CN111261135A - Mie resonance-based double-negative-type acoustic metamaterial for transcranial ultrasonic imaging - Google Patents

Mie resonance-based double-negative-type acoustic metamaterial for transcranial ultrasonic imaging Download PDF

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CN111261135A
CN111261135A CN202010044301.XA CN202010044301A CN111261135A CN 111261135 A CN111261135 A CN 111261135A CN 202010044301 A CN202010044301 A CN 202010044301A CN 111261135 A CN111261135 A CN 111261135A
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黄玉辉
吴勇军
金一铭
陈洁
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Abstract

The invention discloses a double-negative-type acoustic metamaterial for transcranial ultrasonic imaging based on Mie resonance, which comprises an ultrasonic couplant used as a matrix and a scatterer dispersed in the matrix and used for generating the Mie resonance, wherein the scatterer is a porous polyethylene glycol diacrylate hydrogel microsphere; the volume fraction of the porous polyethylene glycol diacrylate hydrogel microspheres in the matrix is 15-25%. The double-negative acoustic metamaterial provided by the invention can effectively eliminate the dissipation and distortion effects of the skull on sound waves, so that transcranial ultrasonic imaging is hopefully realized without depending on the naturally existing or artificially manufactured sound window of the skull.

Description

一种基于米氏共振的用于穿颅超声成像的双负型声学超材料A Double Negative Acoustic Metamaterial Based on Mie Resonance for Transcranial Ultrasound Imaging

技术领域technical field

本发明属于声学超材料领域,特别涉及一种基于米氏共振的用于穿颅超声成像的双负型声学超材料。The invention belongs to the field of acoustic metamaterials, in particular to a double negative acoustic metamaterial based on Mie resonance for transcranial ultrasound imaging.

背景技术Background technique

在医学领域,核磁共振成像(MRI)、计算机断层扫描(CT)和颅脑超声,是颅脑疾病主要的影像学诊断方法。尽管MRI一般被认为是最适合颅脑检查的方法,CT也具有其优秀的诊断价值,但在某些情况下,颅脑超声具有不可取代的作用。首先,颅脑超声可以提供MRI和CT无法获取的血流动力学信息;其次,颅脑超声设备轻便,适用于救护车、急诊室、重症监护室等抢救科室的床旁检测和长期动态监测,尤其对于不能搬动的危重患者可实施床旁检查;另外,超声检测无CT的辐射损伤,无MRI的强磁场造成的不适感。因此颅脑超声成像技术具有重要的临床应用价值。但是,由于颅骨与颅内软组织间存在巨大的声阻抗失配,超声波在颅骨内外两界面处会发生严重反射,再加上颅骨对声波的强烈吸收,携带颅内组织和血流信息的超声波信号到达接收探头时只剩下约1%的能量。目前的颅脑超声成像技术强烈依赖于颅骨天然存在或人工制造的声窗,如“颞骨声窗”和“眼眶声窗”,超声波无法直接穿过大部分较厚的颅骨进行组织和血流成像。且研究发现,随着年龄的增长,颞骨会逐渐增厚,老年女性经颅多普勒超声的失败率可达10%以上。总之,颅骨对超声具有极强的衰减和畸变效应,超声以常规的方式难以有效穿透颅骨实现颅内组织和血流成像。In the medical field, magnetic resonance imaging (MRI), computed tomography (CT) and brain ultrasound are the main imaging diagnostic methods for brain diseases. Although MRI is generally considered to be the most suitable method for brain examination, and CT also has its excellent diagnostic value, in some cases, brain ultrasound has an irreplaceable role. First, cranial ultrasound can provide hemodynamic information that cannot be obtained by MRI and CT; secondly, cranial ultrasound equipment is portable and suitable for bedside detection and long-term dynamic monitoring in emergency departments such as ambulances, emergency rooms, and intensive care units. In particular, bedside examinations can be performed for critically ill patients who cannot move; in addition, ultrasound detection has no radiation damage caused by CT and no discomfort caused by the strong magnetic field of MRI. Therefore, brain ultrasound imaging technology has important clinical application value. However, due to the huge acoustic impedance mismatch between the skull and the intracranial soft tissue, the ultrasound will be severely reflected at the interface between the inner and outer skulls, coupled with the strong absorption of the sound waves by the skull, the ultrasound signals that carry information about the intracranial tissue and blood flow Only about 1% of the energy is left when it reaches the receiving probe. Current cranial ultrasound imaging techniques strongly rely on naturally occurring or artificially created acoustic windows in the skull, such as the "temporal bone window" and "orbital acoustic window," which cannot directly pass through most of the thicker skull for tissue and blood flow imaging . And the study found that with the increase of age, the temporal bone will gradually thicken, and the failure rate of transcranial Doppler ultrasound in elderly women can reach more than 10%. In conclusion, the skull has strong attenuation and distortion effects on ultrasound, and it is difficult for ultrasound to effectively penetrate the skull to achieve intracranial tissue and blood flow imaging in a conventional manner.

