CN118614986A - Multi-head shock wave electrode structure and shock wave balloon catheter - Google Patents
Multi-head shock wave electrode structure and shock wave balloon catheter Download PDFInfo
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Abstract
本发明提供了一种多头冲击波电极结构及冲击波球囊导管。所述多头冲击波电极结构包括至少两个放电单元;每个放电单元都包括间隔设置且延伸方向相同的一个发射电极及一个对应的中间电极,该发射电极一一对应地间隔套设于该中间电极内;所有的中间电极相互电气连接;当所有中间电极的放电端面和所有发射电极的放电端面均位于导电流体内且在任意两个放电单元的发射电极之间形成电势差时,这两个放电单元的发射电极的放电端面与对应的中间电极的放电端面之间同时引发冲击波。所述冲击波球囊导管包括所述多头冲击波电极结构。本发明在实现单次有效放电击穿形成较大冲击波能量的同时,解决了机械冲击力的破坏问题,并具有较长的使用寿命。
The present invention provides a multi-head shock wave electrode structure and a shock wave balloon catheter. The multi-head shock wave electrode structure includes at least two discharge units; each discharge unit includes an emitter electrode and a corresponding intermediate electrode that are arranged at intervals and have the same extension direction, and the emitter electrodes are arranged in the intermediate electrode in an interval-to-one correspondence; all the intermediate electrodes are electrically connected to each other; when the discharge end faces of all the intermediate electrodes and the discharge end faces of all the emitter electrodes are located in a conductive fluid and a potential difference is formed between the emitter electrodes of any two discharge units, shock waves are simultaneously triggered between the discharge end faces of the emitter electrodes of the two discharge units and the discharge end faces of the corresponding intermediate electrodes. The shock wave balloon catheter includes the multi-head shock wave electrode structure. The present invention solves the problem of damage caused by mechanical impact force while achieving a single effective discharge breakdown to form a large shock wave energy, and has a long service life.
Description
技术领域Technical Field
本发明涉及介入类医疗器械技术领域,具体涉及一种多头冲击波电极结构及冲击波球囊导管。The present invention relates to the technical field of interventional medical devices, and in particular to a multi-head shock wave electrode structure and a shock wave balloon catheter.
背景技术Background Art
液电式冲击波产生于导电流体中的电极。导电流体中两个具有电势差的电极通入高压脉冲电流,这两个具有电势差的电极上距离最近的两个点之间会产生高温电弧。高温电弧在形成冲击波的同时,会产生大量的热量并形成较强的机械冲击力。高温电弧的热量能使电极上产生冲击波的这两个位置发生熔融并形成烧蚀物。The electrohydraulic shock wave is generated by electrodes in a conductive fluid. When a high-voltage pulse current is passed through two electrodes with a potential difference in a conductive fluid, a high-temperature arc will be generated between the two closest points on the two electrodes with a potential difference. While forming a shock wave, the high-temperature arc will generate a large amount of heat and form a strong mechanical impact force. The heat of the high-temperature arc can cause the two locations on the electrode where the shock wave is generated to melt and form ablation.
目前的冲击波导管,用于使冠脉或外周血管中的钙化病变组织松解或产生裂痕,进而利用球囊的充胀进行扩张,从而缓解血管的狭窄程度或便于后续的治疗。冲击波导管已经上市推广,其安全性和有效性得到了充分验证。然而,对于无法或者不便进行扩张的部位(例如人体的二尖瓣和主动脉瓣)的硬化组织(例如钙化病变组织),现有的冲击波球囊导管尚无法实现治疗。Current shock wave catheters are used to loosen or crack calcified diseased tissue in coronary or peripheral blood vessels, and then expand them by inflating the balloon, thereby alleviating the stenosis of the blood vessels or facilitating subsequent treatment. Shock wave catheters have been marketed and their safety and effectiveness have been fully verified. However, existing shock wave balloon catheters cannot achieve treatment for hardened tissue (such as calcified diseased tissue) in areas that cannot or are inconvenient to expand (such as the mitral valve and aortic valve of the human body).
发明内容Summary of the invention
有鉴于此,本发明提供一种多头冲击波电极结构及冲击波球囊导管,旨在通过多个放电单元同时释放冲击波,利用冲击波能量的叠加实现较大的冲击波能量,并解决了伴随较大的冲击波能量形成的较大的机械冲击力对电极结构的破坏问题,从而解决现有技术无法使用冲击波能量治疗无法或者不便进行扩张的部位的硬化组织的问题,实现无需借助扩张、仅使用冲击波能量来治疗无法或者不便进行扩张的部位的硬化组织的目的,使这些硬化组织软化、恢复部分组织功能。In view of this, the present invention provides a multi-head shock wave electrode structure and a shock wave balloon catheter, which are intended to release shock waves simultaneously through multiple discharge units, utilize the superposition of shock wave energy to achieve greater shock wave energy, and solve the problem of damage to the electrode structure caused by the greater mechanical impact force formed with the greater shock wave energy, thereby solving the problem that the prior art cannot use shock wave energy to treat hardened tissue in a part that cannot or is inconvenient to expand, and achieve the purpose of using only shock wave energy to treat hardened tissue in a part that cannot or is inconvenient to expand without the help of expansion, so as to soften these hardened tissues and restore some tissue functions.
本发明实施例提供一种多头冲击波电极结构,包括至少两个放电单元;每个放电单元都包括间隔设置且延伸方向相同的一个发射电极及一个对应的中间电极,该发射电极一一对应地间隔套设于该中间电极内;所有的中间电极相互电气连接;当所有中间电极的放电端面和所有发射电极的放电端面均位于导电流体内且在任意两个放电单元的发射电极之间形成电势差时,这两个放电单元的发射电极的放电端面与对应的中间电极的放电端面之间同时引发冲击波。An embodiment of the present invention provides a multi-head shock wave electrode structure, comprising at least two discharge units; each discharge unit comprises an emitting electrode and a corresponding intermediate electrode which are arranged at intervals and have the same extension direction, and the emitting electrodes are arranged in the intermediate electrode at intervals corresponding to each other; all the intermediate electrodes are electrically connected to each other; when the discharge end surfaces of all the intermediate electrodes and the discharge end surfaces of all the emitting electrodes are located in a conductive fluid and a potential difference is formed between the emitting electrodes of any two discharge units, shock waves are simultaneously generated between the discharge end surfaces of the emitting electrodes of the two discharge units and the discharge end surfaces of the corresponding intermediate electrodes.
本发明还提供一种冲击波球囊导管,包括如上所述的多头冲击波电极结构、管本体和能充填导电流体的膨胀元件;膨胀元件密封连接于管本体的远端,所述多头冲击波电极结构的所有发射电极的放电端面和所有中间电极的放电端面均位于膨胀元件内;当膨胀元件内充填有导电流体且在所述多头冲击波电极结构的任意两个发射电极之间形成电势差时,形成电势差的两个发射电极的放电端面与各自对应的中间电极的放电端面之间同时引发冲击波。The present invention also provides a shock wave balloon catheter, comprising the multi-head shock wave electrode structure as described above, a tube body and an expansion element capable of being filled with a conductive fluid; the expansion element is sealed and connected to the distal end of the tube body, and the discharge end faces of all the emitting electrodes and the discharge end faces of all the intermediate electrodes of the multi-head shock wave electrode structure are located in the expansion element; when the expansion element is filled with a conductive fluid and a potential difference is formed between any two emitting electrodes of the multi-head shock wave electrode structure, shock waves are simultaneously triggered between the discharge end faces of the two emitting electrodes forming the potential difference and the discharge end faces of the corresponding intermediate electrodes.
与现有技术相比,本说明书实施例采用的上述至少一个技术方案能够达到的有益效果至少包括:在实现单次有效放电击穿形成较大冲击波能量的同时,解决了伴随较大的冲击波能量形成的较大的机械冲击力对电极结构的破坏问题,从而解决现有技术无法使用冲击波能量治疗无法或者不便进行扩张的部位的硬化组织的问题,实现无需借助扩张、仅使用冲击波能量来治疗无法或者不便进行扩张的部位的硬化组织的目的,使这些硬化组织软化、恢复部分组织功能。同时,本申请的多头冲击波电极结构还具有较多的有效冲击波引发次数,较长的使用寿命。Compared with the prior art, the beneficial effects that can be achieved by at least one of the above technical solutions adopted in the embodiments of this specification include at least: while achieving a single effective discharge breakdown to form a large shock wave energy, the problem of damage to the electrode structure caused by the large mechanical impact force formed by the large shock wave energy is solved, thereby solving the problem that the prior art cannot use shock wave energy to treat hardened tissues in parts that cannot or are inconvenient to expand, and achieving the purpose of using only shock wave energy to treat hardened tissues in parts that cannot or are inconvenient to expand without the help of expansion, so that these hardened tissues are softened and some tissue functions are restored. At the same time, the multi-head shock wave electrode structure of the present application also has a large number of effective shock wave initiation times and a long service life.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
为了更清楚地说明本申请实施例的技术方案,下面将对实施例中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本申请的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其它的附图。In order to more clearly illustrate the technical solutions of the embodiments of the present application, the drawings required for use in the embodiments will be briefly introduced below. Obviously, the drawings described below are only some embodiments of the present application. For ordinary technicians in this field, other drawings can be obtained based on these drawings without paying creative work.
