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开放式灌注系统与冷湿系统在离体牛肝中的双极射频消融

Bipolar radiofrequency ablation in ex vivo bovine liver with the open-perfused system versus the cooled-wet system.

作者信息

Lee Jeong Min, Han Joon Koo, Kim Se Hyung, Sohn Kyu Li, Choi Seung Hong, Choi Byung Ihn

机构信息

Department of Diagnostic Radiology, Clinical Research Institute, Seoul National University Hospital, 28 Yongon-dong, Chongno-gu, Seoul, 110-744, South Korea.

出版信息

Eur Radiol. 2005 Apr;15(4):759-64. doi: 10.1007/s00330-004-2375-4. Epub 2004 Jul 10.

Abstract

The aim of this study was to investigate the efficacy of bipolar radiofrequency ablation (RFA) with the open-perfused electrode and cooled-wet electrode. Bipolar RF was applied for 20 min to the ex vivo bovine liver using either the Berchtold system with two 16-gauge open-perfused electrodes (group A, n=15) or the Radionics system with two 15-gauge cooled-wet electrodes (group B, n=15). In both groups, two electrodes were placed 3 cm apart. The ablation zone was created by the RF energy delivered together with the infusion of 5% hypertonic saline (2 ml/min). The dimension of the ablation zone, its shape and the changes in the impedance and W s of two groups during the RFA were examined and documented. The vertical diameter (Dv) along the probe, the long-axis diameter (Dl) perpendicular to the Dv in the longitudinal plane and the short-axis diameter of the ablation zone (Ds) in the transverse plane through the midpoint between the tips of two probes were measured. The mean accumulated energy output in the Radionics system was higher than in the Berchtold system (159,887.0+/-36,423 W s vs. 87,555.1+/-86,787 W s). The difference was statistically significant (P<0.05). In group A, the impedance intermittently rose to above 700 Omega during the RFA in all sessions, which led to a gradual decrease of the power output to lower than 30 W. In group B, on the other hand, the impedance did not change markedly. The mean Dv value of the coagulation necrosis in group B was significantly longer than in group A (5.0+/-0.4 cm vs. 4.3+/-0.6 cm, P<0.05). The mean Dl and Ds were 6.7+/-0.5 cm and 5.0+/-0.8 cm in group A, and 6.5+/-0.8 cm and 5.5+/-0.7 cm in group B, respectively (P>0.05). The data demonstrate that the cooled-wet electrode generates the more spherical ablation zone than the open-perfused electrode. With approximately doubled power output, the bipolar RFA with the cooled-wet electrodes induces a larger volume of tissue coagulation than with the open-perfused electrodes.

摘要

本研究旨在探讨使用开放式灌注电极和冷却湿润电极的双极射频消融(RFA)的疗效。使用带有两个16号开放式灌注电极的Berchtold系统(A组,n = 15)或带有两个15号冷却湿润电极的Radionics系统(B组,n = 15),对离体牛肝进行20分钟的双极射频消融。在两组中,两个电极相距3 cm放置。通过射频能量与5%高渗盐水(2 ml/分钟)输注一起产生消融区。检查并记录了两组在射频消融过程中消融区的尺寸、形状以及阻抗和瓦特秒的变化。测量了沿探头的垂直直径(Dv)、在纵向平面中垂直于Dv的长轴直径(Dl)以及通过两个探头尖端之间中点的横向平面中消融区的短轴直径(Ds)。Radionics系统中的平均累积能量输出高于Berchtold系统(159,887.0±36,423瓦特秒对87,555.1±86,787瓦特秒)。差异具有统计学意义(P<0.05)。在A组中,在所有疗程的射频消融过程中,阻抗间歇性地升至700Ω以上,这导致功率输出逐渐降低至低于30 W。另一方面,在B组中,阻抗没有明显变化。B组凝固性坏死的平均Dv值显著长于A组(5.0±0.4 cm对4.3±0.6 cm,P<0.05)。A组的平均Dl和Ds分别为6.7±0.5 cm和5.0±0.8 cm,B组分别为6.5±0.8 cm和5.5±0.7 cm(P>0.05)。数据表明,与开放式灌注电极相比,冷却湿润电极产生的消融区更呈球形。冷却湿润电极的双极射频消融在功率输出大约翻倍的情况下,比开放式灌注电极诱导更大体积的组织凝固。

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