近年来,声学超材料的迅速发展为解决上述难题提供了新的思路。声学超材料是目前国际学术界和工程界研究的热点之一,它是由亚波长结构单元构成的具有超常物理特性的人工周期性材料。通过巧妙设计超材料的结构单元,可以精确操控声波的传输方向,从而实现常规材料所不具备的独特功能,例如负折射、负反射、声隐形等,在军事隐形、减振降噪、医学成像等领域具有广泛的应用价值。In recent years, the rapid development of acoustic metamaterials has provided new ideas for solving the above problems. Acoustic metamaterials are currently one of the hotspots in the international academic and engineering circles. They are artificial periodic materials composed of subwavelength structural units with extraordinary physical properties. By ingeniously designing the structural units of metamaterials, the transmission direction of sound waves can be precisely controlled, so as to achieve unique functions that conventional materials do not have, such as negative refraction, negative reflection, acoustic stealth, etc., in military stealth, vibration and noise reduction, medical imaging It has a wide range of application value in other fields.

发明内容SUMMARY OF THE INVENTION

本发明的目的在于提供一种基于米氏共振的用于穿颅超声成像的双负型声学超材料,能够有效消除颅骨对声波的耗散和畸变作用。The purpose of the present invention is to provide a double negative acoustic metamaterial for transcranial ultrasound imaging based on Mie resonance, which can effectively eliminate the dissipation and distortion effects of the skull on sound waves.

本发明提供如下技术方案:The present invention provides the following technical solutions:

一种基于米氏共振的用于穿颅超声成像的声学超材料,所述的双负型声学超材料包括作为基体的超声耦合剂和分散在基体中用于发生米氏共振的散射体,所述散射体为多孔聚乙二醇双丙烯酸酯水凝胶微球。An acoustic metamaterial based on Mie resonance for transcranial ultrasound imaging, the double negative acoustic metamaterial comprises an ultrasonic couplant as a matrix and a scatterer dispersed in the matrix for generating Mie resonance, so The scatterers are porous polyethylene glycol diacrylate hydrogel microspheres.

优选的,所述多孔聚乙二醇双丙烯酸酯水凝胶微球在基体中的体积分数为15~25%。Preferably, the volume fraction of the porous polyethylene glycol diacrylate hydrogel microspheres in the matrix is 15-25%.

优选的,所述超声耦合剂的密度为900~1100kg/m3,声速为1400~1600m/s。Preferably, the density of the ultrasonic coupling agent is 900-1100 kg/m 3 , and the sound speed is 1400-1600 m/s.

优选的,所述多孔聚乙二醇双丙烯酸酯水凝胶微球的质量密度为500~700kg/m3,声速为120~180m/s。Preferably, the mass density of the porous polyethylene glycol diacrylate hydrogel microspheres is 500-700 kg/m 3 , and the sound velocity is 120-180 m/s.

优选的,所述多孔聚乙二醇双丙烯酸酯水凝胶微球的半径为50~70μm。Preferably, the radius of the porous polyethylene glycol diacrylate hydrogel microspheres is 50-70 μm.