图1是本申请的多头冲击波电极结构的第一个具体实施例的俯视结构示意图;FIG1 is a schematic diagram of a top view of a first specific embodiment of a multi-head shock wave electrode structure of the present application;
图2是本申请的多头冲击波电极结构的第一个具体实施例的另一个俯视结构示意图;FIG2 is another schematic top view of the structure of the first specific embodiment of the multi-head shock wave electrode structure of the present application;
图3是本申请的多头冲击波电极结构的第二个具体实施例的立体结构示意图;FIG3 is a schematic diagram of the three-dimensional structure of a second specific embodiment of the multi-head shock wave electrode structure of the present application;
图4是本申请的多头冲击波电极结构的第二个具体实施例的俯视结构示意图;FIG4 is a schematic diagram of a top view of a second specific embodiment of a multi-head shock wave electrode structure of the present application;
图5是本申请的多头冲击波电极结构的第三个具体实施例的立体结构示意图;FIG5 is a schematic diagram of the three-dimensional structure of a third specific embodiment of the multi-head shock wave electrode structure of the present application;
图6是本申请的多头冲击波电极结构的第四个具体实施例的立体结构示意图;FIG6 is a schematic diagram of the three-dimensional structure of a fourth specific embodiment of the multi-head shock wave electrode structure of the present application;
图7是本申请的多头冲击波电极结构的第四个具体实施例的俯视结构示意图;FIG7 is a schematic top view of the structure of the fourth specific embodiment of the multi-head shock wave electrode structure of the present application;
图8是图7的B-B剖视示意图。FIG8 is a schematic cross-sectional view taken along line B-B of FIG7 .
图中附图标记:Reference numerals in the figures:
1、第一发射电极;2、第一中间电极;3、第二发射电极;4、第二中间电极;5、第一电极主体;6、第一绝缘部;7、第二绝缘部;8、第二电极主体;9、第一圆形贯通腔;10、第二圆形贯通腔;11、第五贯通腔体;12、第三发射电极;13、第三中间电极;14、第四发射电极;15、第四中间电极;16、第五发射电极;17、第五中间电极;18、第三电极主体;19、第三绝缘部;20、第四绝缘部;21、第五绝缘部;22、第六贯通腔体。1. First emitting electrode; 2. First intermediate electrode; 3. Second emitting electrode; 4. Second intermediate electrode; 5. First electrode body; 6. First insulating portion; 7. Second insulating portion; 8. Second electrode body; 9. First circular through cavity; 10. Second circular through cavity; 11. Fifth through cavity; 12. Third emitting electrode; 13. Third intermediate electrode; 14. Fourth emitting electrode; 15. Fourth intermediate electrode; 16. Fifth emitting electrode; 17. Fifth intermediate electrode; 18. Third electrode body; 19. Third insulating portion; 20. Fourth insulating portion; 21. Fifth insulating portion; 22. Sixth through cavity.
具体实施方式DETAILED DESCRIPTION
下面结合附图对本申请实施例进行详细描述。The embodiments of the present application are described in detail below with reference to the accompanying drawings.
以下通过特定的具体实例说明本申请的实施方式,本领域技术人员可由本说明书所揭露的内容轻易地了解本申请的其他优点与功效。显然,所描述的实施例仅仅是本申请一部分实施例,而不是全部的实施例。本申请还可以通过另外不同的具体实施方式加以实施或应用,本说明书中的各项细节也可以基于不同观点与应用,在没有背离本申请的精神下进行各种修饰或改变。需说明的是,在不冲突的情况下,以下实施例及实施例中的特征可以相互组合。基于本申请中的实施例,本领域普通技术人员在没有作出创造性劳动前提下所获得的所有其他实施例,都属于本申请保护的范围。The following describes the implementation methods of the present application through specific specific examples, and those skilled in the art can easily understand other advantages and effects of the present application from the contents disclosed in this specification. Obviously, the described embodiments are only a part of the embodiments of the present application, rather than all the embodiments. The present application can also be implemented or applied through other different specific implementation methods, and the details in this specification can also be modified or changed in various ways based on different viewpoints and applications without departing from the spirit of the present application. It should be noted that, in the absence of conflict, the following embodiments and the features in the embodiments can be combined with each other. Based on the embodiments in the present application, all other embodiments obtained by ordinary technicians in the field without making creative work belong to the scope of protection of the present application.
由于现有技术的冲击波球囊导管仅用于在管状(例如冠脉和外周血管)结构的待处理组织上形成裂痕,所以,冲击波发生装置设置在冲击波球囊导管的侧壁且极易紧贴待处理组织,冲击波能量的利用率较高,因此,单次能量较低的冲击波便可实现在血管的待处理组织上形成裂痕。然而,对于无法或者不便进行扩张的部位(例如人体的二尖瓣和主动脉瓣)的硬化组织(例如钙化病变组织),现有的冲击波球囊导管提供的冲击波能量过小,无法实现治疗作用。当使用现有的冲击波球囊导管尝试实现较大的冲击波能量时,伴随较大的冲击波能量而产生的热能使冲击波球囊导管很快便失效于电极的熔融烧蚀和绝缘层的融化裂解。本申请的发明人在实现大能量冲击波的过程中发现,伴随大能量冲击波而形成的机械冲击力,对冲击波发生装置的机械可靠性有非常大的挑战,甚至能够使电极和绝缘层相互移位,使冲击波球囊导管失效,仍然无法实现对于无法或者不便进行扩张的部位的治疗。为此,本申请的多头冲击波电极结构,旨在通过多个放电单元同时释放冲击波,利用多个冲击波能量在空间中相互叠加来实现较大的冲击波能量,彻底避免了伴随较大的冲击波能量而产生的较大的机械冲击力对电极结构的破坏,从而获得更高的累积冲击波能量,实现无需借助扩张、仅使用冲击波能量来治疗无法或者不便进行扩张的部位的硬化组织的目的,使这些硬化组织软化、恢复部分组织功能,解决了病变部位的硬化组织既无法使用现有技术的冲击波球囊导管进行治疗、也无法使用现有技术的冲击波球囊导管配合扩张器械进行治疗的问题。Since the shock wave balloon catheter of the prior art is only used to form cracks on the tissue to be treated of a tubular structure (such as coronary arteries and peripheral blood vessels), the shock wave generating device is arranged on the side wall of the shock wave balloon catheter and is very easy to be close to the tissue to be treated, and the utilization rate of the shock wave energy is high. Therefore, a single shock wave with low energy can form cracks on the tissue to be treated of the blood vessel. However, for hardened tissue (such as calcified lesion tissue) in parts that cannot or are inconvenient to expand (such as the mitral valve and aortic valve of the human body), the shock wave energy provided by the existing shock wave balloon catheter is too small to achieve a therapeutic effect. When using the existing shock wave balloon catheter to try to achieve a larger shock wave energy, the heat energy generated by the larger shock wave energy causes the shock wave balloon catheter to quickly fail due to the melting ablation of the electrode and the melting and cracking of the insulation layer. The inventors of the present application found in the process of realizing high-energy shock waves that the mechanical impact force generated by the high-energy shock waves poses a great challenge to the mechanical reliability of the shock wave generating device, and can even cause the electrode and the insulating layer to shift relative to each other, causing the shock wave balloon catheter to fail, and still cannot achieve the treatment of the part that cannot or is inconvenient to expand. To this end, the multi-head shock wave electrode structure of the present application is intended to release shock waves through multiple discharge units at the same time, and use multiple shock wave energies to superimpose each other in space to achieve a larger shock wave energy, completely avoiding the damage to the electrode structure caused by the larger mechanical impact force generated by the larger shock wave energy, thereby obtaining a higher cumulative shock wave energy, achieving the purpose of using only shock wave energy to treat the hardened tissue of the part that cannot or is inconvenient to expand without the help of expansion, so that these hardened tissues are softened and some tissue functions are restored, solving the problem that the hardened tissue of the lesion part cannot be treated by the shock wave balloon catheter of the prior art, nor can it be treated by the shock wave balloon catheter of the prior art in combination with the expansion device.
