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CN110243454B - Experimental system and method of microbubble synergy kinetics based on dual-frequency superimposed ultrasonic pulses in viscoelastic media - Google Patents

Experimental system and method of microbubble synergy kinetics based on dual-frequency superimposed ultrasonic pulses in viscoelastic media Download PDF

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CN110243454B
CN110243454B CN201910610340.9A CN201910610340A CN110243454B CN 110243454 B CN110243454 B CN 110243454B CN 201910610340 A CN201910610340 A CN 201910610340A CN 110243454 B CN110243454 B CN 110243454B
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陆明珠
刘邺晖
李瑞昕
刘妍杉
李玉娇
王轩
耿一喆
万明习
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Abstract

本发明公开一种粘弹媒质中基于双频叠加的微泡增效动力学实验系统及方法,实验方法包括:1)根据水听器测量的焦区声场实际波形,设置KZK方程参数构建微泡非线性激励波形;2)根据生物组织的粘弹性和微泡在可压缩流体中的振动特性构建HIFU增效模型;3)建立基于双频叠加的微泡增效动力学方法;4)结合以上步骤的仿真结果确定HIFU波形相位、声压、频率参数进行热消融或组织毁损实验。本发明充分利用了生物组织内微泡的动力学特性,设计声波波形、相位参数,在焦区引发微泡的最大振动,增强空化效应,提高了HIFU热消融和组织毁损的安全性和效率。

Figure 201910610340

The invention discloses an experimental system and method for microbubble synergy dynamics in viscoelastic medium based on double-frequency superposition. The experimental method includes: 1) according to the actual waveform of the focal area sound field measured by a hydrophone, setting KZK equation parameters to construct microbubbles nonlinear excitation waveform; 2) build a HIFU synergy model based on the viscoelasticity of biological tissues and the vibration characteristics of microbubbles in compressible fluids; 3) establish a dual-frequency superposition-based microbubble synergistic dynamic method; 4) combine the above The simulation results of the steps determine the HIFU waveform phase, sound pressure, and frequency parameters for thermal ablation or tissue damage experiments. The invention makes full use of the dynamic characteristics of microbubbles in biological tissue, designs sound wave waveform and phase parameters, induces the maximum vibration of microbubbles in the focal area, enhances cavitation effect, and improves the safety and efficiency of HIFU thermal ablation and tissue damage .

Figure 201910610340

Description

粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系 统及方法Experimental system of microbubble synergy kinetics based on dual-frequency superimposed ultrasonic pulses in viscoelastic media systems and methods

技术领域technical field

本发明属于超声技术领域,特别涉及一种粘弹媒质中微泡增效动力学实验系统及方法。The invention belongs to the field of ultrasonic technology, and in particular relates to an experimental system and method of microbubble synergy dynamics in a viscoelastic medium.

背景技术Background technique

高强度聚焦超声(High Intensity Focused Ultrasound,HIFU)以其非侵入、强聚焦的特点已经成为治疗超声领域的热点。目前高强度聚焦超声的作用机制有两种:热消融机制和组织毁损机制。传统的HIFU热消融模式主要利用了超声的热效应,从体外聚焦到靶区的高强度超声能量局部地消融掉组织,使靶区组织由于瞬间高温产生凝固性坏死;组织毁损(Histotripsy)模式主要利用HIFU的空化机械效应,将靶区组织粉碎成微米尺寸的碎片。High Intensity Focused Ultrasound (HIFU) has become a hot spot in the field of therapeutic ultrasound because of its non-invasive and strong focusing characteristics. At present, there are two mechanisms of action of high-intensity focused ultrasound: thermal ablation mechanism and tissue destruction mechanism. The traditional HIFU thermal ablation mode mainly uses the thermal effect of ultrasound, and the high-intensity ultrasonic energy focused from the outside to the target area locally ablates the tissue, causing the target tissue to undergo coagulation necrosis due to the instantaneous high temperature; the tissue destruction (Histotripsy) mode mainly uses The cavitational mechanical effect of HIFU smashes the target tissue into micron-sized fragments.

空化效应指液体中的微小气泡,在正负交替的超声波作用下发生的振荡、拉伸、收缩、破裂的动力学过程,被认为是一种最有潜力的提高HIFU效应的机制,因而得到了广泛的研究。Kawabata等学者在离体以及活体实验都发现了在基频上叠加二次谐波会增强单周期内的定向扩散,显著增强空化效应。国际专利WO2,015,138,781 A1,发明人Kuang-Wei Lin,发明名称“Frequency compounding ultrasound pulses for imaging and therapy”中则提出了利用低频(100kHz~1MHz)声波和高频(2~10MHz)声波(非谐波)同时作用于靶组织,控制两个频率的脉冲时延形成单极脉冲进行组织毁损的方法。G.Iernetti在“Enhancementof high-frequency cavitation effects by a low frequency stimulation”UltrasonicsSonochemistry,vol.4,pp.263-268,1997.中研究了使用高频700kHz和低频20kHz超声波来增强空化效应:低频超声波用于在靶组织区域扩增高频超声波在不同空化阶段的气蚀作用。这种KHz作为低频叠加于高频声波的方法存在焦区体积较大,无法精准损伤靶组织和焦区声波幅度较低,无法高效损伤靶组织的缺点。The cavitation effect refers to the dynamic process of oscillation, stretching, shrinkage and rupture of tiny bubbles in the liquid under the action of alternating positive and negative ultrasonic waves. It is considered to be the most potential mechanism to improve the HIFU effect. extensive research. Kawabata and other scholars have found in both in vitro and in vivo experiments that superimposing the second harmonic on the fundamental frequency can enhance the directional diffusion within a single cycle and significantly enhance the cavitation effect. International patent WO2,015,138,781 A1, inventor Kuang-Wei Lin, in the name of the invention "Frequency compounding ultrasound pulses for imaging and therapy" proposes the use of low-frequency (100kHz-1MHz) sound waves and high-frequency (2-10MHz) sound waves (anharmonics). A method of destroying tissue by controlling the pulse delay of two frequencies to form a monopolar pulse by acting on the target tissue at the same time. G. Iernetti, "Enhancement of high-frequency cavitation effects by a low frequency stimulation" Ultrasonics Sonochemistry, vol.4, pp.263-268, 1997. The use of high frequency 700kHz and low frequency 20kHz ultrasound to enhance cavitation effects: low frequency ultrasound It is used to amplify the cavitation effect of high frequency ultrasound in different cavitation stages in the target tissue area. This method of superimposing low frequency on high-frequency sound waves with KHz has the disadvantages of large focal volume, inability to accurately damage the target tissue, and low acoustic wave amplitude in the focal area, which cannot effectively damage the target tissue.

微泡动力学模型有经典的不可压缩流体中的RPNNP模型,但其不能适应可压缩流体,而空化效应发生在生物组织这类可压缩流体中。最新的Zener模型则能较好地模拟生物组织这类可压缩流体的力学特性,更符合组织的实际情况,在微泡动力学模型研究中有了更深的应用。无论是热消融还是组织毁损,微泡的振动与坍塌时释放的能量在其中发挥着作用,因此探究组织中微泡动力学特性助于完善热消融和组织毁损控制方法提高治疗效率。The microbubble dynamics model has the classical RPNNP model in incompressible fluids, but it cannot adapt to compressible fluids, and cavitation effects occur in compressible fluids such as biological tissues. The latest Zener model can better simulate the mechanical properties of compressible fluids such as biological tissues, which is more in line with the actual situation of tissues, and has a deeper application in the study of microbubble dynamics models. Whether it is thermal ablation or tissue damage, the vibration of microbubbles and the energy released when collapsing play a role in it. Therefore, exploring the dynamic characteristics of microbubbles in tissue can help improve thermal ablation and tissue damage control methods and improve treatment efficiency.

现有的热消融和组织毁损方法仍存在以下缺陷:生物组织是一类具有粘弹性的可压缩流体,以RPNNP不可压缩流体中的微泡模型指导HIFU过程的开展存在理论上的不足,目前还没有一种可压缩流体中的粘弹性模型进行仿真指导HIFU过程,并且以前的激励波形没有考虑非线性效应,导致热消融和组织毁损参数设置不准确,单频模式下焦区的空化活动不够剧烈,使得空化阈值过高,所需峰值声压过高,且单焦点体积只有几个mm3The existing thermal ablation and tissue destruction methods still have the following defects: biological tissue is a kind of compressible fluid with viscoelasticity, and there are theoretical deficiencies in the development of HIFU process guided by the microbubble model in the RPNNP incompressible fluid. There is no viscoelastic model in compressible fluids for simulation to guide the HIFU process, and the previous excitation waveforms did not consider nonlinear effects, resulting in inaccurate thermal ablation and tissue damage parameter settings, and insufficient cavitation activity in the focal zone in single-frequency mode. , so that the cavitation threshold is too high, the required peak sound pressure is too high, and the monofocal volume is only a few mm 3 .