所述声学超材料在0.63~0.73MHz的频率范围下同时实现负等效质量密度和负等效弹性模量。The acoustic metamaterial simultaneously achieves negative equivalent mass density and negative equivalent elastic modulus in the frequency range of 0.63-0.73 MHz.

本发明针对超声波难以穿透颅骨这一难题,提出一种基于米氏共振的双负型声学超材料来精确操控声波传输路径从而提高其穿透率。本发明提供的声学超材料为一种复合材料,其基体为超声耦合剂(密度为900~1100kg/m3,声速为1400~1600m/s),发生米氏共振的散射体为多孔聚乙二醇双丙烯酸酯(PEGDA)水凝胶微球。由于存在大量空气腔,多孔水凝胶微球表现出低的声速(120~180m/s)和适中的质量密度(500~700kg/m3),可引起较大的单极米氏共振,从而产生负的等效弹性模量。同时,大量粘稠的粒子表现出较强的偶极米氏共振,从而产生负的等效质量密度。通过改变多孔水凝胶微球的密度、声速、半径和在基体中的体积分数,可以调控负等效参数产生的频率范围(0.63~0.73MHz)。Aiming at the problem that ultrasound is difficult to penetrate the skull, the present invention proposes a double negative acoustic metamaterial based on Mie resonance to precisely control the transmission path of the acoustic wave to improve its penetration rate. The acoustic metamaterial provided by the present invention is a composite material, the matrix of which is an ultrasonic coupling agent (density is 900-1100kg/m 3 , and the sound speed is 1400-1600m/s), and the scatterer that occurs Mie resonance is porous polyethylene Alcohol diacrylate (PEGDA) hydrogel microspheres. Due to the existence of a large number of air cavities, the porous hydrogel microspheres exhibit low sound velocity (120-180 m/s) and moderate mass density (500-700 kg/m 3 ), which can induce large unipolar Mie resonances, thereby yields a negative equivalent elastic modulus. At the same time, a large number of viscous particles exhibit a strong dipole Mie resonance, resulting in a negative equivalent mass density. By changing the density, sound velocity, radius and volume fraction of the porous hydrogel microspheres in the matrix, the frequency range (0.63-0.73 MHz) generated by the negative equivalent parameter can be regulated.

本发明提供的双负型声学超材料能够有效消除颅骨对声波的耗散和畸变作用。本发明提供的双负型声学超材料有望实现不依赖于声窗的穿颅超声成像,在临床影像学诊断领域具有极大的应用价值。The double negative acoustic metamaterial provided by the invention can effectively eliminate the dissipation and distortion effects of the skull on acoustic waves. The double negative acoustic metamaterial provided by the invention is expected to realize transcranial ultrasound imaging independent of acoustic windows, and has great application value in the field of clinical imaging diagnosis.

附图说明Description of drawings

图1为聚焦超声束声场有限元模拟:(a)只有水存在;(b)水和颅骨;(c)水、颅骨和双负型声学超材料。Figure 1 shows the finite element simulation of the focused ultrasound beam sound field: (a) only water exists; (b) water and skull; (c) water, skull and double negative acoustic metamaterial.

图2为微流控技术制备多孔水凝胶微球的示意图。Figure 2 is a schematic diagram of the preparation of porous hydrogel microspheres by microfluidic technology.

图3为多重散射模型计算的实施例1中的多孔水凝胶微球分散于超声耦合剂中的(a)等效密度实部、(b)等效密度虚部、(c)等效弹性模量实部和(d)等效弹性模量虚部;其中,多孔水凝胶微球密度500kg/m3,声速120m/s,半径50μm,体积分数15%;超声耦合剂密度900kg/m3,声速1400m/s。Figure 3 shows (a) the real part of the equivalent density, (b) the imaginary part of the equivalent density, and (c) the equivalent elasticity of the porous hydrogel microspheres in Example 1 dispersed in the ultrasonic couplant calculated by the multiple scattering model The real part of modulus and the imaginary part of (d) equivalent elastic modulus; among them, the density of porous hydrogel microspheres is 500kg/m 3 , the speed of sound is 120m/s, the radius is 50μm, and the volume fraction is 15%; the density of ultrasonic couplant is 900kg/m 3. The speed of sound is 1400m/s.