在本申请的描述中,用“放电单元”来代替冲击波电极,以更清楚地阐述本申请的实施例。“远端”是指远离操作者的一端,“近端”是指临近操作者的一端。单次冲击波,是指一个放电单元的单次放电击穿所释放出的冲击波。单次能量,是指单次冲击波所释放的冲击波能量。有效冲击波,是指对待处理组织具有治疗作用的单次冲击波。有效放电击穿,是指能形成有效冲击波的放电单元之间的放电击穿。作用距离,是指有效冲击波的发生位置与待处理组织之间的距离。使用寿命,是指冲击波电极结构能够释放的有效冲击波的总次数。累积冲击波能量是指在冲击波电极结构能够释放出的所有有效冲击波所具有的单次能量的总和。放电距离,是指同一个放电单元中的发射电极和中间电极之间的电气间隙(发射电极和中间电极之间仅通过空气绝缘时)或者爬电距离(发射电极和中间电极之间存在影响电气间隙的绝缘体时)。当放电单元单次放电击穿时释放的冲击波能量足够大且作用距离足够近时,才能够对病变更严重的待处理组织具有治疗作用,该次放电击穿才会被认为是有效放电击穿。一次有效放电击穿释放的冲击波能量越大,伴随冲击波产生的热量越多、机械冲击力越大。In the description of the present application, "discharge unit" is used to replace the shock wave electrode to more clearly illustrate the embodiments of the present application. "Distal end" refers to the end away from the operator, and "proximal end" refers to the end close to the operator. A single shock wave refers to a shock wave released by a single discharge breakdown of a discharge unit. Single energy refers to the shock wave energy released by a single shock wave. An effective shock wave refers to a single shock wave that has a therapeutic effect on the treated tissue. An effective discharge breakdown refers to a discharge breakdown between discharge units that can form an effective shock wave. The effective distance refers to the distance between the location where the effective shock wave occurs and the tissue to be treated. The service life refers to the total number of effective shock waves that can be released by the shock wave electrode structure. The cumulative shock wave energy refers to the sum of the single energies of all effective shock waves that can be released by the shock wave electrode structure. The discharge distance refers to the electrical gap between the emitting electrode and the intermediate electrode in the same discharge unit (when the emitting electrode and the intermediate electrode are only insulated by air) or the creepage distance (when there is an insulator between the emitting electrode and the intermediate electrode that affects the electrical gap). When the shock wave energy released by a single discharge breakdown of the discharge unit is large enough and the action distance is close enough, it can have a therapeutic effect on the more seriously diseased tissue to be treated, and the discharge breakdown will be considered an effective discharge breakdown. The greater the shock wave energy released by an effective discharge breakdown, the more heat and mechanical impact force generated by the shock wave.
介入类医疗器械应用于人体时,常常受限于治疗部位的生理尺寸。因此,本申请的过头冲击波电极结构的横截面的面积不能过大,否则,本申请的冲击波球囊导管将无法顺利送至治疗部位。同时,为了实现治疗无法或者不便进行扩张的部位的硬化组织的目的,本申请的多头冲击波电极结构又需要在电极轴向向前的方向上实现较大的冲击波能量。When interventional medical devices are applied to the human body, they are often limited by the physiological size of the treatment site. Therefore, the cross-sectional area of the over-the-head shock wave electrode structure of the present application cannot be too large, otherwise, the shock wave balloon catheter of the present application will not be able to be smoothly delivered to the treatment site. At the same time, in order to achieve the purpose of treating hardened tissue in a site that cannot or is inconvenient to expand, the multi-head shock wave electrode structure of the present application needs to achieve a larger shock wave energy in the axial forward direction of the electrode.
本发明实施例提供了一种多头冲击波电极结构,至少两个放电单元;每个放电单元都包括间隔设置且延伸方向相同的一个发射电极及一个对应的中间电极,该发射电极一一对应地间隔套设于该中间电极内;所有的中间电极相互电气连接;当所有中间电极的放电端面和所有发射电极的放电端面均位于导电流体内且在任意两个放电单元的发射电极之间形成电势差时,这两个放电单元的发射电极的放电端面与对应的中间电极的放电端面之间同时引发冲击波。The embodiment of the present invention provides a multi-head shock wave electrode structure, at least two discharge units; each discharge unit includes an emitting electrode and a corresponding intermediate electrode which are arranged at intervals and have the same extension direction, and the emitting electrodes are arranged in the intermediate electrode at intervals corresponding to each other; all the intermediate electrodes are electrically connected to each other; when the discharge end surfaces of all the intermediate electrodes and the discharge end surfaces of all the emitting electrodes are located in a conductive fluid and a potential difference is formed between the emitting electrodes of any two discharge units, shock waves are simultaneously generated between the discharge end surfaces of the emitting electrodes of the two discharge units and the discharge end surfaces of the corresponding intermediate electrodes.
其中,“间隔设置且延伸方向相同”的发射电极和中间电极,仅指发射电极和中间电极均是在近端和远端之间延伸,无需中间电极的延伸方向与发射电极的延伸方向平行。发射电极和对应的中间电极在延伸方向上的侧面互相绝缘,且绝缘强度值大于施加电压值;发射电极的放电端面和对应的中间电极的放电端面之间为非绝缘。由于发射电极一一对应地间隔套设于对应的中间电极内,如此,发射电极的放电端面和对应的中间电极的放电端面之间的电气距离为发射电极与中间电极之间最短的电气距离。所以,当所有中间电极的放电端面和所有发射电极的放电端面均位于导电流体内且在任意两个放电单元的发射电极之间形成电势差时,属于同一个放电单元的发射电极和对应的中间电极之间为最短的电气距离,因此,这两个放电单元的发射电极的放电端面与对应的中间电极的放电端面之间同时引发冲击波,即同时形成两个冲击波,这两个冲击波的单次能量在空间中的相互叠加,构成了单次有效放电击穿时所释放的冲击波能量,实现了单次有效放电击穿能释放出较大的冲击波能量。由于每一个冲击波的单次能量都大概是这个较大的冲击波能量的一半,所以每一个冲击波带来的机械冲击力也相应削弱了一半,同时,由于一个放电单元和另一个放电单元之间的空间间隔,这个放电单元所释放的冲击波带来的机械冲击力对另一个放电单元的影响被大大削弱,由此,本申请的多头冲击波电极结构在实现单次有效放电击穿形成较大冲击波能量的同时,解决了伴随较大的冲击波能量形成的较大的机械冲击力对电极结构的破坏问题,从而解决现有技术无法使用冲击波能量治疗无法或者不便进行扩张的部位的硬化组织的问题,实现无需借助扩张、仅使用冲击波能量来治疗无法或者不便进行扩张的部位的硬化组织的目的,使这些硬化组织软化、恢复部分组织功能。除此以外,由于发射电极间隔地套设于对应的中间电极内,所以在实施电压和发射电极的烧蚀允许的情况下,发射电极能够和对应的中间电极的整个内周之间放电击穿释放冲击波,有效增加了本申请的多头冲击波电极结构能够引发的有效冲击波的次数,增长了本申请的多头冲击波电极结构的使用寿命。Among them, the emitting electrode and the intermediate electrode "arranged at intervals and extending in the same direction" only refer to that both the emitting electrode and the intermediate electrode extend between the proximal end and the distal end, and it is not necessary for the extension direction of the intermediate electrode to be parallel to the extension direction of the emitting electrode. The lateral sides of the emitting electrode and the corresponding intermediate electrode in the extension direction are insulated from each other, and the insulation strength value is greater than the applied voltage value; the discharge end face of the emitting electrode and the discharge end face of the corresponding intermediate electrode are non-insulated. Since the emitting electrodes are spaced and sleeved in the corresponding intermediate electrodes one by one, the electrical distance between the discharge end face of the emitting electrode and the discharge end face of the corresponding intermediate electrode is the shortest electrical distance between the emitting electrode and the intermediate electrode. Therefore, when the discharge end surfaces of all the intermediate electrodes and the discharge end surfaces of all the emitting electrodes are located in the conductive fluid and a potential difference is formed between the emitting electrodes of any two discharge units, the electrical distance between the emitting electrode and the corresponding intermediate electrode belonging to the same discharge unit is the shortest. Therefore, shock waves are simultaneously induced between the discharge end surfaces of the emitting electrodes of the two discharge units and the discharge end surfaces of the corresponding intermediate electrodes, that is, two shock waves are simultaneously formed. The single energies of the two shock waves are superimposed on each other in space, constituting the shock wave energy released during a single effective discharge breakdown, thereby achieving a single effective discharge breakdown that can release a larger shock wave energy. Since the single energy of each shock wave is approximately half of the energy of the larger shock wave, the mechanical impact force brought by each shock wave is also weakened by half accordingly. At the same time, due to the spatial interval between one discharge unit and another discharge unit, the influence of the mechanical impact force brought by the shock wave released by this discharge unit on the other discharge unit is greatly weakened. Therefore, the multi-head shock wave electrode structure of the present application solves the problem of damage to the electrode structure caused by the large mechanical impact force formed by the large shock wave energy while realizing a single effective discharge breakdown to form a large shock wave energy, thereby solving the problem that the prior art cannot use shock wave energy to treat hardened tissues in parts that cannot or are inconvenient to expand, and achieves the purpose of using only shock wave energy to treat hardened tissues in parts that cannot or are inconvenient to expand without the help of expansion, so as to soften these hardened tissues and restore some tissue functions. In addition, since the emitting electrodes are arranged in the corresponding intermediate electrodes at intervals, when the implementation voltage and the ablation of the emitting electrodes allow, the emitting electrodes can discharge and break down between the entire inner circumference of the corresponding intermediate electrodes to release shock waves, which effectively increases the number of effective shock waves that can be generated by the multi-head shock wave electrode structure of the present application and increases the service life of the multi-head shock wave electrode structure of the present application.