发明内容SUMMARY OF THE INVENTION

本发明的目的在于提供一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统及方法,以解决上述技术问题。本发明首先根据光纤水听器测量焦区实际声场非线性波形,确定KZK方程参数设置构建微泡振动激励非线性波形,确保每个频率的声波都能产生非线性畸变,然后根据生物组织的粘弹性以及微泡在可压缩流体中的振动特性,求解Zener模型与Keller-Miksis方程构建微泡增效模型,再建立粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法并进行仿真计算选择合适的组织粘弹性参数和HIFU波形、频率、声压和相位参数,最后结合仿真结果指导实验开展,提高HIFU的安全性、效率,增强有效性。The purpose of the present invention is to provide a microbubble synergy kinetics experimental system and method based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium, so as to solve the above-mentioned technical problems. The invention first measures the nonlinear waveform of the actual sound field in the focal area according to the optical fiber hydrophone, determines the parameter setting of the KZK equation to construct the nonlinear waveform of the microbubble vibration excitation, and ensures that the sound wave of each frequency can generate nonlinear distortion, and then according to the viscosity of the biological tissue Elasticity and vibration characteristics of microbubbles in compressible fluids, solve the Zener model and Keller-Miksis equation to build a microbubble synergy model, and then establish a microbubble synergy dynamics method based on dual-frequency superimposed ultrasonic pulses in viscoelastic media. The simulation calculation selects appropriate tissue viscoelastic parameters and HIFU waveform, frequency, sound pressure and phase parameters, and finally combines the simulation results to guide the experiment to improve the safety, efficiency and effectiveness of HIFU.

HIFU主要作用于超声治疗领域,但本发明不直接涉及人体病变组织的治疗,而是以丙烯酰胺凝胶仿体为介质确定其控制方法,以猪肝脏,肾脏等发病率较高的离体组织器官等介质为研究对象,探索粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法对于提高效率,提高安全性等的效果。HIFU mainly acts on the field of ultrasonic therapy, but the present invention does not directly relate to the treatment of human diseased tissue, but uses acrylamide gel phantom as a medium to determine its control method, and uses pig liver, kidney and other isolated tissues with high incidence. Organs and other media are the research objects to explore the effects of the microbubble synergistic kinetic method based on dual-frequency superimposed ultrasonic pulses in improving efficiency and safety in viscoelastic media.

为了实现上述目的,本发明采用如下技术方案:In order to achieve the above object, the present invention adopts the following technical solutions:

粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统,包括超声激励系统、监控引导系统、声场测量系统和控制系统;An experimental system of microbubble synergy dynamics in viscoelastic medium based on dual-frequency superimposed ultrasonic pulses, including ultrasonic excitation system, monitoring and guidance system, sound field measurement system and control system;

超声激励系统包括:任意波形发生器、射频功率放大器、阻抗匹配网络以及HIFU换能器;Ultrasonic excitation system includes: arbitrary waveform generator, RF power amplifier, impedance matching network and HIFU transducer;

监控引导系统包括光源、高速摄像机、PCD探头和数字超声;The monitoring and guidance system includes light source, high-speed camera, PCD probe and digital ultrasound;

控制系统包括计算机;The control system includes a computer;

任意波形发生器、射频功率放大器、阻抗匹配网络以及HIFU换能器依次连接;Arbitrary waveform generator, RF power amplifier, impedance matching network and HIFU transducer are connected in sequence;

凝胶仿体或者离体样品放置于恒温装置中,HIFU换能器安装于恒温装置上;光源设置于恒温装置外部,用于提供光照;The gel phantom or the isolated sample is placed in a constant temperature device, and the HIFU transducer is installed on the constant temperature device; the light source is set outside the constant temperature device to provide light;

声场测量系统包括光纤水听器和数据采集卡;所述声场测量系统用于通过光纤水听器和数据采集卡配合,检测HIFU换能器基频声波与倍频声波焦区声场压力波形;The sound field measurement system includes a fiber optic hydrophone and a data acquisition card; the sound field measurement system is used to detect the sound field pressure waveform of the HIFU transducer fundamental frequency sound wave and octave sound wave focal zone through the cooperation of the fiber optic hydrophone and the data acquisition card;

计算机连接任意波形发生器、高速摄像机、PCD探头、数字超声和数据采集卡,用于控制意波形发生器发出设定波形,控制高速摄像机和PCD探头采集实验数据。The computer is connected to the arbitrary waveform generator, high-speed camera, PCD probe, digital ultrasound and data acquisition card, which is used to control the arbitrary waveform generator to send out the set waveform, and control the high-speed camera and the PCD probe to collect experimental data.

进一步的,任意波形发生器生成驱动信号,再由功率放大器放大到后经过阻抗匹配网络后驱动HIFU换能器工作,对对凝胶仿体或者离体样品的焦区施加波形;高速摄像机在光源的辅助下对焦区的空化活动进行监测,PCD探头用于接收空化活动中产生的被动空化信号,数字超声用于定位凝胶仿体或离体样品于焦点位置;计算机负责接收来自信号发生器的驱动信号,同步控制高速摄像机进行拍摄。Further, the arbitrary waveform generator generates the driving signal, which is amplified by the power amplifier and then passed through the impedance matching network to drive the HIFU transducer to work, and apply waveform to the focal area of the gel phantom or the isolated sample; The cavitation activity in the focal area is monitored with the aid of the PCD probe. The PCD probe is used to receive the passive cavitation signal generated in the cavitation activity. The digital ultrasound is used to locate the gel phantom or the isolated sample at the focal position; the computer is responsible for receiving the signal from the cavitation. The driving signal of the generator controls the high-speed camera to shoot synchronously.

进一步的,HIFU换能器为环形阵换能器,其基频阵元工作范围为1~3MHz;倍频阵元工作范围为2~10MHz。Further, the HIFU transducer is a ring array transducer, and the working range of the fundamental frequency array element is 1-3 MHz; the working range of the frequency-doubling array element is 2-10 MHz.

进一步的,HIFU换能器中间带孔,用于安装数字超声探头。Further, there is a hole in the middle of the HIFU transducer for installing a digital ultrasound probe.

粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验方法,包括以下步骤:The experimental method of microbubble synergy kinetics based on dual-frequency superimposed ultrasonic pulses in viscoelastic media includes the following steps:

步骤一、构建微泡振动增强激励波形;Step 1. Construct the vibration-enhanced excitation waveform of the microbubble;

1.1)、使用光纤水听器检测HIFU换能器基频声波与倍频声波焦区声场压力波形;1.1), use the fiber optic hydrophone to detect the sound field pressure waveform of the HIFU transducer fundamental frequency sound wave and double frequency sound wave focal area;

1.2)、构建模型用于产生微泡振动激励波形,求解KZK方程得到焦区声场压力仿真波形;1.2), build a model for generating microbubble vibration excitation waveform, and solve the KZK equation to obtain the focal zone sound field pressure simulation waveform;

1.3)、将仿真波形与水听器测量的实际压力波形进行对比,优化模型参数使得仿真波形与实际测量压力波形一致,并将仿真压力波形作为微泡振动的驱动波形条件;1.3), compare the simulated waveform with the actual pressure waveform measured by the hydrophone, optimize the model parameters so that the simulated waveform is consistent with the actual measured pressure waveform, and use the simulated pressure waveform as the driving waveform condition of the microbubble vibration;

步骤二、根据所实验的凝胶仿体或者离体样品的生物组织的粘弹性以及微泡在可压缩流体中的振动特性构建HIFU增效模型;Step 2: Construct a HIFU synergistic model according to the viscoelasticity of the biological tissue of the tested gel phantom or the in vitro sample and the vibration characteristics of the microbubbles in the compressible fluid;

步骤三:建立所实验的凝胶仿体或者离体样品的粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法并进行仿真计算;Step 3: Establish a microbubble synergistic kinetic method based on dual-frequency superimposed ultrasonic pulses in the viscoelastic medium of the gel phantom or the ex vivo sample and carry out simulation calculation;

3.1)、建立单个正弦波激励条件下粘弹媒质中的微泡振动模型,选择组织粘弹性参数并进行仿真;3.1), establish the microbubble vibration model in the viscoelastic medium under the condition of a single sine wave excitation, select the tissue viscoelastic parameters and simulate;

3.2)、建立持续正弦波激励条件下粘弹媒质中的微泡振动模型,选择组织粘弹性参数并进行仿真;3.2), establish the microbubble vibration model in the viscoelastic medium under the condition of continuous sine wave excitation, select tissue viscoelastic parameters and simulate;

步骤四:根据步骤一至三的结果确定任意波形发生器的波形参数:根据步骤一的声场测量结果调整功率放大器的功率直至焦区声压发生非线性畸变,以及根据生物组织内微泡的振动特性调整任意波形发生器的波形频率,控制HIFU换能器按照波形参数对所实验的凝胶仿体或者离体样品进行HIFU热消融或组织毁损实验。Step 4: Determine the waveform parameters of the arbitrary waveform generator according to the results of steps 1 to 3: adjust the power of the power amplifier according to the sound field measurement results of step 1 until nonlinear distortion of the sound pressure in the focal zone occurs, and according to the vibration characteristics of the microbubbles in the biological tissue The waveform frequency of the arbitrary waveform generator is adjusted, and the HIFU transducer is controlled to perform HIFU thermal ablation or tissue damage experiments on the gel phantoms or in vitro samples to be tested according to the waveform parameters.