图4为多重散射模型计算的实施例2中的多孔水凝胶微球分散于超声耦合剂中的(a)等效密度实部、(b)等效密度虚部、(c)等效弹性模量实部和(d)等效弹性模量虚部;其中多孔水凝胶微球密度600kg/m3,声速150m/s,半径60μm,体积分数20%;超声耦合剂密度1000kg/m3,声速1500m/s。Figure 4 shows (a) the real part of the equivalent density, (b) the imaginary part of the equivalent density, and (c) the equivalent elasticity of the porous hydrogel microspheres in Example 2 dispersed in the ultrasonic couplant calculated by the multiple scattering model The real part of the modulus and the imaginary part of the (d) equivalent elastic modulus; the density of porous hydrogel microspheres is 600kg/m 3 , the speed of sound is 150m/s, the radius is 60 μm, and the volume fraction is 20%; the density of the ultrasonic couplant is 1000kg/m 3 , the speed of sound is 1500m/s.

图5为多重散射模型计算的实施例3中的多孔水凝胶微球分散于超声耦合剂中的(a)等效密度实部、(b)等效密度虚部、(c)等效弹性模量实部和(d)等效弹性模量虚部;其中,多孔水凝胶微球密度700kg/m3,声速180m/s,半径70μm,体积分数25%;超声耦合剂密度1100kg/m3,声速1600m/s。Figure 5 shows (a) the real part of the equivalent density, (b) the imaginary part of the equivalent density, and (c) the equivalent elasticity of the porous hydrogel microspheres in Example 3 dispersed in the ultrasonic couplant calculated by the multiple scattering model The real part of modulus and the imaginary part of (d) equivalent elastic modulus; among them, the density of porous hydrogel microspheres is 700kg/m 3 , the speed of sound is 180m/s, the radius is 70μm, and the volume fraction is 25%; the density of ultrasonic couplant is 1100kg/m 3 , the speed of sound is 1600m/s.

图6为多重散射模型计算的对比例1中的钢珠微球分散于超声耦合剂中的(a)等效密度实部、(b)等效密度虚部、(c)等效弹性模量实部和(d)等效弹性模量虚部;其中,钢珠微球密度7900kg/m3,声速5955m/s,半径60μm,体积分数20%;超声耦合剂密度1000kg/m3,声速1500m/s。Figure 6 shows (a) the real part of the equivalent density, (b) the imaginary part of the equivalent density, and (c) the real equivalent elastic modulus of the steel ball microspheres in Comparative Example 1 dispersed in the ultrasonic couplant calculated by the multiple scattering model. part and (d) the imaginary part of the equivalent elastic modulus; among them, the density of steel ball microspheres is 7900kg/m 3 , the speed of sound is 5955m/s, the radius is 60 μm, and the volume fraction is 20%; the density of ultrasonic couplant is 1000kg/m 3 , the speed of sound is 1500m/s .

图7为多重散射模型计算的对比例2中的空心水凝胶微球分散于超声耦合剂中的(a)等效密度实部、(b)等效密度虚部、(c)等效弹性模量实部和(d)等效弹性模量虚部;其中,空心水凝胶微球密度200kg/m3,声速500m/s,半径60μm,体积分数20%;超声耦合剂密度1000kg/m3,声速1500m/s。Figure 7 shows the (a) real part of the equivalent density, (b) the imaginary part of the equivalent density, and (c) the equivalent elasticity of the hollow hydrogel microspheres in Comparative Example 2 dispersed in the ultrasonic couplant calculated by the multiple scattering model The real part of modulus and the imaginary part of (d) equivalent elastic modulus; among them, the density of hollow hydrogel microspheres is 200kg/m 3 , the speed of sound is 500m/s, the radius is 60μm, and the volume fraction is 20%; the density of ultrasonic couplant is 1000kg/m 3 , the speed of sound is 1500m/s.