在一种实施方式中,本申请的多头冲击波电极结构包括由绝缘材料制成的主体结构;“所有的中间电极相互电气连接”,可以是通过所有的中间电极相互接触来实现,也可以是,所有的中间电极两两间隔设置且电气连接。在中间电极两两间隔设置时,若相邻两个中间电极之间的间距非常小,那么这两个中间电极在电势差很小的情况下就是放电击穿,放电击穿后的两个中间电极,等效于导线连接的状态。当所有中间电极的放电端面和所有发射电极的放电端面均位于导电流体内且在任意两个放电单元的发射电极之间形成电势差时,这两个发射电极的放电端面与对应的中间电极的放电端面之间同时引发冲击波。各放电单元的电气距离为各发射电极的放电端面与各自对应的中间电极的放电端面之间的最短距离。In one embodiment, the multi-head shock wave electrode structure of the present application includes a main structure made of insulating material; "all the intermediate electrodes are electrically connected to each other" can be achieved by all the intermediate electrodes being in contact with each other, or all the intermediate electrodes are arranged in pairs and electrically connected. When the intermediate electrodes are arranged in pairs, if the spacing between two adjacent intermediate electrodes is very small, then the two intermediate electrodes are discharged and broken down when the potential difference is very small, and the two intermediate electrodes after the discharge breakdown are equivalent to the state of being connected by wires. When the discharge end faces of all the intermediate electrodes and the discharge end faces of all the emitting electrodes are located in the conductive fluid and a potential difference is formed between the emitting electrodes of any two discharge units, shock waves are simultaneously triggered between the discharge end faces of the two emitting electrodes and the discharge end faces of the corresponding intermediate electrodes. The electrical distance of each discharge unit is the shortest distance between the discharge end faces of each emitting electrode and the discharge end faces of the corresponding intermediate electrodes.
在另一种实施方式中,本申请的多头冲击波电极结构可以包括由导电材料制成的电极主体,这个电极主体上开设至少两个贯通腔,贯通腔的延伸方向与发射电极的延伸方向相同,发射电极一一对应地套设于贯通腔内。本领域技术人员应当可以理解到,这里的延伸方向相同,也仅指贯通腔和发射电极均是在近端和远端之间延伸,无需贯通腔的延伸方向与发射电极的延伸方向平行。即所有的中间电极为一体结构并构成这个电极主体,发射电极与对应的贯通腔的内腔侧壁互相绝缘,绝缘强度值大于施加电压值;发射电极的放电端面与贯通腔的放电端面(即这个对应的贯通腔与电极主体的交界面)之间为非绝缘。当所有贯通腔的放电端面和所有发射电极的放电端面均位于导电流体内且在任意两个放电单元的发射电极之间形成电势差时,这两个放电单元的发射电极的放电端面与对应的贯通腔的放电端面之间同时引发冲击波。各放电单元的电气距离为各发射电极的放电端面与各自对应的贯通腔的放电端面之间的最短距离。In another embodiment, the multi-head shock wave electrode structure of the present application may include an electrode body made of a conductive material, at least two through cavities are provided on the electrode body, the extension direction of the through cavity is the same as the extension direction of the emitting electrode, and the emitting electrode is sleeved in the through cavity one by one. Those skilled in the art should understand that the same extension direction here only refers to that the through cavity and the emitting electrode both extend between the proximal end and the distal end, and it is not necessary for the extension direction of the through cavity to be parallel to the extension direction of the emitting electrode. That is, all the intermediate electrodes are an integrated structure and constitute this electrode body, the emitting electrode and the inner cavity side wall of the corresponding through cavity are insulated from each other, and the insulation strength value is greater than the applied voltage value; the discharge end face of the emitting electrode and the discharge end face of the through cavity (that is, the interface between the corresponding through cavity and the electrode body) are non-insulated. When the discharge end faces of all through cavities and the discharge end faces of all emitting electrodes are located in a conductive fluid and a potential difference is formed between the emitting electrodes of any two discharge units, shock waves are simultaneously triggered between the discharge end faces of the emitting electrodes of the two discharge units and the discharge end faces of the corresponding through cavities. The electrical distance of each discharge unit is the shortest distance between the discharge end surface of each emitter electrode and the discharge end surface of the corresponding through cavity.
冲击波为球形波,为了获得冲击波在空间中的传播范围更广,优选发射电极的放电端面和与该发射电极相对应的中间电极的放电端面位于同一平面或同一圆弧面,由此,形成于发射电极的放电端面和与该发射电极相对应的中间电极的放电端面之间的冲击波能够基于该平面在180°的范围内进行传播,获得更大的冲击波能量覆盖范围。The shock wave is a spherical wave. In order to obtain a wider propagation range of the shock wave in space, it is preferred that the discharge end face of the emitting electrode and the discharge end face of the intermediate electrode corresponding to the emitting electrode are located in the same plane or the same arc surface. Thus, the shock wave formed between the discharge end face of the emitting electrode and the discharge end face of the intermediate electrode corresponding to the emitting electrode can propagate within a range of 180° based on the plane, thereby obtaining a larger shock wave energy coverage range.
由于冲击波的单次能量与发射电极和中间电极之间的放电距离呈正增长关系,优选地,任一发射电极与其对应的中间电极均匀间隔设置,以在单个放电单元释放冲击波的过程中,单次能量基本均匀。同样优选地,任一发射电极与其对应的中间电极之间的间隔距离相等,以在所有放电单元释放冲击波的过程中,所获得的两个冲击波的单次能量都基本均匀,从而使冲击波能量在空间中的分布的均匀度相对较高,获得相对均匀的治疗效果。Since the single energy of the shock wave is in a positive growth relationship with the discharge distance between the emitting electrode and the middle electrode, preferably, any emitting electrode and its corresponding middle electrode are evenly spaced, so that in the process of releasing the shock wave in a single discharge unit, the single energy is basically uniform. Similarly, preferably, the spacing distance between any emitting electrode and its corresponding middle electrode is equal, so that in the process of releasing the shock wave in all discharge units, the single energy of the two shock waves obtained is basically uniform, so that the uniformity of the distribution of the shock wave energy in space is relatively high, and a relatively uniform treatment effect is obtained.