进一步的,步骤1.2)所构建KZK声场模型为:Further, the KZK sound field model constructed in step 1.2) is:

Figure BDA0002122153220000041
Figure BDA0002122153220000041

其中c0为声速;P为声压;

Figure BDA0002122153220000042
为传播介质的非线性系数;
Figure BDA0002122153220000043
为声波在传播介质中的衰减参数,μ为流体介质中的体积黏性,u′为切边黏性,κ为热传导系数,Δ为拉普拉斯算子,z为轴向距离,t为时间。where c 0 is the speed of sound; P is the sound pressure;
Figure BDA0002122153220000042
is the nonlinear coefficient of the propagation medium;
Figure BDA0002122153220000043
is the attenuation parameter of the sound wave in the propagation medium, μ is the volume viscosity in the fluid medium, u′ is the viscosity of the cutting edge, κ is the thermal conductivity, Δ is the Laplace operator, z is the axial distance, t for time.

进一步的,所构建HIFU增效微泡模型为:Further, the constructed HIFU synergistic microbubble model is:

Figure BDA0002122153220000051
Figure BDA0002122153220000051

Figure BDA0002122153220000052
Figure BDA0002122153220000052

Figure BDA0002122153220000053
Figure BDA0002122153220000053

其中R为微泡的半径;

Figure BDA0002122153220000054
为微泡半径随时间的导数;C0为声速;σ为周围液体表面张力;μ为周围液体的粘滞系数;Pv为周围液体的饱和蒸气压;τ为气体多方指数,为1.4;
Figure BDA0002122153220000055
反应组织弛豫时间,λ为泊松比;
Figure BDA0002122153220000056
反应组织弹性;
Figure BDA0002122153220000057
反应组织表面张力;
Figure BDA0002122153220000058
反应组织粘性。where R is the radius of the microbubble;
Figure BDA0002122153220000054
is the derivative of the microbubble radius with time; C 0 is the speed of sound; σ is the surface tension of the surrounding liquid; μ is the viscosity coefficient of the surrounding liquid; P v is the saturated vapor pressure of the surrounding liquid; τ is the gas polytropic exponent, which is 1.4;
Figure BDA0002122153220000055
Reaction tissue relaxation time, λ is Poisson's ratio;
Figure BDA0002122153220000056
Responsive tissue elasticity;
Figure BDA0002122153220000057
Reactive tissue surface tension;
Figure BDA0002122153220000058
Reactive tissue stickiness.

本发明根据生物组织中的微泡动力学模型以及HIFU高强度聚焦超声导致的非线性效应提出一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统及方法。According to the microbubble dynamics model in biological tissue and the nonlinear effect caused by HIFU high-intensity focused ultrasound, the present invention proposes a microbubble synergistic dynamic experiment system and method based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium.

相对于现有技术,本发明具有以下有益效果:Compared with the prior art, the present invention has the following beneficial effects:

本发明为了克服现有HIFU方法中的不足,提出了一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统及方法;本发明使用光纤水听器对基频与倍频换能器声场进行了测量,保证了声波发生非线性畸变,并充分利用了生物组织这类可压缩流体中的微泡动力学特性,Zener模型比经典的RPNNP模型更接近实际情况,再使用两个叠加的声波使得组织中微泡的振动更剧烈,增强空化效应实现高效热消融和组织毁损。In order to overcome the deficiencies in the existing HIFU method, the present invention proposes a microbubble synergistic dynamic experimental system and method based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium; The sound field of the frequency transducer is measured, which ensures the nonlinear distortion of the sound wave, and makes full use of the dynamic characteristics of microbubbles in compressible fluids such as biological tissues. The Zener model is closer to the actual situation than the classical RPNNP model, and then use The two superimposed acoustic waves make the vibration of the microbubbles in the tissue more intense and enhance the cavitation effect to achieve efficient thermal ablation and tissue damage.

进一步的,本发明采用了双频叠加模式作用于凝胶仿体或离体样品,通过控制基波与谐波幅度与相位在焦区发生干涉,使得负声压峰值增强,更有利于空化;基波与谐波在焦区外不会发生干涉增强,降低了对周围邻近部位的压力,进一步提高了安全性。Further, the present invention adopts the dual-frequency superposition mode to act on the gel phantom or the isolated sample, and by controlling the fundamental wave and the harmonic amplitude and phase to interfere in the focal region, the negative sound pressure peak is enhanced, which is more conducive to cavitation. ; The fundamental wave and harmonics will not interfere and strengthen outside the focal area, which reduces the pressure on the surrounding adjacent parts and further improves the safety.

基于以上两点,本发明便可通过实验进一步的提高HIFU热消融和组织毁损的效率和安全性。Based on the above two points, the present invention can further improve the efficiency and safety of HIFU thermal ablation and tissue damage through experiments.

附图说明Description of drawings

下面结合附图和具体实施方式对本发明做进一步详细说明。The present invention will be further described in detail below with reference to the accompanying drawings and specific embodiments.

图1是本发明实验系统的实现系统框图,1为同步信号控制系统,1为任意波形发生器,2为信号功率放大器,3为阻抗匹配网络,4为光源,5为HIFU换能器,6为凝胶仿体或者离体样品,7为恒温装置,8为高速摄像机,9为被动空化检测(PCD)探头,10为计算机,11为有机玻璃容器。Fig. 1 is the realization system block diagram of the experimental system of the present invention, 1 is the synchronization signal control system, 1 is the arbitrary waveform generator, 2 is the signal power amplifier, 3 is the impedance matching network, 4 is the light source, 5 is the HIFU transducer, 6 7 is a constant temperature device, 8 is a high-speed camera, 9 is a passive cavitation detection (PCD) probe, 10 is a computer, and 11 is a plexiglass container.

图2为本发明采用的光纤水听器FOPH2000搭建的系统示意图。FIG. 2 is a schematic diagram of a system constructed by the optical fiber hydrophone FOPH2000 adopted in the present invention.

图3为本发明采用的HIFU换能器示意图。其中,图3(a)为中间有孔的凹球面环形分裂阵换能器,图3(b)为共焦扇形分裂阵换能器,图3(c)为共焦涡形分裂阵换能器,图3(d)为球壳式相控阵换能器。FIG. 3 is a schematic diagram of the HIFU transducer used in the present invention. Among them, Fig. 3(a) is a concave spherical annular split-array transducer with a hole in the middle, Fig. 3(b) is a confocal sector-shaped split-array transducer, and Fig. 3(c) is a confocal vortex-shaped split-array transducer. Figure 3(d) is a spherical-shell phased array transducer.

图4为本发明方法的流程图。Figure 4 is a flow chart of the method of the present invention.

图5是本发明中采用水听器测量的焦区声场压力波形图和求解KZK方程得到的波形仿真图。5 is a waveform diagram of the sound field pressure in the focal zone measured by a hydrophone in the present invention and a waveform simulation diagram obtained by solving the KZK equation.

图6是不同流体力学参数下生物组织中的微泡振动图。Figure 6 is a graph of the vibration of microbubbles in biological tissue under different hydrodynamic parameters.

图7是控制两个阵元相位差为和135°和60°时的生物组织内微泡振动特性计算。其中,图7(a)为两个阵元相位差为135°时波形叠加曲线示意图;图7(b)为两个阵元相位差为60°时波形叠加曲线示意图;图7(c)为两个阵元相位差为135°时R-t振动曲线示意图;图7(d)为两个阵元相位差为60°时R-t振动曲线示意图。Figure 7 is the calculation of the vibration characteristics of microbubbles in biological tissue when the phase difference between the two array elements is controlled to be 135° and 60°. Among them, Figure 7(a) is a schematic diagram of the waveform superposition curve when the phase difference between the two array elements is 135°; Figure 7(b) is a schematic diagram of the waveform superposition curve when the phase difference between the two array elements is 60°; Figure 7(c) Schematic diagram of the R-t vibration curve when the phase difference between the two array elements is 135°; Figure 7(d) is a schematic diagram of the R-t vibration curve when the phase difference between the two array elements is 60°.

图8是本发明方法在牛血清蛋白丙烯酰胺仿体中实施时采用高速摄像进行监控的典型结果;图8中:(a)~(d)为第一阶段相对较高占空比脉冲作用时的典型结果图,(e)~(h)为第二阶段低占空比脉冲作用时的典型结果图。Figure 8 is a typical result of monitoring by using high-speed camera when the method of the present invention is implemented in the bovine serum albumin acrylamide phantom; in Figure 8: (a) to (d) are relatively high duty cycle pulses in the first stage. The typical result graphs of , (e)~(h) are the typical result graphs when the second stage low duty cycle pulse acts.

图9是本发明方法在离体猪肝脏中应用时的实物解剖图。Figure 9 is an anatomical diagram of the present invention when the method is applied in isolated pig liver.

图10是本发明方法在离体猪肝脏中应用时的H&E染色结果图;图10中:(a)为结束后的损伤边界,(b)(c)为对(a)图像中损伤边界周围图像的放大,(d)为正常组织H&E染色图像。Figure 10 is a diagram of the H&E staining results when the method of the present invention is applied to the isolated pig liver; in Figure 10: (a) is the injury boundary after the end, (b) and (c) are the images around the injury boundary in (a) Magnification of the image, (d) H&E stained image of normal tissue.

图11是本发明方法中任意波形发生器产生的波形图。Fig. 11 is a waveform diagram generated by an arbitrary waveform generator in the method of the present invention.