具体实施方式Detailed ways

下面结合实施例和附图,对本发明做进一步详细说明。在此,本发明的实施例及其说明用于解释本发明,但并不作为本发明的限定。The present invention will be described in further detail below with reference to the embodiments and the accompanying drawings. Here, the embodiments of the present invention and their descriptions are used to explain the present invention, but are not intended to limit the present invention.

本发明提出的基于米氏共振的用于穿颅超声成像的双负型声学超材料,其散射体多孔聚乙二醇双丙烯酸酯水凝胶微球(多孔水凝胶微球)可采用微流控技术进行制备(如图2所示)。For the double negative acoustic metamaterial based on Mie resonance for transcranial ultrasound imaging proposed in the present invention, its scatterer porous polyethylene glycol diacrylate hydrogel microspheres (porous hydrogel microspheres) can be made of microscopic microspheres. The preparation was performed by fluidic technology (as shown in Figure 2).

多孔聚乙二醇双丙烯酸酯水凝胶微球的具体制备方法如下:1)配制分散相溶液。在棕色玻璃瓶中加入聚乙二醇双丙烯酸酯(PEGDA)、2-羟基-2-甲基-1-苯基-1-丙酮(I-1173、光引发剂)、冰乙酸、磁力搅拌10分钟后再加入去离子水,最后,称量碳酸氢钠(造孔剂)加入上述溶液,搅拌后获得分散相溶液。2)配制连续相溶液。在烧杯中加入二甲基硅油、表面活性剂SPAN80,搅拌至完全溶解,获得连续相溶液。3)组装微流控平台。分别将分散相和连续相溶液吸入2mL针筒,并将针筒分别固定在注射泵上,调整注射泵参数(连续相流速为0.5mL/h,分散相流速为0.05mL/h);将微流控芯片安装在夹具上,芯片入口通过软管与针头连接,出口软管通入收集瓶,在收集瓶上方安装紫外灯(7W-365nm)。4)开启注射泵及紫外灯。等待2~3小时,收集到分散的多孔水凝胶微球的溶液。5)分离出多孔水凝胶微球。离心洗涤,重复3次,获得多孔水凝胶微球。The specific preparation method of the porous polyethylene glycol diacrylate hydrogel microspheres is as follows: 1) Prepare a dispersed phase solution. In a brown glass bottle, add polyethylene glycol diacrylate (PEGDA), 2-hydroxy-2-methyl-1-phenyl-1-propanone (I-1173, photoinitiator), glacial acetic acid, magnetic stirring for 10 After a few minutes, deionized water was added, and finally, sodium bicarbonate (pore-forming agent) was weighed into the above solution, and a dispersed phase solution was obtained after stirring. 2) Prepare a continuous phase solution. Dimethicone oil and surfactant SPAN80 were added to the beaker and stirred until completely dissolved to obtain a continuous phase solution. 3) Assemble the microfluidic platform. Inhale the disperse phase and continuous phase solutions into 2mL syringes, respectively, fix the syringes on the syringe pump, and adjust the parameters of the syringe pump (the flow rate of the continuous phase is 0.5mL/h, and the flow rate of the disperse phase is 0.05mL/h); The flow control chip is installed on the fixture, the chip inlet is connected to the needle through a hose, the outlet hose leads to a collection bottle, and an ultraviolet lamp (7W-365nm) is installed above the collection bottle. 4) Turn on the syringe pump and UV lamp. After waiting for 2-3 hours, the solution of dispersed porous hydrogel microspheres was collected. 5) The porous hydrogel microspheres are separated. Centrifugal washing was repeated 3 times to obtain porous hydrogel microspheres.

基于多重散射模型,可以计算得到上述声学超材料的等效质量密度和等效弹性模量随频率的变化曲线,具体的计算公式如下所示,Based on the multiple scattering model, the curves of the equivalent mass density and equivalent elastic modulus of the above acoustic metamaterials with frequency can be calculated. The specific calculation formulas are as follows:

Figure BDA0002368832240000061
Figure BDA0002368832240000061

Figure BDA0002368832240000062
Figure BDA0002368832240000062

其中,ρ为动态等效质量密度,ρ0为静态时的质量密度,η为散射体多孔水凝胶微球的体积分数,k0为波数,f(0)为单个散射体的前向散射函数,f(π)为单个散射体的后向散射函数,M为动态等效弹性模量,M0为静态时的弹性模量。散射函数f(θ)的计算公式如下所示:where ρ is the dynamic equivalent mass density, ρ 0 is the static mass density, η is the volume fraction of the scatterer porous hydrogel microspheres, k 0 is the wavenumber, and f(0) is the forward scattering of a single scatterer function, f(π) is the backscattering function of a single scatterer, M is the dynamic equivalent elastic modulus, and M 0 is the static elastic modulus. The calculation formula of the scattering function f(θ) is as follows:

Figure BDA0002368832240000063
Figure BDA0002368832240000063

其中,Sn为单个散射体的散射系数,Pn(cosθ)为勒让德多项式。where Sn is the scattering coefficient of a single scatterer, and P n ( cosθ) is the Legendre polynomial.

本发明采用有限元仿真模拟了三种情况下的聚焦超声束声场分布情况,结果如图1所示,图1中的(a)只有水存在、(b)水和颅骨、(c)水、颅骨和双负型声学超材料。超声波经过只有颅骨存在的水介质中时能量大幅降低(如图1中的(b)所示)),且聚焦超声束穿颅后聚焦的位置与只有介质水单独存在时大不相同,说明颅骨对超声束存在严重的畸变和衰减作用,这来源于颅骨与水的阻抗失配造成了声波在颅骨表面被大量反射,以及颅骨对声波能量的耗散。在颅骨前加一层本发明提供的双负型声学超材料(实施例1或实施例2或实施例3中的)时(如图1中的(c)所示)),聚焦超声束穿透颅骨后的能量与颅骨单独存在时相比大幅提高,且聚焦的位置与只有水单独存在时极为接近。上述仿真结果从理论上证明了本发明提出的双负型声学超材料确实能够有效消除颅骨对声波的耗散和畸变作用。The present invention uses finite element simulation to simulate the sound field distribution of the focused ultrasound beam in three cases. The results are shown in Figure 1. In Figure 1, (a) only water exists, (b) water and skull, (c) water, Skull and double negative acoustic metamaterials. When the ultrasonic wave passes through the water medium with only the skull, the energy is greatly reduced (as shown in (b) in Figure 1), and the focused position of the focused ultrasonic beam after passing through the skull is very different from that when only the medium water exists alone, indicating that the skull is There is a serious distortion and attenuation of the ultrasonic beam, which is caused by the impedance mismatch between the skull and the water, which causes the sound waves to be reflected on the surface of the skull, and the dissipation of the sound energy by the skull. When a layer of the double negative acoustic metamaterial provided by the present invention (in Example 1 or Example 2 or Example 3) is added in front of the skull (as shown in (c) in FIG. 1 ), the focused ultrasound beam penetrates The energy after penetrating the skull is greatly increased compared to when the skull alone is present, and the focus is very close to that when only water alone is present. The above simulation results prove theoretically that the double negative acoustic metamaterial proposed by the present invention can effectively eliminate the dissipation and distortion effects of the skull on acoustic waves.

