and by it It is fixed on base material (1), obtains the structural model of broadband sound focusing lens, use photosensitive resin material to print this structure mould Type, obtains broadband sound focusing lens.
CN201610589500.2A 2016-07-25 2016-07-25 Based on the broadband sound focusing lens and preparation method thereof for dividing shape acoustic metamaterial Active CN106228971B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610589500.2A CN106228971B (en) 2016-07-25 2016-07-25 Based on the broadband sound focusing lens and preparation method thereof for dividing shape acoustic metamaterial

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610589500.2A CN106228971B (en) 2016-07-25 2016-07-25 Based on the broadband sound focusing lens and preparation method thereof for dividing shape acoustic metamaterial

Publications (2)

Publication Number Publication Date
CN106228971A true CN106228971A (en) 2016-12-14
CN106228971B CN106228971B (en) 2019-07-12

Family

ID=57531499

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610589500.2A Active CN106228971B (en) 2016-07-25 2016-07-25 Based on the broadband sound focusing lens and preparation method thereof for dividing shape acoustic metamaterial

Country Status (1)

Country Link
CN (1) CN106228971B (en)

Cited By (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106650179A (en) * 2017-01-23 2017-05-10 东南大学 Method of designing Acoustic Metamaterials based on CMA-ES optimization algorithm
CN107492370A (en) * 2017-07-31 2017-12-19 北京交通大学 The super surface texture that a kind of adjustable sound wave focuses on
CN107863096A (en) * 2017-11-21 2018-03-30 北京交通大学 A kind of super surface texture and its application method of the regulation and control of reflection-type wavefront
CN108735197A (en) * 2018-04-02 2018-11-02 浙江大学 A kind of locally resonant type acoustic metamaterial condenser lens and its design method
CN108922511A (en) * 2018-07-05 2018-11-30 广东工业大学 A kind of super surface texture of acoustics and acoustic antennas device
CN109119062A (en) * 2018-06-19 2019-01-01 浙江大学 A kind of acoustic resonance condenser lens and its design method
CN109147755A (en) * 2018-07-24 2019-01-04 东南大学 It is a kind of can the artificial surface acoustic wave of high-efficiency transfer acoustic waveguide and its design method
CN109185233A (en) * 2018-07-20 2019-01-11 中国科学院电工研究所 The fractal structure acoustic metamaterial device of for transformer noise reduction
WO2019041299A1 (en) * 2017-09-01 2019-03-07 深圳先进技术研究院 Ultrasonic focusing lens based on planar artificial structure
CN109884188A (en) * 2019-03-06 2019-06-14 北京卫星环境工程研究所 Broadband acoustic beam regulator control system based on Huygens's acoustic metamaterial
CN110491363A (en) * 2019-09-26 2019-11-22 合肥工业大学 A kind of Wideband Focusing lens surpassing surface based on acoustic resonance
CN113032975A (en) * 2021-03-05 2021-06-25 南京理工大学 Parameter modulation method for eliminating sub-wavelength structure of broadband reflection sound wave in curved path
CN113221268A (en) * 2021-04-30 2021-08-06 西安交通大学 Spatial gradient metamaterial for pipeline noise control and design method
CN108735197B (en) * 2018-04-02 2024-04-12 浙江大学 Local resonance type acoustic metamaterial focusing lens and design method thereof

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20110175795A1 (en) * 2008-09-03 2011-07-21 Murata Manufacturing Co., Ltd. Metamaterial
CN102483913A (en) * 2009-03-02 2012-05-30 代表亚利桑那大学的亚利桑那校董会 Solid-state acoustic metamaterial and method of using same to focus sound
US8269168B1 (en) * 2007-04-30 2012-09-18 Physical Logic Ag Meta materials integration, detection and spectral analysis
CN205282658U (en) * 2016-01-14 2016-06-01 武汉碧海云天科技股份有限公司 Super material of electromagnetism

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8269168B1 (en) * 2007-04-30 2012-09-18 Physical Logic Ag Meta materials integration, detection and spectral analysis
US20110175795A1 (en) * 2008-09-03 2011-07-21 Murata Manufacturing Co., Ltd. Metamaterial
CN102483913A (en) * 2009-03-02 2012-05-30 代表亚利桑那大学的亚利桑那校董会 Solid-state acoustic metamaterial and method of using same to focus sound
CN205282658U (en) * 2016-01-14 2016-06-01 武汉碧海云天科技股份有限公司 Super material of electromagnetism

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
J. MCVAY ETC: "High impedance metamaterial surfaces using Hilbert-curve inclusions", 《IEEE JOURNALS & MAGAZINES》 *
周卓辉 等: "超材料在宽频微波衰减吸收材料中的应用研究进展", 《材料工程》 *
陆慧颖 等: "二维声学超材料透镜的设计与实验", 《南京大学学报(自然科学)》 *