具体实施方式Detailed ways

下面结合附图和实施例对本发明作详细说明。The present invention will be described in detail below with reference to the accompanying drawings and embodiments.

基于HIFU技术的研究及应用现状,本发明提出了一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统及方法,根据生物组织的粘弹性和微泡在可压缩流体中的振动特性指导HIFU开展并不断优化组织粘弹性参数和波形、相位参数,最后使用两个叠加且具有一定相位差的声波使得组织中微泡的振动更剧烈,增强空化效应提高HIFU的效率。Based on the research and application status of HIFU technology, the present invention proposes a microbubble synergistic dynamic experimental system and method based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium. The vibration characteristics in the HIFU guide the development of HIFU and continuously optimize the tissue viscoelastic parameters, waveform and phase parameters. Finally, two superimposed acoustic waves with a certain phase difference are used to make the vibration of the microbubbles in the tissue more intense, enhancing the cavitation effect and improving the efficiency of HIFU. .

请参阅图1所示,本发明提供一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统,包括超声激励系统、监控引导系统、控制系统和声场测量系统。Referring to FIG. 1 , the present invention provides a microbubble synergy kinetics experimental system based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium, including an ultrasonic excitation system, a monitoring and guidance system, a control system and a sound field measurement system.

超声激励系统主要由以下几个装置组成:任意波形发生器1、射频功率放大器2、阻抗匹配网络3以及HIFU换能器5。The ultrasonic excitation system is mainly composed of the following devices: an arbitrary waveform generator 1 , a radio frequency power amplifier 2 , an impedance matching network 3 and a HIFU transducer 5 .

监控引导系统则主要由光源4,高速摄像机8,被动空化检测探头(PCD探头)9和数字超声。The monitoring and guidance system is mainly composed of a light source 4, a high-speed camera 8, a passive cavitation detection probe (PCD probe) 9 and digital ultrasound.

控制系统则是由计算机10构成。The control system is composed of a computer 10 .

声场测量系统包括光纤水听器FOPH2000和数据采集卡。计算机10连接数据采集卡和光纤水听器FOPH2000。The sound field measurement system includes a fiber optic hydrophone FOPH2000 and a data acquisition card. The computer 10 is connected to the data acquisition card and the optical fiber hydrophone FOPH2000.

任意波形发生器1、射频功率放大器2、阻抗匹配网络3以及HIFU换能器5依次连接。计算机10连接任意波形发生器1的控制端以及高速摄像机8,用于控制意波形发生器1发出特定波形,控制高速摄像机8进行拍摄。凝胶仿体或者离体样品6放置于恒温装置7中,HIFU换能器5、被动空化检测探头(PCD探头)9和数字超声安装于恒温装置7上;被动空化检测探头(PCD探头)9和连接计算机10,用于反馈监测信息;光源4设置于恒温装置7外部,用于提供光照。数字超声用于定位凝胶仿体或离体样品于焦点位置。The arbitrary waveform generator 1 , the radio frequency power amplifier 2 , the impedance matching network 3 and the HIFU transducer 5 are connected in sequence. The computer 10 is connected to the control terminal of the arbitrary waveform generator 1 and the high-speed camera 8, and is used to control the arbitrary waveform generator 1 to emit a specific waveform and to control the high-speed camera 8 to shoot. The gel phantom or the isolated sample 6 is placed in the constant temperature device 7, and the HIFU transducer 5, the passive cavitation detection probe (PCD probe) 9 and the digital ultrasound are installed on the constant temperature device 7; the passive cavitation detection probe (PCD probe) ) 9 and connected to the computer 10 for feedback monitoring information; the light source 4 is arranged outside the constant temperature device 7 for providing illumination. Digital ultrasound is used to locate gel phantoms or ex vivo samples in focus.

发明提供一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统,首先由任意波形发生器1生成需要的驱动信号,再由功率放大器2放大到指定功率后经过阻抗匹配网络3后驱动HIFU换能器5工作。高速摄像机8则在光源4的辅助下对焦区的空化活动进行监测,PCD探头用于接收空化活动中产生的被动空化信号,数字超声系统用于定位凝胶仿体或离体样品于焦点位置。计算机10负责接收来自信号发生器的驱动信号,同步控制高速摄像机进行拍摄,精准控制时序。The invention provides a microbubble synergy dynamics experimental system based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium. First, an arbitrary waveform generator 1 generates a required driving signal, and then a power amplifier 2 amplifies it to a specified power and then undergoes impedance matching. After the network 3, the HIFU transducer 5 is driven to work. The high-speed camera 8 monitors the cavitation activity in the focus area with the aid of the light source 4, the PCD probe is used to receive the passive cavitation signals generated in the cavitation activity, and the digital ultrasound system is used to locate the gel phantom or the isolated sample in the focus position. The computer 10 is responsible for receiving the driving signal from the signal generator, synchronously controlling the high-speed camera to shoot, and precisely controlling the timing.

本发明提供一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验方法,包括以下步骤:The invention provides a microbubble synergistic kinetic experiment method based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium, comprising the following steps:

步骤一:构建微泡振动增强激励波形。Step 1: Construct the vibration-enhanced excitation waveform of the microbubble.

(1)使用光纤水听器检测HIFU换能器5基频声波与倍频声波焦区声场压力波形,测量系统如图2所示,测量前需要先对光纤水听器进行标定,确保水听器的光散射系数和偏散光系数在仪器指定范围内。测量时,先调节三维移动装置使光纤水听器探针在焦点区域以一定步长进行扫描。由换能器驱动单元驱动HIFU换能器发出聚焦超声波,同时触发数据采集卡对焦区声压进行采集,根据采集信号的信噪比和声压幅值移动光纤水听器的光纤探针直至出现最大值。声压计算公式如下:(1) Use the optical fiber hydrophone to detect the sound field pressure waveform of the HIFU transducer 5 fundamental frequency sound wave and double frequency sound wave focal area. The light scattering coefficient and deviated light coefficient of the instrument are within the specified range of the instrument. During measurement, firstly adjust the three-dimensional moving device so that the fiber optic hydrophone probe scans with a certain step size in the focal area. The HIFU transducer is driven by the transducer drive unit to emit focused ultrasonic waves, and at the same time, the data acquisition card is triggered to collect the sound pressure in the focus area, and the fiber optic probe of the fiber optic hydrophone is moved according to the signal-to-noise ratio and sound pressure amplitude of the collected signal until it appears. maximum value. The sound pressure calculation formula is as follows:

Figure BDA0002122153220000081
其中α为光纤水听器的光散射系数;
Figure BDA0002122153220000082
为光纤水听器置于水中测得的光电压值;UB为光纤水听器置于空气中测得的背景噪声光电压值;Ui为采集的测量光电压值。
Figure BDA0002122153220000081
where α is the light scattering coefficient of the fiber optic hydrophone;
Figure BDA0002122153220000082
is the photovoltage value measured by the fiber optic hydrophone placed in water; U B is the background noise photovoltage value measured by the fiber optic hydrophone placed in the air; U i is the collected measured photovoltage value.

得到的结果如图5所示,由于非线性效应,当大振幅的单频声波在介质中传播时,声波波形由于与介质的相互作用逐渐发生畸变,形成冲击波。The obtained results are shown in Figure 5. Due to the nonlinear effect, when a single-frequency sound wave with large amplitude propagates in the medium, the sound wave waveform is gradually distorted due to the interaction with the medium, forming a shock wave.

(2)构建模型用于产生微泡振动激励波形,求解KZK方程得到焦区声场压力仿真波形。(2) Build a model to generate the vibration excitation waveform of the microbubble, and solve the KZK equation to obtain the simulation waveform of the sound field pressure in the focal area.

Figure BDA0002122153220000091
Figure BDA0002122153220000091

其中c0为声速;P为声压;

Figure BDA0002122153220000092
为传播介质的非线性系数;
Figure BDA0002122153220000093
为声波在传播介质中的衰减参数,μ为流体介质中的体积黏性,u′为切边(剪断)黏性,κ为热传导系数,Δ为拉普拉斯算子,z为轴向距离,t为时间。where c 0 is the speed of sound; P is the sound pressure;
Figure BDA0002122153220000092
is the nonlinear coefficient of the propagation medium;
Figure BDA0002122153220000093
is the attenuation parameter of the sound wave in the propagating medium, μ is the volume viscosity in the fluid medium, u′ is the edge-cut (shear) viscosity, κ is the thermal conductivity, Δ⊥ is the Laplace operator, and z is the axial direction distance, t is time.

KZK方程是对Westervelt方程做轴向近似变换,符合实际中的小开口聚焦声源情况。其右边第一项代表声场的衍射效应,第二项代表声波的衰减效应,第三项代表声传播的非线性效应。The KZK equation is an axial approximation transformation of the Westervelt equation, which is in line with the actual situation of a small opening focused sound source. The first term on the right side represents the diffraction effect of the sound field, the second term represents the attenuation effect of the sound wave, and the third term represents the nonlinear effect of the sound propagation.