实施例1Example 1

多孔水凝胶微球的密度为500kg/m3,声速为120m/s,半径为50μm;超声耦合剂的密度为900kg/m3,声速为1400m/s;将多孔水凝胶微球均匀分散在超声耦合剂基体中,获得所需的双负型声学超材料,其中多孔水凝胶微球的体积分数为15%。基于多重散射模型计算得到的等效质量密度和等效弹性模量随频率的变化曲线如图3所示,该声学超材料在0.63~0.67MHz频率下同时表现出负等效质量密度和负等效弹性模量。The density of the porous hydrogel microspheres is 500kg/m 3 , the speed of sound is 120m/s, and the radius is 50 μm; the density of the ultrasonic coupling agent is 900kg/m 3 , the speed of sound is 1400m/s; the porous hydrogel microspheres are uniformly dispersed In the ultrasonic couplant matrix, the desired double negative acoustic metamaterial was obtained, in which the volume fraction of porous hydrogel microspheres was 15%. The variation curves of equivalent mass density and equivalent elastic modulus with frequency calculated based on the multiple scattering model are shown in Fig. 3. The acoustic metamaterial exhibits both negative equivalent mass density and negative equivalent mass density at frequencies from 0.63 to 0.67 MHz. Effective elastic modulus.

实施例2Example 2

多孔水凝胶微球的密度为600kg/m3,声速为150m/s,半径为60μm;超声耦合剂的密度为1000kg/m3,声速为1500m/s;将多孔水凝胶微球均匀分散在超声耦合剂基体中,获得所需的双负型声学超材料,其中多孔水凝胶微球的体积分数为20%。基于多重散射模型计算得到的等效质量密度和等效弹性模量随频率的变化曲线如图4所示,该声学超材料在0.67~0.70MHz频率下同时表现出负等效质量密度和负等效弹性模量。The density of the porous hydrogel microspheres is 600kg/m 3 , the speed of sound is 150m/s, and the radius is 60 μm; the density of the ultrasonic coupling agent is 1000kg/m 3 , the speed of sound is 1500m/s; the porous hydrogel microspheres are uniformly dispersed In the ultrasonic couplant matrix, the desired double negative acoustic metamaterial was obtained, in which the volume fraction of porous hydrogel microspheres was 20%. The variation curves of equivalent mass density and equivalent elastic modulus with frequency calculated based on the multiple scattering model are shown in Fig. 4. The acoustic metamaterial exhibits both negative equivalent mass density and negative equivalent mass density at frequencies from 0.67 to 0.70 MHz. Effective elastic modulus.

实施例3Example 3

多孔水凝胶微球的密度为700kg/m3,声速为180m/s,半径为70μm;超声耦合剂的密度为1100kg/m3,声速为1600m/s;将多孔水凝胶微球均匀分散在超声耦合剂基体中,获得所需的双负型声学超材料,其中多孔水凝胶微球的体积分数为25%。基于多重散射模型计算得到的等效质量密度和等效弹性模量随频率的变化曲线如图5所示,该声学超材料在0.68~0.73MHz频率下同时表现出负等效质量密度和负等效弹性模量。The density of the porous hydrogel microspheres is 700kg/m 3 , the speed of sound is 180m/s, and the radius is 70 μm; the density of the ultrasonic coupling agent is 1100kg/m 3 , the speed of sound is 1600m/s; the porous hydrogel microspheres are uniformly dispersed In the ultrasonic couplant matrix, the desired double negative acoustic metamaterial was obtained, in which the volume fraction of porous hydrogel microspheres was 25%. The variation curves of equivalent mass density and equivalent elastic modulus with frequency calculated based on the multiple scattering model are shown in Fig. 5. The acoustic metamaterial exhibits both negative equivalent mass density and negative equivalent mass density at frequencies of 0.68-0.73 MHz. Effective elastic modulus.

对比例1Comparative Example 1

钢珠微球的密度为7900kg/m3,声速为5955m/s,半径为60μm;超声耦合剂的密度为1000kg/m3,声速为1500m/s;将钢珠微球均匀分散在超声耦合剂基体中,获得声学复合材料,其中钢珠微球的体积分数为20%。基于多重散射模型计算得到的等效质量密度和等效弹性模量随频率的变化曲线如图6所示,该声学复合材料0~1MHz内均表现为正等效质量密度和正等效弹性模量。The density of the steel ball microspheres is 7900kg/m 3 , the sound speed is 5955m/s, and the radius is 60 μm; the density of the ultrasonic couplant is 1000kg/m 3 , and the sound speed is 1500m/s; the steel ball microspheres are uniformly dispersed in the matrix of the ultrasonic couplant , an acoustic composite material was obtained, in which the volume fraction of steel ball microspheres was 20%. The variation curves of equivalent mass density and equivalent elastic modulus with frequency calculated based on the multiple scattering model are shown in Fig. 6. The acoustic composite material exhibits positive equivalent mass density and positive equivalent elastic modulus within 0-1 MHz. .

对比例2Comparative Example 2

空心水凝胶微球(空心聚乙二醇双丙烯酸酯水凝胶微球)的密度为200kg/m3,声速为500m/s,半径为60μm;超声耦合剂的密度为1000kg/m3,声速为1500m/s;将空心水凝胶微球均匀分散在超声耦合剂基体中,获得声学复合材料,其中空心水凝胶微球的体积分数为20%。基于多重散射模型计算得到的等效质量密度和等效弹性模量随频率的变化曲线如图7所示,该声学复合材料仅在0.82~1MHz内表现出单一的负等效弹性模量。The density of the hollow hydrogel microspheres (hollow polyethylene glycol diacrylate hydrogel microspheres) is 200kg/m 3 , the sound speed is 500m/s, and the radius is 60 μm; the density of the ultrasonic couplant is 1000kg/m 3 , The speed of sound is 1500m/s; the hollow hydrogel microspheres are uniformly dispersed in the ultrasonic couplant matrix to obtain an acoustic composite material, wherein the volume fraction of the hollow hydrogel microspheres is 20%. The variation curves of equivalent mass density and equivalent elastic modulus with frequency calculated based on the multiple scattering model are shown in Fig. 7. The acoustic composite only exhibits a single negative equivalent elastic modulus within 0.82-1 MHz.

以上所述的具体实施方式对本发明的技术方案和有益效果进行了详细说明,应理解的是以上所述仅为本发明的最优选实施例,并不用于限制本发明,凡在本发明的原则范围内所做的任何修改、补充和等同替换等,均应包含在本发明的保护范围之内。The above-mentioned specific embodiments describe in detail the technical solutions and beneficial effects of the present invention. It should be understood that the above-mentioned embodiments are only the most preferred embodiments of the present invention, and are not intended to limit the present invention. Any modifications, additions and equivalent substitutions made within the scope shall be included within the protection scope of the present invention.

Claims (6)

1. The double-negative-type acoustic metamaterial for transcranial ultrasonic imaging based on Mie resonance is characterized by comprising an ultrasonic couplant serving as a matrix and a scatterer dispersed in the matrix and used for generating the Mie resonance, wherein the scatterer is a porous polyethylene glycol diacrylate hydrogel microsphere.
2. The bipnegative-tone acoustic metamaterial for transcranial ultrasound imaging based on mie resonance according to claim 1, wherein the volume fraction of the porous polyethylene glycol diacrylate hydrogel microspheres in the matrix is 15-25%.
3. The dual-negative-tone acoustic metamaterial for trans-cranial ultrasound imaging based on Mie's resonance in claim 1 or 2, wherein the density of the ultrasonic couplant is 900-1100 kg/m3The sound velocity is 1400-1600 m/s.
4. The double-negative-tone acoustic metamaterial for transcranial ultrasonic imaging based on Mie's resonance in claim 1 or 2, wherein the mass density of the porous polyethylene glycol diacrylate hydrogel microspheres is 500-700 kg/m3The sound velocity is 120-180 m/s.
5. The double-negative-tone acoustic metamaterial for transcranial ultrasonic imaging based on Mie's resonance in claim 1 or 2, wherein the radius of the porous polyethylene glycol diacrylate hydrogel microsphere is 50-70 μm.
6. The biprimary negative acoustic metamaterial for transcranial ultrasound imaging based on mie resonance according to claim 1 or 2, wherein the acoustic metamaterial achieves both negative equivalent mass density and negative equivalent elastic modulus at a frequency range of 0.63-0.73 MHz.
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