本发明人在本申请中还提出在任一发射电极与其对应的中间电极之间填充设置有由无机固体绝缘材料制成的绝缘部,绝缘部的放电端面与中间电极的放电端面位于同一平面或同一圆弧面。由于无机固体绝缘材料的热传导率、熔点且抗冲击强度都高于现有技术使用的高分子绝缘材料,因此,由无机固体绝缘材料制成的绝缘部在伴随冲击波形成的热量的作用下产生的熔化物极少,也不会产生大量的熔化物和分子结构未知的裂解物,彻底解决了现有冲击波电极使用高分子绝缘材料会使冲击波电极的放电条件迅速发生较大改变从而导致冲击波电极失效无法继续放电的问题。特别是,当发射电极的放电端面、与该发射电极相对应的中间电极的放电端面和填充于该发射电极和该中间电极之间的绝缘部位于同一平面或同一圆弧面时,伴随冲击波的形成所产生的机械冲击力,发射电极和中间电极在放电击穿过程中由于烧蚀而产生的熔融物和绝缘部的熔化物会在被该平面反射的冲击力的作用下被导电流体带走,从而使本申请的多头冲击波电极结构具有自清洁的功能,以避免发射电极和中间电极的熔融物以及绝缘部的熔化物的堆积对有效放电击穿产生较大的负面影响,彻底避免本发明实施例由此而失效。其中,无机固体绝缘材料包括氧化物陶瓷、矿物质、玻璃和石英,优选为单斜晶相的氧化锆、四方晶相且稳定剂为氧化铱的氧化锆或者立方晶相且稳定剂为氧化铱的氧化锆。The inventors of the present invention also propose in the present application that an insulating part made of an inorganic solid insulating material is filled between any emitting electrode and its corresponding intermediate electrode, and the discharge end face of the insulating part and the discharge end face of the intermediate electrode are located in the same plane or the same arc surface. Since the thermal conductivity, melting point and impact strength of the inorganic solid insulating material are higher than those of the polymer insulating material used in the prior art, the insulating part made of the inorganic solid insulating material produces very little melt under the action of the heat generated by the shock wave, and will not produce a large amount of melt and cracked products with unknown molecular structure, which completely solves the problem that the use of polymer insulating materials in the existing shock wave electrode will cause the discharge conditions of the shock wave electrode to change rapidly and significantly, thereby causing the shock wave electrode to fail and be unable to continue to discharge. In particular, when the discharge end face of the emitter electrode, the discharge end face of the intermediate electrode corresponding to the emitter electrode, and the insulating part filled between the emitter electrode and the intermediate electrode are located in the same plane or the same arc surface, the mechanical impact force generated by the formation of the shock wave, the melt produced by the ablation of the emitter electrode and the intermediate electrode during the discharge breakdown process and the melt of the insulating part will be carried away by the conductive fluid under the action of the impact force reflected by the plane, so that the multi-head shock wave electrode structure of the present application has a self-cleaning function, so as to avoid the accumulation of the melt of the emitter electrode and the intermediate electrode and the melt of the insulating part from having a greater negative impact on the effective discharge breakdown, and completely avoid the failure of the embodiment of the present invention. Among them, the inorganic solid insulating material includes oxide ceramics, minerals, glass and quartz, preferably monoclinic zirconium oxide, tetragonal zirconium oxide with iridium oxide as the stabilizer, or cubic zirconium oxide with iridium oxide as the stabilizer.
本申请的多头冲击波电极结构还可以包括至少两个与发射电极的延伸方向相同的第一贯通腔体。例如该贯通腔体位于由绝缘材料制成的主体结构或者位于由导电材料制成的电极主体;若该贯通腔体位于主体结构或电极主体的中心位置,可以用作导丝腔;若该贯通腔体临近发射电极和中间电极设置,可以用作导电流体的流入腔和导电流体的流出腔。The multi-head shock wave electrode structure of the present application may also include at least two first through cavities extending in the same direction as the transmitting electrode. For example, the through cavity is located in the main structure made of insulating material or in the electrode body made of conductive material; if the through cavity is located in the center of the main structure or the electrode body, it can be used as a guide wire cavity; if the through cavity is arranged near the transmitting electrode and the intermediate electrode, it can be used as an inflow cavity for conductive fluid and an outflow cavity for conductive fluid.
下面以放电单元设置于本申请的多头冲击波电极结构的远端面为例说明本申请的多头冲击波电极结构的结构。The structure of the multi-head shock wave electrode structure of the present application is described below by taking the example that the discharge unit is arranged on the distal end surface of the multi-head shock wave electrode structure of the present application.
在适于实用的一个实施方式中,本申请的多头冲击波电极结构,包括第一放电单元和第二放电单元;第一放电单元包括圆柱结构的第一发射电极1及均匀间隔套设在第一发射电极1的外圆周的第一中间电极2;第二放电单元包括圆柱结构的第二发射电极3及均匀间隔套设在第二发射电极3的外圆周的第二中间电极4,第二发射电极3与第一发射电极1的外径等大。In an embodiment suitable for practical use, the multi-head shock wave electrode structure of the present application includes a first discharge unit and a second discharge unit; the first discharge unit includes a first emitting electrode 1 with a cylindrical structure and a first intermediate electrode 2 evenly spaced on the outer circumference of the first emitting electrode 1; the second discharge unit includes a second emitting electrode 3 with a cylindrical structure and a second intermediate electrode 4 evenly spaced on the outer circumference of the second emitting electrode 3, and the outer diameter of the second emitting electrode 3 is the same as that of the first emitting electrode 1.
在第一个具体实施例中,第一中间电极2和第二中间电极4外设置有由绝缘材料制成的第一电极主体5,第一中间电极2与第二中间电极4为内径等大且外径等大的筒状结构。或者如图1所示,第一中间电极2和第二中间电极4相互接触。或者如图2所示,第一中间电极2和第二中间电极4之间间隔设置,且第一中间电极2和第二中间电极4之间电气连接,例如第一中间电极2和第二中间电极4通过导线连接,或者,第一中间电极2和第二中间电极4之间的间距非常小,在很小的电势差下便形成了放电击穿,等效于通过导线连接。由前述可知,当第一发射电极1和第二发射电极3为相同的导电材料时,第一放电单元和第二放电单元为相同的放电单元(放电距离、电极放电时的裸露面积及电极材料均相同)。由于第一放电单元中的电气距离和第二放电单元中的电气距离相等,所以在单次放电击穿时,第一放电单元形成的冲击波的单次能量和第二放电单元形成的冲击波的单次能量相等。在本实施例的一个优选的实施方案中,第一发射电极1和第一中间电极2之间还可以填充设置由无机固体绝缘材料制成的第一绝缘部6,第二发射电极3和第二中间电极4之间还可以填充设置由无机固体绝缘材料制成的第二绝缘部7。进一步地,第一发射电极1的放电端面、第一中间电极2的放电端面和第一绝缘部6的外表面组成第一放电单元的外表面,第二发射电极3的放电端面、第二中间电极4的放电端面和第二绝缘部7的外表面组成第二放电单元的外表面,第一放电单元的外表面和第二放电单元的外表面位于同一平面。In the first specific embodiment, a first electrode body 5 made of insulating material is arranged outside the first intermediate electrode 2 and the second intermediate electrode 4, and the first intermediate electrode 2 and the second intermediate electrode 4 are cylindrical structures with equal inner diameters and equal outer diameters. Alternatively, as shown in FIG1 , the first intermediate electrode 2 and the second intermediate electrode 4 are in contact with each other. Alternatively, as shown in FIG2 , the first intermediate electrode 2 and the second intermediate electrode 4 are arranged at intervals, and the first intermediate electrode 2 and the second intermediate electrode 4 are electrically connected, for example, the first intermediate electrode 2 and the second intermediate electrode 4 are connected by a wire, or the spacing between the first intermediate electrode 2 and the second intermediate electrode 4 is very small, and a discharge breakdown is formed under a very small potential difference, which is equivalent to being connected by a wire. As can be seen from the above, when the first emitting electrode 1 and the second emitting electrode 3 are made of the same conductive material, the first discharge unit and the second discharge unit are the same discharge unit (the discharge distance, the exposed area during electrode discharge, and the electrode material are all the same). Since the electrical distance in the first discharge unit is equal to the electrical distance in the second discharge unit, the single energy of the shock wave formed by the first discharge unit and the single energy of the shock wave formed by the second discharge unit are equal during a single discharge breakdown. In a preferred implementation of this embodiment, a first insulating portion 6 made of an inorganic solid insulating material may be filled between the first emitting electrode 1 and the first intermediate electrode 2, and a second insulating portion 7 made of an inorganic solid insulating material may be filled between the second emitting electrode 3 and the second intermediate electrode 4. Further, the discharge end surface of the first emitting electrode 1, the discharge end surface of the first intermediate electrode 2, and the outer surface of the first insulating portion 6 constitute the outer surface of the first discharge unit, the discharge end surface of the second emitting electrode 3, the discharge end surface of the second intermediate electrode 4, and the outer surface of the second insulating portion 7 constitute the outer surface of the second discharge unit, and the outer surface of the first discharge unit and the outer surface of the second discharge unit are located in the same plane.
在第二个具体实施例中,如图3至图4所示,第一中间电极2和第二中间电极4为一体结构并构成第二电极主体8,由导电材料制成的第二电极主体8上开设有内径等大的第一圆形贯通腔9和第二圆形贯通腔10,第一发射电极1均匀间隔地套设于第一圆形贯通腔9内,第二发射电极3均匀间隔地套设于第二圆形贯通腔10内。此时:第一中间电极2由第一圆形贯通腔9及第一圆形贯通腔9和第二电极主体8的外表面的交界位置构成,且第一中间电极2的放电端面即第一圆形贯通腔9和第二电极主体8的外表面的交界位置;第二中间电极4由第二圆形贯通腔10及第二圆形贯通腔10和第二电极主体8的外表面的交界位置构成,且第二中间电极4的放电端面即第二圆形贯通腔10和第二电极主体8的外表面的交界位置。同样地,第一放电单元和第二放电单元为相同的放电单元,第一放电单元形成的冲击波的单次能量和第二放电单元形成的冲击波的单次能量相等。在本实施例的一个优选的实施方案中,第一圆形贯通腔9和第二圆形贯通腔10内可以分别填充设置由无机固体绝缘材料制成的第一绝缘部和第二绝缘部。进一步地,第一发射电极1的放电端面、第一中间电极2的放电端面和第一绝缘部的外表面组成第一放电单元的外表面,第二发射电极3的放电端面、第二中间电极4的放电端面和第二绝缘部的外表面组成第二放电单元的外表面,第一放电单元的外表面和第二放电单元的外表面位于同一平面。图3和图4所示的实施例中,本申请的多头冲击波电极结构设置了两个第五贯通腔体11,以用作导电流体的流入腔和导电流体的流出腔。In the second specific embodiment, as shown in FIG3 and FIG4, the first intermediate electrode 2 and the second intermediate electrode 4 are an integral structure and constitute the second electrode body 8. The second electrode body 8 made of a conductive material is provided with a first circular through cavity 9 and a second circular through cavity 10 of equal inner diameter. The first emitting electrode 1 is evenly spaced in the first circular through cavity 9, and the second emitting electrode 3 is evenly spaced in the second circular through cavity 10. At this time: the first intermediate electrode 2 is composed of the first circular through cavity 9 and the intersection of the first circular through cavity 9 and the outer surface of the second electrode body 8, and the discharge end face of the first intermediate electrode 2 is the intersection of the first circular through cavity 9 and the outer surface of the second electrode body 8; the second intermediate electrode 4 is composed of the second circular through cavity 10 and the intersection of the second circular through cavity 10 and the outer surface of the second electrode body 8, and the discharge end face of the second intermediate electrode 4 is the intersection of the second circular through cavity 10 and the outer surface of the second electrode body 8. Similarly, the first discharge unit and the second discharge unit are the same discharge unit, and the single energy of the shock wave formed by the first discharge unit is equal to the single energy of the shock wave formed by the second discharge unit. In a preferred embodiment of this embodiment, the first circular through cavity 9 and the second circular through cavity 10 can be filled with a first insulating part and a second insulating part made of an inorganic solid insulating material, respectively. Further, the discharge end face of the first emitting electrode 1, the discharge end face of the first intermediate electrode 2 and the outer surface of the first insulating part constitute the outer surface of the first discharge unit, the discharge end face of the second emitting electrode 3, the discharge end face of the second intermediate electrode 4 and the outer surface of the second insulating part constitute the outer surface of the second discharge unit, and the outer surface of the first discharge unit and the outer surface of the second discharge unit are located in the same plane. In the embodiments shown in Figures 3 and 4, the multi-head shock wave electrode structure of the present application is provided with two fifth through cavities 11 to serve as the inflow cavity of the conductive fluid and the outflow cavity of the conductive fluid.
第三个具体实施例如图5所示,第一发射电极1的放电端面和第一中间电极2的放电端面位于同一个平面,第二发射电极3的放电端面和第二中间电极4的放电端面位于同一个平面,所述多头冲击波电极结构的远端面却不是一个平面,能有效降低所述多头冲击波电极结构的通过尺寸,且第一个放电单元和第二个放电单元释放的冲击波在空间中的分布范围更大,适用到达待处理组织的通过空间较窄且待处理组织分布范围更大的情况。The third specific embodiment is shown in Figure 5, the discharge end face of the first emitting electrode 1 and the discharge end face of the first intermediate electrode 2 are located in the same plane, the discharge end face of the second emitting electrode 3 and the discharge end face of the second intermediate electrode 4 are located in the same plane, but the distal end face of the multi-head shock wave electrode structure is not a plane, which can effectively reduce the passing size of the multi-head shock wave electrode structure, and the shock waves released by the first discharge unit and the second discharge unit have a larger distribution range in space, which is suitable for situations where the passing space to reach the tissue to be treated is narrow and the distribution range of the tissue to be treated is larger.
在第一个具体实施例、第二个具体实施例和第三个具体实施例中,第一个发射电极1和第二个发射电极3中的一个为正极时,另一个便为负极。由于正极在放电击穿时的烧蚀速度较快,所以作为正极的发射电极可以使用熔点较高的电极材料,也可以在放电过程中,通过正负极交换来延长本申请的多头冲击波电极结构的使用寿命。例如,100次冲击波,正负极做一次交换。即,前100次释放冲击波时,第一个发射电极1为正极,第二个发射电极3为负极;后100次释放冲击波时,第一个发射电极1为负极,第二个发射电极3为正极。实施正负极交换策略,即在每组固定次数释放冲击波后交替电极的极性,能够平衡烧蚀速率,延长使用寿命,提高放电效率和设备的可靠性。In the first specific embodiment, the second specific embodiment and the third specific embodiment, when one of the first emitting electrode 1 and the second emitting electrode 3 is a positive electrode, the other is a negative electrode. Since the ablation speed of the positive electrode is faster during discharge breakdown, the emitting electrode as the positive electrode can use an electrode material with a higher melting point, and the service life of the multi-head shock wave electrode structure of the present application can also be extended by exchanging the positive and negative electrodes during the discharge process. For example, the positive and negative electrodes are exchanged once for 100 shock waves. That is, when the shock waves are released for the first 100 times, the first emitting electrode 1 is the positive electrode and the second emitting electrode 3 is the negative electrode; when the shock waves are released for the last 100 times, the first emitting electrode 1 is the negative electrode and the second emitting electrode 3 is the positive electrode. Implementing a positive and negative electrode exchange strategy, that is, alternating the polarity of the electrodes after each group of fixed number of shock wave releases, can balance the ablation rate, extend the service life, and improve the discharge efficiency and reliability of the equipment.
在适于实用的另一个实施方式中,本申请的多头冲击波电极结构,包括第三放电单元、第四放电单元和第五放电单元;第三放电单元包括圆柱结构的第三发射电极12及均匀间隔套设在第三发射电极12的外圆周的第三中间电极13;第四放电单元包括圆柱结构的第四发射电极14及均匀间隔套设在第四发射电极14的外圆周的第四中间电极15;第五放电单元包括圆柱结构的第五发射电极16及均匀间隔套设在第五发射电极16的外圆周的第五中间电极17;第三发射电极12、第四发射电极14和第五发射电极16的外径等大。In another embodiment suitable for practical use, the multi-head shock wave electrode structure of the present application includes a third discharge unit, a fourth discharge unit and a fifth discharge unit; the third discharge unit includes a third emitting electrode 12 of a cylindrical structure and a third intermediate electrode 13 evenly spaced on the outer circumference of the third emitting electrode 12; the fourth discharge unit includes a fourth emitting electrode 14 of a cylindrical structure and a fourth intermediate electrode 15 evenly spaced on the outer circumference of the fourth emitting electrode 14; the fifth discharge unit includes a fifth emitting electrode 16 of a cylindrical structure and a fifth intermediate electrode 17 evenly spaced on the outer circumference of the fifth emitting electrode 16; the outer diameters of the third emitting electrode 12, the fourth emitting electrode 14 and the fifth emitting electrode 16 are equal.
在第四个具体实施例中,第三中间电极13、第四中间电极15和第五中间电极17外设置有由绝缘材料制成的第三电极主体18,第三中间电极13、第四中间电极15和第五中间电极17为内径等大且外径等大的筒状结构。可以是,第三中间电极13、第四中间电极15和第五中间电极17相互接触。也可以是,如图6至图8所示,第三中间电极13、第四中间电极15和第五中间电极17之中的任意两个均相互间隔设置且电气连接,通过导线连接或者间距非常小均可。同样地,第三放电单元、第四放电单元和第五放电单元为相同的放电单元,第三放电单元形成的冲击波的单次能量、第四放电单元形成的冲击波的单次能量和第五放电单元形成的冲击波的单次能量相等。在本实施例一个优选的实施方案中,第三发射电极12和第三中间电极13之间还可以填充设置由无机固体绝缘材料制成的第三绝缘部19,第四发射电极14和第四中间电极15之间还可以填充设置由无机固体绝缘材料制成的第四绝缘部20,第五发射电极16和第五中间电极17之间还可以填充设置由无机固体绝缘材料制成的第五绝缘部21。进一步地,第三发射电极12的放电端面、第三中间电极13的放电端面和第三绝缘部19的外表面组成第三放电单元的外表面,第四发射电极14的放电端面、第四中间电极15的放电端面和第四绝缘部20的外表面组成第四放电单元的外表面,第五发射电极16的放电端面、第五中间电极17的放电端面和第五绝缘部21的外表面组成第五放电单元的外表面,第三放电单元的外表面、第四放电单元的外表面和第五放电单元的外表面位于同一平面。还可以进一步设置有三个第六贯通腔体22。In the fourth specific embodiment, the third intermediate electrode 13, the fourth intermediate electrode 15 and the fifth intermediate electrode 17 are provided with a third electrode body 18 made of an insulating material, and the third intermediate electrode 13, the fourth intermediate electrode 15 and the fifth intermediate electrode 17 are cylindrical structures with equal inner diameters and equal outer diameters. It can be that the third intermediate electrode 13, the fourth intermediate electrode 15 and the fifth intermediate electrode 17 are in contact with each other. It can also be that, as shown in Figures 6 to 8, any two of the third intermediate electrode 13, the fourth intermediate electrode 15 and the fifth intermediate electrode 17 are spaced apart from each other and electrically connected, either by wire connection or with a very small spacing. Similarly, the third discharge unit, the fourth discharge unit and the fifth discharge unit are the same discharge unit, and the single energy of the shock wave formed by the third discharge unit, the single energy of the shock wave formed by the fourth discharge unit and the single energy of the shock wave formed by the fifth discharge unit are equal. In a preferred implementation of this embodiment, a third insulating portion 19 made of an inorganic solid insulating material may be filled between the third emitting electrode 12 and the third intermediate electrode 13, a fourth insulating portion 20 made of an inorganic solid insulating material may be filled between the fourth emitting electrode 14 and the fourth intermediate electrode 15, and a fifth insulating portion 21 made of an inorganic solid insulating material may be filled between the fifth emitting electrode 16 and the fifth intermediate electrode 17. Further, the discharge end surface of the third emitting electrode 12, the discharge end surface of the third intermediate electrode 13 and the outer surface of the third insulating portion 19 constitute the outer surface of the third discharge unit, the discharge end surface of the fourth emitting electrode 14, the discharge end surface of the fourth intermediate electrode 15 and the outer surface of the fourth insulating portion 20 constitute the outer surface of the fourth discharge unit, the discharge end surface of the fifth emitting electrode 16, the discharge end surface of the fifth intermediate electrode 17 and the outer surface of the fifth insulating portion 21 constitute the outer surface of the fifth discharge unit, and the outer surface of the third discharge unit, the outer surface of the fourth discharge unit and the outer surface of the fifth discharge unit are located in the same plane. Three sixth through cavities 22 may be further provided.
在第五个具体实施例中,第三中间电极13、第四中间电极15和第五中间电极17为一体结构并构成第四电极主体,第四电极主体上开设有半径等大的第三圆形贯通腔、第四圆形贯通腔和第五圆形贯通腔,第三发射电极12均匀间隔地套设于第三圆形贯通腔内,第四发射电极14均匀间隔地套设于第四圆形贯通腔内,第五发射电极16均匀间隔地套设于第五圆形贯通腔内。此时:第三中间电极13由第三圆形贯通腔及第三圆形贯通腔和第四电极主体的外表面的交界位置构成,且第三中间电极13的放电端面即第三圆形贯通腔和第四电极主体的外表面的交界位置;第四中间电极15由第四圆形贯通腔及第四圆形贯通腔和第四电极主体的外表面的交界位置构成,且第四中间电极15的放电端面即第四圆形贯通腔和第四电极主体的外表面的交界位置;第五中间电极17由第五圆形贯通腔及第五圆形贯通腔和第四电极主体的外表面的交界位置构成,且第五中间电极17的放电端面即第五圆形贯通腔和第四电极主体的外表面的交界位置。同样地,第三放电单元、第四放电单元和第五放电单元为相同的放电单元,第三放电单元形成的冲击波的单次能量、第四放电单元形成的冲击波的单次能量和第五放电单元形成的冲击波的单次能量相等。在本实施例的一个优选的实施方案中,第三圆形贯通腔、第四圆形贯通腔和第五圆形贯通腔内可以填充设置由无机固体绝缘材料制成绝缘部。本领域技术人员应当能够理解第三放电单元的外表面、第四放电单元的外表面和第五放电单元的外表面的构成。进一步地,第三放电单元的外表面、第四放电单元的外表面和第五放电单元的外表面位于同一平面。In the fifth specific embodiment, the third intermediate electrode 13, the fourth intermediate electrode 15 and the fifth intermediate electrode 17 are an integrated structure and constitute a fourth electrode body, and the fourth electrode body is provided with a third circular through cavity, a fourth circular through cavity and a fifth circular through cavity with equal radius, the third emitting electrode 12 is evenly spaced in the third circular through cavity, the fourth emitting electrode 14 is evenly spaced in the fourth circular through cavity, and the fifth emitting electrode 16 is evenly spaced in the fifth circular through cavity. At this time: the third intermediate electrode 13 is composed of the third circular through cavity and the intersection of the third circular through cavity and the outer surface of the fourth electrode body, and the discharge end surface of the third intermediate electrode 13 is the intersection of the third circular through cavity and the outer surface of the fourth electrode body; the fourth intermediate electrode 15 is composed of the fourth circular through cavity and the intersection of the fourth circular through cavity and the outer surface of the fourth electrode body, and the discharge end surface of the fourth intermediate electrode 15 is the intersection of the fourth circular through cavity and the outer surface of the fourth electrode body; the fifth intermediate electrode 17 is composed of the fifth circular through cavity and the intersection of the fifth circular through cavity and the outer surface of the fourth electrode body, and the discharge end surface of the fifth intermediate electrode 17 is the intersection of the fifth circular through cavity and the outer surface of the fourth electrode body. Similarly, the third discharge unit, the fourth discharge unit and the fifth discharge unit are the same discharge units, and the single energy of the shock wave formed by the third discharge unit, the single energy of the shock wave formed by the fourth discharge unit and the single energy of the shock wave formed by the fifth discharge unit are equal. In a preferred implementation of this embodiment, the third circular through cavity, the fourth circular through cavity and the fifth circular through cavity may be filled with an insulating portion made of an inorganic solid insulating material. Those skilled in the art should be able to understand the composition of the outer surface of the third discharge unit, the outer surface of the fourth discharge unit and the outer surface of the fifth discharge unit. Further, the outer surface of the third discharge unit, the outer surface of the fourth discharge unit and the outer surface of the fifth discharge unit are located in the same plane.
在第四个具体实施例和第五个具体实施例中均设置了第三发射电极13、第四发射电极15和第五发射电极17,每次选择其中两个作为放电击穿的正极和负极,并在每组固定次数释放冲击波后交替电极的极性,能够有效平衡烧蚀速率,大大延长使用寿命,有效提高放电效率和设备的可靠性。In the fourth specific embodiment and the fifth specific embodiment, a third emitting electrode 13, a fourth emitting electrode 15 and a fifth emitting electrode 17 are provided, two of which are selected each time as the positive and negative electrodes for discharge breakdown, and the polarity of the electrodes is alternated after each group of shock waves are released a fixed number of times, which can effectively balance the ablation rate, greatly extend the service life, and effectively improve the discharge efficiency and reliability of the equipment.
在前述的五个具体实施例中,发射电极都均匀间隔地套设于对应的中间电极内,所以在实施电压和发射电极的烧蚀允许的情况下,发射电极能够和对应的中间电极的整个内圆周之间放电击穿释放冲击波,有效增加了本申请的多头冲击波电极结构能够引发的有效冲击波的次数,增长了本申请的多头冲击波电极结构的使用寿命。In the aforementioned five specific embodiments, the emitting electrodes are evenly spaced within the corresponding intermediate electrodes, so when the applied voltage and the ablation of the emitting electrodes permit, the emitting electrodes can discharge and break down between the entire inner circumference of the corresponding intermediate electrodes to release shock waves, thereby effectively increasing the number of effective shock waves that can be generated by the multi-head shock wave electrode structure of the present application and increasing the service life of the multi-head shock wave electrode structure of the present application.
由上述可知,本申请的多头冲击波电极结构也适用于设置在其侧圆周面,此时,放电单元的外表面(包括发射电极的放电端面和中间电极的放电端面,也可以包括绝缘部的外表面)位于同一圆弧面。From the above, it can be seen that the multi-head shock wave electrode structure of the present application is also suitable for being arranged on its side circumferential surface. At this time, the outer surface of the discharge unit (including the discharge end surface of the emitting electrode and the discharge end surface of the intermediate electrode, and may also include the outer surface of the insulating part) is located on the same arc surface.
本发明实施例还提供了一种冲击波球囊导管,包括如上所述的多头冲击波电极结构、管本体和能充填导电流体的膨胀元件;膨胀元件密封连接于管本体的远端,所述多头冲击波电极结构的所有发射电极的放电端面和所有中间电极的放电端面均位于膨胀元件内;当膨胀元件内充填有导电流体且在所述多头冲击波电极结构的任意两个发射电极之间形成电势差时,形成电势差的两个发射电极的放电端面分别与对应的中间电极的放电端面之间同时引发冲击波。管本体包括进入人体的导管本体和其他体外部分,其他体外部分例如包括手柄、侧支以及其他的电路接口和液路接口等。The embodiment of the present invention also provides a shock wave balloon catheter, comprising the multi-head shock wave electrode structure as described above, a tube body and an expansion element capable of being filled with a conductive fluid; the expansion element is sealed and connected to the distal end of the tube body, and the discharge end faces of all the emitting electrodes and the discharge end faces of all the intermediate electrodes of the multi-head shock wave electrode structure are located in the expansion element; when the expansion element is filled with a conductive fluid and a potential difference is formed between any two emitting electrodes of the multi-head shock wave electrode structure, the discharge end faces of the two emitting electrodes forming the potential difference respectively induce shock waves simultaneously with the discharge end faces of the corresponding intermediate electrodes. The tube body includes a catheter body that enters the human body and other external parts, and the other external parts include, for example, a handle, a side branch, and other circuit interfaces and fluid circuit interfaces.
采用液电式在形成冲击波的过程中,发射电极的放电端面和中间电极的放电端面会形成小气泡,来不及处理的小气泡也会在导电流体内形成大气泡,大气泡若不及时处理,会慢慢移动至膨胀元件的内壁。放电表面堆积的小气泡会影响导电流体的导电性能,进而影响发射电极的放电端面和中间电极的放电端面之间的放电击穿。导电流体内大气泡则会在冲击波传递过程中影响冲击波的强度(冲击波能量大小)。同时,大气泡和小气泡都会使冲击波能量散射,削弱冲击波能量。为此,本申请的冲击波球囊导管进一步设置导电流体的循环系统,使导电流体在放电击穿的过程中实现流动,以通过流动的导电流体带走大气泡和小气泡。In the process of forming shock waves by using the liquid-electric method, small bubbles will be formed on the discharge end face of the emitting electrode and the discharge end face of the intermediate electrode. The small bubbles that are not handled in time will also form large bubbles in the conductive fluid. If the large bubbles are not handled in time, they will slowly move to the inner wall of the expansion element. The small bubbles accumulated on the discharge surface will affect the conductive properties of the conductive fluid, and then affect the discharge breakdown between the discharge end face of the emitting electrode and the discharge end face of the intermediate electrode. The large bubbles in the conductive fluid will affect the intensity of the shock wave (the size of the shock wave energy) during the shock wave transmission process. At the same time, both large bubbles and small bubbles will scatter the shock wave energy and weaken the shock wave energy. For this reason, the shock wave balloon catheter of the present application is further provided with a circulation system of the conductive fluid, so that the conductive fluid can flow during the discharge breakdown process, so that the large bubbles and small bubbles can be taken away by the flowing conductive fluid.
在第一个实施例中,所述多头冲击波电极结构包括至少两个第一贯通腔体,且所有第一贯通腔体的远端开口均位于膨胀元件内。位于本申请的多头冲击波电极结构的中心位置的第一贯通腔体,可以用作导丝腔。临近发射电极和中间电极设置的第一贯通腔体(例如前文的第五贯通腔体11和第六贯通腔体22),可以用作导电流体的流入腔和导电流体的流出腔。导电流体自流入腔进入并通过流出腔排出,随着导电流体的流动,能带走大气泡。由于流入腔和流出腔临近发射电极和中间电极,导电流体能冲刷发射电极的放电端面和中间电极的放电端面,能有效地带走小气泡。In the first embodiment, the multi-head shock wave electrode structure includes at least two first through cavities, and the distal openings of all the first through cavities are located in the expansion element. The first through cavity located at the center of the multi-head shock wave electrode structure of the present application can be used as a guide wire cavity. The first through cavity arranged near the emitting electrode and the intermediate electrode (such as the fifth through cavity 11 and the sixth through cavity 22 mentioned above) can be used as the inflow cavity of the conductive fluid and the outflow cavity of the conductive fluid. The conductive fluid enters from the inflow cavity and is discharged through the outflow cavity, and large bubbles can be taken away with the flow of the conductive fluid. Since the inflow cavity and the outflow cavity are close to the emitting electrode and the intermediate electrode, the conductive fluid can flush the discharge end surface of the emitting electrode and the discharge end surface of the intermediate electrode, and can effectively take away small bubbles.
在第二个实施例中,本申请的冲击波球囊导管的所述管本体开设有至少两个第二贯通腔体,且所有第二贯通腔体的远端开口均位于膨胀元件内。随着导电流体的流动,能带走大气泡和小气泡。In the second embodiment, the tube body of the shock wave balloon catheter of the present application is provided with at least two second through cavities, and the distal openings of all the second through cavities are located in the expansion element. As the conductive fluid flows, large and small bubbles can be taken away.
在第三个实施例中,所述多头冲击波电极结构包括至少一个第三贯通腔体,且所述管本体开设有至少一个第四贯通腔体,且所有第三贯通腔体的远端开口及所有第四贯通腔体的远端开口均位于膨胀元件内。位于所述多头冲击波电极结构的中心位置的第三贯通腔体,可以用作导丝腔。临近发射电极和中间电极设置的第三贯通腔体,可以用作导电流体的流入腔和导电流体的流出腔,优先用作导电流体的流入腔。第四贯通腔体可以用作导电流体的流入腔和导电流体的流出腔,优先用作导电流体的流出腔。在临近发射电极和中间电极设置的第三贯通腔体用作导电流体的流入腔、且第四贯通腔体用作导电流体的流出腔时,导电流体自流入腔进入并通过流出腔排出,导电流体会自临近发射电极和中间电极的流入腔流动至位于管本体的流出腔,有一个较长的流动距离,因此,导电流体能有效带走大气泡和小气泡。In a third embodiment, the multi-head shock wave electrode structure includes at least one third through cavity, and the tube body is provided with at least one fourth through cavity, and the distal openings of all third through cavities and the distal openings of all fourth through cavities are located in the expansion element. The third through cavity located at the center of the multi-head shock wave electrode structure can be used as a guide wire cavity. The third through cavity arranged near the transmitting electrode and the middle electrode can be used as an inflow cavity and an outflow cavity of the conductive fluid, and is preferably used as an inflow cavity of the conductive fluid. The fourth through cavity can be used as an inflow cavity and an outflow cavity of the conductive fluid, and is preferably used as an outflow cavity of the conductive fluid. When the third through cavity arranged near the transmitting electrode and the middle electrode is used as an inflow cavity of the conductive fluid, and the fourth through cavity is used as an outflow cavity of the conductive fluid, the conductive fluid enters from the inflow cavity and is discharged through the outflow cavity, and the conductive fluid flows from the inflow cavity near the transmitting electrode and the middle electrode to the outflow cavity located in the tube body, and has a longer flow distance, so the conductive fluid can effectively take away large and small bubbles.
由上述可知,本申请的多头冲击波电极结构在实现单次有效放电击穿形成较大冲击波能量的同时,解决了伴随较大的冲击波能量形成的较大的机械冲击力对电极结构的破坏问题,从而解决现有技术无法使用冲击波能量治疗无法或者不便进行扩张的部位的硬化组织的问题,实现无需借助扩张、仅使用冲击波能量来治疗无法或者不便进行扩张的部位的硬化组织的目的,使这些硬化组织软化、恢复部分组织功能。同时,本申请的多头冲击波电极结构还具有较多的有效冲击波引发次数,较长的使用寿命。As can be seen from the above, the multi-head shock wave electrode structure of the present application solves the problem of damage to the electrode structure caused by the large mechanical impact force formed by the large shock wave energy while achieving a single effective discharge breakdown to form a large shock wave energy, thereby solving the problem that the prior art cannot use shock wave energy to treat hardened tissues in parts that cannot or are inconvenient to expand, and achieves the purpose of using only shock wave energy to treat hardened tissues in parts that cannot or are inconvenient to expand without the help of expansion, so that these hardened tissues are softened and some tissue functions are restored. At the same time, the multi-head shock wave electrode structure of the present application also has a large number of effective shock wave initiation times and a long service life.
以上所述,仅为本申请的具体实施方式,但本申请的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本申请揭露的技术范围内,可轻易想到的变化或替换,都应涵盖在本申请的保护范围之内。因此,本申请的保护范围应以权利要求的保护范围为准。The above is only a specific implementation of the present application, but the protection scope of the present application is not limited thereto. Any changes or substitutions that can be easily thought of by a person skilled in the art within the technical scope disclosed in the present application should be included in the protection scope of the present application. Therefore, the protection scope of the present application shall be based on the protection scope of the claims.
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| CN104582597A (en) * | 2012-06-27 | 2015-04-29 | 冲击波医疗公司 | Shock wave balloon catheter with multiple shock wave sources |
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| CN118614986B (en) | 2025-02-07 |
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