考虑到在实际应用当中,超声波需要通过耦合介质进入生物体组织,避免声波能量的无益损耗,所以先模拟5cm的水介质,然后按照尽可能真实情况设置组织参数和超声换能器的特征参量。取水介质中的声速c1=1482m/s;密度ρ1=1000kg/m3;非线性参量β1=3.5;组织吸收系数η1=2。取生物组织中的声速c2=1629m/s;密度ρ2=1000kg/m3;非线性参量β1=4.5;组织吸收系数η1=1。换能器的内径R1=1cm;外径R2=2.5cm;聚焦深度d=8cm;中心频率f=1~5MHz;声功率P=40~200W。Considering that in practical applications, ultrasound needs to enter the biological tissue through the coupling medium to avoid the useless loss of acoustic energy, so first simulate a 5cm water medium, and then set the tissue parameters and the characteristic parameters of the ultrasonic transducer according to the real situation as much as possible. The sound velocity c 1 =1482m/s in the water intake medium; the density ρ 1 =1000kg/m 3 ; the nonlinear parameter β 1 =3.5; the tissue absorption coefficient η 1 =2. Take the sound velocity in biological tissue as c 2 =1629m/s; density ρ 2 =1000kg/m 3 ; nonlinear parameter β 1 =4.5; tissue absorption coefficient η 1 =1. The inner diameter of the transducer R 1 =1cm; the outer diameter R 2 =2.5cm; the focal depth d=8cm; the center frequency f=1~5MHz; the sound power P=40~200W.

如图5所示解KZK方程得到的仿真波形与水听器实际测得的声场压力波形一致,说明构建的激励波形能很好地符合实际情况发生了非线性畸变,可以将其作为微泡振动的驱动波形条件。As shown in Figure 5, the simulated waveform obtained by solving the KZK equation is consistent with the sound field pressure waveform actually measured by the hydrophone. drive waveform conditions.

(3)将仿真波形与水听器测量的实际压力波形进行对比,改变波形的声功率和频率参数使得仿真波形与实际测量波形一致,并将仿真压力波形作为微泡振动的驱动波形条件。(3) Compare the simulated waveform with the actual pressure waveform measured by the hydrophone, change the sound power and frequency parameters of the waveform to make the simulated waveform consistent with the actual measured waveform, and use the simulated pressure waveform as the driving waveform condition for microbubble vibration.

步骤二:根据组织的粘弹性以及微泡在可压缩流体中的振动特性构建HIFU增效模型。Step 2: Build a HIFU synergistic model based on the viscoelasticity of the tissue and the vibration characteristics of microbubbles in compressible fluids.

结合Zener力学模型和Keller-Miksis方程,得到以下HIFU增效模型:Combining the Zener mechanics model and the Keller-Miksis equation, the following HIFU synergy model is obtained:

Figure BDA0002122153220000094
Figure BDA0002122153220000094

Figure BDA0002122153220000101
Figure BDA0002122153220000101

Figure BDA0002122153220000102
Figure BDA0002122153220000102

Figure BDA0002122153220000103
Figure BDA0002122153220000103

其中R为微泡的半径;

Figure BDA0002122153220000104
为微泡半径随时间的导数;C0为声速;σ为周围液体表面张力;μ为周围液体的粘滞系数;Pv为周围液体的饱和蒸气压;τ为气体多方指数,为1.4。
Figure BDA0002122153220000105
反应组织弛豫时间,λ为泊松比(λ<0.5),水的泊松比为0.5;
Figure BDA0002122153220000106
反应组织弹性;
Figure BDA0002122153220000107
反应组织表面张力;
Figure BDA0002122153220000108
反应组织粘性。where R is the radius of the microbubble;
Figure BDA0002122153220000104
is the derivative of the microbubble radius with time; C 0 is the speed of sound; σ is the surface tension of the surrounding liquid; μ is the viscosity coefficient of the surrounding liquid; P v is the saturated vapor pressure of the surrounding liquid; τ is the gas polytropic exponent, which is 1.4.
Figure BDA0002122153220000105
Reaction tissue relaxation time, λ is Poisson's ratio (λ<0.5), and Poisson's ratio of water is 0.5;
Figure BDA0002122153220000106
Responsive tissue elasticity;
Figure BDA0002122153220000107
Reactive tissue surface tension;
Figure BDA0002122153220000108
Reactive tissue stickiness.

由于生物组织的弹性模量G在0~10MPa范围内,粘度μ在0.004~0.03Pa.s范围内,因此构建生物组织模型时,仿真参数设定如下:Ca=0.01~5;De=0~1;We=1~20;Re=0~10。不同的生物组织中的各项参数不尽相同,导致微泡在不同生物组织中的振动特性出现差异。Since the elastic modulus G of biological tissue is in the range of 0-10MPa, and the viscosity μ is in the range of 0.004-0.03Pa.s, when constructing the biological tissue model, the simulation parameters are set as follows: Ca=0.01-5; De=0- 1; We=1~20; Re=0~10. Various parameters in different biological tissues are not the same, resulting in different vibration characteristics of microbubbles in different biological tissues.

步骤三:建立粘弹媒质(凝胶仿体或者离体样品(6))中基于双频叠加超声脉冲的微泡增效动力学方法并进行仿真计算。Step 3: Establish a microbubble synergistic kinetic method based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium (gel phantom or in vitro sample (6)) and perform simulation calculation.

(1)由公式(3)、(4)、(5)建立单个正弦波激励条件下粘弹媒质中的微泡振动模型:仿真参数取Ca=0.01~1;De=0~0.5;We=1~10;Re=0~5。(1) The microbubble vibration model in the viscoelastic medium under the excitation of a single sine wave is established by formulas (3), (4) and (5): the simulation parameters are Ca=0.01~1; De=0~0.5; We= 1~10; Re=0~5.

结果如图6所示,生物组织的弹性、粘性、弛豫时间和表面张力都会影响到微泡的振动幅度、平衡半径和破裂过程。所以根据生物组织的粘弹特性改变声波的声压和频率相位等条件可增大微泡在生物组织中的振动幅度,增强空化效应,高效地指导HIFU热消融和组织毁损的开展。The results are shown in Fig. 6. The elasticity, viscosity, relaxation time and surface tension of biological tissue all affect the vibration amplitude, equilibrium radius and rupture process of microbubbles. Therefore, changing the sound pressure and frequency phase of the acoustic wave according to the viscoelastic properties of the biological tissue can increase the vibration amplitude of the microbubbles in the biological tissue, enhance the cavitation effect, and effectively guide the development of HIFU thermal ablation and tissue damage.

(2)建立持续正弦波激励条件下粘弹媒质中的微泡振动模型:在实际的HIFU热消融和组织毁损过程中,微泡处于持续的激励状态下。在双频叠加的条件下,两组超声脉冲具有一定的相位差。仿真参数取Ca=0.01~1;De=0~0.5;We=1~10;Re=0~5。(2) Establish the vibration model of microbubbles in viscoelastic media under the condition of continuous sine wave excitation: in the actual process of HIFU thermal ablation and tissue damage, the microbubbles are in a continuous excitation state. Under the condition of double-frequency superposition, the two groups of ultrasonic pulses have a certain phase difference. The simulation parameters take Ca=0.01-1; De=0-0.5; We=1-10; Re=0-5.

得到的持续激励双频叠加下的微泡振动特性如图7所示,在基频与2倍频模式下,相位差为135°时,两个频率的负压正好叠加在一起,微泡的振动半径达到最大幅值,空化效应得到增强,提高了HIFU热消融和组织毁损的效率。The obtained vibration characteristics of the microbubble under the continuous excitation double-frequency superposition are shown in Figure 7. In the fundamental frequency and the double-frequency mode, when the phase difference is 135°, the negative pressures of the two frequencies are just superimposed together, and the microbubble When the vibration radius reaches the maximum amplitude, the cavitation effect is enhanced, which improves the efficiency of HIFU thermal ablation and tissue damage.

步骤四:结合以上所述增效方法的仿真结果确定波形参数进行HIFU热消融或组织毁损。Step 4: Determine the waveform parameters to perform HIFU thermal ablation or tissue damage in combination with the simulation results of the above-mentioned synergistic methods.

任意波形发生器1发出图11中的波形,经过功率放大器后,通过阻抗匹配网络驱动HIFU换能器,在监控引导系统的监控下对凝胶仿体或离体样品6进行热消融或组织毁损。使用两组超声脉冲驱动HIFU换能器,其中一个任意波形发生器发出的激励脉冲经功率放大之后驱动基频阵元,其工作范围为1~3MHz;另一个任意波形发生器发出的激励脉冲经功率放大之后驱动谐波频率阵元,其工作范围为2~10MHz。脉冲聚焦超声波会产生沸腾气泡以及冲击波等,形成松散的局部结构,而惯性空化以及冲击波等多种机械作用则将损伤内部进一步的均匀化,并形成大量的空化核。两组激励脉冲之间的相位差为135°,在焦区中能使微泡达到最大振动半径,增强空化效应,缩短HIFU热消融和组织毁损所需时间。Arbitrary waveform generator 1 sends out the waveform shown in Figure 11. After passing through the power amplifier, it drives the HIFU transducer through the impedance matching network, and performs thermal ablation or tissue damage on the gel phantom or the isolated sample 6 under the monitoring of the monitoring and guidance system. . Two sets of ultrasonic pulses are used to drive the HIFU transducer. One of the excitation pulses sent by an arbitrary waveform generator is amplified by power to drive the fundamental frequency array element, and its working range is 1-3MHz; the excitation pulses sent by the other arbitrary waveform generator are After power amplification, the harmonic frequency array element is driven, and its working range is 2-10MHz. Pulse focused ultrasound will generate boiling bubbles and shock waves to form loose local structures, while inertial cavitation and shock waves and other mechanical effects will further homogenize the damage and form a large number of cavitation nuclei. The phase difference between the two sets of excitation pulses is 135°, which can make the microbubbles reach the maximum vibration radius in the focal zone, enhance the cavitation effect, and shorten the time required for HIFU thermal ablation and tissue damage.

当实验对象为凝胶仿体时,用高速摄像观察损伤形成的过程和最终形态。When the experimental object is a gel phantom, the process and final shape of the damage formation are observed by high-speed videography.

当实验对象为离体猪肾脏时,要切开观察损伤形态,并通过染色来观察细胞形态的变化。When the experimental object is an isolated pig kidney, the damage morphology should be observed by incision, and the changes of cell morphology should be observed by staining.

附图4为本发明的流程图,首先根据水听器测量得到的基频与倍频声波焦区实际声场波形,确定KZK方程参数设置构建增强微泡振动激励波形,然后根据组织的粘弹性以及微泡在可压缩流体中的振动特性,求解Keller-Miksis方程构建微泡增效模型,再建立粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法并进行仿真计算选取合适的组织粘弹性参数和HIFU波形、相位参数,最后结合仿真结果指导实验开展并不断优化参数。Accompanying drawing 4 is the flow chart of the present invention, first according to the fundamental frequency that the hydrophone measures and obtains the actual sound field waveform of the frequency-octave sound wave focal area, determine the KZK equation parameter setting to construct the enhanced microbubble vibration excitation waveform, then according to the viscoelasticity of the tissue and Based on the vibration characteristics of microbubbles in compressible fluids, the Keller-Miksis equation was solved to build a microbubble synergy model, and then a microbubble synergy dynamics method based on dual-frequency superimposed ultrasonic pulses in viscoelastic media was established and simulated to select the appropriate model. Tissue viscoelastic parameters, HIFU waveform and phase parameters, and finally combined with the simulation results to guide the experiment and continuously optimize the parameters.

附图5为水听器测量的基频声波与倍频声波焦区声场波形和解KZK方程得到的焦区声场仿真波形。如图5(a)、图4(c)为水听器测量到的焦区声场实际波形,高强度声波在传播过程中会发生非线性效应,由标准的正弦波畸变成冲击波,而冲击波的形成对空化效应是有利的。图5(b)、图5(d)则是求解KZK方程得到的焦区声场仿真波形。通过两者对比,可以看到仿真波形和实际波形符合的很好,将其作为激励波形。FIG. 5 is the focal area sound field waveforms of fundamental frequency sound wave and double frequency sound wave measured by the hydrophone and the focal area sound field simulation waveform obtained by solving the KZK equation. Figures 5(a) and 4(c) are the actual waveforms of the focal area sound field measured by the hydrophone. High-intensity sound waves will have nonlinear effects during the propagation process, and the standard sine waves will be distorted into shock waves. The formation is favorable for the cavitation effect. Figures 5(b) and 5(d) are the simulation waveforms of the focal area sound field obtained by solving the KZK equation. By comparing the two, it can be seen that the simulated waveform is in good agreement with the actual waveform, and it is used as the excitation waveform.

附图6为生物组织不同流体力学参数下的微泡振动仿真图。如图6所示,可以发现,在生物组织内,微泡最终的平衡半径随着Ca数值减小(弹性减小)而增大,震荡的幅度随之减小,这是由于减小的弹性增大了阻尼,限制了微泡的震荡,De(弛豫时间)取值的增大,微泡脉动的平衡半径保持恒定,在低弹性介质中(低Ca取值),De的取值(弛豫时间)对微泡的震荡特性起着主要作用,支配着阻尼的大小。而在高弹性介质中(高Ca取值),Re的取值(粘性)对微泡的脉动特性起着主要作用。随着压强的增大,微泡脉动的幅度和频率都随之增大(即振动的又快又剧烈);达到平衡时所用时间减少。6 is a simulation diagram of microbubble vibration under different hydrodynamic parameters of biological tissue. As shown in Fig. 6, it can be found that in biological tissue, the final equilibrium radius of microbubbles increases with decreasing Ca value (reduced elasticity), and the amplitude of oscillation decreases, which is due to the decreased elasticity The damping is increased and the oscillation of the microbubble is limited. The value of De (relaxation time) increases, and the equilibrium radius of the microbubble pulsation remains constant. In a low elastic medium (low Ca value), the value of De ( The relaxation time) plays a major role in the oscillation characteristics of the microbubbles and dominates the magnitude of the damping. In highly elastic media (high Ca value), the value of Re (viscosity) plays a major role in the pulsatile properties of microbubbles. As the pressure increases, the amplitude and frequency of the microbubble pulsation increase (ie, the vibration is fast and intense); the time taken to reach equilibrium decreases.

附图7为基频阵元和倍频阵元相位差为135°和60°时的微泡振动仿真图。当基频与倍频的相位差为135°时,两个频率的负压正好叠加在一起,达到最大幅值,此时微泡振动的最大半径也达到最大,空化效应得到增强,大大提高了HIFU的效率。当相位差为60°时,微泡振动的最大半径减小,出现明显的谐振。FIG. 7 is a simulation diagram of the microbubble vibration when the phase difference between the fundamental frequency array element and the frequency-doubling array element is 135° and 60°. When the phase difference between the fundamental frequency and the doubling frequency is 135°, the negative pressures of the two frequencies are superimposed together and reach the maximum amplitude. At this time, the maximum radius of the microbubble vibration also reaches the maximum, and the cavitation effect is enhanced, greatly improving the the efficiency of HIFU. When the phase difference is 60°, the maximum radius of the microbubble vibration decreases, and obvious resonance occurs.

实施例1:Example 1:

1)制备质量分数为7%的牛血清蛋白(BSA)聚丙烯酰胺凝胶仿体,并加入牛血清蛋白作为温度变化指示剂。凝胶仿体的密度为1.06g/cm3,成品凝胶仿体中声速为1477±5m/s,声衰减系数为0.42±0.01dB/cm。1) Prepare a bovine serum albumin (BSA) polyacrylamide gel replica with a mass fraction of 7%, and add bovine serum albumin as a temperature change indicator. The density of the gel phantom is 1.06g/cm 3 , the sound velocity in the finished gel phantom is 1477±5m/s, and the sound attenuation coefficient is 0.42±0.01dB/cm.

2)将环形HIFU换能器5,以及B超探头等如图1所示进行放置与固定,向反应容器中注入适量的除气水,并打开恒温装置7。开启超声成像设备,根据图像引导调节凝胶仿体中需要损伤的点至换能器的焦点处。2) Place and fix the annular HIFU transducer 5 and the B-ultrasound probe as shown in FIG. 1 , inject an appropriate amount of degassed water into the reaction vessel, and open the thermostat 7 . Turn on the ultrasound imaging equipment and adjust the point to be damaged in the gel phantom to the focal point of the transducer according to the image guidance.

3)按照图11编写任意波形发生器所要产生的信号波形。3) Write the signal waveform to be generated by the arbitrary waveform generator according to Figure 11.

4)通过计算机10控制信号激励模块和监控引导模块的时序,使得对凝胶仿体或离体样品的毁损和监控同时触发。4) The timing sequence of the signal excitation module and the monitoring and guiding module is controlled by the computer 10, so that the damage and monitoring of the gel phantom or the isolated sample are triggered at the same time.

分析结果:Analysis results:

如图8所示,在焦区中心首次出现了沸腾气泡的时间为1.29s,时间比1.06MHz单频结果6.67s首次出现沸腾气泡的速度提升了417.05%,如图8(b)所示轴向随机分布的微泡向两端聚集、融合形成尺寸更大的微泡,图8(c)、图8(d)表明焦区出现了更多更大的沸腾气泡,损伤的尺寸也逐渐扩大,该阶段使用较高占空比脉冲,主要利用HIFU热效应产生沸腾气泡,沸腾气泡破裂产生更多的空化核;空化泡破裂后产生机械效应粉碎靶区,图8(e)~(h)表明随着时间的延长,损伤的体积向远离换能器一端扩大,微泡在辐射力的作用下向远离换能器一端游动,说明损伤内部已经完全液化,形成一个梭状的空腔。As shown in Fig. 8, the time for the first appearance of boiling bubbles in the center of the focal zone was 1.29s, which was 417.05% faster than the first appearance of boiling bubbles in the 1.06MHz single frequency result of 6.67s, as shown in Fig. 8(b). The randomly distributed microbubbles aggregate and fuse to form larger-sized microbubbles. Figure 8(c) and Figure 8(d) show that more and larger boiling bubbles appear in the focal area, and the size of the damage gradually expands. , this stage uses a higher duty cycle pulse, mainly using the HIFU thermal effect to generate boiling bubbles, and the boiling bubbles burst to generate more cavitation nuclei; after the cavitation bubbles burst, a mechanical effect occurs to smash the target area, Figure 8(e)~(h ) shows that with the extension of time, the damage volume expands towards the end away from the transducer, and the microbubbles swim towards the end away from the transducer under the action of radiation force, indicating that the interior of the injury has been completely liquefied, forming a fusiform cavity .

实施例2:Example 2:

1)制备丙烯酰胺仿体液。选取新鲜的猪肾脏,切成5mm×3mm×30mm的尺寸,并将其固定在仿体液中,在常温下进行凝固。1) Preparation of acrylamide mimic body fluid. Select fresh pig kidneys, cut them into a size of 5mm×3mm×30mm, fix them in imitation body fluid, and coagulate them at room temperature.

2)将环形阵HIFU换能器5,以及B超探头等如图1进行固定,向反应容器中注入适量的除气水,并打开恒温装置7。开启超声成像设备,根据图像引导调节猪肾脏的中心位置至换能器的焦点处。2) Fix the annular array HIFU transducer 5 and the B-ultrasound probe as shown in Figure 1, inject an appropriate amount of degassed water into the reaction vessel, and open the thermostat 7. Turn on the ultrasound imaging equipment and adjust the center position of the porcine kidney to the focus of the transducer according to the image guidance.

3)按照图11编写任意波形发生器所要产生的信号。在整个过程中,声功率均被设置为240W。3) Write the signal to be generated by the arbitrary waveform generator according to Figure 11. Throughout the process, the sound power was set to 240W.

4)将同步信号控制系统中的任意波形发生器的通道1与超声激励系统相连,通道2与引导监控系统相连。开启各个设备,手动触发同步信号控制系统。通道1连接超声激励系统中的任意波形发生器的外部触发端,触发超声激励系统中发出的信号经过射频功率放大器,阻抗匹配网络并驱动HIFU换能器。通道2则出发高速摄像设备进行实时监控。4) Connect channel 1 of the arbitrary waveform generator in the synchronization signal control system to the ultrasonic excitation system, and channel 2 to the guidance monitoring system. Turn on each device and manually trigger the synchronization signal control system. Channel 1 is connected to the external trigger terminal of the arbitrary waveform generator in the ultrasonic excitation system, and the signal sent in the trigger ultrasonic excitation system passes through the RF power amplifier, the impedance matching network and drives the HIFU transducer. Channel 2 starts high-speed camera equipment for real-time monitoring.

5)当HIFU过程结束后先通过B超设备对损伤进行观察,然后将猪肾脏取出,剖开后再仔细分析损毁情况。对损毁的猪肾脏进行H&E染色,利用高倍显微镜观察其组织学结果。5) When the HIFU process is over, first observe the damage through B-ultrasound equipment, then take out the pig kidney, cut it open, and then analyze the damage carefully. The damaged porcine kidneys were stained with H&E, and the histological results were observed under a high-power microscope.

分析结果:Analysis results:

如图9所示,实际的损伤体积与凝胶仿体实验中所观察到的损伤体积近似。在猪肾脏组织中形成的损伤边界光滑、清晰无明显白色热损伤,图10(a)显示,损伤区域组织和正常区域组织间出现了明显的边界,图10(b)和图10(c)显示,将边界放大后,可以明显看出:边界内部的损伤区域被完全均匀化,边界外部的正常区域细胞结构保持完整,说明粘弹媒质基于双频叠加超声脉冲的微泡增效动力学方法效果优异。另外,我们剖开离体组织查看内部损伤时可以看到损伤内部已经被完全乳化,流动性增强,变成了可以直接被周围组直接吸收的液体。As shown in Figure 9, the actual damage volume is similar to that observed in the gel phantom experiments. The lesion boundary formed in pig kidney tissue is smooth and clear without obvious white thermal damage. Figure 10(a) shows that there is a clear boundary between the damaged area tissue and the normal area tissue, Figure 10(b) and Figure 10(c) After zooming in on the boundary, it can be clearly seen that the damaged area inside the boundary is completely homogenized, and the cell structure of the normal area outside the boundary remains intact. The effect is excellent. In addition, when we dissect the ex vivo tissue to look at the internal injury, we can see that the inside of the injury has been completely emulsified, the fluidity has been enhanced, and it has become a liquid that can be directly absorbed by the surrounding group.

由技术常识可知,本发明可以通过其它的不脱离其精神实质或必要特征的实施方案来实现。因此,上述公开的实施方案,就各方面而言,都只是举例说明,并不是仅有的。所有在本发明范围内或在等同于本发明的范围内的改变均被本发明包含。It is known from the technical common sense that the present invention can be realized by other embodiments without departing from its spirit or essential characteristics. Accordingly, the above-disclosed embodiments are, in all respects, illustrative and not exclusive. All changes within the scope of the present invention or within the scope equivalent to the present invention are encompassed by the present invention.

Claims (6)

1.粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验方法,其特征在于,基于一种粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统;所述粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学实验系统,包括超声激励系统、监控引导系统、声场测量系统和控制系统;超声激励系统包括:任意波形发生器(1)、射频功率放大器(2)、阻抗匹配网络(3)以及HIFU换能器(5);监控引导系统包括光源(4)、高速摄像机(8)、PCD探头(9)和数字超声;控制系统包括计算机(10);任意波形发生器(1)、射频功率放大器(2)、阻抗匹配网络(3)以及HIFU换能器(5)依次连接;凝胶仿体或者离体样品(6)放置于恒温装置(7)中,HIFU换能器(5)安装于恒温装置(7)上;光源(4)设置于恒温装置(7)外部,用于提供光照;声场测量系统包括光纤水听器和数据采集卡;所述声场测量系统用于通过光纤水听器和数据采集卡配合,检测HIFU换能器(5)基频声波与倍频声波焦区声场压力波形;计算机(10)连接任意波形发生器(1)、高速摄像机(8)、PCD探头(9)、数字超声和数据采集卡,用于控制意波形发生器(1)发出设定波形,控制高速摄像机(8)和PCD探头(9)采集实验数据;1. the microbubble synergy kinetics experimental method based on dual-frequency superimposed ultrasonic pulses in viscoelastic medium, is characterized in that, based on the microbubble synergistic kinetics experimental system based on dual-frequency superimposed ultrasonic pulses in a viscoelastic medium; The microbubble synergistic kinetics experimental system based on dual-frequency superimposed ultrasonic pulses in the viscoelastic medium includes an ultrasonic excitation system, a monitoring and guidance system, a sound field measurement system and a control system; the ultrasonic excitation system includes: an arbitrary waveform generator (1), A radio frequency power amplifier (2), an impedance matching network (3) and a HIFU transducer (5); the monitoring and guidance system includes a light source (4), a high-speed camera (8), a PCD probe (9) and a digital ultrasound; the control system includes a computer (10); the arbitrary waveform generator (1), the radio frequency power amplifier (2), the impedance matching network (3) and the HIFU transducer (5) are connected in sequence; the gel phantom or the isolated sample (6) is placed at a constant temperature In the device (7), the HIFU transducer (5) is installed on the constant temperature device (7); the light source (4) is arranged outside the constant temperature device (7) for providing illumination; the sound field measurement system includes an optical fiber hydrophone and a data acquisition card; the sound field measurement system is used to detect the sound field pressure waveform of the HIFU transducer (5) the fundamental frequency sound wave and the multiplied frequency sound wave focal zone through the cooperation of the optical fiber hydrophone and the data acquisition card; the computer (10) is connected to an arbitrary waveform to generate device (1), high-speed camera (8), PCD probe (9), digital ultrasound and data acquisition card, used to control the waveform generator (1) to send out the set waveform, control the high-speed camera (8) and the PCD probe (9) ) collect experimental data; 所述微泡增效动力学实验方法包括以下步骤:The microbubble synergy kinetics experimental method comprises the following steps: 步骤一、构建微泡振动增强激励波形;Step 1. Construct the vibration-enhanced excitation waveform of the microbubble; 1.1)、使用光纤水听器检测HIFU换能器基频声波与倍频声波焦区声场压力波形;1.1), use the fiber optic hydrophone to detect the sound field pressure waveform of the HIFU transducer fundamental frequency sound wave and double frequency sound wave focal zone; 1.2)、构建模型用于产生微泡振动激励波形,求解KZK方程得到焦区声场压力仿真波形;1.2), build a model for generating microbubble vibration excitation waveform, and solve the KZK equation to obtain the focal zone sound field pressure simulation waveform; 1.3)、将仿真波形与水听器测量的实际压力波形进行对比,优化模型参数使得仿真波形与实际测量压力波形一致,并将仿真压力波形作为微泡振动的驱动波形条件;1.3), compare the simulated waveform with the actual pressure waveform measured by the hydrophone, optimize the model parameters so that the simulated waveform is consistent with the actual measured pressure waveform, and use the simulated pressure waveform as the driving waveform condition of the microbubble vibration; 步骤二、根据所实验的凝胶仿体或者离体样品(6)的生物组织的粘弹性以及微泡在可压缩流体中的振动特性构建HIFU增效模型;Step 2, constructing a HIFU synergistic model according to the viscoelasticity of the biological tissue of the tested gel phantom or the in vitro sample (6) and the vibration characteristics of the microbubbles in the compressible fluid; 步骤三:建立所实验的凝胶仿体或者离体样品(6)的粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法并进行仿真计算;Step 3: establish a microbubble synergistic kinetic method based on dual-frequency superimposed ultrasonic pulses in the viscoelastic medium of the tested gel phantom or the in vitro sample (6), and perform simulation calculation; 3.1)、建立单个正弦波激励条件下粘弹媒质中的微泡振动模型,选择组织粘弹性参数并进行仿真;3.1), establish the microbubble vibration model in the viscoelastic medium under the condition of a single sine wave excitation, select the tissue viscoelastic parameters and simulate; 3.2)、建立持续正弦波激励条件下粘弹媒质中的微泡振动模型,选择组织粘弹性参数并进行仿真;3.2), establish the microbubble vibration model in the viscoelastic medium under the condition of continuous sine wave excitation, select tissue viscoelastic parameters and simulate; 步骤四:根据步骤一至三的结果确定任意波形发生器(1)的波形参数,控制HIFU换能器(5)按照波形参数对所实验的凝胶仿体或者离体样品(6)进行HIFU热消融或组织毁损实验。Step 4: Determine the waveform parameters of the arbitrary waveform generator (1) according to the results of steps 1 to 3, and control the HIFU transducer (5) to perform HIFU heating on the gel phantom or in vitro sample (6) to be tested according to the waveform parameters. Ablation or tissue destruction experiments. 2.根据权利要求1所述的粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法,其特征在于,步骤1.2)所构建模型为:2. in the viscoelastic medium according to claim 1, the microbubble synergy kinetics method based on dual-frequency superimposed ultrasonic pulse is characterized in that, step 1.2) built model is:
Figure FDA0002422015260000021
Figure FDA0002422015260000021
其中c0为声速;P为声压;
Figure FDA0002422015260000022
为传播介质的非线性系数;
Figure FDA0002422015260000023
为声波在传播介质中的衰减参数,μ为流体介质中的体积黏性,u′为切边黏性,κ为热传导系数,Δ为拉普拉斯算子,z为轴向距离,t为时间。
where c 0 is the speed of sound; P is the sound pressure;
Figure FDA0002422015260000022
is the nonlinear coefficient of the propagation medium;
Figure FDA0002422015260000023
is the attenuation parameter of the sound wave in the propagation medium, μ is the volume viscosity in the fluid medium, u′ is the viscosity of the cutting edge, κ is the thermal conductivity, Δ is the Laplace operator, z is the axial distance, t for time.
3.根据权利要求1所述的粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法,其特征在于,所构建HIFU增效模型为:3. in the viscoelastic medium according to claim 1, based on the microbubble synergistic dynamics method of double-frequency superposition ultrasonic pulse, it is characterized in that, the built HIFU synergy model is:
Figure FDA0002422015260000024
Figure FDA0002422015260000024
Figure FDA0002422015260000025
Figure FDA0002422015260000025
Figure FDA0002422015260000026
Figure FDA0002422015260000026
其中R为微泡的半径;
Figure FDA0002422015260000027
为微泡半径随时间的导数;C0为声速;σ为周围液体表面张力;μ为周围液体的粘滞系数;Pv为周围液体的饱和蒸气压;τ为气体多方指数,为1.4;
Figure FDA0002422015260000028
反应组织弛豫时间,λ为泊松比;
Figure FDA0002422015260000029
反应组织弹性;
Figure FDA00024220152600000210
反应组织表面张力;
Figure FDA0002422015260000031
反应组织粘性。
where R is the radius of the microbubble;
Figure FDA0002422015260000027
is the derivative of the microbubble radius with time; C 0 is the speed of sound; σ is the surface tension of the surrounding liquid; μ is the viscosity coefficient of the surrounding liquid; P v is the saturated vapor pressure of the surrounding liquid; τ is the gas polytropic exponent, which is 1.4;
Figure FDA0002422015260000028
Reaction tissue relaxation time, λ is Poisson's ratio;
Figure FDA0002422015260000029
Responsive tissue elasticity;
Figure FDA00024220152600000210
Reactive tissue surface tension;
Figure FDA0002422015260000031
Reactive tissue stickiness.
4.根据权利要求1所述的粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法,其特征在于,任意波形发生器(1)生成驱动信号,再由功率放大器(2)放大到后经过阻抗匹配网络(3)后驱动HIFU换能器(5)工作,对对凝胶仿体或者离体样品(6)的焦区施加波形;高速摄像机(8)在光源(4)的辅助下对焦区的空化活动进行监测,PCD探头(9)用于接收空化活动中产生的被动空化信号,数字超声用于定位凝胶仿体或离体样品于焦点位置;计算机(10)负责接收来自信号发生器的驱动信号,同步控制高速摄像机进行拍摄。4. The microbubble synergy dynamics method based on dual-frequency superimposed ultrasonic pulses in the viscoelastic medium according to claim 1, is characterized in that, the arbitrary waveform generator (1) generates a driving signal, and then the power amplifier (2) After zooming in, the HIFU transducer (5) is driven to work after passing through the impedance matching network (3), and a waveform is applied to the focal area of the gel phantom or the isolated sample (6). The cavitation activity in the focal area is monitored with the aid of the PCD probe (9) to receive the passive cavitation signal generated in the cavitation activity, and the digital ultrasound is used to locate the gel phantom or the isolated sample at the focal position; the computer ( 10) Responsible for receiving the driving signal from the signal generator, and synchronously controlling the high-speed camera for shooting. 5.根据权利要求1所述的粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法,其特征在于,HIFU换能器(5)为环形阵换能器,其基频阵元工作范围为1~3MHz;倍频阵元工作范围为2~10MHz。5. in the viscoelastic medium according to claim 1, the microbubble synergistic dynamics method based on dual-frequency superimposed ultrasonic pulse is characterized in that, the HIFU transducer (5) is an annular array transducer, and its fundamental frequency array The working range of the element is 1~3MHz; the working range of the frequency doubling array element is 2~10MHz. 6.根据权利要求1所述的粘弹媒质中基于双频叠加超声脉冲的微泡增效动力学方法,其特征在于,HIFU换能器中间带孔,用于安装数字超声探头。6 . The microbubble synergy kinetics method based on dual-frequency superimposed ultrasonic pulses in the viscoelastic medium according to claim 1 , wherein the HIFU transducer has a hole in the middle for installing a digital ultrasonic probe. 7 .
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US12005130B2 (en) 2019-10-16 2024-06-11 Agitated Solutions Inc. Generating microbubbles for bubble studies
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US11191888B1 (en) 2020-05-18 2021-12-07 Agitated Solutions Inc. Syringe-based microbubble generator
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CN113129659B (en) * 2021-04-28 2022-10-04 郭山鹰 Synchronous teaching device and system
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CN114947739B (en) * 2022-04-18 2024-06-21 重庆邮电大学 Dual-frequency microwave induced thermoacoustic imaging system and method

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5601086A (en) * 1995-05-12 1997-02-11 The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration Beat frequency ultrasonic microsphere contrast agent detection system
CN101623203A (en) * 2009-08-07 2010-01-13 西安交通大学 Multi-mode multi-parameter synchronous detection imaging monitoring system in transient physical process and monitoring method
CN103028200A (en) * 2011-10-09 2013-04-10 北京汇福康医疗技术有限公司 Ultrasound therapy method and ultrasound therapy device
CN103028199A (en) * 2011-10-09 2013-04-10 北京汇福康医疗技术有限公司 Monitoring method and monitoring device of ultrasound energy converter sound filed
CN104225810A (en) * 2014-09-09 2014-12-24 西安交通大学 Ultrasonic mechanical damage and thermal coagulation device and method based on double-frequency con-focal ultrasonic time-sharing excitation
CN106730424A (en) * 2016-12-19 2017-05-31 西安交通大学 The microsecond pulse ultrasonic tissue of confocal harmonic superposition hundred damages mode control method
CN107789029A (en) * 2017-11-21 2018-03-13 青岛理工大学 Electrostatic atomization ultrasonic-assisted biological bone low-damage controllable grinding process and device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8257338B2 (en) * 2006-10-27 2012-09-04 Artenga, Inc. Medical microbubble generation
CN103776524B (en) * 2014-02-21 2016-02-10 南京大学 A kind of method measuring strong focusing ultrasound non-linear sound-filed simulation

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5601086A (en) * 1995-05-12 1997-02-11 The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration Beat frequency ultrasonic microsphere contrast agent detection system
CN101623203A (en) * 2009-08-07 2010-01-13 西安交通大学 Multi-mode multi-parameter synchronous detection imaging monitoring system in transient physical process and monitoring method
CN103028200A (en) * 2011-10-09 2013-04-10 北京汇福康医疗技术有限公司 Ultrasound therapy method and ultrasound therapy device
CN103028199A (en) * 2011-10-09 2013-04-10 北京汇福康医疗技术有限公司 Monitoring method and monitoring device of ultrasound energy converter sound filed
CN104225810A (en) * 2014-09-09 2014-12-24 西安交通大学 Ultrasonic mechanical damage and thermal coagulation device and method based on double-frequency con-focal ultrasonic time-sharing excitation
CN106730424A (en) * 2016-12-19 2017-05-31 西安交通大学 The microsecond pulse ultrasonic tissue of confocal harmonic superposition hundred damages mode control method
CN107789029A (en) * 2017-11-21 2018-03-13 青岛理工大学 Electrostatic atomization ultrasonic-assisted biological bone low-damage controllable grinding process and device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
基于NaKagami统计参量的活体微波热消融超声监控成像研究;吴珊 等;《生物医学工程学杂志》;20190630;第36卷(第3期);第371-378页 *

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