Cited By (23)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106650179A (en) * 2017-01-23 2017-05-10 东南大学 Method of designing Acoustic Metamaterials based on CMA-ES optimization algorithm
CN106650179B (en) * 2017-01-23 2019-11-12 东南大学 A method of based on CMA-ES Optimization Algorithm acoustic metamaterial unit
CN107492370A (en) * 2017-07-31 2017-12-19 北京交通大学 The super surface texture that a kind of adjustable sound wave focuses on
CN107492370B (en) * 2017-07-31 2020-11-17 北京交通大学 Super surface structure capable of adjusting sound wave focusing
WO2019041299A1 (en) * 2017-09-01 2019-03-07 深圳先进技术研究院 Ultrasonic focusing lens based on planar artificial structure
CN107863096B (en) * 2017-11-21 2021-06-08 北京交通大学 Reflection type wavefront-regulated super-surface structure and application method thereof
CN107863096A (en) * 2017-11-21 2018-03-30 北京交通大学 A kind of super surface texture and its application method of the regulation and control of reflection-type wavefront
CN108735197B (en) * 2018-04-02 2024-04-12 浙江大学 Local resonance type acoustic metamaterial focusing lens and design method thereof
CN108735197A (en) * 2018-04-02 2018-11-02 浙江大学 A kind of locally resonant type acoustic metamaterial condenser lens and its design method
CN109119062A (en) * 2018-06-19 2019-01-01 浙江大学 A kind of acoustic resonance condenser lens and its design method
CN109119062B (en) * 2018-06-19 2023-07-18 浙江大学 Acoustic resonance focusing lens and design method thereof
CN108922511B (en) * 2018-07-05 2023-05-05 广东工业大学 Acoustic super-surface structure and acoustic antenna device
CN108922511A (en) * 2018-07-05 2018-11-30 广东工业大学 A kind of super surface texture of acoustics and acoustic antennas device
CN109185233A (en) * 2018-07-20 2019-01-11 中国科学院电工研究所 The fractal structure acoustic metamaterial device of for transformer noise reduction
CN109185233B (en) * 2018-07-20 2020-09-18 中国科学院电工研究所 Fractal structure acoustic metamaterial device for noise reduction of transformer
CN109147755A (en) * 2018-07-24 2019-01-04 东南大学 It is a kind of can the artificial surface acoustic wave of high-efficiency transfer acoustic waveguide and its design method
CN109884188B (en) * 2019-03-06 2021-04-27 北京卫星环境工程研究所 Broadband sound beam regulation and control system based on Huygens acoustic metamaterial
CN109884188A (en) * 2019-03-06 2019-06-14 北京卫星环境工程研究所 Broadband acoustic beam regulator control system based on Huygens's acoustic metamaterial
CN110491363A (en) * 2019-09-26 2019-11-22 合肥工业大学 A kind of Wideband Focusing lens surpassing surface based on acoustic resonance
CN113032975B (en) * 2021-03-05 2022-09-06 南京理工大学 Parameter modulation method for eliminating sub-wavelength structure of broadband reflection sound wave in curved path
CN113032975A (en) * 2021-03-05 2021-06-25 南京理工大学 Parameter modulation method for eliminating sub-wavelength structure of broadband reflection sound wave in curved path
CN113221268A (en) * 2021-04-30 2021-08-06 西安交通大学 Spatial gradient metamaterial for pipeline noise control and design method
CN113221268B (en) * 2021-04-30 2022-12-09 西安交通大学 Spatial gradient metamaterial for pipeline noise control and design method

Also Published As

Publication number Publication date
CN106228971B (en) 2019-07-12

Similar Documents

Publication Publication Date Title
CN106228971A (en) Broadband sound focusing lens based on fractal acoustic metamaterial and preparation method thereof
CN106328115B (en) Sound insulation room artificial material based on fractal structure
Kowalczyk et al. Modeling frequency-dependent boundaries as digital impedance filters in FDTD and K-DWM room acoustics simulations
CN110163213A (en) Remote sensing image segmentation method based on disparity map and multiple dimensioned depth network model
JP2021093154A (en) Holographic quantum dynamics simulation
Pruthi et al. Simulation and analysis of nasalized vowels based on magnetic resonance imaging data
Wongkasem et al. Development of chiral negative refractive index metamaterials for the terahertz frequency regime
Defraene et al. Real-time perception-based clipping of audio signals using convex optimization
Chardon et al. Gridless three-dimensional compressive beamforming with the Sliding Frank-Wolfe algorithm
CN112765835B (en) Aluminum honeycomb test piece collision simulation and test benchmarking method and device
CN114417908A (en) Multi-mode fusion-based unmanned aerial vehicle detection system and method
Bezzola Numerical optimization strategies for acoustic elements in loudspeaker design
CN103793897B (en) A kind of digital picture halftoning method based on wavelet multi-scale information fusion
Georgiou et al. Incorporating directivity in the Fourier pseudospectral time-domain method using spherical harmonics
Bilbao Percussion synthesis based on models of nonlinear shell vibration
Zigoneanu Design and experimental applications of acoustic metamaterials
Chen et al. Long-term scalogram integrated with an iterative data augmentation scheme for acoustic scene classification
Sanalatii et al. Estimation of loudspeaker frequency response and directivity using the radiation-mode method
Courcoux-Caro et al. Sequential sensor selection for the localization of acoustic sources by sparse Bayesian learning
CN105488521A (en) Kernel function based expanded sample screening method
Shalev et al. Indoors audio classification with structure image method for simulating multi-room acoustics
Enhos et al. Transmitting CMUT arrays without a DC bias
Zhang et al. Influence of the Relative Height of a Dome-Shaped Diaphragm on the Directivity of a Spherical-Enclosure Loudspeaker
Ahnert et al. Binaural Auralization from a sound system simulation program
Seipel Music instrument identification using convolutional neural networks

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant